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NASA

Conference

Publication

3142

Computational Structures Technology for Airframes and Propulsion Systems Compiled by Ahmed K. Noor Center

for Computational

Structures Technology University of Virginia Hampton, Virginia Jerrold

NASA

NASA

M. Housner

and James H. Statues, Jr. Langley Research Center Hampton, Virginia Dale A. Hopkins and Christos C. Chamis Lewis Research Center Cleveland,

Ohio

Proceedings of two workshops sponsored by the National Aeronautics and Space Administration, Washington, D.C., and the Center for Computational Structures Technology, University of Virginia, Hampton, Virginia, and held at Lewis Research Center, Cleveland,Ohio, June 26-27, 1991, and at Langley Research Center, Hampton, Virginia, September 4-5, 1991

National Aeronautics and Space Administration Office of Management Scientific and Technical Information Program 1992

PREFACE This document contains the proceedings of the two Workshops on Computational Structures Technology for Airframes and Propulsion Systems. The Workshops were jointly sponsored by the Center for Computational Structures Technology of the University of Virginia and NASA. The first workshop was held on June 26-27, 1991 at NASA Lewis Research Center and focused on computational technology for advanced propulsion systems. The second workshop was held on September 4-5, 1991 at NASA Langley Research Center and focused on computational technology for airframes. The attendees of the workshops came from government agencies, airframe and engine manufacturers and universities. The objectives of the workshops were to assess the status of CST in the aerospace industry, to identify the technical needs in the CST area, and to provide guidelines for focused future research leading to an enhanced capability for future national programs, such as the High-Speed Civil Transport and the National Aerospace Plane. Certain materials and products are identified in this publication in order to specify adequately the materials and products that were investigated in the research effort. In no case does such identification imply recommendations or endorsement of products by NASA nor does it imply that the materials and products are the only ones or the best ones available for the purpose. In many cases equivalent materials and products are available and would probably produce equivalent results.

Ahmed K. Noor Center for Computational University of Virginia

Structures

Technology

Jerrold M. Housner and James H. Starnes, NASA Langley Research Center Hampton, Virginia

Jr.

and Dale A. Hopkins and Christos NASA Lewis Research Center Cleveland, Ohio

C. Chamis

pF_C.EOK._G PAGE

m

BLANK

NOT

FILMED

CONTENTS °°.

PREFACE

....................................

ATTENDEES

111

..................................

vi_

INTRODUCTION

'

COMPUTATIONAL

STRUCTURES

Ahmed

K. Noor

COMPUTER

CODES

Christos

Pramote

CSM

DEVELOPED

IN INTEGRATED ....................................

AND

UNDER

ANALYSIS

WITH

AND

UVA

DEVELOPMENT

FOR

CST

AT NASA

....

LEWIS

5

43

ADAF17VE

UNSTRUCTURED 59

OF COMPUTATIONAL AT NASA LEWIS

STRUCTURES TECHNOLOGY RESEARCH CENTER ............

81

A. Hopkins

ACTIVITIES Jerrold

AT THE

NASA

LANGLEY

RESEARCH

CENTER

...........

91

M. Housner

OVERVIEW OF MECHANICS OF MATERIALS BRANCH COMPUTATIONAL STRUCTURES AREA ...................... C. C. Poe, ANALYSIS

ACTIVITIES

IN THE 121

Jr.

AND

James HIGH

CENTER

Dechaumphai

OVERVIEW ACTIVITIES

Dale

TECHNOLOGY

1

C. Chamis

PROGRESS MESHING

A BRIEF RELATED

" ..............

DESIGN

H. Stames,

SPEED

CML

Jr.

TECHNOLOGY and Charles

TRANSPORT

FOR

HIGH-SPEED

AIRCRAFT

STRUCTURES

. 137

J. Camarda .

.

.- ......................

173

R. L. McKnight STRUCTURES AEROSPACE

TECHNOLOGY PLANE

APPLICATIONS

FOR

THE

NATIONAL ...........

189

...........

209

T. E. Little m

i

LARGE

SCALE

Vipperla LIGHT

OPTIMIZATION

AN OVERVIEW

AND

MATERIALS

STRUCTURES

FOR

HIGH

SPEED

FLIGHT

.....

231

A. Thornton

MODELING

"BR_VVFLE"

K. T. Kedward, ALGORITHMIC Frank

ASTROS:

B. Venkayya

THERMAL

Earl

USING

HIGH-TEMPERATURE

R. M. McMeeking

DEVELOPMENT

COMPOSITE

STRUCTURES

......

253

and S. Janson

IN STRUCTURES

TECHNOLOGY

...........

269

Sagendorph V

PRE_ED_,r_

PAGE

BLA,"!K NOT

FILMLCD

STRUCTURAL Johnny

MECHANICS

SIMULATIONS

......................

H. Biffle

STRUCTURAL ANALYSIS FOR PRELIMINARY CIVIL TRANSPORT (HSCT) ............................. Kumar

303

DESIGN

OF HIGH

SPEED 321

G. Bhatia

APPLICATION OF INTEGRATED STRUCTURAL CIVIL TRANSPORT .................................

ANALYSIS

TO THE

HIGH

SPEED 335

C. R. Saff OVERVIEW MILITARY

OF COMPUTATIONAL STRUCTURAL AIRCRAFF ...............................

METHODS

FOR

MODERN 395

J. N. Kudva A PERSPECTIVE STRUCTURES Frank

ON TECHNICAL NEEDS IN COMPUTATIONAL TECHNOLOGY ............................

F. Abdi,

Gregory

COMPUTATIONAL PRACTICE]FUTURE Allan AIRFRAME

and Kenneth

STRUCTURES TECHNOLOGY NEEDS .........

B. Pifko LIFE

L. Savoni

and Harvey

375

J. Newell AT GRUMMAN-CURRENT ....................

395

Eidinoff

PREDICTION

............................

431

G. P. Sendeckyj PROBABILISTIC MAIN ENGINES Kevin

DESIGN APPLICATIONS .................................

FOR

THE

SPACE

TRANSPORTATION 447

O'Hara

COMPUTATIONAL STRUCTURAL ANALYSIS COMMERCIAL ENGINES ..............................

AND

ADVANCED 473

R. B. Wilson MILITARY Daniel

ENGINE

STRUCTURES

TECHNOLOGY

..........

491

E. Thomson

COMPUTATIONAL Bruce

COMPUTATIONAL

STRUCTURES

TECHNOLOGY

ENGINE/AIRFRAME

C. McClintick

vi

COUPLJ2qG

....

507

Specialty Technology

Workshops on for Airframes

Computational Structures and Propulsion Systems

Attendees Prof. Mr. Frank Abdi D/734-11-GB 13 Rockwell International 201 North Douglas Street E1 Segundo, CA 90245 (213) 922-0990; Fax (213)

Keith

Mechanical Engineering Department University of California Santa Barbara, CA 93106 (805) 893-3381; Fax (805) 893-8651 Dr. N. J. Kudva

414-0430

MS Dept. 3852-MF Northrop Aircraft Division Northrop Corporation One Northrop Avenue Hawthorne, CA 90250-3277 (213) 332-8300; Fax (213)

Dr. Kumar Bhatia Mail Stop 3T-AF Boeing Corporation P.O. Box 3707 Seattle, WA 98124 (206) 393-6993; Fax (206) 477-2345

Mr. Bruce Dr. Johnny H. Biffle Applied Mechanics Ill, Div. Sandia National Laboratory P.O. Box 5800 Albuquerque, NM 87185 (505) 844-5385; Fax (505) Dr. Chrisms

583-5170

846-9833 Mr. R. L. McKnight Mail Drop A333 General Electric Aircraft Engines P.O. Box 156301 Cincinnati, OH 45215 (513) 583-5068; Fax (513) 583-5170

Center

2,1000 Brookpark Road Cleveland, OH 44135 (216) 433-3252; Fax (216) 433-8011 Dr. Pramote Dechaumphai Mail Stop 395 NASA Langley Research Hampton, VA 23665 (804) 864-1357

332-5853

C. McClintick

Mail Drop A33A General Electric Company Highway 75 Cincinnati, OH 45215 (513) 583-5146; Fax (513)

1523

C. Chamis

Marl Stop 49-8 NASA Lewis Research

T. Kedward

Mr. James E. Newell Mail Code D/545-055-J'B 11 Rockwell International 6633 Canoga Park Canoga Park, CA 91303 (818) 773-5505; Fax (818) 773-5542

Center

Mr. Dale A. Hopkins Mail Stop 4%8 NASA Lewis Research Center 21000 Brookpark Road Cleveland, OH 44135 (216) 433-3260; Fax (216) 433-8011

Prof.

Ahmed

K. Noor

Dr. Jerrold M. Housner Mail Stop 240 NASA Langley Research Hampton, VA 23665 (804) 864-2906

Mr. Kevin T. O'Hara Mail Code D/611-055-RA02 Rockwell International 2227 Drake Avenue, Suite 45 Huntsville, AL 35805 (205) 880-4519; Fax (205) 880-4596

Center for Computational Structures Technology Mail Stop 210 NASA Langley Research Center Hampton, VA 23665 (804) 864-1978; Fax (804) 864-8089

Center

vii

Dr. Allan B. Pifko Mail StopA08-35 ResearchDepartment GrummanCorporation Bethpage,NY 11714 (516)575-1965;Fax (516)575-7716

Mr. Samuel Code RM

NASA Headquarters Washington, D.C. 20546 (202) 453-2760; Fax (202) 755-4068 Mr. Raymond B. Wilson Mail Stop 163-10 Engineering Division Pratt & Whimey 400 Main Street East Hartford, CT 06108 (203) 565-2901; Fax (203)

Mr. ClarenceC. Poe,Jr. Mail Stop 188E NASA LangleyResearchCenter Hampton,VA 23665 (804)864,3467 Dr. CharlesR. Saff Mail Code1021322 McDonnellDouglas P.O.Box 516 St. Louis,MO 63166 (314)233-8623;Fax(314)777-1171 Mr. FrankE. SagendorphIV Mail DropA333 GeneralElectricAircraftEngines P.O.Box 156301 Cincinnati,OH 45215 (513)583-5001;Fax (513)583-5170 Dr. GeorgeP. Sendeckyj WL/FIBEC Wright PattersonAir ForceBase,OH 45433 (513)255-6104;Fax (513)255-3717 Dr. JamesH. Starnes,Jr. Mail Stop190 NASA LangleyResearchCenter Hampton,VA 23665 (804)864-3168;Fax (804)864-7791 Mr. DanielE. Thomson WL/POTC Wright PattersonAir ForceBase,OH 45433 (513)255-2081;Fax (513)476-4531 Prof. Earl

A. Thornton

Light Thermal Structures Center School of Engineering and Applied Thornton Hall

L. Venneri

Science

University of Virginia Charlottesville, VA 22903 (804) 924-6291; Fax (804) 982-2037 Dr. V. B. Venkayya WI./FIBR Wright Patterson Air Force Base, OH 45433 (513) 255-7191; Fax (513) 255-3740 viii

565-9615

INTRODUCTION Performance requirements for future flight vehicles are rapidly increasing due to ambitious objectives of the U.S. civil and military aerospace programs. In aeronautics, future goals include higher cruising speeds, altitudes and thrust-to-weight ratios. The technology drivers for future aircraft include reduction in material, fabrication and maintenance costs; reduction in weight; extended life; higher operating temperature; and signature reduction. In space, future goals include lower transportation costs to space; long-duration space flights; planetary missions; and extraterrestrial bases. To successfully achieve the performance requirements space systems major advances are needed in: 1) computational and engineered materials such as high-temperature composites solution of coupled multidiscipline problems; 4) computational 5) accurate quantification of risk. The timely development essential to insure U.S. superiority in the aerospace field.

for planned and h, ture aeronautical and structures technology (CST); 2) advanced and advanced metallics; 3) formulation and simulation of concurrent engineering; and and deployment of these technologies is

Several national programs such as High-Speed Civil Transport (HSCT), National Aerospace Plane (NASP), National Launch System (NLS), and Integrated High-Performance Turbine Engine Technology (IHPTET) need major advances in a number of key areas of computational structures technology. To this end, there are a number of primary pacing items and related tasks that must be addressed by the research community. The joint NASA/University of Virginia Workshops held at NASA Lewis Research Center, June 26-27, 1991 and at NASA Langley Research Center, September 4-5, 1991 focused on the status of computational structures technology and the pacing items of this technology. The list of pacing items given in this introduction was compiled from a number of participants. It is anticipated that the items in the list can impact the design and operation of future flight vehicles in the following four ways: 1) by providing better understanding of the phenomena associated with response, failure and life, thereby identifying the desirable structural design attributes; 2) by improving the productivity of the design team, and reducing the response time to resolve operability problems; 3) by verifying and certifying designs, and making low-cost design modifications during the design process; and 4) by allowing major improvements and innovations in the design process so as to achieve a fully integrated design in a concurrent engineering environment. In such an environment, computer simulation is made of the entire life cycle of the flight vehicle including material selection and processing, multidisciplinary design, automated manufacturing and fabrications, quality assurance, certification, operation, health monitoring and control (e.g., maintenance and repairs), retirement and disposal. The ultimate aim of CST research is to impact the fully integrated design process. Primary.

Pacing

Items

The primary pacing items identified by the participants can be grouped into the following six headings: 1) computational material modeling; 2) fail.ure and life prediction methodologies; 3) hierarchical, integrated multiple methods and adaptive modeling techniques; 4) probabilistic analysis, stochastic modeling and risk assessment; 5) validation of numerical simulations; and 6) multidisciplinary analysis and design optimization. For each of the aforementioned items attempts should be made to exploit the major characteristics of high-performance computing technologies, as well as the future computing environment. The six primary pacing items are described subsequently. Note that some of the tasks within the pacing items are of generic nature, others are specific to either propulsion systems or airframes. 1. Computational Material Modeling. The reliability of the predictions of response, failure and life of structures is critically dependent on the accurate characterization and modeling of material behavior. The simple material models used to date are inadequate for many of the future applications, especially those involving severe environment (e.g., high temperatures). Needed work on material modeling'can be grouped in two general areas', a) modeling the response and damage of advanced material systems in the actual operating environment of future flight vehicles; and b) numerical simulation of manufacturing (fabrication) processes.

Advancedmaterialsystemsincludenewpolymercomposites,metalmatrix composites,ceramic composites,carbon/carbonandadvancedmetallics. The length scaleselectedin the model must be adequatefor capturing the responsephenomenaof interest (e.g., micromechanics,mesomechanics, macromechanics).For materialsusedin propulsionsystems,work is neededon themodelingof damage accumulationandpropagationto fracture;modelingof thermoviscoplasticresponse,thermal-mechanical cycling andratcheting;andpredictionof long-termmaterial behaviorfrom short-termdata, which are particularlyimportant. 2. Failure and Life Prediction Methodologies. Practical numerical techniques are needed for predicting the life, as well as the failure initiation and propagation in structural components made of new, high-performance materials in terms of measurable and controllable parameters. Examples of these materials are high-temperature materials for hypersonic vehicles; piezoelectric composites; and electronic, optical, and smart materials for space applications. For some of the materials, accurate constitutive descriptions, failure criteria, damage theories, and fatigue data are needed, along with more realistic characterization of interface phenomena (such as contact and friction). The constitutive descriptions may require investigations at the microstructure level or even the atomic level, as well as carefully designed and conducted experiments. Failure and life prediction of structures made of these materials is difficult and numerical models often constructed under restricting assumptions may not capture the dominant and underlying physical failure mechanisms. Moreover, material failure and structural response (such as instability) often couple in the failure mechanism. 3. Hierarchical. Inte_m'ated Multiple Methods and Adaptive Modeling Techniques. The effective use of numerical simulations for predicting the response, life, performance and failure of future flight vehicles requires strategies for treating phenomena occurring at disparate spatial and time scales, using reasonable computer resources. The strategies are based on using multiple mathematical models in different regions of the structure to take advantage of efficiencies gained by matching the model to the expected response in each region. To achieve the full potential of hierarchical modeling, there should be minimal reliance on a priori assumptions about the response. This is accomplished by adding adaptivity to the strategy. The key tasks of the research in this area are the following: 1) simple

2)

design-oriented

3) simulation

of local phenomena

4) automated

(or semiautomated)

6)

stages

of the design

process

and adaptive

through

global/local

methodologies

coupling

of different

mathematical/discrete

modeling

models

strategies

high fidelity modeling of details (such as damping, material nonlinearities, joints). For propulsion systems, this may require, among other things, efficient full three-dimensional multi-load analyses;

7) efficient 8) sensitivity neglected 4. developed conditions,

for use in the early

rational selection of a set of nested mathematical models for different regions, and discretization techniques for use in conjunction with the mathematical models. This, in turn, requires the availability of a capability for holistic modeling from micro to structural response with varying degrees of accuracy.

5) error estimation

2

models

methods

for engine

airframe

and rotor/engine-frame

analysis to assess the sensitivity of the response in the current mathematical model.

coupling. to each of the parameters

Probabilistic Analysis. Stochastic Modeling and Risk Assessment. The new methodology for treating general forms of uncertainties in geometry, material properties, boundary loading, and operational environment in the structural analysis formulation of structural

components to quantify

needs to be extended inherent uncertainties

to probabilistic design/risk assessment in the response of flight vehicles

of full flight vehicles. is obviously of great

The ability advantage.

However, the principal benefit of using any stochastic method consists of the insights into engineering, safety, and economics that are gained in the process of arriving at those quantitative results and carrying out reliability analyses. As future flight-vehicle structures become more complicated, failure mechanisms will be probabilistically modeled from the beginning of the design process, and potential design improvements will be evaluated to assess their effects on reducing overall risk. The results, combined with economic considerations, will be used in systematic cost-benefit analyses (perhaps also done on a probabilistic basis) to determine the structural design with the most acceptable balance of cost and risk. 5. Validation of Numerical Simulations. In addition to selecting a benchmark set of flight-vehicle structures for assessing new computational strategies and numerical algorithms, a high degree of interaction and communication is needed between computational modelers and experimentalists. This is done on four different levels, namely, 1) laboratory tests on small specimens to obtain material data; 2) component tests to validate computational models; 3) full-scale tests to validate the modeling of details; and 4) flight tests to validate the entire modeling process. 6. Multidisciplinary_ Analysis and Design Optimization. The realization of new complex aerospace vehicles requires integration between the structures discipline and other traditionally separate disciplines such as aerodynamics, propulsion and control. This is mandated by significant interdisciplinary interactions and couplings which need to be accounted for in predicting response, as well as in optimal design of these vehicles. Examples are the couplings between the aerodynamic flow field, structural heat transfer, and structural response of high-speed aircraft and propulsion systems; and the couplings between the control system and structural response in control-configured aircraft and spacecraft. This activity also includes design optimization with multi-objective functions (e.g., performance, durability, integrity, reliability and cost), and multi-scale structural tailoring (micro, local, and global levels). For propulsion systems it also includes design with damping for high-cycle fatigue, low-cycle-fatigue, and acoustic fatigue. Typically, in the design process questions arise regarding influence of design variable changes on system behavior. Answers to these questions, quantified by the derivatives of behavior with respect to the design variables or by parametric studies, guide design improvements toward a better overall system. In large applications this improvement process is executed by numerical optimization, combined with symbolic/AI techniques, and human judgement aided by data visualization. Efficiency of the computations that provide data for such a process, is decisive for the depth, breadth, and rate of progress achievable, and hence, ultimately, is critical for the final product quality. R¢li_*;cd Tasks For CST to impact the design process, the following three tasks need to be addressed by the research community: 1) development of automated or semi-automated model (and mesh) generation facilities; 2) pre- and postdata processing and use of advanced visualization technology; 3) adaptation of AI tools (knowledge-based/expert systems and neural networks) to CST.

3

N9e- 5912

Computational Structures Technology UVA Center for CST Ahmed University

and

K. Noor of Virginia

Ft_C-ED._t-J,G PAGE

BLA;_K

NOT

FILMED

5

OUTLINE Rapid

advances

disciplines,

including

computational modeling,

in computer

structural science,

outgrowth

of finite

is on some newly

the materials,

structures

computer

aspects

established

environment

technology

numerical

methods

Center

along

developed

for CST.

The outline

with the motivations Third,

and research

directions.

Fourth,

as an insightful

on the one hand, theory,

airframes

on the other

CST.

we look at the future

of the Center

the newly

established

is describe.d,

UVA

andfinally

systems,

modeling

,

• A look at the future • TechniCal needs • Computing environment • Research directions • UVA Center for CST • Description

of one research

• Summary Figure

l

project

such as

the background

CST is an

of technical Center

and goals

a brief discussion needs,

is made

computing

for CST is described.

a brief summary

goals for CST and motivations of CST material

material

as well as on the

is given.

• Computational

6

between

The focus of this presentation

Second,

in terms

blend

hand (see Ref. l).

in Fig. I. First,

for developing

and mechanics

and other disciplines

and propulsion

is shown

engineering

A new technology,

over the last three decades. future

modeling.

disciplines.

emerged

and approximation

• Background, development

_i __

and synthesis

can impact

projects

effect on various

and dynamics has recently

material

Fifth, one of the research presentation

analysis

of CST which

had a profound

(CST),

analysis

element

UVA

have structures

and dynamic

for CST are described on computational

hardware

for

of the

DIFFERENT

Current

CST work includes

• computational

material

• computational

methods

components (Refs.

thereof.

Some

ASPECTS

the following

facets

OF CST WORK

(Fig. 2):

modeling for predicting

the response,

of these activities

performance,

failure

have been labeled

computational

and optimization.

In addition,

and life of structures structural

mechanics

2 and 3).

• automated component

methods

of structural

in multidisciplinary

synthesis

analysis

and design

of many

engineering

CST is an important

fields.

• Computational material modeling • CSM - Computational methods for predicting

• •• •

Performance Failure, Responseand Life

}

structures a n_lfcomponents thereof

• Automated methods of structural synthesis and optimization. Also, CST is an important component in the multidisciplinary analysis and design of many engineering systems.

Figure

2

and - CSM

GOALS FOR CST Within

the aeronautics

First.

To predict,

structures

and space fields, in a reasonable

and their components

S_ond.

To complement

the following

amount

at actual

goals of CST can be identified

of time, the response,

operating

and supplement

four major

failure

(Fig. 3):

and life of flight-vehicle

conditions_

experiments

and flight testing,

and to help in the design

of

experiments. Third.

To explore

new phenomena,

which

are difficult

to understand

simulations. Fou_h.

To aid in the design

process

of flight vehicles.

First To predict response, perfor_nce, failure and life of flight-vehicle structures at actual operating conditions Second To design, complement and supplement experiments and other tests for flightvehicle structures Third To study ph_oomena which are difficult to understand by means other than numerical simulations (e,g,, damage and failure mechanisms of high-performance materials at high temperatures) Fourth To aid in the design of flight-vehicle structures Figure

8

3

by means

other than numerical

MOTIVATIONS There compelling

Some

the capacity

components

concepts

components

and expensive

mission-critical

and space

A third major emerging potential

testing,

and future

motivation

strategies

explored

is frequently

computer

modeling

awaits

experiment

Thefirst and/or

so large and complex

numerical

that they overtax

are the simulation

and the study of thermoviscoplastic

of

response

In other

structural

problems,

(e.g., damage

initiation

and propagation

simulation component-

CST relates

computing

systems

to reduce

or mission-oriented. replace

the limits

tests.

of

the in

in solving

that exploit

power

large-scale

only by developing the capabilities

the dependence

on

Moreover,

in some

This is because

of ground-test

to the anticipated

can be realized

algorithms

is needed

may, of necessity,

are likely to exceed

for developing

and mlmerical

CST (Fig. 4).

systems).

which

computers

CST

of these problems

systems.

is that numerical

high-performance

of these high-performance

computational

are still being

structures

simulations

forces,

propulsion

developing problems

Examples

crash impact

reason

areas in space,

large aerospacecrafts

numerical

made of new material

compelling

practical

large computers.

used in advanced

mechanics

for vigorously

of unsolved

involve

to multidirectional

A second extensive

is that a number

of even present-day

fundamental

motivations

of these problems

response

structural

structural

compelling

motivation

solutions.

aircraft

are three

FOR DEVELOPING

future

technology. and potential

structural

problems.

of The

new formulations,

of the new machines.

9

• Practicalproblems

awaithTg solutions

• Very large problems (e.g., due to high-degree and/or high-degree of sophistication needed

of integration in modeling)

• Problems for which fundamental mechanics concepts explored (e.g., failure mechanisms of structural components made from new _----_. material systems) • Reduce dependence on testing • Reliability of testing large space structures questionable • Exploit new and emerging

computing

required

are still being 7

in 1-G environment

technology

is

] •

It, tool

IMSOOO3

_=-

I

I

Transputers

Figure

10

4

COMPUTATIONAL MATERIAL MODELLING Objective and Status Considerable

attention has recently been devoted to computational

CST, the objective and status of the activity are summarized a hierarchy of material models (multilevel/multiscale) response, life and failure of structures. physics-based

material modeling.

in Fig. 5. The overall objective

to describe the different phenomena

This has resulted in a gradual evolution

models that predict the processing

In the context of

response

and properties.

is to develop

associated with

from empirical

However,

models to

many gaps still exist

in the hierarchy of models.

Objective: Development of a hierarchy (multilevel/ multiscale) of material models to describe the different phenomena associated with response, life and failure of structures Status: Gradual evolution from empirical models to physics-based models that predict processing response and properties. •

Many gaps of models

still exist

in the hierarchy

Figure

5

11

COMPUTATIONAL MATERIAL MODELING Hierarchy of models A hierarchy phenomena meter). quantum

of material

they describe

The disciplines mechanics;

used range

models

are shown

and the length involved

from atomistic

scale at which

include

computational

in Fig. 6. The models

computational

material

to single crystals

this phenomena

science;

chemistry,

which

and computational

to polycrystals

are arranged is studied covers

(from

10d°m

molecular

structural

to micromechanical

according

to the to one

dynamics

mechanics.

The models

and macromechanical

models.

Models Phenomenological/ macromechanical

Length scale, m

Discipline Computational structural mechanics

Polycrystals (homogenized models)

Computational material science

Single crystals Atomistic models

Molecular dynamics

Computational

Quantum mechanics

chemistry

Figure

12

Phenomena

10 0 10-2

• Structural response • Metal forming

10 4

• Plastic strain localization • Crack tip fields • Indentation fracture

N

Micromechanical

10 -6

• Void growth ° Polycrystalline slip • Microstructural effects

10 "8

• Dislocations • Particles and interfaces

10"10

• Creep diffusion • Cleavage • Discrete defects • Basic transport properties • Phase transformation

6

and

A LOOK AT THE FUTURE CST is likely

to play a significant

in the multidisciplinary advances number Ref.

design

and computational of primary

tools are needed pacing

three factors

1) characteristics

adapted

and certification

and secondary

1). The following

role in the future of future

computing

3) recent

and projected

flight vehicles.

in a number

are taken into account

environment;

of structures

in identifying

their technical

technology

For this to happen

of key areas of CST.

items that must be addressed

of future flight vehicles,

2) future

development

as well as

major

To this end, there are a

by the research the pacing

community items

needs and implications

(see

(Fig. 7):

for CST;

and

developments

in other fields of computational

technology

which

can be

to CST.

• Computational technology will play a significant role in the development of structures technology and in the multidisciplinary design and certification of future flight vehicles • Major and secondary

pacing

• Basis for determining

the pacing items

• Characteristics their technical for CST

items

of future flight vehicles, needs and the implications

• Future computing

environment

• Recent and projected developments in other fields of computational technology which can be adapted to CST Figure

7

13

TECHNICAL NEEDS FOR FUTURE FLIGHT-VEHICLE STRUCTURES AND THEIR COMPUTATIONAL IMPLICATIONS The technical

needs for future

flight vehicles

can be grouped

into three

major

areas

(Fig. 8),

namely: 1) new high-performance metallics

material

as well as intelligent/smart 2) novel structural

systems.

material

concepts

which

These

include

new composite

materials,

advanced

systems; include

structural

tailoring

and smart/adaptive

structural

concepts; 3) expanding complex

phenomena,

couplings

1) development stress/strain/temperature 2) highfidelity 3) development

14

of engineering

such as damage

problems

tolerance

(e.g., structure/fluid/thermal/control

The implications

V

the scope

of new material interaction

of the aforementioned of computational range

considered

models

technical

to include

systems;

investigation

of more

and study of interdisciplinary

problems). needs for CST include:

for new material

systems

over the entire

of interest;

representation of effective

of details computational

(e.g., material strategies

response, for large-scale

joints

and damping);

coupled

problems.

and

Needs • New high-performance material systems (including intelligent/smart materials) •

Novel structural concepts (e.g., structural tailoring and smart/adaptive structures)

• Investigation of complex phenomena interdisciplinary couplings Implications • Computational

material

• High fidelity

representation

• Strategies

for large-scale

and

models of details coupled

problems

Figure 8

15

TRENDS IN HIGH-PERFORMANCE COMPUTING

The trends in the 1950's

in high-performance

and early

and vectorization late 1970's. that before

1960's was a result

was introduced.

Recent

trend is moving

towards

teraflop

is shown

of advances

Development

the end of the century

point operations

computing

in device

of computers

distributed

computing

in Fig. 9. The increase

in speed of computers

technology.

In the late 1960's

with homogeneous

parallelism

heterogeneous

will be achieved

supercomputing. (speeds

reaching

began

trillion

floating-

Distributed heterogeneous supercomputing Homogeneous

Pipelining parallelism & vectorization Device tec

1950

1960

1970 Figure

16

1980 9,

1990

in the

It is anticipated

per second).

Speed

pipelining

2000

DISTRIBUTED HETEROGENEOUS MULTICOMPUTERS The basic The concept which

concept

refers

to an integrated

the network

is the computer.

numerical

simulations

accomplished networks.

New

CRAY

(Cedarlike); advanced

imposed

by combining buzzwords

The hardware (e.g.,

of distributed

3, C-90, massively

workstations

multicomputers

environment

The use of DHM

of disparate

like "META

Computer"

a plethora

minisuper systems RISC,

speeds

are currently

(e.g., Convex

SUN,

...); and HDTV

is highlighted

of networked

alleviate

used to refer

systems

in

This is

through

high-speed

to this concept.

large-grain clustered

application-specific hardware

in Fig. 9a.

on the size of

capacities.

platforms

C-380);

computer

the limitations

and memory

such as:

(e.g., Intel Touchstone);

SGI,

(DHM)

supercomputing

of architectures

computers

consisting

can greatly

supercomputer

the resources

parallel (IBM

computing

by current

can include SSI),

heterogeneous

vector

supercomputers

processors computer

and software

systems;

with video

facilities.

Description: An integrated computing environment consisting of networked computer systems - Garden (or Plethora) of new architectures - META Computer. Hardware

includes:

• Large-grain vector supercomputers (e.g., CRAY 3, C-90, SSI) • Minisuper computers (Convex C380) • Clustered processors (Cedarlike) • Massively-parallel systems (Touchstone - gamma, delta or sigma) • Application-specific computer systems • Advanced workstations (IBM RISC, SGI, SUN,...) • HDTV hardware and software with video facilities Figure

9a

17

DISTRIBUTED

HETEROGENEOUS

MULTICOMPUTERS (CONT'D.) The effectiveness area networks

parallel

is strongly

dependent

for data transfer

between

For local area networks

(LAN),

interface)

links are currently

net T-3 internet

be needed. the following

and UltraNet will be upgraded

Because

media,

of DHM

the different

computers.

FDDI

distributed

mass storage

key elements:

and a massive

systems

being

HiPPI

local and wide

(high-performance

For wide area networks

(WAN)

improvement

directly

connected

(IEEE through

in mass storage reference HiPPI

model),

channels;

facilities

mass

network.

LAN

FDDI HiPPi

100 Mb/sec. 1 Gb/sec.

WAN

T3-1nternet T5-1nternet

60 Mb/sec.

Mass Storage: • High bandwidth mass storage (IEEE reference model) • Large disk arrays directly connected through HiPPI (> 100 G Bytes) • Mass robotic media file transfer

network (> 200 M Bytes/sec.) Figure

z

18 i

!

!

10

will

and include

Networking:

• Massive

the NSF

(Fig. 10).

will have high bandwidth

file transfer

of high-speed

data interface),

used.

of data, significant

large disk arrays

high-speed

(Fiber

to the T-5 interact

of the very large volumes

Future

on the availability

robotic

WHY DISTRIBUTED HETEROGENEOUS MULTIPROCESSORS? The primary parallelism

motivations

than can be done on a single

superconcurrency

(Fig.

Experience be relatively

In distributed

algorithms

vector

(or ineffective) applications

heterogeneous

are to achieve

architecture.

These

higher

are referred

speeds

and higher

levels

to as hypercomputing

of and

11).

with different

effective

most of the practical

numerical

for using DHM

and parallel

on different

the sustained

multiprocessors,

used in each module,

architectures

sections

has shown

of the computational

speed is a fraction the physical

process.

of the peak performance

characteristics

will form the basis

that different

of the problem,

for identifying

architectures Therefore,

can for

of the machine. and the

the most suitable

platform

for that module.

Hypercomputing

and superconcurrency

• Optimal support for algorithmically diverse parts of an application program on architectually diverse machines. • Different architectures can be relatively effective or ineffective on different sections of the computational process (code profiling and machine matching), • Parameters and data lengths can affect choice of architecture. Figure

11

19

CROSS OVER POINTS As an example, a function vector

the speed

of the vector

lengths,

higher

of performing

length

the operation

is depicted

speed is achieved

FOR SAXPY

Z(I) = R*X(I)

in Fig. 12. As can be seen from by a different

this figure

t

I_

8K Conn Mach

_



mmi.w

,

,

wwl_w==w

/: -'C'i_AY X-MP

7,,I,4,

,/

MFLOPS

for each range

Y(I)

4K DAP 100

computers

machine.

Z(I) = R*X(I).

1000

+ Y(I) on four different

/

4,0

40 e o 4, ,i,° # @* @@

10

Convex 210

@@@ @@

@@@ ,@

I

110'

I

,,,,,,,I

llllJ

IO0

,,,,,,,I

1000 10000 Vector size Figure

2O

,

12

, ,,,,,,J

, ,,,,,,,!

100000 1000000

of

as

PROFILES The results analysis identified

of the previous

on a network

figure

OF PROCESSOR

are extrapolated

of n supercomputer

as the one which

results

to the entire computation

platforms.

in the highest

For each module,

speed for that module

•",

//\/_

: "

typel_::

spectrum

of a finite

the most suitable (Fig.

element

platform

is

13).

Processor " type 2 ",, -7

m

Processor

TYPES

_",

/

Speed

/

v

_--

Processor type n

Element Assembly form.

Constraint and

Solution of

boundary conditions

equations

Computation

Error analysis

Adaptive refinement

spectrum

Figure

13

21

FORMS OF DISTRIBUTED

HETEROGENEOUS

MULTICOMPUTERS (DHM) Three different second

different

forms

of DHM

workstations

are shown

are connected.

is the site DHM,

in which

DHM

are the NSF Centers

DHM,

in which

An example

different

at Illinois,

supercomputing

in Fig. 14. The first is micro

architectures

is executed

are connected

and San Diego,

at different

sites, the application

program

concept,

the four NSF Supercomputing

connecting

of this is the PASMproject

Pittsburgh

platforms

DHM,

platforms. Centers

and NOSC.

site.

Examples

National

of global

Metacenter

DHM.

Global DHM

Front-end Processor

J Complementary

(e.g., PASM

Purdue Project)

(e.g.,

Back-end

NSF-NCSA,

SDSC,

Processors

PSC

and NOSC)

Maximum databases interface

Figure

22

14

The of site

The third is the global

The proposed

is an example

of

University.

in each of the different

SITE DHM

Micro DHM

a number

at Purdue

at the same

sites are connected,

on different

in which

use of or display/ capabilities

DHM

SUPPORT Despite

its potential,

of adequate

DHM

transfer

the data format

rates

fraction,

computers

must cross

affect the overall

interfaces different

several

include:

of potential

pitfalls.

high computing

For DHM

effective

networks,

such mismatches

of support

facilities

Thus,

to be viable,

bandwidth. as packet

networks

must be capable

on the supercomputers.

to that of another.

data must be measured. into the overall

In particular,

speeds

is not likely to be identical

since it figures

transfer

In addition,

express);

to sustain

or translating

significant

Linda,

in order

of one computer

spent transforming

15). These

also has a number

FACILITIES

In addition,

the amount

this should

If transfers

between

size and transfer

of time

not be a two

rate differences

could

rate.

a number distributed

high-level

operating

programming

to aid in the partitioning

system

are needed

(e.g., MARK

abstractions

of the program

to realize

the full potential

or KRONOS);

of DHM,

network

and object-oriented

tools; expert

into tasks and scheduling

the tasks

(Fig.

language systems

(e.g.,

and user

on processors

of

types.

• Distributed

• Network

operating

language

• Object oriented

system

(e.g., MARK, KRONOS)

(e.g., Linda, Express)

tools and user interfaces Figure

15

23

FUTURE

The future directions

DIRECTIONS

FOR RESEARCH

for research in CST are listed in Fig. 16. For convenience,

they are divided into

major pacing items and related tasks. The major pacing items include the following 1) high fidelity modeling of material response, structural, geometrical well as the environmental

3) effective computational fluid/thermal/structural/control

details as

made of new materials;

strategies for large-scale problems which include:

analysis; sensitivity analysis; and multidisciplinary

integrated

analysis and

of large systems; and

4) validation and assessment

of the reliability of numerical

The related tasks include predata, postdata processing technology;

and topological

effects;

2) life prediction and analysis of failure of structural components

optimization

four:

and integration

simulations.

and effective use of visualization

of analysis programs into CAD/CAE

and concurrent

engineering

systems.

Major Pacing Items • High fidelity modeling of material response, structural, geometrical and topological details, environmental effects (e.g., boundary-layer transition, interference heating) Life prediction and analysis of failure for structural components and structures made of new materials Effective computational strategies for large-scale problems • Integrated fluidthermalstructural analysis • Sensitivity analysis • Multidisciplinary design and optimization Validation and assessment of reliability of aerodynamic/thermal/structural response predictions. Secondary • •

Pacing

Items

Predata, postdata processing and effective use of visualization technology Integration of analysis programs into CAD/CAE and concurrent engineering systems Figure 16

24

UVA CENTER The background was established Headquarters.

in July 1990. Research

The overall modeling,

and objectives

analysis,

four specific

goal

grants

high-risk

sensitivity

for CST are highlighted

Langley.

The primary

from NASA

funding

Langley

and use of AI methods.

source

17. The Center is NASA

and AFOSR.

is to serve as a focal point for the diverse optimization

in Fig.

CST activities

The Center

including

has the following

research

on advanced

topics

of CST;

by demonstrating

to the research

community

future

of research

in support

results

and in broadening

what can be done

(high-

research);

of the twenty-first

of the aeronautical

and space

and,

transfer

of the state-of-the-art CST (notably

directions

century;

4) to help in the rapid

can impact

at NASA

also been obtained

studies,

innovative

3) to help in identifying

and engineers

have

of the Center

2) to act as pathfinder,

missions

It is located

Center

objectives:

1) to conduct

potential,

of the UVA

FOR CST

of research

awareness

in CST as well as in other areas of computational

CFD and computational

among technology

researchers which

mathematics).

25

BACKGROUND: • Established in July 1990 • Located at NASA Langley in Hampton • Funded by NASA Headquarters, NASA Langley, AFOSR,... OVERALL

GOAL:

Serve as focal point for CST development

(including modeling,

analysis, sensitivity studies, optimization and use of AI methods) SPECIFIC OBJECTIVES: • Conduct innovative reseach on advanced topics of CST • Act as pathfinder, by demonstrating what can be done (highpotential, high-risk research) • Help in identifying future directions for research • Help in the rapid transfer of research results and broaden awareness of the state-of-the-art in CST as well as other areas of computational technology that can impact CST (serve as central clearing house for information) Figure

26

17

FUTURE

To accomplish 1) research.

This will be done in strong collaboration

a series of seminars,

4) publish quarterly newsletter research centers and universities,











with NASA (Langley and Lewis), UVA

workshops

and national symposia; and state-of-the-art

monographs

on timely topics; and

listing CST research activities at various government

as well as recent contributions

laboratories,

on selected topics.

Items

High fidelity modeling of material response, structural, geometrical and topological details, environmental effects (e.g., boundary-layer transition, interference heating) Life prediction and analysis of failure for structural components and structures made of new materials Effective computational strategies for large-scale problems • Integrated fluid/thermal/structural analysis • Sensitivity analysis • Multidisciplinary design and optimization Validation and assessment of reliability of aerodynamic/thermal/structural response predictions.

Related •

Pacing

four major activities (Fig. 18):

researchers;

3) write survey papers, special publications

Major

FOR RESEARCH

its mission the Center will carry out the following

faculty, industry, and university 2) organize

DIRECTIONS

Tasks

Predata, postdata processing and effective use of visualization technology Integration of analysis programs into CAD/CAE and concurrent engineering systems Figure

IIIIIII

18

27

The initial research • Design-oriented This activity techniques

include effective

UVA CENTER

FOR CST

projects

include

CST

technique

to high-speed

(see Fig. 19):

transport

and large

for evaluating

the sensitivity

for large-scale

and coupled

flexible

derivatives,

spacecrafts.

optimization

for large systems.

• Innovative

computational

hierarchical

adaptive

use of artificial

for the Center

with application

will focus on effective and AI methods

selected

strategies

modeling

neural

networks,

strategies,

hybrid

analysis

and development

problems.

techniques,

of intelligent/smart

novel

This activity partitioning

computational

will strategies,

modules.

INITIAL RESEARCH PROJECTS: • Design-oriented CST(with application to high-speed transport and large flexible spacecrafts) • Optimization, sensitivity analysis and Ai methods • Innovative computational and coupled problems. • • • •

strategies for large-scale structural

Hierarchical adaptive modeling Hybrid techniques Novel partitioning strategies Neural networks

• Intelligent computational modules Figure

28

19

UVA CENTER FOR CST (Cont'd.) The initial

research

• Computational development

also include

modeling

for heat transfer

thermal

buckling

(Refs.

(Refs.

buckling

modeling

of flight-vehicle

computational

and modeling

and damping.

of joints

• Failure

analysis

• Quality

assessment,

models,

and mechanisms adaptive

multilayered

4 and 5), analytic

analysis

and engine effective

of structural

and validation

lamination

models

for

for the accurate

9, 10 and 11).

structures.

coupling

thermal

thermoelastic

procedures

(Refs.

This includes

of composites,

three-dimensional

responses

of failure

control

composites.

predictor-corrector

and postbuckling

(mulfilevel/multiscale)

four (Fig. 20):

for thermoviscoplastic

6, 7 and 8), and effective

of the thermal

• High fidelity

models

analysis

the following

of high-temperature

of micromechanical

theories

prediction

projects

This includes:

of numerical

components

of numerical

hierarchical

simulations

and experiments,

made of new materials.

simulations.

INITIAL RESEARCH PROJECTS: • Computationalmodeling composites

of high-temperature

multilayered

• Micromechanical models • Thermal lamination models for heat transfer • Computational models for thermal buckling and postbuckling • High-fidelity modeling of flight-vehicle

and engine structures

• Hierarchical (multilevel/multiscale) computational material models • Effective coupling of numerical simulations and experiments • Modeling of joints and damping • Failure analysis and mechanisms of failure of structural components made of new materials • Quality assessment and adaptive controlof numerical solutions; and validation of numerical simulations Figure

20

29

CHARACTERISTICS OF AN EFFECTIVE COMPUTATIONAL STRATEGY FOR LARGE STRUCTURAL SYSTEMS The remainder Center,

of the presentation

viz., development

of effective

is devoted

computational

to a description strategies

of one of the research

for large-scale

projects

and complex

at the

structural

systems. The three major

characteristics

First, the strategy hierarchical

adaptive

sophistication,

modeling

as needed,

must be the simplest The second computational

should

computational

insight

strategy

about the response.

are listed

the actual

structure.

As was suggested

in Fig. 21.

This is accomplished

- in the sense of starting from a simpler model

and increasing

by Einstein,

by using

the level of

"The model

used

one, but not simpler."

characteristic

model.

give physical

to model

possible

of an effective

of the strategy

This is accomplished

is that it should

by obtaining

help in assessing

sensitivity

information

the adequacy about

of the

the modeling

details

as part of the analysis. The third characteristic by linking

the degrees

new computing

3O

systems

of freedom (vector,

of the strategy is that it should be highly used in the initial discretization, parallel

and AI capabilities).

efficient,

and by exploiting

which

is accomplished

the major

features

of

Characteristics

Accomplished

by

• Gives physical insight about response

=Hierarchical adaptive modeling - start from a simpler model and increase the level of sophistication, as needed, to model the actual structure 'The model used must be the simplest possible one, but not simpler."

• Helps in assessing adequacy of computational model

• Obtain sensitivity modeling details

• High computational efficiency

• Reduce number of degrees of freedom used in original discretization • Exploit major features of new computing systems (vector, parallel and AI capabilities)

Figure

information

about

21

31

BASIC IDEA OF PROPOSED COMPUTATIONAL STRATEGIES The basic idea of the strategies, response

of a complex

system

using

either the simpler

system

discrete

of the simpler

Sensitivity available

equations

derivatives

of the response

process

the response

to satisfy

model

are then embedded

of the system cost.

conjugate

is to generate model

of the original

to modeling

of the simpler gradient-PCG

model

the

associated

system

into those of the original

with respect

The response

the three criteria,

from that of a simpler

mathematical/discrete

(e.g., preconditioned of the original

appear

large perturbations

system

at very small computational

and an iterative generate

or a simpler

which

(Fig. 22).

complex

details

with

neglected,

system. are directly

is then used as a predictor

or multigrid-MG)

is applied

model.

• Response of a complex system is generated using large perturbations from that of a simpler model associated with either: • Simpler system • Simpler mathematical/discrete model of original system • Discrete equations of simpler system are embedded of original complex system

into those

• Sensitivity derivatives of the response of the system with respect to modeling details neglected, are directly available • Response of simpler model used as a predictor and an iterative process (PCG or MG) is appl,ed to generate response of original model Figure

32

22

_

_

The

to

APPROACHES FOR SELECTING SIMPLER MODEL Two general

approaches

The f'n'st is hierarchical multigrid

approach

dimensionality. mathematical

based

transformations.

on selecting

the simpler

which

a simpler

and restriction

model

includes model,

are outlined

the classical associated

operators

reflect

in Fig. 23 (Refi

multigrid

technique

with a mathematical the physical

12).

and the physical

model

assumptions

of lower

of that

model.

domain

or uncoupling

modeling

The interpolation

The second physical

for selecting

approach

is the decomposition

decomposition.

It is based

of the load-carrying

on either

mechanisms

The two approaches

or partitioning

are briefly

uncoupling

in structural discussed

strategy

which

of different

problems,

can be thought

fields

in coupled

of as problems,

or using symmetry

in the succeeding

figures.

• Hierarchical modeling (multimodel or multigrid) • Mathematical model of a lower dimensionality (multimodel or physical multigrid-PMG) • Coarse finite element grid (classical multigrid) • Decomposition or partitioning (physical domain decomposition-PDD) • Uncoupling of different fields in coupled problems (e.g., aerodynamics, thermal and mechanical fields) • Uncoupling of load-carrying mechanisms in structural problems (e.g., extensional and bending components) • Symmetry transformations Figure

23

33

HIERARCHICAL

The application The structure is referred

of the hierarchical

is modeled

by using

to as the actual

beam model.

Although

similar,

of the simpler

those

The degrees interpolation two-dimensional operation

the governing structure

model

structure

discrete

equations

are much

smaller

reflects

structure

to one-dimensional

are given

to a composite

corresponds

are related

beam model).

structure

and

{z} = [r](z}

[F]t = restriction [k] = [F]t[K][F] {q} = [F]t{Q}

assumptions

operator w °,

1

Figure

34

i1,112

24

As usual

and load vectors

Governing equations: Actual structure [K]{Z} = {Q} Simpler structure [k]{z} = {q}

Interpolation [F] reflects basic in dimensionafity reduction

and simpler

in Fig. 24.

discrete

model

thin-walled

structures

model

used in the dimensionality

the stiffness

actual

The resulting

to those of the simpler

in Fig. 24.

Relationship between simpler model:

is outlined

are

in number.

thin-walled

between

airframe

to a one-dimensional

for both the actual

the basic assumptions

is taken to be IF] t. The relations

and the simpler

strategy

STRATEGY

plate and shell elements.

The simpler

of the actual

IF], which

shell model

modeling

two-dimensional

structure.

of freedom

operator

MODELING

by the

reduction

(from

the restriction

of the actual

structure

GEOMETRIC INTERPRETATION OF SYMMETRY TRANSFORMATION APPROACH

The geometric unsymmetric

domain,

subvectors, statement

component. vector.

It is important requires

governing

The transformation

vector

matrices

transformation

process

of the domain).

can be repeated The strategy

to an

into two equal

The equation

by applying

a matrix

length

in Fig. 25 is a

as the sum of a symmetric

and antisymmetric

model

as applied

and an transformation

to

in the figure.

for their determination. The simpler

in Fig. 25.

can be obtained

are shown

approach,

{Z} is partitioned

can be written

to note that each of the symmetric

only half the model

partitioning

vector

in the form shown

Each of the two vectors

{Z}s and {Z}as are coupled.

The symmetry

transformation

in Fig. 25. The response

of the fact that each unsymmetric

the original

(further

is given

for the symmetry

{Z}I and {Z}2, and can be written

antisymmetric

vector

interpretation

components

For an unsymmetric corresponds

to effect further

has several

advantages

domain

to the uncoupled reduction

of the response the equations set of equations.

in the size of the model

including

its suitability

for

parallelism.

35

Decomposition and Transformation matrices

t' tzl (Zl

+Z21 l+ z_ 1½ (z_ + Z2

o {Z}I nodes

{Z}1

1 (ZI.Z2) (Zl - Z 2 ))

= {Z}s + {Z}as

:'/---1

_____ :

tt

= [[T] s + [T]as]{Z}

/zl.--.--_

............. {Z} 2

13[']_[']

3

I:_[']_-['_

Comments on computational procedure • Each of {Z} s and {Z}a s can be determined by using a smaller (reduced-size) model or subdomain • Simpler model corresponds to uncoupled set of equations in {Z} s and {Z}a s

Figure

36

25

®

OPERATOR SPLITTING AND ITERATIVE SOLUTION PROCESS

!

The application partitioning

strategy,

The vector correspond

of operator is outlined

of fundamental

to the degrees

(uncoupled

equations).

unknowns

components

terms are identified

and iterative

solution

process,

in conjunction

with the

in Fig. 26.

of freedom

symmetric/antisymmetric The coupling

splitting

is partitioned

associated

with either different

of response.

by the parameter

The PCG iterative

into two subvectors

process

The discrete k. The simpler

{Z1} and IZ2}.

load-carrying

equations

are partitioned

structure

is used for generating

mechanisms,

corresponds the response

These or

accordingly. to the case k=0

of the actual

structure.

Partitioned

Equations

and Unknowns

{Z}I

O {Z}_1 nodes

. ...........

,A {Z} 2 nodes

([Kll ["21K:1 ){':}-{O.} Z1Q1 where L is a tracing parameter. = 1 --> original equations _, = 0 _ simpler-structure equations

[z}

Uncoupling of load-carrying mechanisms {Zl }' {Z2} are associated with

Iterative

Solution

different load-carrying mechanisms (e.g., membrane and bending)

Symmetry

transformation

symmetric/antisymmetric components of response vector

Process

• PCG used for solution • Left-hand-side matrix corresponding

to _,= 0 used as a preconditioner

Figure

26

37

APPLICATION TO NONLINEAR DYNAMIC ANALYSIS Cylindrical

The strategy center

circular

was applied cutout

to a nonlinear

subjected

i

\

/

dynamic

to uniform

,,,,1

j

panel with cutout

problem

pressure

of a composite

loading

cylindrical

panel

with an off-

(Fig. 26a).

x h_

u

w \

Boundary

3818 nonzero displacement degrees of freedom 6144 stress degrees of freedom

conditions

At x = 0, LI: u=v=w=

Loading

At y = 0, L2:

Uniform normal loading with intensity Po

W=_I=O

Figure

38

26a

_1= (_2 = 0

PERFORMANCE EVALUATION OF STRATEGY CRAY-Y MP4/432 (MENDOTA HEIGHTS)

The performance

of the proposed

27.

resulting

The speedup

of the study

are given

from

in Ref.

strategy

on the CRAY-YMP4/432

the use of four processors

at Mendota

was over an order

3818 displacements 6144 stress

971 displacements 1536 stresses

Semibandwidth of equations

700

315

Wall clock time

171

58.6 one processor 29.7 two processors 16.4 four processors

1.0

2.92 one processor 5.76 two processors 10.43 four processors

Speedup

in Fig.

The details

Partitioned Structure (Nearly Optimized Code) (246 MFLOPS)

Number of degrees of freedom

(first ten steps)

of magnitude.

is shown

12.

Full Structure (Optimized Code) (278 MFLOPS)

(see.)

Heights

ON

Figure

\

27

39

SUMMARY In summary

(Fig. 28), the goals

environment,

technical

needs,

aeronautical

and space

systems

UVA CST Center

structures.

(for example,

computational

contribute future flight

Its future

tools for structural

for research

development CFD,

advanced

complement

of planned

and activities

phenomena

interaction

and computational material

analysis

and synthesis

and future

to the development

of structures

technology,

computing

and projected

of the newly

established

projects.

associated

to experimental

strong

computational

high performance

of one of the research

of physical

requires

Future

in support

The mission

with the details

a valuable

mathematics,

of CST is bright;

significantly

along

our understanding

CST provides

flight-vehicle

computational

directions

have been identified.

enhanced

of structures.

The future

and future

have been described,

CST has greatly and failure

of CST have been described.

with the response

and analytical

with researchers

methods

for

in other fields

electromagnetics). models,

smart/intelligent

high performance

computers

as well as to improving

should

the design

of

vehicles.

• Goals of CST described • Future high-performance computing environment; technicaineeds and future directions for research, in support of aeronautical and space systems, identified • Mission

and activities

of UVA CST Center

described

• CST technology has greatly enhanced our understanding of physical phenomena associated with high temperatures • Future development of CST requires strong interaction with researchers in other fields (e.g., computational mathematics, CFD, and computational electromagnetics). Figure

4O

28

i

=.

REFERENCES 1. Noor, A. K. andVenneri, S.L. "AdvancesandTrendsin ComputationalStructuresTechnology," ComputingSystemsin Engineering,Vol. 1,No. 1, 1990,pp. 23-36. 2. Noor,A. K. andAtluri, S.N., "AdvancesandTrendsin ComputationalStructuralMechanics,"AIAA Journal,Vol. 25, 1987,pp. 977-995. 3. Grandhi,R. V., Stroud,W. J. andVenkayya,V. B. (eds),ComputationalStructuralMechanicsand MultidisciplinaryOptimization,AD Vol. 16,AmericanSocietyof MechanicalEngineers,NewYork, 1989. 4. Noor,A. K. andBurton,W. S., "Steady-State HeatConductionin MultilayeredCompositePlatesand Shells,"ComputersandStructures,Vol. 39,No. 1/2,March 1991,pp. 185-193. 5. Noor, A. K. andTenek,L.H., "Steady-State NonlinearHeatTransferin Multilayered Composite Panels,"Journalof EngineeringMechanics,ASCE 1992. 6. Noor, A. K. andBurton,W. S., "Three-DimensionalSolutionsfor ThermalBuckling of Multilayered AnisotropicPlates,"Journalof EngineeringMechanics,ASCE 1992. .

Noor, A. K. andBurton,W. S., "Three-DimensionalSolutionsfor theFreeVibrationsandBuckling of ThermallyStressedMultilayeredAngle-PlyCompositePlates,"Journalof AppliedMechanics 1992.

8. Noor, A. K. andBurton, W. S.,"Three-DimensionalSolutionsfor theThermalBuckling and SensitivityDerivativesof Temperature-Sensitive MultilayeredAngle-PlyPlates,"Journalof Applied Mechanics1992. .

Noor, A. K. andBurton,W. S.,"Predictor-CorrectorProceduresfor ThermalBuckling of Multilayered CompositePlates,"ComputersandStructures,Vol. 40, No. 5, 1991,pp. 1071-1084.

10.Noor,A. K. andPeters,J. M., "Postbucklingof MultilayeredCompositePlatesSubjectedto CombinedAxial andThermalLoads,"FiniteElementsin AnalysisandDesign1992. 11.Noor, A. K. andPeters,J. M., "ThermalPostbucklingof Thin-WalledCompositeStiffeners," ComputingSystemsin Engineering,Vol. 2, No. 1, 1991,pp. 1-16. 12. Noor,A. K. andPeters,J. M., "Strategiesfor Large-ScaleStructuralProblemson High-Performance Computers,"Communicationsin AppIied NumericalMethods,Vol. 7, 1991,pp. 465-478. 41

N92-25913

Computer

Codes Developed and Under Development at Lewis Christos C. Chamis NASA Lewis Research Center Cleveland, Ohio

. _,JC BLAt;K

NOT F!L ._t;D

43

Codes IPACS

The objective of this summary is to provide developed or under development at Lewis and with some typical early results.

a brief description (2) the development

of: status

(i) of

The computer codes that have been developed and/or are under development at Lewis Research Center are listed in the accompanying Charts 1 - 5. This list includes (i) the code acronym, (2) select physics descriptors, (3) current enhancements and (4) present (9/91) code status with respect to its availability and documentation. The computer codes llst is grouped by related functions such as: (i) Composite Mechanics, (2) Composite Structures, (3) Integrated and 3-D Analysis, (4) Structural Tailoring, and (5) Probabilistic Structural Analysis. These codes provide a broad computational simulation infrastructure (technology base-readlness) for assessing the structural integrity/durability/reliability of propulsion systems. These codes serve two other very They provide an effective means of technology transfer depository of corporate memory.

CODES

DEVELOPED

STRUCTURAL

BY AND ARE AVAILABLE

MECHANICS

Probabilistic Code

BRANCH,

Structural

Probabilistic

Structural

as the analysis

Analysis

functions: (i) they constitute a

FROM

THE

2 Oct 91

Analysis

Description/Current Enhancements

Name NESSUS

important and (2)

Status

includes

module/component

MHOST

risk and

Available

with

documentation

reliability CLS

IPACS

Probabilistic

Loads

Simulation

Shuttle

Available

with

Main Engine components/loads based on deterministic models

simulation

documentation

Probabilistic

of Composites/

Development

Couple

PCAN

Structural

Analysis

with NESSUS

Chart

44

for Space

1

CODES

DEVELOPED

STRUCTURAL

BY AND ARE AVAILABLE

MECHANICS Structural

Code

BRANCH,

FROM

2 Oct 91

Tailoring

Description/Current Enhancements

Name STAHYC

Structural

Tailoring

Computational

Status

of Hypersonic

efficiency,

THE

Structures/

Operational

documentation

STAEBL

Structural

STAEBL/ GENCOMP

Structural Tailoring Structures/Improved documentation

STAEBL/AERO

Structural Tailoring of Engine Blades for Aerodynamic Performance and Flutter

Completed and documented

STAEBL/TURBINE

Structural

Tailoring

of Turbine

Completed

& documented

STAT

Structural

Tailoring

of Swept Turboprops

Completed

& documented

CSTEM

Coupled

Tailoring

of Engine

Blades

Completed

of General Composites finite element and

Operational no documentation

Blades

Structural/Thermal/Electromagnetic

Tailoring/Gain

& documented

Available with documentation

familiarity

Chart 2

CODES

DEVELOPED

STRUCTURAL

MECHANICS

Integrated Code

and 3-D Inelastic

and large problem

FROM THE

2 Oct 91

Analyses Status

Lewis-owned Finite Element Analysis Computer Code - based on mixed iterative scheme/add mix-element

3.D INAN

BRANCH,

Description/Current Enhancements

Name MHOST

BY AND ARE AVAILABLE

Available with documentation

capabilities

A compilation of 9 different 3-D finite element codes for nonlinear structural and stress

Available with documentation

analysis with progressive level of sophistication, nonlinear simulation models/Dormant - needs code user familiarity BEST3D

Boundary Element with heat transfer

Structural

ESMOSS

Engine

Modeling

Structures

Dormant COSMO

Analysis

Software

code

Available with documentation

System/

Available

- needs code user familiarity

Component Specific Modular for Hot Engine Structures/Dormant - needs code user

with

documentation Available with documentation

familiarity

Chart 3

45

CODES DEVELOPED STRUCTURAL

BY AND ARE AVAILABLE

MECHANICS Composite

Code Name

BRANCH,

Composite

Blade Structural

MHOST, add updated CODSTRAN

HITCAN

Structures

Composite

Durabilily

Extension

to complete

Analysis/Add

CODES

DEVELOPED

STRUCTURAL

Structural

Analysis/

METCAN

BY AND ARE AVAILABLE BRANCH,

FROM

Composite

Analyzer

Incorporate

damping

capability

Probabilistic Probabilistic

Integrated capability

Ceramic

features;

Status

Available

- PMC/

Composite to ICAN

Metal Matrix Composite

Analyzer/

Analyzer/rime

and

documentation

Matrix Composite ply/fiber

Analyzer

- based

from COSMIC

Development

Operational sketchy documentation Development

substructuring

Inlegrate Composite Analysis for Structural Composite Sandwiches/Dormant - needs recovery

THE

2 Oct 91

Mechanics

Integrated

stress

Available

with

documentation

capability

Metal Matrix Laminate Tailoring/Capability to tailor for specific life

Chart

46

Operational

4

MECHANICS

on progressive ICAN/SCS

Analysis/

Description/Current Enhancements

unloading CEMCAN

Development

structures

Composite Code Name

Operational

ICAN

Chart

MMLT

Status

High Temperature Composite Structural Computational efficiency, documentation

PICAN

2 Oct 91

Description/Current Enhancements

COBSTRAN

ICAN

FROM THE

5

Development

The

schematic

embodied

in

progressive of

the

in an

fracture

local

through

computer

in

various

composite

constituent initiation

closes

the

loop

materials

state

local

STRUCTURE

the to

illustration

structural

The

code

the

global

material

capability

specific similar

PROGRESSIVE

to

the

corresponding

global

for

it local

simulation

structural are

VIA

evaluated.

CODSTtTAN

o GLOBAL

GLOBAL

0

ANALYSIS

ANALYSIS

f,';._'F:n _ :-,

/ I I

time

feedback

FRACTURE

STRUCTURAL

/

same

design concepts to CODSTRAN.

effects

response

the

computational

and

of

at

continuous the

physics

the

structural

response

Thus,

the

simulation

synthesizes

And

permits

growth.

of

computational

composites.

which

and

where component/system and HITCAN have structures

COMPOSITE

in

global

accumulation

excellent for

behavior

inherent the

between

an code

structures.

materials

scales

decomposes

damage

performance COBSTRAN

1 represents

constituent

the

progressively local

Figure

integrated

STRUCTURAL _

/

\

A ;:-;:lT_r.

\ LAMINATE

I,"_o..',.__ I

LAMINATE_ THEORY

r ICAN PLY-_t'."':!ifl;_il)i";ii__/; __

\ \ \ \

COMPOSITE MICROMECHANICS THEORY

UPWARD _ INTEGRATED _ OR "SYNTHESIS"

,,. "%

/"

, .. .,,_!!i;il;i;i)ii_i_ PLY

"_.

_ /--.

/ P '

.,-.,

C.O, _M..P..O_T.. ,E,,,,,,iCS / _L_)_c_,n,_mn,-un /

d t"

U,--"

/

CONSTITUENTS

/ MATERIAL PROPERTIES

"_

P (m T, M) _-- --_ -_

Simulation

of Composite

Damage

and Fracture

Figure

I I / /

LAMINATE, THEORY #

/ /

J

Propagation

/

/

TRACED OR "DECOMPOSITION"

/

via CODSTR

TOP DOWN

AN

I

47

Typical during slit

results progressive and

obtained by fracture

subjected

to

using CODSTRAN to in this composite

internal

pressure

is highly localized exemplifying this deformation evolution in monitoring. in

The

Figure

remains

3. so

damage

corresponding

The

the

tolerance,

surface

defect

(damage

tolerance)

defect

location exhibits

simplistic aspects

P

the

= 288

AFTER

a

to

internal is

PSI

(1.379

growth

the

usefulness

and

to

4.

PLY

BEFORE

DAMAGE

some

internal that

with these

I LONGITUDINAL (PSI)

Fracture

of Plies

PA)

TO 14

1 Longitudinal

Composite

Stresses

after

l,,itial

Shell T300/Epoxy[902/&lS/90,/+lS/9%/TIS/9%]

Figure 2

in with

1 and 9.

shown and the plan,

the

pressure the two

simulation

process.

_ 6,895

is case

inspection shell

computational

(I PSI

this

difference

Obviously, of

deformation

slit

in

The

higher

IN

I g 2

embedded

However,

development

MPA)

Ply

48

and

STRESSES

PLIES

PROGRESSION PLIES 13 _

an

The

evolution surface

sensors to capture in service health

The

behavior.

component/system

2.

localized

Figure

fracture.

DEFECT

IMPOSITION

Figure

for

more

in

deformation a longitudinal

locating tests or

pressure

shown

damage

structural

demonstrate

structural

in of

even

the with

catastrophically.

damage

limited to

is

"brittle-fracture-llke"

examples of

the

prior

exhibits

fractures

respect of

shown

pattern

evolution

shell

with

the

are

difficulty verification

deformation

deformation

until

between

the either

assess shell

embedded rather in

all

P

-

344

PSI

(2.375

MPA)

PLY I LONGITUDINAL STRESSES (PSI) (I

IHITIAL DEFECT PLIES

PSI

-

G,SgS

PA)

IN 9

&

220000.

18

19S000.

IMMEDIATELY BEFORE I

&

2

PLIES

16B000.

FRACTURE

158080.

IS000B. If

Ply

1 Longitudinal

Composite

Shell

Stresses

at 2.375

MPa;

before

Ply

1 Fracture_

T300/Epoxy[90_/=ElS/902/+lS]90_/_=lS/90_}

Figure 3

400

....

2.758

350 t

2.413

g

_ 250

_

A Defect in plies 1 & 2 (Case II)

1.724

tl/ ° °e_°_ 'n_''e__ _ _°_°°__v_ 200_

_

1.379

150 I 0.0

,

0.'2 DAMAGE

Damage

Propagation

Composite

Shell

wlth

,

, 0.4

1.034

(_)

Pressure

"r300/Epoxy[DO2/_-15/90_/=l=lS/90_/_FIS/90_]

Figure 4

49

Modules from the various codes in the llst can be stacked up (assembled) to develop computational simulation capability for specific structural response. The schematic in Figure 5 illustrates a combination to evaluate acoustic fatigue in composite panels In a hygrothermal environment. The combination of codes include: (I) CSTEM for acoustic source, (2) ICAN for composite properties synthesis, (3) MHOST for structural dynamic analysis due to acoustic excitations, (4) ICAN for ply stresses and strengths and (5) ICAN for cyclic load effects.

Computational

Simulation

of Acoustic

R.T. Constituent Properties

Fatigue

:-............. , /CAN _

_

EnvironmentDegraded Properties

Vibrating Panel

l

Acoustically Excited Panel

Acoustic Pressure

Dynamic Force Response MttOST_

CSTEM I

time

time

/CAN

Safety

I

_

No. of Cycles Figure

511

5

__1

Ply Stress/ Strength

Typical results from the computational simulation of acoustic fatigue on composites are shown in Figure 6 where the remaining strength in terms of margin of safety is plotted versus the number of cycles. Three different curves are shown: (i) The bottom curve is the base case. It is for a [(0/± 45/902)3] AS/E laminate at room temperature conditions. (2) The middle curve is for the base laminate at (200°F, I% moisture by weight) environmental conditions. The top curve is the base laminate with rearranged plies. Environmental effects enhance composite fatigue because they tend to soften the composite. Ply stacking sequences can be selected to significantly increase acoustic fatigue provided that other design requirements are not violated. The significant observation is that the infrastructure available in the computer codes listed in Charts 1 - 5 provide a base to tackle a variety of problems as they arise.

Demonstration:

acoustic

fatigue

0.60 .... : :_;,.

0.48

....

>.,

/

.............

([45/0/-45/9012)

;L,Q._ -- . ./-.

s

" ......................................................................................................

(]3 N-,-.

O9



0.36

4--"

o ED

""_,_-(200

°g, 1%

Moisture)"Q...

0.24 *.

0.12

.

Base

Case

-

. *.'-%

',,

0

I

10

5

6

7

10

10

Number

I__LLIJJ

8 10

10

9

of Cycles

Figure 6

51

The major elements of the Advanced Composites Technology Program are depicted within the ellipse in Figure 7. These elements include activities in all major aspects of advanced composites technology: {i) Constituent materials development and characterization (top). {2) Demonstration of these constituent materials in simple structural elements {right). {3) Structural components made from these simple elements {bottom right). (4) Analysis methods development {bottom left). (5) Design and fabrication process {left). Another small element of this relatively inclusive program is the development of probabilistic methods to incorporate the uncertainties associated with the major technology elements. These uncertainties are depicted schematically around the ellipse in Figure 7 next to their respective program element.

ADVANCED (,4 Bold

New

COMPOSITE

Program

in Composites

TECHNOLOGY Research

& Technology)

I

Probability

J%

/ I

°%%'_'I_I' ] "'_//I/I I\\

IJ

S,re.. S,,.,,_.

Probab,,,,y L//._/__l A

1_, _

._-_,

/

.

_

Pr°b'b"tY I

lJ

Probability

/

/ Magnitude

Crileria

Figure7

52

]

oo=,_"a°"'e

/ __-_

"e'_°°'°I

_

I

/

The different

probabilistic computer codes.

Probabillstlc

Integrated

capability probabilistic

in

methods to The first Composite

for

two

uncertainties

are

integrated

for

using scale

uncertainties

of

40

the

process

The -

the

available

result

different

are is

computational

simulation

in

(bottom).

different

ICAN.

as

probabilistic

composite

properties

the

composite uncertainties,

integration

description which

accepts

These

inherent

Additional

introduced

the

code and

are

progresses

of

the

required

to

fully

composite.

Probabilistic

Simulation

Composite Material Level

of Composite

Deterministic Properlies f/:.__

Mechanics

with PCAN

Fabrication Variables

Probabilistic Propedies

-_ _ PI)F

le o o o o oL-_l-/_'-%-_q lo_o o.o.0 ? ooL2.__pt I= = = _ _ ___jpv-

Laminate

embodied into two as PICAN for

in Figure 8. The material properties

variables

through

descriptors

scale.

will be identified

The

illustrated constituent

upward

mechanics

composite

to

characterize

fabrication

composite

respective

from

Analyzer.

PICAN is schematically uncertainties for 29

uncertainties scales

be developed of these is

40

tI, OI Fabrication Variables

Properly

Prolierly

I 0

=3 (I

"'"

_(

4o

Ply

I

PI)F

tp, 0p

I

0........ 0 0 0 ]:".-1

Fabr |cation Variables

Property

PDF I o_o o o I_'--"

Subply

37

ts, 0 s Property

/\

l"rolleily

CDF

Fabrication

I

-

Properly

Variables

Constituents (fiber/matrix)

[ _'-_-["i_ ._._//f-J_

17 for tiber 12 for matrix

fvr, vvr Property

NOTAIION:

I = CDF

lhickness. =

Cllmlllalivo

0 =

nfisnliqnmeld, Dishihulion

fvr Ea]clion,

=

fiber

volume

Sulls(:ripls

ralio,vvr I =

Figure

"-

=

void

laminale,

p

volume =

ply,

ralin, s

=

PDF

=

probnbilily

(|e.sily

EJnc|iol}

_uhllly

8

53

Probabilistically "laminates and

for

values major

are two are

standard

for

ratio,

Figure

PICAN

in

9,

results

Figure

deviations

included

Poisson's

results in stiffness.

described

tabulated

9. on

though

are

preliminary,

lower

stiffnesses

side

All

line)

VERIFICATION

l_aminale

either

comparisons. (last

for

Probabilistic the

of the

verify

boulld

two

PICAN

mean.

111.5"111

different

given

for

Average values,

standard predictions

LAMINATE

(111c.,'111-2o)

[0I + 45_I0/±

the

three

are

experimental

within

FOR

of

values

experimenlal value

the

except

the

deviations. for

The

laminate

STIFFNESS

llpper houild (111_711 { 2o'}

45],

Long.

tllodilhlS

(MSI)

5.40

6.19

6.30

6.98

Trans.

niodiihls

(MSI)

2.46

3 .(17

3 O8

3.68

.l_lliZ;ll tlll)(hlhls

([tl']_[)

3.3.1

3.84

3.21

4.35

0.690

(}.8116

0 803

0.922

Majol

Poisson's

ralio

'

[0/_t:45/0/90/0)], l.ong,

lnl_duhls

(MSI)

11.41

13.30

131K)

15.09

'rranL

inodilhls

(M,_I)

3.69

4.30

4.20

4.96

(MSI)

1.40

1.59

1.50

1.78

ratio

0.276

0.313

0.325

0.350

[.ong. Illodulus

(MSI)

6.12

7.15

6.68

8.18

Trans.

(MSI)

6.12

7.15

6.62

8.18

2.37

2.72

2.34

3.07

0.290

0.317

0.350

0.344

Shear modulus Major I'oisson's I(0/+45/90),1,

,qlicar

Majoi

inoduhis lllodulus

(M_I)

PoiSSOli'S ialio

Figure i

54

9

mean

experimental

The other computer code under development as a part of the ACT program IPACS, Integrated Probabillstic Assessment of Composite Structures. This consists of PICAN and NESSUS with modules from COBSTRAN for automatic finite element model generation and composite configuration description. A schematic the computational simulation capability in IPACS is depicted in Figure i0. Preliminary probabilistic results obtained from IPACS of a composite panel, loaded in compression (Figure II), are tabulated in Figure 12. Inclusion of probabilistic boundary conditions for two panels appear to verify IPACS' predictions for buckling loads. A few summary remarks are listed in Chart 6.

IPACS

: Inlegraled

Probabilistic

Assessmont

of Composito

is

of

Slrucluros

COMPONENTS

ELEMENT

_

_

FINITE

ELEMENT

_

FINITE

GLOBAL

GLOBAL

.a j LAMINA

TE

(

N_SSUS

_)

LAMINA

LA

_

°OMPOS,TE %

MICRO-MECHANICS THEORY

I I I

TE

LAMINATE

'_'

....OM OS.E MICRO-MECHANICS THEORY

NONUNEAR MULTIFACTOR MODEL CONSTITUENTS

MATERIAL

PROPERTIES

P - F(I+ T, M)

Figure I0

55

GEOMETRY

-:/

OF

THE

PLATE

-/ Figure il

II'ACS

VERIFICATION

I ;lnlhl;llc

FOl+t BUCKLING

lowt'r

ht_tllld

(nlcm,

lilt'till

2,0

I+,OAI)S

CXl+elin+cnlal

Ulq+Ct llmmd

vahlc

...................................................

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I crack I length (ram)

o Test B

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Average Half Crack Length (ram)

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average crack predicti0n measurements

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Cycles (thousands) Figure

136

15

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i

50

60

were

crack

as

cycles

whereas,

the

the

cracks

growth

plotted

cycles;

exceeded

with

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interaction

are

predictions

measured

proximity rates

holes

of

the and

growth

sheets

crack

and

AIBE

the

open

Fatigue

evaluating

developed

crack

thick

lengths

lengths

average growth

The of

for

was

fatigue

co-linear

lengths.

cycles.

method

cracks

2.3-mm

hole.

crack

DAMAGE

(AIBE)

wide,

each

crack

load

crack

code

of

within

than

interacting

equal

unequal

on

closer

element

contained

of

MULTI-SITE

multiple

sides

method

the

OF

boundary

on

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basis

were

The

computer

both

versus

100%.

for

conducted

The out

crack

a

were

2024-T3.

propagating

MECHANICS

unequal

predictions as caused

much

as

-25918

Analysis and Design Technology for High-Speed Aircraft Structures James

.=

F

H. Starnes, Jr. and Chades J. Camarda NASA Langley Research Center HamptOn, Virginia

137

INTRODUCTION

Viable supersonic and hypersonic aircraft structures must be structurally efficient and designed to operate reliably with combined mechanical and thermal loads. To provide such structures requires the development of verified structural analysis and design technology that is necessary to predict the response and failure characteristics of wing and fuselage structures made from advanced metallic and composite materials. Research is being conducted at NASA Langley Research Center to understand the response and failure characteristics of high-speed aircraft structures and to develop the necessary structural analysis and design technology for future high-speed aircraft. The present paper describes selected recent high-speed aircraft structures research activities at NASA Langley Research Center. Selected topics include: the development of analytical and numerical solutions to global and local thermal and structural problems, experimental verification of analysis methods and identification of failure mechanisms, and the incorporation of analysis methods into design and optimization strategies. The paper describes recent NASA Langley advances in analysis and design methods, structural and thermal concepts, and test methods.

138

AIRCRAFT

STRUCTURES

RESEARCH

High-speed aircraft structures research at NASA Langley Research Center is focused on the development of structural mechanics technology for supersonic and hypersonic aircraft primary structures. A goal of the research is to understand the thermal and structural behavior of complex structures made from advanced metallic and non-metallic materials using advanced fabrication techniques. Another goal is to develop structurally efficient and cost-effective structural concepts which exploit the beneficial characteristics of advanced metallic and non-metallic composite materials.

Provide the scientific basis and structural mechanics technology

for

aircraft primary structures

Develop structurally

efficient, cost-effective

structural concepts that

exploit the benefits of advanced composite and advanced metallic materials

139

STRUCTURAL

MECHANICS

RESEARCH

APPROACH

The key to understanding the physics of a structural mechanics problem is the ability to conduct precise structural and thermal experiments. Optimally designed experiments, which insure satisfaction of prescribed boundary and loading conditions and the accurate measurement of response quantities, are essential. Experiments are designed so parameters can be varied systematically and representative failure mechanisms can be identified and understood. The development of verified analytical methods, whether classical or numerical or combinations of both, is closely coupled to the experiments. The ability of the analysis methods to predict accurately the actual response and failure mechanisms verifies the methods. Anomalies in the correlation between analysis and experiment are resolved by careful studies of the observed behavior and, if necessary, additional experiments are conducted and improved analytical methods and models are developed. Once the analytical methods are verified and an understanding of a given problem is assured, the next logical step is the appropriate simplification of the analysis to increase computational efficiency and enable its incorporation into a formal optimization or structural sizing procedure. During the optimization process, many analysis and response sensitivity calculations must be performed and, hence, it is often necessary to simplify the analyses as much as possible to make the optimization process tractable. Iteration between the development of analysis and optimization procedures is necessary to insure accuracy of the analysis and proper representation of constraint boundaries. Iteration between experiments and optimization methods development is needed to assure that optimally designed structures represent actual physical behavior and to insure an accurate physical description of the response. The overall goal of structural mechanics research is to provide a better understanding of the physics of the problems of interest, including the true limits of performance, which leads to less conservatism in the design and, hence, a more structurally efficient design for wing and fuselage primary structures.

!

f_

140

Y

Experiments

_"

"_

" (Des,gn)

"_

J

_iMathematics)

• Systematically * Understand , Identify STRUCTURAL

Computational

) _

vary parameters true limits

failure

MECHANICS

Methods

of performance

mechanisms RESEARCH

APPROACH

141

STRUCTURAL

ANALYSIS

AND

DESIGN

TECHNOLOGY

One contribution that will decrease the time needed to design a new aircraft structure is a structural modeling tool that will decrease the time needed to develop a discrete structural model of a complex aerospace vehicle. Work is underway at NASA Langley to enhance the Solid Modeling Aerospace Research Tool (SMART) to enable rapid structural modeling of external and internal structure from a given aerodynamic shape. In addition, it is intended that the enhancements to SMART will allow the rearrangement and resizing of internal and external structural elements in a rapid manner. Both global and local analysis methods are being developed to predict the structural and thermal response for static and transient, linear and nonlinear problems. Some of the analytical methods currently being investigated are: advanced reduced basis methods, operator splitting techniques, flux- or stressbased finite element algorithms, Ritz-based methods, and classical solution methods. Several methods for optimizing large structural systems, such as a future supersonic transport wing which has thousands of degrees of freedom and is subjected to hundreds of mechanical and thermal constraints, are currently being explored. Equilibrium programming and other structural sizing methods are being developed to address the structural optimization of large nonlinear systems. Efficient methods to calculate structural and thermal sensitivity derivatives are being implemented into existing general-purpose finite element codes to facilitate formal optimization and to explore other uses for sensitivity derivative information such as parameter estimation. These structural sizing tools are being used to tailor structural designs to exploit the beneficial properties of advanced materials. Structural

modeling

aerodynamic

tools for internal

external

Detailed and local analysis thermal loads optimization constraints

Sensitivity parameters

142

analyses

configurations

from

shape

Global analysis methods and thermal loads

Design, thermal

structural

for combined

methods

and tailoring

to identify

that affect

structural

mechanical,

for combined

methods

important

pressure

mechanical

for mechanical

geometric

performance

internal

and

and material

and

THERMAL-STRUCTURAL

CONCEPTS

The degree of coupling between the structural, thermal, and fluids disciplines increases proportionally as the speed of the vehicle increases. For a hypersonic vehicle such as the National Aero-Space Plane, which is designed to cruise at Mach numbers exceeding 16 and to fly single stage to orbit, the selection of a hot structures concept, an insulated structural concept, and a cooled structural concept is not straight forward and often requires re-evaluation of the concepts at the vehicle design level. A good understanding of fluid flow, heat transfer, and structural mechanics is often necessary early in the design cycle to insure proper synergism in the design. Examples of solutions to coupled problems include the design of a refractory-metal/refractory-composite heat-pipe-cooled wing leading edge and a liquid-metal-cooled engine cowl leading edge. Both of these concepts will be discussed in detail later in the paper. Supersonic vehicles such as a future supersonic transport may not experience the same degree of coupling between the thermal and structural disciplines as a hypersonic vehicle; however, important structural design options will be governed by heat transfer. For example, the selection of wing structural concepts which contain fuel may be governed by the inherent insulative properties of a sandwich structure that may be lighter in weight than a stiffened structure with insulation. Organic composite and metallic structures will be compared in the preliminary design of a supersonic transport. Cost is an important consideration in the competitiveness of a commercial supersonic transport in addition to weight. Also, damage tolerance, durability and thermal stability may become critical design constraints in addition to traditional strength and buckling constraints. Details of preliminary studies for a wing structure will be presented later in the paper. Some hypersonic structural concepts currently being investigated include: a carbon-carbon elevon (hot structure), a refractory-composite/heat-pipe-cooled wing leading edge (passively cooled structure), and a liquid-metal-cooled engine cowl leading edge (actively cooled structure). Structural materials for these concepts include advanced refractory-composite materials and advanced metal-matrix composites.

143

Speed, weight, cost, and supportability - Uncooled or hot structures - Cooled structures

influence concept selection

- Thermal protection systems and insulated structures Current HSCT wing and fuselage concept candidates - Sandwich structure - Stiffened-skin structure with or without fuel tanks and fuselage insulation - Organic composites and metals Some current HSCT structural issues Some -

Weight and cost Damage tolerance and damage containment Durability for 60,000 flight hours at Mach 2.4 cruise Thermal stresses and thermal stability at global and local levels current hypersonic structural concepts Actively cooled structure C/C, C/SiC, advanced metal matrix Heat pipes THERMAL-STRUCTURAL f

144

CONCEPTS

TEMPERATURE

i

DISTRIBUTIONS FOR CIVIL TRANSPORT

HIGH-SPEED WINGS

SUPERSONIC

Temperatures of a future high-speed supersonic civil transport (HSCT) wing were calculated for two different flight Cruise Mach numbers. Temperatures were calculated assuming radiation equilibrium on the heated surfaces and neglecting conduction. As shown in the upper left figure, a Mach 3 cruise flight condition results in temperatures close to 500 °F, 50 ft. aft of the leading edge. Corresponding maximum temperatures for a Mach 2.4 cruise flight condition are approximately 300 °F. The large difference in wing temperatures between a Mach 2.4 and a Mach 3 cruise condition has a significant impact on the selection of materials to satisfy the life and durability requirements of the vehicle. Lower-surface skin temperature distributions for both the Mach 3 and Mach 2.4 cruise flight conditions are shown in the figures at the right. For a Mach 3 flight trajectory, temperatures over the acreage areas on the lower surface of the vehicle are about 460 °F and temperatures along the stagnation lines of the wing leading edges are approximately 525 °F. Temperatures along lower surface acreage areas for the Mach 2.4 flight case are 275 °F and are 315 °F near the leading edges. Temperature gradients through the depth of a threedimensional model of a section of the wing bounded by ribs and spars is shown in the figure at the lower right for a Mach 2.4 flight condition. The model accounts for flow of heat by conduction near massive sections of the wing such as ribs and spars. The model accounts for unsteady flow of heat through the honeycomb wing skins to the fuel contained within the wing structure. Detailed three-dimensional thermal models are necessary to predict accurately the temperature gradients which are necessary for accurate determination of thermal stresses.

145

WEIGHTS AND STRESS SUPERSONIC CIVIL

RESULTANTS TRANSPORT

FOR WING

HIGH-SPEED COVER

Stress resultants in a future high-speed supersonic civil transport wing cover are shown in the figure. Thermal and mechanical loads for a 2.5g pullup maneuver were used to size the vehicle and to determine stresses and unit weights. Two different materials were used for the wing structure, a conventional titanium alloy, Ti-6AI-4V, and a quasi-isotropic graphite reinforced organic matrix composite material. The normal stresses in the wing upper cover panels are shown in the figures at the right. As shown in the figure, maximum normal stresses occur in the section of the wing where the leading edge crank occurs. In addition, thermal stresses were considerably lower for the composite structural design than for the titanium structural design due to the lower coefficient of thermal expansion for the composite material. Unit weight distribution in the upper wing cover is shown in the figure at the left. As expected, the weight of the composite wing cover is much less than that of the titanium wing cover.

Unit wei

146

Iht, Ibs/ft 2

INTERACTIVE INTERNAL

MODEL GENERATION CAPABILITY STRUCTURAL CONFIGURATION

FOR AIRFRAME RESEARCH

The time required to generate a three-dimensional structural finite element model from an external aerodynamic shape can be very long, on the order of months. Work is underway at NASA Langley to enhance the Solid Modeling Aerospace Research Tool (SMART) to enable rapid structural modeling of external and internal structure from a given aerodynamic shape. Currently, the computer time required for linear structural analysis is much less than the actual time to create and modify a structural finite element model. As shown in the figure, the purpose of the present research is to reduce the time to model internal and external structure from months to days. This reduction in modeling time will enable a more rapid assessment of internal structural dimensions and arrangements and speed up the optimum placement and sizing of internal structure. Planned enhancements will enable the generation of internal structural configurations such as those shown and enable the rapid rearrangement of internal structures as illustrated by the different structural arrangements in the models shown. Planned enhancements to SMART include a means for: 1) creating and editing structural elements for the wing and fuselage; 2) integrating wing and fuselage structural components; 3) integrating tail and fuselage components; 4) remapping aerodynamic loads data to the structural model; 5) applying point and distributed loads to the structural model; and 6) preparing loads data for visual presentation. Examples of structural elements and components to be modeled include wing spars, ribs, shear webs and cover panels and fuselage skin, frames, bulkheads, Iongerons, and keel beams.

147

DESIGN CONSTRAINT CRITICALITY SPEED SUPERSONIC CIVIL

FOR MINIMUM WEIGHT TRANSPORT WING DESIGN

HIGH-

A future high-speed supersonic civil transport (HSCT) model was optimized using formal optimization procedures to satisfy element stress, local buckling, and displacement constraints. The vehicle structure was sized for a 2.5g pullup maneuver and a 12-foot tip deflection constraint. Sine-wave rib and spar elements were used to minimize thermal stresses in the wing and honeycomb sandwich panels were used for the upper and lower cover panels. Various regions of the structure were governed by different design constraint conditions, either element stress, local buckling or minimum gage constraints. The degree of criticality of each element can be easily monitored by using a simple color coding scheme to identify regions where constraints are critical or satisfied. Upon investigation of a critical region, it can be determined which constraint is approaching

criticality.

Element

Stress

and

Local

Buckling

Constraints

12 ft. Tip Deflection Constraint ...... 2.5g Symmetric Pull-up Maneuver

CONSTRAINT_ CRITICAL

m

Honeycomb

148

Sandwich

Upper

Cover

Panels

SATISFIED

i

I

I

SENSITIVITY OF CIVIL TRANSPORT

MINIMUM-WEIGHT WING DESIGNS

HIGH-SPEED TO MATERIAL

SUPERSONIC PROPERTIES

The sensitivity of a future high-speed supersonic civil transport (HSCT) to the wing-tip deflection constraint is illustrated in the figure. The minimum-weight wing design of a candidate supersonic transport wing is plotted as a function of wing-tip deflection limit for three different structural material choices: a titanium alloy(Ti-6AI-4V), an advanced aluminum alloy (FVS0812), and a quasi-isotropic graphite-bismalimide (Gr/BMI) material (IM7/5260). When the tip displacement is relaxed (e.g., for a tip displacement limit of 15 feet), the titanium and advanced aluminum designs are similar inweight and considerably heavier than the Gr/BMI composite design. As the dip deflection limit is reduced and approaches 5 feet, the advanced aluminum and Gr/BMI designs become similar in weight and considerably less than the titanium design. The advanced aluminum chosen is similar in stiffness to a quasi-isotropic Gr/BMI composite structure. The benefits of the composite material in producing a lighter weight design can be realized if tailoring the structural design to exploit the benefits of the directional properties of the material is permitted. Future work will address the potential benefits of structural tailoring on minimum weight design.

2.5 G Supersonic Strength,

Buckling,

Pull-up

and Tip Displacement

Constraints

70000 __,,,,__Ti-6AI-4V

60000

50000

Minimum Wing Weight, Ibm

_AI

(FVS0812) Gr/BMI (quasi-isotropic)

4000£

30000 20000

10000

0 5

10 Tip Displacement

15 Limit, ft

149

STIFFENED

PANEL

DESIGN

CODE

m

PASCO

The Panel Analysis and Sizing Code (PASCO) (refs. 1 and 2) is a computer design code which combines a rigorous buckling analysis with a nonlinear mathematical optimization algorithm to perform structural analysis and minimum-weight optimization of longitudinally-stiffened composite panels. PASCO is restricted to prismatic structures having an arbitrary cross section. The PASCO program can accommodate the design of fuselage and wing structural panels which can be loaded by any combination of in-plane loads, lateral pressure and thermal loads. Initial "bow-type" imperfections in the panel geometry can also be analyzed using PASCO. PASCO uses a linked-plate representation of geometry in which individual plates are assembled to construct a structural panel cross section such as those shown in the figure. Two or more individual plates are assembled to form a substructure, which is repeated to create the entire panel cross section. Plates are constructed as a balanced symmetric laminate of a prescribed number of plies with orthotropic material properties. PASCO can perform a local or global buckling analysis of a stiffened panel for various combinations of free or supported boundary conditions along the panel edges. Local buckling loads and mode shapes, such as those shown in the figure, are routinely calculated by PASCO. In addition, PASCO can perform a structural analysis of the loaded panel and minimize panel weight subjected to various stress and buckling constraints. A Macintosh version of PASCO has been developed (ref. 3) and an interactive graphical interface to the Macintosh version of PASCO, called MacPASCO, has also been developed. The graphical interface was created to simplify user input and model checkout (ref. 4). PASCO, the Macintosh version of PASCO, and the graphical interface, MacPASCO, are available through COSMIC.

150

STRUCTURALPANEL

-----

LOADING

BUCKLING MODE UNDEFORMED

BLA i i

e

COMPLEX BUCKLING MODES OF ARB ITRARY PANEL CONFIGURATIONS

STIFFENED

,

PANEL

BOW-TYPE IMPERFECTION

DESIGN

CODE

-- PASCO

151

STRUCTURAL EFFICIENCY DETERMINED GRAPHITE/THERMOPLASTIC

FOR OPTIMIZED PANELS

One application of PASCO to size structurally efficient stiffened composite panels is shown in the figure. Minimum weight designs for compression-loaded graphite-thermoplastic panel concepts were developed for a range of loading intensities and the results are compared with current aluminum designs in the figure. The weight, normalized by the planform area, A, and the panel length, L, is shown for different values of applied load, Nx, normalized by the panel length. Two graphite-thermoplastic concepts are compared, one with a corrugated core and two face sheets and one with a hat-stiffened configuration. The concepts are based on a cost-effective fabrication process that allows the corrugated core and hat-stiffened section to be thermoformed and subsequently attached to the face sheets.

-4

.............................................................

20 x 10 j- Commercial aircraft | aluminum wing

.,/

| compression panels _. [. _ 101 __..--r"TC/__j'_

Graphite-thermoplasti. . c panel_ _Corrugated-core

ibiin 3

at-sti

I*.... 5O0

100 NxtL,Ibtin

i

i : [:7' ; b

152

2

L---_ 1000 --_

STRUCTURAL

EFFICIENCY

PANELS

IS

OF

INSENSITIVE

OPTIMIZED TO

CORE

SANDWICH DENSITY,

COVER

Pcore

A structural optimization study of a sandwich panel concept with composite face sheets has been conducted which includes damage tolerance constraints as well as strength and bucking constraints (ref. 5). The results of the study indicate that imposing a maximum strain constraint of 0.0045 in./in, will provide designs with thick enough face sheets to tolerate reasonable low-speed impact damage.

The

significantly compressive weights, minimum

results

of the study

indicate

that core

density

Pcore does

not

affect the weight, W, of the designs over a range of applied loads, Nx. Since core density did not strongly affect these

a heavier more damage-tolerant weight increase.

core

can

be used

for the design

design with

8 6

PCORE = 9.5 Ib/ft 3

W, 4 Ib/ft 2

__

• Orthotropic

I b/ft 3

facesheets

• Response mechanisms: global buckling, facesheet wrinkling, material failure

2

0

I

I

I

10

20

3O

• Damage tolerance _x < 0.0045

constraint:

in./in.

N x, kips/in.

153

EFFICIENT RITZ-BASED ELEMENTS DEVELOPED STRUCTURAL ANALYSIS OF BEAM AND PLATE

FOR THERMALSTRUCTURES

The structural design of supersonic and hypersonic aircraft requires the efficient and accurate calculation of structural temperatures, the transfer of these temperatures to a discrete structural model, and the efficient and accurate calculation of the structural response. Discrete thermal and structural models are often dissimilar and require some form of mapping to transfer temperatures from the thermal model to the structural model. In addition, discrete structural elements like beam and plate elements have no analogous thermal elements which can be used to calculate the temperature distribution through the element thickness. Thermal models require significantly more detail to predict the through-the-thickness variation of temperature. The objective of the present research is to develop thermal elements which are compatible with structural beam and plate elements. Compatible thermal and structural elements can reduce modeling time, problem size, and the computation time required to obtain accurate thermal stresses. Ritz-based thermal and structural elements were developed as a means to alleviate some of the problems associated with thermal-structural analysis. Structural and thermal energy functionals are developed which include parallel formulations for internal energy and the energy associated with boundary conditions. The Ritz method is used to develop the governing equations for the thermal and structural elements. Temperature and thermal stress results for a Ritz-based analysis of a heated beam are compared to linear finite element results as shown in the figure. The structure has mixed thermal boundary conditions and is fixed against translations and rotations at each end as shown in the upper sketch. Results from finite element thermal and structural analyses are shown for comparative purposes. Both the Ritz and finite element results were chosen from convergence studies which examined changes in the temperature and stress as a function of degrees of freedom. Convergence studies for the Ritz-based element required only an increase in the interpolation function order while finite element studies necessitated mesh refinement and associated changes in loads and boundary conditions defined at nodes. The Ritz-based analysis requires only 12 degrees-of-freedom for accurate prediction of temperatures and 34 degrees-of-freedom for accurate prediction of thermal stresses. The conventional finite element analysis requires 99 degrees-offreedom for accurate temperature calculation and 198 degrees-of-freedom for accurate thermal stress calculation. The Ritz-based elements are capable of representing mixed boundary COnditions including convection for a steady-state thermal analysis and prescribed displacements for structural analysis. Orthotropic and layered media can also be modeled with the Ritz-based elements. More detailed information on Ritz-based elements can be found in reference 6.

154

4O 100

225

Z

ends restrained against translation and rotation --o

prescribed

temperature °F

_/_G_'[_> heat load

Btu / in. Temperature

45

2O

375.

°F

324.

Thermal

Analysis

- Temperature

273

I

223 172 i_¸¸

_121

Ritz-based element

Finite element - 99 degrees of freedom

12 degrees of freedom

70.7 20.0

Stress -52.5

StrUctural

Analysis

- Thermal

Stress

-64.9

o x

ksi

-77.3

F

-89,6 -102

F

-114

Ritz-based element 34 degrees of freedom

Finite element - 198 degrees of freedom

EFFICIENT RITZ-BASED ELEMENTS DEVELOPED STRUCTURAL ANALYSIS OF BEAM AND PLATE

-127 -139

FOR THERMALSTRUCTURES

155

NASA/BOEING STUDY THERMOPLASTIC

OF POSTBUCKLING BEHAVIOR SHEAR WEBS WITH HOLES

FOR

Graphite-thermoplastic panels are being considered for supersonic aircraft applications. The results of an experimental study of graphite-thermoplastic shear webs with circular cutouts is shown in the figure (ref. 7). The cutout size was varied in the study from a diameter of 0 to 3 inches and the specimens were loaded to failure in a picture-frame shear test fixture. All panels buckled before failure. The results in the figure show the out-of-plane deflection as a "function of applied shear load for difference cutout sizes. All panels had out-ofplane deflections ranging from approximately 4 to 6 times the 0.080 inch-thick shear-web thickness.

5000 4000 Applied shear flow, Ib/in.

16-ply

quasi-isotropic d=0 /

Q

Failure

3000

/rd /?

= .75 in. d=l.5in.

.30

.40

2000 1000

.10 .20 0 Out-of-plane ................

156

_:_::

-.

deflection,

.50

e_

|_

.............................

in. ...........

............

_-=;:_;_;

..........

POSTBUCKLING

The

results

RESPONSE

of a typical

AND SHEAR

postbuckling

FAILURE WEBS

analysis

OF

THERMOPLASTIC

of a graphite-thermoplastic

shear

web with a 0.75-inch-diameter cutout is shown in the figure. Large shear stress gradients are shown in the right figure that correspond to the locations of failure in the panel shown in the lower figure. The analytical response prediction compares well with the test data as shown in the left figure.

_ 4000

Experiment I

3000F

Nonlinear analys_s | Thickness , *

| lb q'in.

........... __-_--stress

shear resultants

Ib Qmax = 396 in. _:i

Failure ,l_ r

q

200

W

.q

* |

q

d

q

looo_

0

1

2 W't

3

4

Qmin = -165 specimen

Ib In.

157

CARBON-CARBON

CONTROL SURFACE (UNASSEMBLED)

TEST

COMPONENT

Based on results of previous conceptual studies, it is believed that a refractorycomposite material such as Advanced Carbon-Carbon (ACC) offers significant advantages which warrant its selection for control surfaces on a hypersonic vehicle. A generic elevon configuration was selected which would carry significant mechanical loads and reach maximum temperatures as high as 3000 °F. At the present time the elevon system has been designed, fabricated and assembled. The elevon was fabricated by LTV Corporation under the direction of NASA Langley. The major carbon-carbon (C/C) and refractorymetal (Rene' 41) parts which compose the elevon assembly are shown in the figure. The C/C parts consist of a 3-foot by 5-foot built-up structure with rib and skin panels, a torque tube, ten rib-to-tube attachment fittings, a closure piece, and many C/C fasteners and nuts. Rene' 41 pieces include: attachment rings, lugs, fasteners and cleats used to join the C/C torque tube to the wing support structure. Sub-component testing has begun on the C/C torque tube at NASA Langley as will be shown later in the paper. Testing of the full-scale elevon component will be performed in the structures laboratory at NASA Dryden. Significant advancements in C/C design, analysis, and fabrication technology were necessary for fabrication of the test component. The large size of the test article and the need for close tolerances were a significant challenge that required advancement in the state of the art. Fabrication of the rib and skin panel built-up structure, the torque tube, and the rib-to-tube attachment fittings required significant expertise to develop. The high design torque loads and the large difference in coefficients of thermal expansion between the C/C torque tube and the Rene' 41 actuator lug posed a major challenge. The high design temperatures (up to 3000 °F) required the use ofc/c fasteners for the assembly and is the first application of C/C fasteners to a structure that will be subjected to cycllc thermal and mechanical loads. Further details of the C/C elevon can be found in reference 8.

158

I !

!

CARBON-CARBON

CONTROL

SURFACE

TEST

COMPONENT

(UNASSEMBLED)

ORtCtNAL BLACK

AND

WHITE

F;',_ E I>HOTOC, RApH

159

i

CARBON-CARBON

CONTROL

SURFACE

TEST

COMPONENT

(ASSEMBLED)

The figure illustrates a completely assembled Carbon-Carbon (C/C) elevon for a hypersonic vehicle complete with C/C fasteners and attachment rings and Rene' 41 fasteners and attachment pieces. The accurate fit-up and adherence to close dimensional tolerances is a testament to the significant advances in C/C

manufacturing

and

rigorous

fabrication

procedures

program.

OR_GIN,A,L P;,GE BLACK

-

160

AND

WHITE

PHOTOGRAPr_

made

during

this

ELEVON

A three-dimensional

NASTRAN

NASTRAN

MODEL AND DISTRIBUTION

thermal

finite

ITS

element

TEMPERATURE

model

of the carbon-

carbon elevon was developed to calculate detailed temperatures and temperature distributions. The detailed model was necessary to accurately predict temperatures and thermal loads necessary for accurate thermal stress calculation. Temperatures at critical regions where the refractory-metal Rene' 41 fasteners and fittings are located also necessitated accurate temperature prediction. The finite element model uses over 2000 elements and has over 11,000 degrees of freedom. Temperature contours in the elevon and torque tube for a generic flight profile which simulated ascent, cruise, and descent are shown at the right of the figure. Maximum temperatures in the ACC carboncarbon elevon are 3000 °F and maximum temperatures of the Rene' 41 fasteners are 1600 °F.

TEMPERATURE DISTRIBUTION 3100 _ NASTRAN MODEL

2800

2200

161

DETAILED

STRESS

ANALYSIS

OF TUBE

CARBON-CARBON

TORQUE

The carbon-carbon short torque tube is being tested to obtain preliminary performance data for a 9.5-in.-diameter torque tube constructed of 42plies of woven carbon-carbon material. All loads and attachments are similar to those of the carbon-carbon elevon torque tube which will be tested later. The short torque tube model, shown in the figure, was taken from a larger model which consisted of the torque tube, attachment rings, load arms, and support collar. The 0.5-inch-walls of the torque tube were modeled with plate bending elements having quasi-isotropic material properties. Cleat holes and bolt holes were included in the model since the proximity of these openings has an influence on the stress field. Mechanical fasteners were modeled with rigid beam elements which transmit only compressive loads to bearing surfaces. Perfect fit-up was assumed at all bolt holes and cleat holes. The torque loads are transferred to the tube at the bolt holes resulting in a clockwise rotation. These loads are reacted by the cleat holes of the support collar. The compressive bearing strains at the bolt holes occur on the opposite face from the compressive strains at the cleat holes. The largest compressive strains in the torque tube occur where the couple forces from the load arms are applied to the tube. The compressive strain limit of .0013 in./in, for a carboncarbon lamina is about one-third of the tensile strain limit. There is some local bending at the cleat holes and bolt holes since single-lap joints are used to transfer loads. A local three-dimensional finite element model was used to investigate bending effects. Displacements from the planar model analysis were specified as boundary conditions for the local model analysis. The outer fiber compressive strains from the solid model analysis were about 2.5 times greater than the membrane strains obtained from the planar model analysis. This maximum Value iS a.ppr0ximately equal to the allowable compressive strain specified by the LTV Corporation which fabricated the torque tube.

162

I I-

F-

Ee .onng14

.non?g4

CLEAT BEARING .ono494

iiiiiili_ i;i!!ii!i_N. .nn0283

.nonf1728

-.

nno

138

-,

n00340

-,

0n0550

r BEARING BOLT Z DETAILED

STRESS

ANALYSIS

OF

CARBON-CARBON

/ TORQUE

TUBE

163

REFRACTORY-METAL/REFRACTORY-COMPOSITE COOLED WING LEADING

HEAT-PIPEEDGE

A refractory-metal/refractory-composite heat-pipe-cooled wing leading edge concept, shown schematically in the left of the figure, is currently being considered for use on a hypersonic aircraft. The heat-pipe concept has the potential to reduce leading edge weight by 50 percent over an all actively cooled leading edge and to result in a more reliable and redundant design. In addition, the heat-pipe-cooled leading edge concept eliminates the need for active cooling during descent and even the more severe ascent portions of the trajectory. Elimination of active cooling from the leading edge design greatly reduces systems complexities and weight. The concept uses thin refractory-metal "D-shaped" heat pipes embedded within a refractory-composite structure. The heat pipes are spaced close to one another and arranged normal to the leading edge. The heat pipes cool the stagnation region by efficiently transporting heat aft to the upper and lower surfaces of the wing where the heat is rejected by external radiation to space. The heat pipes effectively isothermalize the leading edge because the mechanism for transporting the heat is very efficient and relies on the evaporation and condensation of a high temperature working fluid; lithium in this particular design. The heat pipes are self contained and require no external pumping for the lithium working fluid. The lithium evaporates in the stagnation region and condenses in the aft sections of the heat pipe. The liquid condensate is pumped back to the stagnation region by the capillary pumping action of an internal wick structure. The heat pipes are sized to be redundant in the event of an individual heat pipe failure and the refractory-composite structure surrounding the heat pipes is also designed to offer ablative protection in the event of a massive heat pipe malfunction. If active cooling is necessary during ascent, it can be accommodated by internal radiation to an actively cooled heat exchanger as shown in the figure. A thermal parametric trade study was performed (ref. 9) using a threedimensional finite element model of a portion of a single heat pipe, shown by the shaded region in the figure on the left. Maximum temperatures for a 0.5-inch-radius design are shown in the figure on the right for the case of an uncooled leading edge and an internally cooled leading edge design. Parameters varied in the study were the wetted length of the heat pipes and the heat-pipe spacing. As shown in the figure, if the spacing between heat pipes is less than 0.1 in., a 24-in.-Iong heat pipe cools the stagnation region sufficiently to reduce maximum temperature below a 3000 °F temperature limit for the refractory-composite structure.

164

REFRACTORY METAL/REFRACTORY COMPOSITE HEAT-PIPE-COOLED WING LEADING EDGE

-o-

uncooled

--o-

cooled

/----

L = 12 in.

3600

thp = 0"005 in'_

3400

tsic=0.01in.--__.__ ___.,,.

_

3200

H2 coolant

3000 Trnax, °F

__-D

layup

2800

L=36in._

__-

2600 2400

'- _/

\ -"_/

trc = 0.04 in. J

"

/

3-D weave _Reqion

\

modeled in FEA

2200 200( 0

t_ rh p = 0.25 in.

HEAT PIPES EMBEDDED IN REFRACTORY COMPOSITE WITH OPTIONAL INTERNAL RADIATIVE COOLING

0.04 Distance

0.08

0.12

0.16

between

heat pipes,

0.20 x, in.

THERMAL PARAMETRIC STUDY FROM 3-D FINITE ELEMENT ANALYSIS FOR R = 0.5 in.

165

CARBON-CARBON/HEAT-PIPE-COOLED STRESSES AT

A detailed thermal ACC4 carbon-carbon

THE

LEADING STAGNATION

EDGE LINE

THERMAL

stress analysis of a molybdenum heat pipe embedded structure, results in very high compressive stresses

within in the

molybdenum tube as shown in the figure (ref. 9). At elevated temperatures, the refractory-metal molybdenum "D" tube expands into the lower coefficient of thermal expansion refractory-composite structure. The linear structural analysis does not account for the relief in thermal stress by yielding of the metallic tube. In addition, the structural analysis assumes a perfect bond between the refractory-metal and refractory-composite materials. Methods for alleviating the high thermal stresses are currently being investigated. The use of a soft carbon strain isolator material placed between the metal "D" tube and the refractorycomposite differential stresses.

structure thermal

is currently being expansion without

investigated the creation

as a means of excessive

of allowing thermal

the

ay, psi _

coolant

'x t¢..¢

/"

Region modeled

__ in FEA

qs = 900 Btu/ft2-s R = 0.5 in. s =36 tc_c = 0.06 in.

y

166

in.

x = 0.5 in.

3-D Carbon-carbon

structure

THERMAL-STRUCTURAL

PARAMETER

ESTIMATION

Parameter estimation methods are currently being developed to determine thermal as well as structural parameters and to help facilitate correlation between experimental and analytical results. Parameter estimation techniques are currently being used to determine the thermal contact resistance of refractory-metal heat pipes embedded within a refractory-composite structure. The estimation procedure is implemented within a commercially available thermal-structural finite element program called the Engineering Analysis Language (EAL) System (ref. 10). The flow chart illustrated in the figure depicts the procedural flow which begins with the development of a finite element model which represents a physical experiment. Certain parameters are considered known constants in the finite element model and certain parameters are considered to be variable. Analytical results are compared with actual or test results and a measure of the error or lack of correlation between results is calculated. If the correlation is poor, the sensitivity of the response to parameter variations is calculated and a least-squares procedure is used to minimize the error and predict a new value for the parameters. The procedure is repeated until the error or lack of correlation between actual and calculated responses is reduced below some prescribed tolerance. A numerical experiment is illustrated in the figure to highlight the convergence of the parameter estimation procedure implemented into EAL. The transient thermal history of a point located on the outer surface of a tube heated internally is predicted numerically assuming a known value for thermal conductivity (kactual=0.0013875 Btu/in.-s-R). The estimation procedure begins with an initial estimate for kactual which is kcalculated=0.001 Btu/in.-s-R. The procedure automatically converges to the actual value for thermal conductivity in only three iterations. General methods for estimating multiple parameters of complex problems have been incorporated into the program. Future plans include extension of the methods to structural problems and the use of sensitivity information to optimally design experiments to determine accurately the variable parameter values.

167

THERMAL-STRUCTURAL

Initial Model

PARAMETER

ESTIMATION

[ !

Select Parameters _, Model with Compare Actual

I

re= 0.30

I

"";

ri = 0.25

k = '_

]



,





J

¢

Convergenceof Thermal Conductivity 1.5e-3

kactual

1.4e-3

= 0.0013875 •

k

1.3e-3

(Btu/s-ln-R)

I e

Update

Minimize Error

I Parametersl-

I (Least Squares)

lated

1.2e-3

1.1e-3 1.0e-3

i

0

I

I

i

I

2 Iteration

168

Btu/s-in-R O

i

I

3

i

!

4

ANALYSIS

OF

LIQUID-METAL-COOLED LEADING EDGE

NASP

ENGINE

COWL

Hypersonic vehicles experience extremely high aerodynamic heating because of the high Mach numbers that the vehicle attains while traveling within the earth's atmosphere. A particularly severe condition exists when the vehicle accelerates and the bow shock from the nose of the vehicle intersects the bow shock of the engine cowl lip. The shock-shock interference produces extremely high and local heating, 50,000 to 100,000 Btu/ft2-s acting over a region 0.01 to 0.02 inches wide. To predict accurately the thermal performance of a convectively cooled cowl leading edge subject to high local heating requires an accurate description of the internal fluid flow and heat transfer. Computational fluid dynamics (CFD) analysis of the coupled convective flow field and solid conduction to the cowl skin was used to predict accurately the maximum temperatures and temperature gradients within the thin copper skin of an engine cowl leading edge. Previous results, using engineering approximations to determine heat transfer characteristics, did not adequately represent the growth of a local thermal boundary layer and were overly conservative. A section of the curved cowl lip (see figure) was analyzed as a planar section. The schematic diagram in the figure is not to scale; the true horizontal scale is on the order of inches, the vertical scale is on the order of hundredths of inches, and the heat pulse width is on the order of thousandths of inches. The coolant enters the cowl lip with a uniform temperature and velocity profile. Velocity boundary layers develop and cause the velocity profile to change to one having a nearly uniform velocity core with regions of high shear near the walls. Near the region of the high heat pulse, a thermal boundary layer begins to form in the coolant. The coolant outside this thermal boundary layer is at, or very close to, the inlet temperature while the temperature within the thermal boundary layer is hotter than the inlet temperature. Results for a local 0.015-in.-wide heat pulse which has a magnitude of 50,000 Btu/ft2-s is shown at the right of the figure. The cowl lip walls are 0.02-in.-thick copper with a temperature limit of 1200 °F. Results of maximum surface temperature as a function of coolant velocity are shown in the figure for three different coolants: hydrogen, water, and liquid sodium. The high conductivity and thermophysical properties of sodium result in high heat transfer coefficients and lower maximum temperatures. Results of the study indicate that, depending on coolant velocity constraints, several liquids could potentially accommodate high local heating representative of the shock-shock heating condition for a hypersonic vehicle.

169

ANALYSIS OF CONVECTIVELY COOLED ....... ENGINE COWL L_DING EDGE

"

"_ _Coolant

Velocity boundary layers Thermal boundary layer :::¢

Metal skins

170

NASP

AIRCRAFT

STRUCTURES

RESEARCH

TOPICS

The development of verified structural analysis and design technology for future supersonic and hypersonic vehicles requires research on a number of topics as indicated on the figure. Advanced structural concepts are needed for costeffective structurally efficient designs. Structural tailoring can be used to exploit the beneficial properties of advanced materials. Failure often initiates at stress gradients in a structure, so gradient producing discontinuities and eccentricities must be understood. Local two-dimensional and three-dimensional analyses of these local gradients are needed that are consistent with global twodimensional plate and shell models. Nonlinear effects associated with postbuckling design philosophies and pressure and thermal loads must be accurately predicted analytically and minimum-weight designs developed for nonlinear structural response. Failure mechanisms must be understood and failure analyses developed to predict accurately the onset of these failure mechanisms. Damage tolerance requirements must be understood for future high speed vehicles and designs must be developed that safely tolerate local damage. The interaction between subcomponents and elements in built-up structures needs to be understood and minimum-weight joint technology needed to connect the elements and subcomponents is needed. Scaling laws for composite and metallic structures are needed to minimize vehicle development costs. Thermal effects and heat transfer into the structure must be predicted addition,

to determine thermal stresses light-weight thermal protection

concepts withstand

are needed. High-speed combined mechanical,

and thermal buckling systems and actively

aircraft pressure

of a structure. In cooled structural

structures must be designed and thermal loading during

to their

flight profiles so the interaction of these loads on structural performance must understood. All of the analysis and design methodology developed for highspeed vehicles must be verified in the laboratory with the appropriate experiments with panels and wing-box and fuselage-shell models. •

Structural

efficiency

studies

and advanced



Structural

tailoring



Gradients,



2-D global analysis with 2-D and 3-D local analysis



Postbuckling



Nonlinear



Failure mechanisms



Damage tolerance



Subcomponent



Scaling



Thermal



Thermalstresses



Combined



Panels and subscale

and anisotropic

discontinuities,

cutouts,

and geometric

analysis

be

concepts

effects and eccentricities

nonlinear

effects

and sizing procedures and failure analysis and low-speed

interaction

and optimum

laws for composite

andthermal

effects

joints

structures

effects and heat transfer

mechanical,

impact damage

into interior structure

buckling

pressure, fuselage-shell

and thermal

loads

and wing-box

models

171

REFERENCES

Anderson, M. S.; Stroud, W. J.; Durling, B. J.; and Hennessy, K. W.: PASCO: Structural Panel Analysis and Sizing Code, User's Manual. NASA TM 80182, November 1981.

.

Stroud, W. J.; and Anderson, and Sizing Code, Capability 80801, November 1981.

.

Structural Panel Analysis Foundations. NASA TM

Lucas, S. H.; and Davis, Randall C.: User's Manual for the Macintosh Version of PASCO. NASA TM 104115, September 1991.

,

Lucas, S. H.; and Davis, NASA TM 104122, 1991.

,

Randall

C.:

User's

Manual

for MacPASCO.

Cruz, Juan R." Optimization of Composite Sandwich Cover Panels Subjected to Compressive Loading. NASA CP 3104, Part 2, 1990.

.

Vause, R. F.: Compatible Thermal and Structural Elements for Thermal Analysis of Beam and Plate Structures. Presented at AIAA/ASME/ASCE/AHS/ASC 32nd Structures, Structural Dynamics, Materials Conference, Baltimore, MD, April 8-10, 1991. AIAA Paper 91-1154.

.

the the and No.

Rouse, M.: Effect of Cutouts and Low-Speed Impact Damage on the Postbuckling Behavior of Composite Plates Loaded in Shear. Part 2, A Collection of Technical Papers presented at the AIAA/ASME/ASCE/AHS/ASC 31st Structures, Structural Dynamics, and Materials Conference, Long Beach, CA, April 2-4, 1990, pp. 877-892. AIAA Paper No. 90-0966.

.

.

.

10.

172

M. S." PASCO: and Analytical

Ho, T.; Matza, E. C.; Medford, J.; and Watabe, S.: Design Concept for NASP Control Surface. NASA CR 18173, October, 1988.

Study

Glass, David D.; and Camarda, Charles J.: Preliminary Thermal/Structural Analysis of a Carbon-Carbon/Refractory-Metal HeatPipe-Cooled Wing leading Edge. Presented at the First Thermal Structures Conference, University of Virginia, Charlottesville, Virginia, November 13-15, 1990. Whetsone, W. D.: EISI-EAL Engineering Analysis Language Reference Manual- EISI-EAL System Level 2091. Engineering Information Systems, Inc., July 1983.

_92-25919

High Speed Civil Transport General

R. L. McKnight Electric Aircraft Engines Cincinnati, Ohio

173

CONCORDE

HSCT

3,000

RANGE

100

PAYLOAD

400,000 EXEMPT

COHHUNITY FARE

APPROX20 of

5,000

(PASSENGERS)

WEIGHT

PREHIUH

Comparison

(NML)

250

STANDARD

LEVELS

HSCT

design

requirements

TO

300

STANDARD

N0x EMISSIONS (GM/KG) the

6,000

750,000 FAR 36 STAGE III

(LB)

NOISE

TO

3

with

the

TO

8

present

CONCORDE.

HIGH SPEED CIVIL TRANSPORT ENVIRONMENTAL

IMPACT MAJOR DRIVER

-

EMISSIONS

-

NOISE

CRITICAL COMPONENTS -

HIGH TEMPERATURE

COMBUSTOR

-

LIGHT WEIGHT EXHAUST NOZZLE

NEW AND ADVANCED MATERIALS

174

-

HIGH TEMPERATURE CMC'S

-

HIGH TEMPERATURE IMC'S/MMC'S

day

KEYM_R

MATERIAL REO_UIREMENTS

HIGH OPERATING TEMPERATURE HIGH THERMAL STRESS RESISTANCE ACOUSTIC/VIBRATORY DURABILITY ENVIRONMENTAL DURABILITY DAMAGETOLERANCE SHAPE-FORMING CAPABILITY REASONABLE COST Design combustor

projections material

indicate will

need

that to

a

successful

possess

the

HSCT noted

characteristics.

175

KEY NOZZLE MATERIAL REOUIREMENTS

HIGH SPECIFIC STRENGTH THERMAL STABILITY ENVIRONMENTAL RESISTANCE THERMAL MECHANICAL/ACOUSTIC FATIGUE RESISTANCE THERMAL SHOCK/STRESS CAPABILITY DAMAGE TOLERANCE GOOD FABRICABILITY AFFORDABLE COST Design

projections

nozzle

material

characteristics.

i

176

indicate will

need

that to

a

possess

successful the

noted

HSCT

HSCT PROGRAM WILL PROVIDE HIGH-TEMPERATURE ADVANCED COMPOSITE MATERIALS, INCLUDING FIBERS AND MATRICES IMPROVED PROCESSES FOR FABRICATING ADVANCED COMPOSITE COMPONENTS ANALYTICAL TOOLS FOR COMPOSITE AND COMPONENT DESIGN, FABRICATION, AND LIFE PREDICTION IMPROVED PROCEDURES FOR TESTING COMPOSITE SUBCOMPONENTS

COMPOSITE SUBCOMPONENTS FOR ENGINE TEST ANALYTICAL TOOLS DEPEND ON MATERIAL CHARACTERISTICS MANUFACTURINGBEHAVIOR FUNCTIONAL BEHAVIOR FAILURE BEHAVIOR FAILURE MODES DAMAGEACCUMULATION CONSTITUTIVE MODELS THERMAL i

STRUCTURAL

i

MACRO, MESO, MICRO

LIFE MODELS -

MACRO, MESO, HICRO

CLOSE COUPLING BETWEEN LIFE MODELS AND CONSTITUTIVE MODELS 177

.4.

Tailodng of Composite Structures I

Thermal. and GasDynm_ic

_r

_; ........

..,

..

, .;_._._._:_; Probablislic

(Analysis OpSmlzer I_lhods) Moisture - Temperature - Stress Mat_al ProperSes Space

_-_J

SensiSvity Methods

CSTEMOVERVIEW _CSTEM"

is

contract, of

Graded

gram

the

were

to

produce

tailoring.

ulation

specialized

The

enabling

element

effective, CSTEM of

nate.

The

element

tural

analysis

CSTEM

178

and

shown

are

analysis

tailor

are

structures

having

disciplines large acoustics,

prohigh

involved

deformation

of

and

are

struccoupled

dis-

the of

sim-

aeropropulsion

implemented

simultaneously

carried

with to

model out.

mesomechanics

system.

the

obtain

micromechanics the

this

a computerizedmultidiscipline

problems

complexities

begins

finite

design

is

NASA

in

structures.

a

special

geometrical,

composite

3D

finite

material,

structures

for

cost

performance.

models

Also

the

for

multiple

analysis,

system

the

objectives

anisotropic,

thermal

environment

analysis

The

capabilities

composite

elements

under

Analysis/Tailoring

technical

cost.

include

CSTEM

for

to

optimum

ety

developed

heterogeneous

low

They

technical

and

The

and

The

formulated

loading,

program

The

anisotropic

cipline

computer

anisotropic,

nonlinear.

analysis,

the

Structures."

performance

highly

tural

for

Structural/Thermal/Electromagnetic

Composite

structural all

acronym

"Coupled

is The

constituent material then

analysis

models

to models

properties

and

characteristics constructed is obtain and

and

then

how

the

carried

local they

uses

for

are

global down

stresses

a vari-

the

lamistruc-

through and

related

the

strains. to

the

In

each

enabling

element

code

iterative

technical

has

been

solution

participating

discipline,

developed.

An

techniques

analysis

performs

modules.

Each

passing only the required input the modules as well as returning an

analysis

The

by

structural

similar

The

on portions

advanced

heterogeneous ative to the tion

point

coordinate emental global

system. coordinate

of

the

or

coupling

module

is

finite-

among

self

the

contained,

information be needed

20-nodedisoparametric

finite

set

of

of

the

structural

desired

Material

version

element nodal

the

as

between input for

bricks

codes

in many

displacement,

equations

with

the The

of

module

orientation may

of also

orientation structural

nodal

computer

is

It

force,

used is amultiproblems since

include

the be

can point

between

the material properties of the based on the volume ratios of

anisotropic,

be input relby integrawith

referenced

module

program

its

material

to

the the

elemental

can

it needs for composite make up the composite. the

and

ways.

separately.

Material properties skewed integration

properties

properties properties that

data bank containing erties are calculated

3D

controlling

loadings. The solution technique allows the solution of very large

internally.

adapted

nonlinear

analysis

acceleration,

system,

calculated

internal

16-,

material capability. material axes and then

anisotropicmaterial the constituent an

8-,

features

to obtain

with

geometry and control any results that may

isoparametric

and pressure solver, which

work

more

uses

other

the

stand-alone,

program

module.

centrifugal,

temperature, block column can

module

to many

accommodates

it

a following

a decoupled, executive

also

el-

and

generate

materials, This is done INHYD,

global

which

constituents. the constituents.

the

using using

accesses The

a

prop-

179

COUPLED STRUCTURAL/THERHAL/? COHPUTERHARDWARE/ALGORITHHS DESIGN OF EXPERIHENTS (TAGUCHI) TOO HUCH DATA-NEED EVALUATION STRATEGY/DATA BASE STRATEGY ANALYSIS-EXPERIHENT-ANALYSIS

FEEDBACKLOOP

HARDWARE/CODE/USERGOODNESS-OF-FIT PROBABILISTIC

DESIGN

-

HATERIAL SYSTEM

-

STRUCTURES

RISK ANALYSIS -

DETERMINISTIC

-

PROBABILISTIC

STRUCTURALTAILORING AND OPTIHIZATION

180

-

HULTIDISCIPLINE

-

HULTIOBJECTIVE

HIGH SPEED CIVIL TRANSPORT A NEW LEVEL OF COOPERATION AMONG t

GOVERNMENT/INDUSTRY/UNIVERSITIES

181

tNI_UT GEOMETRY

/

LOAD

NO

BUCKLING ANALYSIS?

ANALYSIS?

YES

NO

STRUCTURAL RESULTS PRINT

MATERIAL

NO

_

TRANSFORM STRESS/STRAIN UPDATE

STIFFNESS

NO

EIOENVALUE ANALYSIS7

DISPLACEMENT

UPDATE STRUCTURAL STIFFNESS

HGURE 1. CSTEM FLOWCHART

Flowchart CSTEM.

executive

to

182

the

These

analysis

the

of

modules

package

modules

process

as -

at

modules

used

entry

or

is

analysis are

with

routine,

tailoring these

major

the

a

through

the in

as

load

stand-alone the

analysis

which

of

case case

main

portion the level.

entry

of

F.SIGN VARIAB_ 0NSTRAINTS

1

DESIGN VARIABLE SET INITIAL VALUES

co NSTRAINT

FIGURE

CSTEM

tailoring

computer

program

consists

of

the

actual

to

abstracted

from

structural,

2, TAILORING

obtained major

tailoring,

parameters

VALUES

capability

two

be

and

been

built

from

NASA

Lewis.

and

CONMIN,

The

and

FLOWCHART

has

ANALIZ,

tailored.

thermal,

PROCESS

modules:

STAEBL

]

coupled

acoustic

the This

which

which CONMIN

on

with analysis

the

program

performs

supplies module

STAEBL

the was

CSTEM modules.

183

I I Compression

Tension

Tension q

I i

A

I I

I I Compression

ILT/ILS Ten/Camp Static/Fatigue Creep/Stress Oxidation

© Tension/Compression Load e/d, w/d (Ten) ab (Camp 8 = 4%)

Tension/Compression Load Static/Fatigue Creel:#Stross Oxidation

Impacl After Impact

t

Static/Fatigue compresslon/Tenslon Creep/Stress Oxidation

Joined Panels Biaxial Loading

Validation is

an

of

important

required

for

Configuration

part the

for

interactions

]84

of

the

models

HSCT

stress

laboratory

oxidation

in

will

shapes.

difficulties

and simpler

design

methodology

Validation

specimens

component

represented

and

process.

creep,

generic

fabrication not

of

analytical

static,

shaped

representative account

the

and be

When stress

laboratory

will fatigue

designed tested

or

be arenas. to these

failure specimens.

mode

be will

CRITICAL

SCREENING

THERMAL

CYCLING

THERMAL

MECHANICAL

FATIGUE DETAILED

ACOUSTIC

TENSILE

1 PRELIMINARY m

PRELIMINARY

CHARACTERIZATION

LOW

CYCLE

BURNER

:

CREEP

LCF

FATIGUE

FATIGUE

RIG EVALUATION

AND

HCF

CRACK

GROWTH

TOUGHNESS THERMAL

MECHANICAL

EFFECT

OF

EFFECT

OF

ORIENTATION

PHYSICAL

PROPERTIES

SCREENING

ORIENTATION

FATIGUE

OXIDATION

EFFECTS

EFFECT

ON

OF

STRENGTH

DOWN SELECT 4 MATL'S.

CREEP OXIDATION THERMAL

AND

STRENGTH

SHOCK

STATISTICAL

ON

STRENGTH BURNER

CONFIDENCE

DETERMINED THERMAL

THERMAL

ON

CYCLIC

EXPOSURE

TENSILE

PHYSICAL

CHARACTERIZATION

FATIGUE

PROPERTIES

SHOCK DESIGN

DATA

PACKAGE

MATERIAL

PROPERTIES

A

detailed

HSCT

evaluation

materials

will

test be

developed.

mechanical

and

physical

techniques

for

environmental

and

candidate

NDE

plan

testing, and

for

the It

candidate

will

include

characterization thermal

behavior,

techniques.

185

CONSTITUTIVE

I

HEAT

MODELS

TRANSFER

ATTAC HM E NTS ACOUSTICS

INTEGRATED

DESIGN

CODE

METHODOLOGY

DAMAGE

PROBABILISTIC

METHODS

THEORIES

o STRENGTH

(WEIBULL)

o DESIGN

(MONTE

1

I COUPON

BENCHMARK

TESTS

TESTS

The

theoretical

the

rISCT

design base

186

program

models

and

will

methodology established

CARLO)

be

and by

the

analytical integrated

life

prediction

coupon

and

tools to

provide system

benchmark

developed an with tests.

in

overall a

firm

MMC

model-

Creep

.35

vf,

1 IOOF,

Redistribution 120ksi fiber-stress

300

250 n

13--x--

matrix-stress

2OO ,u

J_ V

(n 150 (n (I) i,. (,n

I O0

5O

I

0

200

I

I

I

4OO

6OO

8O0

time

A

creep

model has

simulation in

not

a

of

nonlinear

occurred

(hours)

an

MMC

finite after

I

1000

50

unit element

cell

utilizing

code.

an

overlay

Stabilization

hours.

187

MMC

model-

Creep ..35 vf,

Redistribution

1 IOOF,

120ksi

250"

--B--

fiber-stress

---x--

motrix-stress

...-----El

200

'_ 150 (/I (/)

.,-, 100 ¢)

5O

0

0

!

_

10

20

w

time

A

creep

model not

188

simulation in

a nonlinear

totally

complete

of

Ir

30

!

40

50

(hours)

an

MMC

finite after

unit

cell

element I000

utilizing

code.

hours.

an

overlay

Stabilization

is

N92-25920

Structures Technology Applications National Aerospace Plane

for the

T. E. Little Pratt & Whitney West Palm Beach, Florida

189

NASP

Design

Requirements Challenge Structure Technologies

Current

Achieving the National Aerospace Plane (NASP) operational objectives of Mach 25 and single stage to orbit (SSTO) will subject the vehicle to extreme loading conditions and will require large, actively cooled structures while meeting very stringent weight goals.

• Mach 25 • Single stage to orbit (SSTO)

Lo_oad g

Configuration

• High temperatures

• Actively

• High acoustic

• Large panels

loads

• Minimum

• High pressures • Shock interactions • Aerodynamic

190

loads

cooled structure

weight

Trajectories

For

Hypersonic

Vehicles

The NASP is an air breathing, single stage to orbit vehicle (A/B SSTO) which is to take off, achieve orbit and land under its own power. Typical trajectories for the X15 experimental aircraft, the Space Shuttle and NASP show that NASP will achieve much higher velocities at lower altitudes.

400 [-

_

//

x.15 7

.

/

,, "_SHUTTLE

A/B SSTO

100 / 0

_ ___-- -

._//

(ASCENT) Z

_ 10 VELOCITY,

j

I 20

I

1

3O

k ft/s

191

Heat

The

combination

of

very

Flux/Life

high

speed

Comparison

at

relatively

low

altitudes

causes

the NASP airframe to experience heat fluxes greater than current gas turbine blades. The Cowl Leading Edge (CLE) is subjected to extremely high heat fluxes from the convergence of different shock waves on a very small position of the leading edge. Fortunately, the NASP design life requirement is "only" 150 cycles compared to 4000 cycles for a gas turbine engine. However, the cyclic application of such extreme thermal loads presents a very challenging structural problem.

GAS

TURBINE BLADE 4,0OO

CLE 4,000_oo.00o-

g5.000 3,500-

.b

_

3,000-

_

2,500-

_2,000X 1,500_

40.O00NOZZLE

SSME

__I.000(.o 09

TFi:IOAT i 4,400 NASP

ol___J

192

ENGINE

2, IO0

NASP 200

A/F

GAS

TLII_INE

I----]

BLADE

_J_J

IO0

500-

ENGINE t 50

SSME 50

Engine

Predicted

acoustic

engine.

levels

These

the

NASP

the

percentage

acoustic

design.

permissible

for

NASP

static

Gee

Engine

1 77

Load

much

greater

are

a

pressure

very levels

pressure

continued

.196

are loads

Dynamic of

Acoustic

Comparison

than

for

a

have

fluctuation

gas

been in

estimated

the

f

,

in based

on

combustor

operation.

Turbine

Shuttle Payload 159

Bay_

100

NASP 200

turbine

consideration

signiffcant

¢

Engine

18.3 /

ffl

1SO

_


-_Vctiv dCL > C' _h -

flutter

speed

divergence lift-curve

frequency

speed slope

217

Having

identified

the

performance

measure

sign variables and the constraints, mization problem is given in this F(x) _

Performance

Function

_(x) _

Constraint

Functions

xl,x2,...,Xn--*

.Minimize

Design

(such

a formal slide.

as

weight),

statement

of

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F(x)

F(_) = r(x,, _,_,..._,,) subject

to the

inequality

constraints

_,(xl,z,...x.}

and

eq.ality

< _,

constraints

_,(z,, z2...x,,)= _,

218

j = 1,2...k

j = k-I-

l,...s

the the

de-

opti-

A

two

ble)

variable and

lines.

The

constraint gradients

design

space

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of

functions provide

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i ×2 COHSII1AINr

z'

kx_

!

FEASIBLE

_oNsTRAINF

V _ INFEASIBLE

REGION

BOUND

AI1Y

VG2

REGION _

Xl

--

219

The key elements of the trated in this schematic tified i.

by

dotted

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boxes

of an aircraft The three main

are illusareas iden-

are:

determination

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line

preliminary design (block) diagram.

loads

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Two key transformations (load and often contribute to singularities polations

(spline

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interpolations).

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Step Size Optimality

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220

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STARS •

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221

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AUTOMATEDSTRUCTURALOPTIMIZATIONSYSTEM

222

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MAPOL

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OBJECTIVES AND PAYOFFS OBJECTIVES •

t

AN AUTOMATED PRELIMINARY





DESIGN

INTERDISCIPLINARY

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PROVIDE

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I

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223

Architectural Highlights •



Executive

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for Engineering

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Level

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224

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225

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[ F,NA, ANA,¥S,S [

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l

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Resources

Structural

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226

for ASTROS NASTRAN

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Static Aerodynamic

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227

AN ARCHETYPICAL

ASTROS APPLICATION

GIVEN: STRUCTURAL MATERIAL

CONFIGURATION PROPERTIES

DESIGN

FLIGHT

CONDITIONS

DESIGN

ALLOWABLES

DETERMINE THICKNESSES

OF DESIGNED

OPTIONALLY POSSIBLE

705 276 1167

NODES

DESIGNED

FIXED

-

MASS

DESIGN

BALANCE

CONSIDERATIONS

BOUNDARY CONDITIONS FLIGHT CONDITIONS

MULTIPLE

STORE

LOADINGS

ELEMENTS

ELEMENTS

VARIABLES

I • ROD AREAS • SHEAR ELEMENT • MEMBRANE • BARS

THICKNESSES

ELEMENT

• CONCENTRATED

THICKNESSES

MASSES

CONSTRAINTS • STRESS-STRAIN • DISPLACEMENT • MODAL FREQUENCY •

AEROELASTIC EFFECTS - LIFT EFFECTIVENESS -



22.8

AILERON EFFECTIVENESS DIVERGENCE SPEED

FLUTTER

VALUES

MULTIPLE MULTIPLE

DESIGN PARAMETERS DESIGN

ELEMENTS

RESPONSE

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Solution

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Programmer's

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Code Installation Module Description Data Base Calls Utility Calls 229

Conclusions



Potential

for Realization

in Multidisciplinary •

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Interest



Need Extensive



Validation

of CAD

Environment Around

the World

Applications

to Assure

Reliability

i I i

• SHORTER SCHEDULES • EXTENSIVE PARAMETRIC STUDIES • OPTIMALDESIGNS - BESTPERFORMANCE • LIGHTWEIGHTSTRUCTURES • TECHNOLOGY TRANSFER • RESEARCH TOAPPLICATION • SYSTEMTO SYSTEM(LESSONS LEARNED)

230

N92-25922

Light Thermal Structures and Materials for High Speed Flight Earl A. Thornton Light

Thermal

Structures

University Charlottesville,

:of V|rg]n

Center ia

Virginia

231

INTRODUCTION

As a hypersonic interacting

with local

local pressures experience

intense,

not possible

a means

shocks

highly

years

because

viscoplastic

rate dependent

localized

flow, creep

edges

expose

of integrated

sweep

across

structural engine

surfaces

structures

have evolved

at elevated material

temperatures

to severe

which

behavior.

to meet this need.

from the elastic

and stress relaxation.

due to dynamic

loads

Over the last twenty

years,

These

constitutive

through

the plastic

Rate-dependent

plasticity

range

models

including

effects

was

provide strain-

are known

is to describe

Structures

Center

computational

focused

on the investigation

In the first part of the paper,

In the second

part of the paper,

and experimental

research

of the response

finite element

the thermal-structures

programs of structures

thermoviscoplastic

to be

experimental

INTERACTION

FOR

AEROSPACE

PLANE

_

COWL

program

Vehicle

LEADING

underway and

analysis

I

FLOW

it

loads.

inelastic

response

interactions

shocks

temperatures.

to local heating.

highlighted.

These

response

to model

models

in the atmosphere,

is leading

aerothermal

a material's

of this paper

at the Light Thermal

layers.

One example

constitutive

at elevated

The purpose

materials

and boundary

of an inability

plastic

at high speeds

the study of structural

for representing

important

accelerates

and heat fluxes.

Until recent

unified

vehicle

is

is outlined. IIII

EDGE

nose

b°whock°?sCh \ , -\ __

inlet -_ Cowl _ uw,-

_ _

_\

"_'_

_ _ " _

_t

(_ _.

_'__...

X Cowl bow / shock -/ Figure

232

_(_

1

Internal

\_oo,ing

__"_

_//

RESEARCH

Finite element years

analysis

and provides

an important

thermoviscoplastic convectively

method

presented

structures

to localized

of structures

problems

at elevated quasistatic

Reference

method

illustrate

has been under 1 describes

for hypersonic

the effectiveness temperatures.

finite element

development past efforts

structures.

15

and presents

Applications

of the approach

References

for about

a

to

and provide

insight

2-3 use the computational

thermoviscoplastic

analysis

of aerospace

heating. studies

for intense

thermoviscoplastic

therrnoviscoplastic

O

behavior

is a need for further

to represent

design

structures

models

capability.

computational

in ref. 1 to perform

subjected

There response

hypersonic

viscoplastic

constitutive

simulation

finite element

cooled

into the transient

with unified

OBJECTIVES

computational such as leading

to:

(1) understand

local heating, behavior,

edges

(2) investigate

(3) perform

methods,

the phenomena

finite element

thermal-structural

and (4) understand

of hypersonic

that occur

in the viscoplastic

modeling

experiments

the high-temperature

techniques

required

to validate behavior

of difficult

vehicles.

Investigate Thermoviscoplastic (TVP) response of thin panels subject to intense local heating. Evaluate finite element Thermal-Structural analyses with unified TVP constitutive models by comparison with experimental data.

..,H

ii

......

i iiiiiiii!iiiiiiiiiii::i_i::iiiiii_i_ '....

.....

Figure

2

233

THERMOVISCOPLASTICSTRUCTURALANALYSIS

The behaviorof a thermoviscoplastic structuresubjectedto intenseheatingis analyzedassumingthat: (1) thermo-mechanical couplingin theconservationof energyequationcanbeneglected,(2) thestructural responseis quasistatic,and(3) deformationsareinfinitesimal. With theseassumptions,anunsteady thermalanalysismay beperformedfirst to determinethetemperatures.Then,usingthesetemperatures, thestructure'sviscoplasticresponseis determined.The structuralresponseis obtainedby solvingthe equilibriumequationswritten in rateform. The solutionis obtainedby solvingtheinitial value-boundary valueproblemby time marching(ref. 1).

[KII_}

= {Fp} +/FT]

+ {i_} + {Fs}

where: r [K]

=

_Jf2e [ B ]T [ E(T)

{FP}

=

f_e [ B

]T

{iTT}

=

f_2e

] T [ E(T)

[ B

Stiffness

] [B] dC2

Plastic

[ E(T) ] {_P}d_

A'i _ dE2

] {a(T)}

Matrix

Strain

Temperature

m

{[_c}

=

f

{FB}

=

f_e

Surface

oa_e [NI T {_} ds •

[NIT

113} dE2

Body

Figure

234

3

Tractions

Forces

CONSTITUTIVE

The Bodner-Partom phenomenological model

constitutive

observations

has gone through

The current

model

The strategy temperature

integration

employed

rates.

Then

is of the internal

modifications

and was extended

thermal

in the viscoplastic variables

the constitutive

time, the equilibrium

equations

are solved

rates, then advancing

the constitutive

value boundary-value

problem

concepts

related

to dislocation

for anisotropic

is as follows:

the equilibrium

equations

again.

with

equations

are integrated

of the stresses,

equations

type that is based

on dynamics.

work hardening

The

materials.

effects.

algorithm

specified,

ALGORITHM

state variable

by physical

values

At time

AND VISCOPLASTIC

and supported

With updated

1.

points.

several

model

(ref. 4) also includes

and internal

displacement

MODEL

This sequence

are solved

forward

temperatures

the initial distribution

the nodal

in time at the element

and internal

of determining

in time is continued

to obtain

variables the nodal

until the desired

of stress,

Gauss

at the new displacement

history

of the initial-

has been obtained.

= t, initialize

(3ij

and

Z

P

1

2.

Calculate

3.

Assemble

4.

Calculate

1_} = [B]{fl}

5.

Calculate

{6} = [El{ _-

6.

Calculate

Z = ml(

7.

Integrate

(3"ij and

8.

If

_ij

-- (Sij

and

( t + At )
I

component Quantifiable reliability

I --

"

Figure 10 SIMPLIFIED

PROBABILISTIC

ANALYSIS

Fatigue Strength

Stress Probability of Occurrence

9a,, ,,_

Factor of Safety on Endurance /

/

/

Factor of Safety

_end F'S(end)

=

Ftu m- nOp.nd Sm- nOalt

n = 2 - 95% Reliability in = 3 - 99.7% Reliabilityg

Fa,,o;o-/ Region

Deslcln Herdwpre to Demaqe over

to be Insensitive Time

i • •

Thicker Walls (lower o) Low Stress Concentrations Smooth surface finishes



Alternating

Stresses

below

O'al t (Ksi) (_end on Endurance

Cycle to Failure

Figure 11 460

Operatlng_'_ Stress

[

DAMAGE

TOLERANT

DESIGN

APPROACH

Fracture Mechanics

Cht_r_¢terlze Material Flaw Sizes • Establish a Flaw Size/Distribution

_a

Probability of Occurrence

I •

3,_

,

-J

• • • •

Design Flaw Size

!

Database

Collect historical databases - typical castings Fully characterize material properties Conduct 1st article - section castings Section production hardware - random selection

-4.

Flaw Size, a -4 10

De$1an Hardware Flaw Tolerant • • • •

to be Dama0e/ d_dn

Thicker walls (lower stress) Minimize stress concentrations Established maximum flaw size Stress intensity below AKth

:/

-5

f

10

-6

:

10

AKIh

a t0

I 100

AK

Figure

DETAILED

12

PROBABILISTIC Most Sophisticated

Engine

Component

Component

J Component

Loads

ANALYSIS

Approach

Reliabilities

Responses

• Can be assessed

• Develop model of physical process

using closed form or FEM solution

• Anchor model to prior engine data

• Define analysis approach

• Define primitive engine variables

• Characterize variables

• Calculate

• Calculate response

component loads

input

Component

Failure

Rate

• Define failure mode algorithms • Define material property characteristics • Characterize other input variables • Conduct analyses

component

Enalne Reliability •

Sum of component failure rates • Probabilistic analysis component reliabilities, and • Deterministic component reliabilities for remainder of components

Figure 13 461

COMPONENT LOADS ANALYSIS Vibralion Measurements

]_,_,,A,A I _ rV W"1 time

# /

/ Pressure Measuremenls

Influence Coefficients • Relateengineenvironment Io component environment • Relalecomponenlenvironment Iocomponent loads

Temperalure Measuremenls lime

Turbine BladeLoading

'

I Com_nent Load# • V'bratory

P _lory

• Pressure • Thermal

P

Terr_ralure Pressuret,

|_

• TotalLoa_ng

P

Figure 14 COMPONENT

RESPONSE

ANALYSIS NessusTurbineBlade Course Model

TurbineBladeLoading

P I _,_lory

Input Variables i p

pI I

P e, ure, /'_

Geometric

P _._ances P

Structural / Response

Occurrence ProbabililYol

I p

Figure

462

OperalingStress

15

COMPONENT Generic

FAILURE

RATE

Model Process

Failure Model Input Variables ¢.,I

Failure Model

I i

• Dimensions/Geometry • Environment/Loads

_.

• Stress Concentrations • Model Accuracy

Finite Element

J

"""

• • • •

Predicted Failure Risk

Strength Fatigue (HCF, LCF) Crack Growth Displacement

t

Model

s

Material Characterization Model

• Stress Response • Displacement Response

• Material

Capability /_

Operating

\

'/

'

Failure Region Computed

Data

: Design Curve Statistical Variance • Surface Finish • Environment

Figure 16

BENEFITS

Quantitative

OF PROBABILISTIC

measure

of integrity

Uncertainty of each variable the analysm process

APPROACH

of design and reliability

is explicitly

considered

Most significant design variables (drivers) the order of their effect on reliability Design trade studies

can be assessed

in

are ranked in

via reliability

Gaps in the design data are surfaced - program resources can be effectively used to obtain necessary data

Figure 17

463

SPACE

TRANSPORTATION

MAIN

ENGINE

_Operational Parameters • • • • • • • • •

Thrust, klb (vac) Specific impulse, s (vac) Chamber pressure, psia Engine mixture ratio, o/f Area ratio, E Mission life Weight, Ib Gimbal capability, deg Throttling

583 430 2,250 6.0 45:1 10 7,900 _+10 70%

Design Features • Gas generator cycle • Liquid hydrogen/liquid oxygen • Milled channel chamber/tubular gas cooled nozzle • 3 stage H2T/P-1 stage O2T/P • Tank headstart • Open loop control • No bleeds • 152 in. long x 87 in. dia

Figure 18

MAIN

COMBUSTION

CHAMBER

Figure 19

464 _=

..... J_

COMPONENT

RELIABILITY

STME Initial Reliability

ALLOCATION Allocation

Requirement 0.99 at 90% Confidence

Y

0.99982

Reliability Design Goal Rsy s = 0.999

Combustion Devices Components

Design to Allocation

Injector Combustion Chamber Nozzle Gas Generator Total

0.99997 0.99991 0.99986 0.99993 0.99967

Controls 0.99997

Figure 20 STME

GAS

GENERATOR

Initial Reliability

Engine

ENGINE

Allocation

Level 0999

Turbomschtnery

Controls

i

Mo_llorln

9

Fuel

0¸99997

PCA IG

& SLt! Co,nt

CC CC

Con

M.dl

Ignile_

A

I_ter

8

Fuel

TurboPump

990998

0

999090

0

999990

Inducer

0 999g94

Pump

0

999999

Btg

0 099097

[nduce_

Pump

Assy

.k

0

gggggg

Til

_gniter

B

0

999999

Pep

0

099998

MQin

0

99991)2

1st

0

999994

2nd

0

999999

Inlerstg

Mcl

HG

(15)

Temp

C_o

"rm_

Flow VI_

O 999990

9oli Inlet

Wear

099990

TurT_n4

999996

Tufb

999999

2rid

0

999991

MelLn

(2)

0

999990

Rtg

Ring

Module

0

999999

Tud)

Whl

0

9999g9

Torqmlr

& Cond

Hams/Connect

Mdl

0

ts!

999998

2rid

5h=llt

Ass

0 999739

Pneum

Cnkl

0

999969

PC),

Inie¢lo[

0

099999

Elect

90g993

Ignlt_

AHF

0

909902

0

99999g

Spark

P_ugs

0

99999ii

0

999990

0

099990

9

Spdng

Chamt:_

In|e¢lor

0¸9999?0

Combustn

C, hrr_

Camp_|s

Controt

Ylv/Ach:

Valves

0999910

Main Main

Liner

0

0¸999990

Manifold

0 ggggTo

Ht

0¸009993

Body

0

99999O

tgnlf

Seal

0

Seel9

0¸999980

0

999860

GG

0

999930

(,I)

Ring

Stg

Brgs

999994

0 990975 0

Mild Noz]_te

SI9

0¸999997

999903

Housing

TUrt_ne "ru_blne

0¸990994

Tmb

0

Tu,b

999594

.41ty

Manilo_(I Whl

0¸999004

tst

Seal

0¸990958

2nd

Assy

0 999932

B_ds _lds

(2) (2)

0

099908

0

99997!

0

999994

Stg

999943

0

099060

0¸999900

/_ay

SIg

0

Gene_'_lo¢

Injector Combusloq

Body Bodl,

O 999975

Ht

B_gs

)4)

Ox;_zr

Contd

0

vlv

lntrcnc!

9g99g0

Heal

O=ld;zr

9909,1f

Contd

V_

E:changer

Bea;Ing

0

Attaching

900099

0

999999

0 909990

0 099997

O=_zr

Ocis/t.ns

0¸999940

0

0 990997

Ex(:tmngr

Glmbal

900g50

999906

0

0 999967 0 099997

5cisaorl

ggggg0

999999

0

0 9ggggg

Oxi_zr

GG

0

ggg9g4

0

0 999999

Exc_

Igntr

Bids

[4)

Fuel

Moln

0999955

Bids

0

0 999974

Actuators Mean Fuel

Inle!

Beadnge

H_drosl¢

GaS

Assy

9999S0

0¸999993

Disk B;all

Noztte

^ssy

Body

Impeller

Boadngs

Hydros(c

Malo

Thmt

Main

0¸999914

Comp 0 99g02

Volule

Oisk Gall

Br 9

0

999537

Syteme

0¸90999!

Assy

9

0¸999991 090097

0

Assy

GO

0¸990901

I.Is 0

In_t SIg

Tuf_epump

Pump

9

O gggG7

In_r

R_

0

Oxidizer

TCA

TIP 09984

imf_r

StO

0

(4)

Hsg

Pep stg

0

(t0)

(0|

De,ect

FTP/GG

(_)

SenSor Pos

Accel

TCA

(2)

0 909930

Sprmg

Igniler

Plesm

0.099722

0

0

GG

Senso¢s

el

0¸99972

(3(3

OTPhJEX

099959

TIP

Ac_u_

0

099997

0

99g980

0

999997

0

999997

0

999900

0

9gggg2

9

ggggg8

0

99999,_

Figure 21

465

MAIN COMBUSTION FUEL OUTLET MANIFOLD

TO COMPONENT FUEL DRAIN MANIFOLD

_ ',,\'_|

CHAMBER

! __ OVER.OARD ORA,. UNE tT/f_'/.J b_lln

BURST

PROGRAM

,_#_E_T

PLUG-AFT

CAVITY

[ "%/-_1_._-'_

c.osEouT_,._,.r/#C. , SLOTTED NARLOY (INNER WALL)

Z LINER

STRUCTURAL

__

_AC_. LINER/JACKET

-'_\I

CAVITY

\\

\

\\

""_,b__

_\

¢...,,...,_/_ _ z. _ __

_

\.

y

\\

(-/--7--7--T_-J_

COOLANT

.

\)\|

.

,,,C_EL

CLOSEOUT

coPpER

_ e__z ._ ...L_.:,,_

SECTION

BARRIER

A-A

Figure 22 PROBABILISTIC

Primitive

Varlabte_

• Characteristic exhaust velocity --.il,,. • Inlet nozzle area of the LOX turbine • Fuel pump efficiency

ANALYSIS

OF THE MCC LINER

Engine Model • Numerical solution • Influence coefficients • Statistics of primitive variables

Variables

that affect the MCC

• Inlet coolant temperature • Chamber pressure • Coolant flow rate

Loca! Variables • Curvature enhancement •

MCC Liner Thermal Model • Closed form solution

Hot spots

• Thermal conductivity • Hot gas wall thickness • Channel



Heat load

• Scaling • FE/FD models

depth and width Correlated Pressures

Liner Structural

Local Variables • Hot-gas wall thickness • Channel width • Land width • Material

properties

--Ii,,-

• Channel bending stress • Land tensile stress • Low-cycle fatigue • Ratcheting

Figure 23 466

Model

Temperatures & on the HOt Ga_ Wall

PROBABILISTIC Channel .0016

,0014

-

I

STATISrf¢

1,000,000

Stress '

''

'

..............

Mean ................... Slondard Deviation Coef of Varialion Minimum Maximum

,0012

z

Bending

I

--

ANALYSIS

I

STREH,;rH

3950.46 367.30 0 09

16032 65 2112 5t 0 13

2579.76 6255 08

4456.73 22628 16

..... .....

................ ................

I

SrRESS --

Simulations

0010 Probabi|ily < .000 00¥

._

at

Reaching

Y eld

Moment

.0008

._% .0006 o_

:::::JIEND:STR ,5o0.

t2500, STRESSI

17.500 PSI

Figure 24 PROBABILISTIC Land ,0025

.0020

-

:'UOI5

-_

0010

-

• 0005

-

Tensile

Stress

I I -STATISTIC .............. Mean ' Slandard Deviation ..... Coef. of Variation .....

I STRESS 5747.47 253.65 0,04

Minimum Maximum

4759.17 7011.44

1,000,000



ANALYSIS

................ ................

--

I STRENGTH 18057.10 1279.84 0.07 7287.27 23354.15

Simulations

Probability

_f

Reach+i_

_ield

Stress:

_%

I _OQDi 4500.

.... 8500.

1-2500.

' 16500

20500:

STRESS. PSI

Figure 25

467

PROBABILISTIC

ANALYSIS

Low Cycle Fatigue

OOO5

Mean ................... S|ond_rd Oeviotion ..... Coe[. o( V_¢ialion ..... Minimum ................ Maximum ................ Number of Simulalions ..

3098.31 1309.05 0,42 476.t7 27216.11 I000000

ooo z w

000.

0O02

O0Ol

oooo 40o

5400.

10400. 15400. 20400. NUMSE_ OF CYCLES TO FAILURE

25400.

Figure 26 PROBABILISTIC

ANALYSIS

Ratcheting

0.14

LINER

Failure Rate at a Hot Spot

Mean life Standard deviation Coefficient of variation Minimum life in simulation Maximum lile in simulation Number of simulations

0.16

OF MCC

9.69 4.62 0.48 0.59 59.96 1,000,000

0.12 _" 0.10

A I| . |rJ 6 I i_ iIv "ll_l|l] _IV r_l/lll iI " 11 if J _,[tJ

--

o

0.08 A- 0.06

Random V_rlables Channel width Thermal conductivity Wall thickness Characteristic efficiency, C* Land width Channel depth Curvature enhancement

Sensitivity 0.977 0.176 0.102 0.056 0.018 0.017 0.002 0.002

0.O4 0.02

/"

"'

I 0

10

_1_

_

Fuel pump efficiency

r-'-------J 20 Number

3O

I 5O

of Cycles to Failure

Figure 27 468

I 4O

6O

PROBABILITY DENSITY HIGH CYCLE Main Combustion

FUNCTIONS FATIGUE

Chamber

Failure FirsI-Order

Mode:

AFT Manifold

High-Cycle

Rellablllly

FOR

Casting

Fatigue

Method

(Level

III)

0006 Pressure ............. Thickness ............ Stress Cone .......... Ro_dom Vibration Force Ullim0te Strength .... Mo4elin 9 Error ....... [nduronce Limit ......

.0005

-0.39 0,29 -0,64 -0,25 0.iT -0.32 0.40

.0004 z EHDURAHCE .0003

=

[OUIVALENT

AL(ERKAT]HG

LIMIT

[HORIAAL

STRESS

.0002

0001

0000 0

5000.

10000

15000.

20000

STRESS,

Figure

PRELIMINARY RELIABILITY USING PROBABILISTIC Combustion

Chamber

25000,

30000

,]5000

PSI

28

ASSESSMENT ANALYSIS Aft Manifold

Manifold DETERMINISTIC

SAFETY

FACTORS (OeJlgn Reqm'l)

Primary High Shell

Stress:

Cycle

Fatigue:

Fracture Mechanics: (&K threshold/AK dynamic)

Probabilistic

3.9

(1.5)

2.2

(1,25)

1.0

(1,0)

Analysis

Random

Variables

Manifold

Pressure

Mean

STD Dev

Reliability Shell

Thickness

Sldeload

psi

360 psi

0.400

in.

.007

184,000lbs

Vibration Stress

3,600

Load

Concert,

Ultimate Endurance

87,000 Factor

27,600

Ibs

4,350

1.7

Burst HCF Crack Initiation

In. Ibs

R > 0.9to0 R = 0.998

Ibs

Chamber

0.10

Strength

96,700

psi

4,833

Umlt

27,800

psi

1,390 psi

Reliability

Allocation:

psi

R -- 0.99992

Figure

29

469

COMBUSTION CHAMBER SAFETY AND RELIABILITY SUMMARY Aft Msnlfold Inlet

t.

Jackel Forwerd

t = 0.75

itl

in,

J

FS. y = 1.7 F.S. en¢l >4.0

] J

F.S. FS

u y

= 39 =2_

AN Flange

r--

6Kih/_K

I

_l

F.S

end

- 2.2

(Nozzle}

I_ _

_ t 1

6Klh/AK

= 3.5

_

I

Fbnge

'_-I

- 0.94

Rbult _

>

RHC F

>.*0

gt00

Weld

,.2Sin.

FS.

u

• 4.0

FS_ F.S

_d

>4.0 = 2.4

I

-20 -15

F.S. _d

.2_6

Att CIoRI

= 1.2

M:

l llll_,_

I

lilll .... IIIII__ ":. "

I I l---J

I i

I

I

I

Combustion

Figure

Allocation

HCF

LCF

_/

Impeller

_/

q

q ",,/

Devices

Injector LOX post Injector close-out welds

_

_/ ",,/

Interpropellant

_

q

q

_/

V

_/

inlet

manifold

Fuel

inlet splitter

Manifold to Liner

_/

",,/ _/

q, -y

close-out

MCC liner

= 0.99992

Fract. Mech. Wear

_/

Fuel

II

APPLICATIONS*

_/ _/

plate

• 9100 • .9100

30

Turbine blades Turbine disk Hydrostatic bearings Inducer blades Combustion

Rb_l R HCF

.,,ooII

Turbomachinery

vanes

-39 >4.0

II

""_ ""°°

Reliability

FUTURE

>40

FS.y F.S end

F.S.o,_ ,4.o II ,,KmI_,K ._.4 II

I

Chamber

Hardware/Process

F.S,u

"_"'--I-.'/_"

llbl_"..... I

V

* Not complete list Figure31 470

,=

kl.

FS, FSy

&K_/t,K

Slats

0.40

FSu ._9

Splitter Jacket

Shell

Shell

Buckling/ Displ. Instabilit_

FUTURE

Hardware/Process

HCF

Systems Hardware Interactions Fluid Coupling in LOX system

Fract. Mech.

Wear

Displ.

Buckling/ Instability

_/

Process Control Casting flaw size Material surface finish

"J

joints

* Not complete

LCF

q

Stability issues

Welds/braze

APPLICATIONS*

_/

_

q

_/

-_

list

Figure 32

RECOMMENDED

TECHNOLOGY

• Simplified probabilistic analysis tools (rapid analysis) • Required early in design process (sizing, trend analysis) • Closed-form solutions for estimating variable distributions • Simplified probabilistic analyses or estimates from FS solutions • Simplified reference guide for conducting PDA • Many engineers are not familiar with process • Elimination result misinterpretation (due to lack of knowledge) • General purpose probabilistic tool for empirically derived equations • Nonlinear solutions - define by empirical relationships • Process control problems - fabrication issues • Meaningful graphics display of results • Graphic overlays - solution comparisons as a result of trade studies • Carpet plots showing reliability versus selected variables • Risk

management

tools

for

evaluation

of technical

risk

Figure 33

471

N92- 59zz

Computational Advanced

Structural Analysis and Commercial Engines R. B. Wilson Pratt & Whitney

PRECEDING

PAC_

BLANK

NOT

FILMED

473

ENGINE

ENVIRONMENT

- PRESENT



Materials - Monolithic TI, NI alloys, limited composites (not primarily structure)



Engine configurations



Limiting Issues - Compressor - Turbine

primarily turbofans

exit temperature

inlet temperature

(1150 to 1300 ° F)

(2000 to 3000 ° F)

The history of computational structural analysis at Pratt & Whitney will be reviewed and anticipated requirements for the design, development and support of advanced commercial engines will be discussed throughout the following paper. The present commercial engine environment titanium and nickel alloys.

474

is comprised primarily

of turbofan engines containing

monolithic

ENGINE

ENVIRONMENT

- FUTURE

• Materials - Monolithics

with modestly higher capability

- Composite

primary structure

- Woven and braided composites - Metal matrix and ceramic matrix composites temperature areas •

in high

Engine Configurations - Derivatives

of existing turbofans

"- Ducted or unducted propfans (efficiency noise requirements)

and 1997

- HSCT - "Super" Turbojet •

Key Issues - Engine/airframe

integration

- Gear systems - Fan integrity - Reliance on load sharing

Future commercial engines will make extensive use of composite materials to meet demanding high temperature requirements and aggressive weight goals, since only modestly higher capabilities can be anticipated in monolithic materials. Engine configurations will include ducted and/or unducted propfans and "super" turbojets (HSCT) in addition to turbofans.

475

BUSINESS

ENVIRONMENT

Intense competition - Shorter design cycle - Reduced design/development Increased

costs

emphasis on:

- Safety - Reliability - Durability - Cost - Efficiency - Environmental

impact - emissions

and noise

Competitive pressures will require a shorter design/development cycle and continuing reduction in costs. same time a variety of economic, durability and environmental issues will assume increasing importance.

476

At the

DESIGN/ANALYSIS

ENVIRONMENT



Fewer S/Task



Fewer, less experienced



Less time



Vast increase in computing



Increasingly

people

resources

complex analysis

- Three-dimensional - Increasing

models required

nonlinear requirements

- Detailed analysis of assemblies - Off-design

analysis to assure robust designs

- Closer fluids/structures

coupling



Sharing of analytical work among joint venture partners



Increasing

reliance on vendors for:

- Software - Design - Analysis - Testing

Structural design and analysis will need to be accomplished more quickly, with fewer personnel resources. Increasingly complex analysis will be required. The process will benefit from vastly increased computing resources.

477

ROLE OF ANALYSIS ENGINE

LIFE

IN

CYCLE

A brief historical overview of the role of structural analysis during the commercial engine life cycle is given in the next few figures.

478

PRE-HISTORY

Mechanical - Handbook

(1968?)

Design calculations

- One-dimensional

- sometimes

analysis

- Modest use of two-dimensional



Engine development/support through testing

"THE ONLY ENGINE!"

computerized

SIMULATION

analysis

addressed

primarily

FOR AN ENGINE

IS AN

Twenty to twenty-five years ago design issues were addressed primarily through handbook calculations, modest use of two-dimensional analysis. Major structural issues arising during engine development support were addressed primarily through testing, frequently of full engines.

with very and field

479

PRESENT

Mechanical

Design

- Supported by extensive 2D and 2.5D analysis, and selective 3D analysis, during design cycle - Additional

3D analysis for design verification

Significant

investment

Engine Development/Field

of highly trained personnel

Support

- Analysis drives design changes - Testing to provide analysis input and verify changes

"IT'S

GOING

TO TAKE

HOW

LONG?"

Presently, mechanical design is supported by extensive analysis, primarily two-dimensional. Development and field support are usually driven by analysis, with testing to provide analysis input and verify changes.

480

FUTURE



Mechanical

(1993-2005)

Design

- Use of "artificial intelligence" will require hands-off automation of much 2D and 3D analysis - Vastly increased

3D requirements

- Routine use of nonlinear capabilities - Requirement for concurrent organizations

(2D and 3D)

work by diverse

- Increased problem sizes - driven by automation closer coupling in engines

and

- Vast increase in analysis throughput • Design automation • Concurrent engineering • Evaluation of off-design • Engine Development/Field

conditions Support

Mostly 3D analysis needed Frequently nonlinear - Rapid turnaround necessary

"YOU WANT ME TO BUY HOW COMPUTERS?"

MANY

Future designs will require much more complex analysis types to be used on a routine basis. cycles will require increasing automation of portions of the design and analysis process.

Shortened design

481

ADVANCES

1. Analysis

- What problems can be solved?

2. Computing

3. Analysis

- What resources

482

are available?

Process - What does the user have to do?

4. Data/Information

Advances in computational requirements.

REQUIRED

structural

Handling.

analysis will be required in several

areas in order to support

future

TRANSIENT/DYNAMIC

ANALYSIS



Fan and containment design more exotic - design concepts and materials



Durability standards



Pressure on weight and manufacturing



Testing very expensive,



Analysis must be:

more demanding

with long lead times

- Timely Reliable - Usable by non-specialist •

Improvements

needed in:

- Element technology - Time integration - Material modeling •

HSCT will introduce new problems - i.e., thermal shock

Transient and dynamic analysis will become more important due to economic pressures, the use of exotic materials and the requirements of new engine types.

483

COUPLED

ANALYSES



Typically CFD, thermal and stress analysis done separately



Inefficient,



When coupled analysis is done, level of individual analyses considerably simplified

error prone process

Advanced engines will require some coupled analyses in full detail - for example, thrust reverse transition for a propfan will require full Navier-Stokes sophisticated structural analysis.

Many problems in future engines will require coupling of structural analysis with thermal and/or computational fluid dynamics analysis.

484

MATERIAL

MODELS

Further refinement of state variable models for monolithic materials - cover entire range of thermal/mechanical loading



Increased complexity of"traditional composites"woven and braided fiber configurations

°

Metal and ceramic matrix composites - material model must recognize environmental effects



Stress analysis and damage accumulation coupled problem

become a

Material modeling requirements, and the interfacing of these models with stress analysis programs will become vastly more complex. High temperature requirements will require further development of state variable models and computationally effective material models will be required for a variety of traditional and exotic composite materials.

485

OTHER

AREAS



Contact analysis



Improved triangular



Quality assurance



Rezoning/remeshing/substructuring



Hybrid (FEM/BEM)

and tetrahedral

elements

for analysis results

methods

Sensitivity analysis Coupled

stress/fracture

mechanics

Advances in many other areas will also be required, especially to support timely, complex analysis by relatively inexperienced personnel.

486

COMPUTING

Improvements in available analysis demands.

CAPABILITY

computing

capability



All predictions are too conservative.



All available capability will be utilized.



Networked workstations of increasing pre-/post-processing and analysis Compute

Massively

power for

supercomputers parallel systems

- Use of workstation

Computer

increased

Servers

"Traditional"



will support

networks as a parallel system

development

is ahead of analytical software

Computational structural analysis will depend on networks including supercomputers functioning as compute servers. In general, structural hardware capabilities.

capability from workstations through analysis software lags behind current

487

ANALYSIS

PROCESS

The analysis process is driven by design/development

requirements.

Only three time scales matter Impact the design process - Verify design while low cost changes possible



- Respond quickly to development/field

problems

Processes must be usable by "ordinary" technicians

engineers

and

Analytical tools must be usable by line technicians and engineers. Analysis results must be available in a timely manner in order to have impact on design and development.

488

REQUIREMENTS



Close coupling of stress pre-processors

with CAD tools



(Close to) automated



Order of magnitude improvement boundary condition definition



Simple geometry changes should be simple to evaluate!

meshing

in load and

Major improvements are needed to allow the more complex analyses required for future engines to impact the design process.

489

CONCLUSIONS



Vastly more analysis will be required.



More complex analysis will be required.

Analytical

development

required

- Material models - Dynamics Nonlinear



Analysis

problems

process improvements

equally important.

Real challenges exist for all communities involved in the development government, software developers and industrial users.

490

and use of structural

analysis tools -

Na2- 5934

Military Engine Computational Structures Technology Daniel E. Thomson WL/POTC Wright

Patterson

Air Force

Base,

Ohio

491

Agenda

IHPTET

overview

Codes we use now Codes we are developing The Future Summary

Integrated High Performance Turbine Engine Technology Initiative (IHPTET)

Goal: Double turbine engine propulsion capability by the year 2003

50% of goal will come from advanced materials and structures, the other 50% will come from increasing performance

492

IHPTET's _Effect on Computational Advanced

Structures Materials

Ceramics Intermetallics Single crystal castings Composites Organic

Matrix Composites

Metal Matrix Composites Ceramic

(MMC)

Matrix Composites

Higher Temperature

IHPTET's

(OMC)

(CMC)

Conditions

Effect on

Computational (continued)

Structures

Advanced Tactical Requirements 4000 hours/8000 section 2000 hours/4000 section Advanced

Structural

Fighter

Service

Life

TAC cycles

- cold

TAC cycles

- hot

Designs

Integrated design

structures/materials

Integrated

structures/aero

design 493

i_ Codes We Use Now MSC NASTRAN NOSAP-M X3D UDHeat CRACKS

90

PATRAN

NOSAP-M

Soft body (birds, ice) impact analysis Developed by General Air Force Contract Scaled-down

version

Electric

under

of ADINA

20 node brick element Uses water jet to model impact Implicit time integration Orthotropic

494

material

capability

X3D

Nonlinear

dynamics

and impact

analysis

Developed by University of Dayton under Flight Dynamics Directorate Explicit Model

Research contract

Institute

time integration both the structure

Includes

and the impactor

solid and shell elements

Fiber failure Currently

and delamination

performing

analysis

code verification

Z F-16 BIRD DISPLACEMENTS

IMPACT FOR

05-JUN-91 F16BE

AT F.S, TIME

112, STEP

=

SYMMETRIC, 173I

/

350 TIME

KNOTS 6.0000001E-03

04:27:38 -

0.5

INCH

-

POLYCARBONATE:

SY=7140

!

SU=16000

495

UDHeat

Explicit in time) transfer

code (finite element in space, for steady state and transient

Boundary

finite difference conductive heat

Conditions

Convective Surface

or volume

Heat sources

heat flux

and sinks

(applied

to nodes)

2D elements Infinite

in one direction

Axisymmetric 3D elements Orthotropic

CRACKS

material

capability

90

Preprocessing Material

database

Spectrum

profile graphs

Stress intensity and plotting Generation Residual

496

and plotting

factor generation

of analysis

input file

stress table generation

CRACKS

90

Analysis Residual

strength

Crack growth Residual

life

stress

Load interaction Crack growth

rates

Comprehensive

tabular

Brief summary

of results

output

Postprocessing Single or multi-curve plots

growth

Single or multi-curve

life plots

Residual

strength

rate

plots

497

P" Codes We Are Developing Blade Life Analysis (BLADE) Engine Structural (ENSAC) CRACKS

and Design Evaluation Analysis

Consultant

xx

Probabilistics

Background

(BLADE-ST)

Stress Technology Inc (STI) has worked under the sponsorship of the Electric Power Research Institute (EPRI) since 1980 Developed menu

BLADE-ST driven

contains blade preprocessing generic blade and root types contains

materials

library

of over 40

data base

computes steady stresses, natural frequencies, mode a life analysis

dynamic stresses, shapes, and performs

Recent Accomplishments

Integrally

bladed rotor analysis

F110 high pressure analysis 498

turbine

blade

Blade Life Analysis ahead Design Evaluation for _ Gas Turbine Engines (BLADE-GT) OBJECTIVE: "start-to-finish"

To develop a user-friendly, finite element solver

FEATURES: User friendly

geometry

input

Automated

mesh generation

Automated

boundary

Static Forced

and dynamic vibration

Heat transfer

condition finite

generation

element

solver

solver

and thermal

stress

solver

Life analysis

Funding

for BLADE-GT

Small

Business

Jointly

funded

Innovative

(SBIR)

from four AF organizations

Aero Propulsion Engine

Research

System

and Power Program

Directorate

Office

(SPO)

B2 SPO Arnold

Engineering

Development

Center

499

Engine Structural _ Analysis Consultant (ENSAC)

i_

Application Characterization GOAL: Build an expert system that advises engineers in the use of general purpose structural analysis codes USERS: Engineers with some background in structural analysis, limited practical experience

500

but

Application

Overview

Preparation of input data files for general purpose finite element structural analysis programs Find applicable Complex hardware

and reliable

combination capabilities,

material

properties

of software capabilities, and CPU costs

Analysis model must simulate correct physical behavior, preserve desired accuracy, and minimize CPU costs A similar capability currently exists in an expert YAstem called Structural Analysis Consultant CON)

Status

Selected ART-IM language

as programming

pull down menus dialog boxes windowing Preliminary

demo due I July 1991

prototype partial capability

501

CRACKS xx

OBJECTIVE: Extend the capabilitiy include crack growth in composite

of CRACKS90 systems

to

Completed: An influence function-based method was developed to calculate the stress intensity factor as a function of crack length for either an edge crack or a surface crack in bimaterial construction In Progress: Models of several additional damage accumulation modes are being developed Interface

crack

Delamination

growth

Crack-to-delamination

5O2

transition

Probabilistic Design System Development

Probabilistic

Methodology

Conventional, deterministic design uses single values for material properties, manufacturing tolerances, mission usage, and other parameters Safety factors variability Method

are applied

is inherently

to account

for

conservative

Probabilistic design makes full use of the known statistical distribution of all parameters, and combines them to produce a statistical prediction the result Conservatism level

is reduced

to known,

Design can be optimized for weight, life, or any selected criterion

of

acceptable performance,

503

Probabilistic Design System Development Probabilistic with General Started

Rotor Design Electric (GE)

September

System

(PRODS)

1990

Similar program was also started terminated due to lack of funding,

with P&W but was in February 1991

Both GE and P&W have very large probabilistic method development Anticipate one or more proposals design later this summer Other engine probabilistics

GE PRODS

Program

companies

IR&D efforts

in

on probabilistic

also show

interest

in

Program

OBJECTIVE: probabilistic

Develop, validate and apply a rotor design system methodology

APPROACH:

Six phase

program

Data acquisition Method

Development

Validation Application Application Method PAYOFF: materials; FUNDING:

504

Test

Extension Improved predicted

design safety;

$1.8 million,

capability in advanced and weight savings

over 4 years

Probabilistics

Summary

Probabilistic Improved

design

is real

computational

power

makes

it feasible

More knowledge of the variability of material properties, behavior, usage, and manufacturing effects is necessary Efficient essential

usage

But acceptance

of composite

of the methodology

must be demonstrated, must

materials

it

will take time

validated

be sold as a design

makes

and applied

tool

The Future

Improved

composite

AI Programming/Expert Composite

analysis

methods

Systems

Life Prediction

User Friendly

Systems

Animation/Simulation

of Dynamic

Phenomena

Crude animation of X3D results has revealed phenomena unseen in "snap-shots" Structural

optimization

for composite

components

5O5

Summary

IHPTET Effective

goals

require

analysis

a strong

of composite

analytical

base

materials

is critical

Life Analysis Structural Accurate critical

Optimization

life prediction

User friendly

systems

Post processing

506

for all material

systems

are desirable

of results

is very important

is

N92-25935

Computational Structures Technology Engine/Airframe Coupling Bruce

C. McClintick

General Electric Cincinnati,

Company Ohio

507

COMPUTATIONAL STRUCTURES TECHNOLOGY ENGINE / AIRFRAME COUPLING BC McCLINTICK

There experience,

are many

happening.

of engine

for the past 14 years,

3-dimensional engine static load conditions. utilization

aspects

structures However,

of the 3-dimensional Since

/ airframe

coupling

has been with the generation

to structures.

and analysis

My personal

of full

with regard to the design and operation of the engine under several problems arose about 6 years ago which required the models

then, full 3-dimensional

under

dynamic

engine

basis to help understand dynamics related problems. addresses, is engine related aircraft vibration.

508

related

loads

structural

to more models

fully understand have

One such problem,

been which

what

was

used on a regular this paper

Engine related aircraft vibration is noise within the fuselage of the aircraft which can be both felt and heard. This noise is generally caused by rotor imbalance and is transmitted from the engine

through

from the lower aircraft

system.

the structural

speed Many

only during certain unloaded, variations major

roles

vibration

rotor,

engine/airframe

PERCEIVED CAUSED •

encountered

must

Also, nearly

the primary matches

cause

frequencies

have also been non-linear

To effectively be treated

RELATED

NOISE

BY ROTOR

predict

engine

of noise

is

of the

and observed

related

becoming used play aircraft

as a system.

AIRCRAFT

VIBRATION

IS BOTH FELT AND HEARD IMBALANCE

PRIMARILY FAN ROTOR - LARGEST ROTOR - LOWEST SPEED ROTOR

CAN BE NON-LINEAR

IN NATURE



BEARING

TYPE



BEARING

STIFFNESS



MOUNT

ROTORS

STIFFNES_

=_ FRAMES

FUSELAGE •

more

Engine mounts becoming unloaded, bearings and bearing stiffness, and the types of bearings

of vibration.

ENGINE

of the aircraft.

as this rotor

of the problems

flight envelopes. in both mount

in the transmission

the entire

,

components

or fan rotor,

MUST

:=_ MOUNTS

:=_ CABIN/COCKPIT BE TREATED

=_ STRUT

=_ WING

=_

=_ PASSENGERS/CREW

AS A SYSTEM

509

Historically the engine has always been treated as a necessary evil to 'make the airplane go' and little emphasis was given to the engine other than making sure it stayed on the wing. The engine manufacturers sized the engine for thrust, designed for ultimate loads, minimized the affects of rotor modes and provided a reasonable balance at factory acceptance. The main point is not to over simplify the aircraft and engine design, which is indeed quite complex, but to point out that little was done in the design of the system to reduce or understand noise within the fuselage.

HISTORICAL #

#

ENGINE

/ STRUT

SYSTEM



ENGINE

A NECESSARY



FLU'ITER

STABILITY



ULTIMATE

LOADS



LIVE

RESULTS

WITH

EVIL

STRENGTH

ENGINE •

SIZED -

FOR LIKE



ULTIMATE



ENGINE



510

/ WING

THRUST ENTROPY LOADS

MODES

-

NOT

-

SIMPLE

-

RELIANCE

REASONABLE

- REQUIREMENT

ALWAYS

INCREASES

STRENGTH OUT

OF ROTOR

AT NORMAL DYNAMIC

OPERATING TEST

RANGE

SPEEDS

ANALYSES

ON ENGINE BALANCE

OPERATING UTILIZED DATA

AT FACTORY

ACCEPTANCE

As new

aircraft

were developed

it became

were less tolerant to noise and to maintain cockpit and cabin. Thus, tighter vibration on-wing some

trim balance

of the more

previously beginning

procedures

troublesome

used only for static of aircraft/engine

were

the norm.

vibration

problems,

analyses,

began

design

PASSENGERS/CREW

apparent

that both the passengers

for structural

Also,

as an aid to determining

3-dimensional

to be utilized borne

finite

for dynamics.

of

models,

This marked

the

80'S

LESS TOLERANT

TO PERCEIVED

SMOOTH TIGHTER

• •

ON-WING TRIM BALANCE PROCEDURES AFFER MARKET STRUCTURAL CHANGES

VIBRATION

AND QUIET REQUIRED TO SELL AIRPLANES PRODUCTION VIBRATION LIMITS

ELEMENT / STRUT

TO 'SYSTEM'

MODELS



ENGINE

• •

LARGE, COMPLEX MODELS (100,000 - 200,000 USED ONLY FOR SPECIAL PROBLEMS



SPECIAL

BEGINNING

the cause

element

noise.

• •

3-D FINITE

and crew

sales it was imperative to have a quiet, vibration free limits were imposed on engine manufacturers and

EARLY



more

PRIMARILY

ROUTINES

OF DESIGN

WRITTEN

FOR STATIC LOADS

FOR ROTOR

FOR STRUCTURAL

BORNE

DOF)

DYNAMICS NOISE

511

Large, complex engine structural models used for static models used for studying engine related aircraft vibration.

TYPICAL

512

ENGINE

STRUCTURAL

loads

MODEL

and deflections

were the first

FOR STATICS

New aircraft development in the later 1980's saw the integration of the engine and airframe as a system in attempts to predict the response of the aircraft cabin and cockpit to rotor imbalance. Aircraft / engine teams were formed to develop the necessary methodology to analyze, test and modify the system design to decrease structurally transmitted noise from the engine.

LATE *

GE UNDUCTED •





ENGINE

FAN - UDF _ RELATED

-

SIGNIFICANT

-

ENGINE

ENGINE

MOUNT

-

BLADE

-

AND

'ACTIVE'

80'S

AIRCRAF'I" DESIGN

/ AIRCRAFt

VIBRATION PARAMETER TREATED

AS

A SYSTEM

DESIGN OUTLOADS

- VIBRATION

VIBRATION

TRANSMISSION

REDUCTION

CONTROL

513

GE's Unducted Fan program vibration related data throughout analytically

monitored

GE UNDUCTED

514

for various

utilized a full airplane/engine structural model the airframe. Thus, cabin and cockpit vibration design

to generate was

changes.

FAN - UDF ® DUAL

ENGINE

DYNAMIC

ANALYSIS

Engine vibration related noise is now included in engine specifications. Thus, it is now necessary to include engine vibration transmission as a design parameter and develop the necessary methodology to predict noise within the aircraft before designs become 'fixed' and expensive to modify and change. Part of this methodology development is the correlation of the 3-dimensional finite element dynamic models with both engine testing and aircraft flight testing. Modelling techniques also need to be developed which address the specific needs for dynamic analyses and vibration transmission.

THE ENGINE

SPECIFICATION

3-D

- ENGINE



DESIGN

PARAMETER



ENGINE

MOUNTS

VIBRATION ENGINE



HARDWARE

• • •

- ENGINE DESIGNED

/ AIRCRAFT

RELATED

VIBRATION

NOISE

TRANSMISSION

TO REDUCE

TREATED

DESIGNED

ELEMENT TESTS

ENGINE

MODELS

FLIGHT

TESTS MODEL

AND

AS A SYSTEM BUILT

TO REDUCE

NOISE

MODELS

ENGINE

SYSTEM

VIBRATION

TRANSMISSION



FINITE

90'8

- PLANNED WITH

- PLANNED

AND

ACTUAL AND

PREDICTIONS

MODELLING TECHNIQUES USED FOR DYNAMICS AND VIBRATION

DESIGNED

TO CORRELATE

HARDWARE DESIGNED TO TEST

TO CORRELATE DATA

SPECIFICALLY TRANSMISSION

515

The complex, many DOF static structural model is still utilized for dynamic analyses; however, each of the structural components are reduced to a more manageable number of DOF's using dynamic reduction. The dynamic reduction reduces the components to its boundary DOF plus a limited number of DOF used to describe its vibratory modes. Also, many routines have been written to include such items as rotor gyroscopic stiffening, structural and viscous damping, non-linear stiffness and damping versus load and/or frequency and non-linear rub springs.

CURRENT 3-DIMENSIONAL

516

ANALYSIS

STRUCTURAL MODEL

TECHNIQUES

SYSTEM

- ALSO



COMPLEX



REDUCTION OF COMPONENTS TO DYNAMIC EQUIVALENCY - RETAIN OVERALL COMPONENT FLEXIBILITIES -

RETAIN

LOCAL

-

RETAIN

ALL

-

SIGNIFICANT



ROTOR



BEARINGS

USED

MODEL

INTERNAL

INTERNAL

STATICS

FLEXIBILITIES IMPORTANT

REDUCTION

GYROSCOPIC

FOR

MODES

IN DOF

STIFFENING

TERMS

- NON-LINEAR

-

STIFFNESS

VS ROTOR

-

STIFFNESS

/ DAMPING

VS FREQUENCY

-

STIFFNESS

/ DAMPING

VS BEARING



STRUCTURAL



ENGINE

MOUNT

LOADING LOAD

DAMPING STIFFNESS

VS LOAD

VS FREQUENCY

NASTRAN is currently used as a common analysis base between the aircraft and engine manufacturers and agreements are obtained between companies as to modelling number ranges. This permits ease of transmitting models to each other and similar DMAP can be utilized. Unique post-processing routines are utilized to review results from the steady state frequency response analyses.

CURRENT COMMON

ANALYSIS



DIRECT



LARGE

UNIQUE

ANALYSIS

TECHNIQUES

BASE

- NASTRAN

SOLUTION, AMOUNT

STEADY OF 'DMAP'

-

MATRIX

-

GYRO

-

NON-LINEAR

BEARINGS

-

NON-LINEAR

MOUNTS

-

SPECIAL

COMPONENT



RESPONSE



ANIMATION



BEARING

STATE

FREQUENCY

RESPONSE

WRITI'EN

INPUT STIFFENING

OUTPUT

POST-PROCESSING



(CONTINUED)

ROUTINES

ENERGIES (LOADS,

REQUIREMENTS

(POTENTIAL

DEFLECTIONS)

AND

KINETIC)

VS FREQUENCY

PLOTS / MOUNT

RESPONSE

517

This current static

and dynamic

on approximately than 5000.

new generation analyses. 15 major

strut/nacelle/engine

For dynamic components

__MODEL USED TO GENERATE

518

analysis to reduce

structural the model the number

DYNAMICAIJLY

model

is being

will undergo of DOF

SIM!!,AR

utilized

dynamic

from over

for both reduction

150,000

COM_PONENTS

to less

Component dynamic matrices are generated using fixed boundary component modes. The resulting mass and stiffness matrices are of the form shown. Each of the N component modes can be obtained from Ki]Mi and are coupled to the M boundary DOF by only the mass matrix. Also, full structures

can be generated

from

matrices generated from both a symmetric with the aircraft structure.

a symmetric

and anti-symmetric

COMPONENT N: COMPONENT MASS

DYNAMIC

structure

by combining analysis.

DYNAMIC

This is commonly

done

MATRICES

M: COMPONENT

DOF

the dynamic

BOUNDARY

STIFFNESS

MATRIX

DOF

MATRIX |

M1

|

M2