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Modeling Reliability of Ceramics Under Transient Loads and Temperatures Noel N. Nemeth Osama M. Jadaan Eric H. Baker The 26 th Annual International Conference on Advanced Ceramics & Composites January 13-18, 2002, Cocoa Beach Florida Glenn Research Center at Lewis Field E-mail: [email protected] Life Prediction Branch

Modeling Reliability of Ceramics Under Transient Loads and Temperatures Noel N. Nemeth Osama M. Jadaan Eric H. Baker The 26 th Annual International Conference

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Modeling Reliability of Ceramics Under Transient Loads and Temperatures

Noel N. Nemeth

Osama M. Jadaan

Eric H. Baker

The 26th Annual International Conference on Advanced Ceramics & Composites

January 13-18, 2002,

Cocoa Beach Florida

Glenn Research Centerat Lewis Field

E-mail: [email protected]

Life Prediction Branch

Outline Objective Background - CARES/Life

- References to previous work

Theory - Power law & Walker law

- Computationally efficient method for cyclic loading

Examples - Diesel exhaust valve

- Alumina static fatigue

Conclusions

Objective

Develop a methodology to predict the time-dependent reliability (probability of survival) of brittle material components subjected to transient thermomechanical loading, taking into account the change in material response with time.

Transient reliability analysis

Fully Transient Component Life Prediction

MOTIVATION: To be able predict brittle material component integrity over a simulated engine operating cycle

REQUIRES:

• Life prediction models that account for: - transient mechanical & temperature loads - transient Weibull and fatigue parameters (temperature/time)

• Interface codes that transfer transient analysis finite element results into life prediction codes (CARES/Life)

CARES/Life (Ceramics Analysis and Reliability Evaluation of Structures)

Software For Designing With Brittle Material Structures

CARES/Life – Predicts the instantaneous and time-dependent probability of failure of advanced ceramic components under thermomechanical loading

Couples to ANSYS, ABAQUS, MARC, NASTRAN

CARES/Life Structure

Reliability EvaluationComponent reliability analysis determines “hot spots” and the

risk of rupture intensity for each element

Parameter EstimationWeibull and fatigue parameter

estimates generated fromfailure data

Finite Element InterfaceOutput from FEA codes

(stresses, temperatures, volumes)read and printed toNeutral Data Base

Paluszny and Nicholls (1978) -- Discrete time steps, SCG, Weibull and fatigue parameters were constant: Paluszny, A., and Nicholls, P. F., “Predicting Time-Dependent Reliability of Ceramic Rotors,” Ceramics for High Performance Applications-II, edited by Burke, J., Lenoe, E., and Katz, N., Brook Hill, Chesnut Hill, Massachuestts, 1978.

Jakus and Ritter (1981) -- Probabilistic parameters for both applied stress (truncated Gaussian distribution) and component strength (Weibull distribution): Jakus, K., and Ritter, J, “Lifetime Prediction for Ceramics Under Random Loads,” Res Mechanica, vol. 2, pp. 39-52, 1981.

Stanley and Chau (1983) – Failure probability for non-monotonically increasing stresses (maximization procedure): Stanley, P., and Chau, F. S.; “A Probabilistic Treatment of Brittle Fracture Under Non-monotonically Increasing Stresses,” Int. J. of Frac., vol. 22, 1983, pp. 187-202.

Bruckner-Foit, A., and Ziegler (1999) – 3 Reliability formulations; no SCG, SCG governed by a power law,\ and SCG governed by a power law with a threshold: (1) Bruckner-Foit, A., and Ziegler, C., “Design Reliability and Lifetime Prediction of Ceramics,” Ceramics:Getting into the 2000’s, edited by Vincenzini, P., 1999. (2) Bruckner-Foit, A., and Ziegler, C., “Time-Dependent Reliability of Ceramic Components Subjected to High-Temperature Loading in a Corrosive Environment,” ASME paper number 99-GT-233, International Gas Turbine and Aeroengine Congress and Exhibition, Indianapolis, Indiana, 1999.

Ziegler (1998) -- SCG parameters vary with temperature/time: Ziegler, C., Bewertung der Zuverlassigkeit Keramischer Komponenten bei zeitlich veranderlichen Spannungen und bei Hochtemperaturbelastung, Ph.D. Thesis, Karlsruhe University, 1998.

Jadaan and Nemeth (2001) – Cyclic loading + Weibull and SCG parameters vary with temperature/time: (1) Jadaan, O, and Nemeth, N. N.;”Transient Reliability of Ceramic Structures.” Fatigue & Frac. Of Eng. Mater. Struct., vol. 24, pp. 475-487. (2) Nemeth, N. N., and Jadaan, O.; “Transient Reliability of Ceramic Structures For Heat Engine Applications,” Proceedings of the 5th Annual FAA/Air Force/NASA/Navy Workshop on the Application of Probabilistic Methods to Gas Turbine Engines, June 11-14, 2001, Westlake Ohio.

Some References Regarding Transient Reliability Analysis

Transient Life Prediction TheoryFor Slow Crack Growth

Assumptions:

• Component load and temperature history discretized into short time steps

• Material properties, loads, and temperature assumed constant over each time step

• Weibull and fatigue parameters allowed to vary over each time step – including Weibull modulus

• Failure probability at the end of a time step and the beginning of the next time step are equal

Transient Life Prediction Theory -Slow Crack Growth and Cyclic Fatigue Crack Growth Laws

Power Law: - Slow Crack Growth (SCG)

t),(K A(t) = dt

t),da( N(t)Ieq

Combined Power Law & Walker Law: SCG and Cyclic Fatigue

- Denotes location and orientation

t),(K ))(R1(f(t)A

t),(K g(t)A = dt

t),da(

N(t)Ieq

)t(Qc2

N(t)Ieq1

Transient Life Prediction Theory -Power Law

}]]...

....]]

)([[...[[4V{-exp)(

211

210

11,

20

,)2(

)2(

20

,

2

0

max,,in

1=i

1

1

1

1

)2(

)2(

iN

m

VNBV

NIeq

j

VjNBVj

jN

jIeqNm

Nm

kVk

NBVk

kN

kIeq

N

BVk

TkIeqkSV

dB

t

B

t

B

t

tP

V

V

V

V

VjNVim

ViNVjm

Vj

Vj

VkVj

VjVk

Vk

Vk

Vk

General reliability formula for discrete time steps:

33n22n1nnn yx

!3

2n1nnyx

!2

1nnynxxyx

Binomial Series Expansion:

(x + y)n xn + nxn-1 y , when x >> y

When x>>y the series can be approximated as a two term expression

Binomial Series Approximation Used to Derive Computationally

Efficient Solution For Cyclic Loading

)21VN(km

)2kN(1Vm

1V

1V)2)1k(VN()2k(Vm

)2)2k(VN()1k(Vm

)1k(V

)1k(V)2VkN()1k(Vm

)2)1k(VN(Vkm

Vk

Vk

)21VN(km

)2kN(1Vm

1V

1V)2)1k(VN()2k(Vm

)2)2k(VN()1k(Vm

)1k(V

)1k(V)2VkN()1k(Vm

)2)1k(VN(Vkm

Vk

Vk

11V

2N1BV0

1nN

1,Ieq1k

)1k(V2N)1k(BV0

)1k(nN

)1k(,Ieqk

Vk2N

BVk0

knN

k,Ieq

11V

2N1BV0

12N

1,Ieq1k

)1k(V2N)1k(BV0

)1k(2N

)1k(,Ieqk

Vk2N

BVk0

k2N

k,Ieq

]B

tZ.......]

B

tZ]

B

tZ...

...]B

tZ.......]

B

tZ]

B

tZ

)21VN(km

)2kN(1Vm

1V

1V)2)1k(VN()2k(Vm

)2)2k(VN()1k(Vm

)1k(V

)1k(V)2VkN()1k(Vm

)2)1k(VN(Vkm

Vk

Vk

Vk

11V

2N1BV0

11N

1,Ieq1k

)1k(V2N)1k(BV0

)1k(1N

)1k(,Ieqk

Vk2N

BVk0

k1N

k,Ieq

2N

BVk0

maxT,k,Ieq1

]B

tZ.......]

B

tZ]

B

tZ

[[[...[[[...[[...[...X

}]d]X[[4V{-exp)t(P i21vN

1vm

11i

n

1=i

kSV

n

1i

iTotal ZZComputationally efficient transient reliability formulafor cyclic loading- full solution

Computationally efficient transient reliability formulafor cyclic loading- full solution

Transient Life Prediction Theory - Slow Crack Growth Modeled With Power Law

Computationally efficient transient reliability formulafor cyclic loading- simplified version

Computationally efficient transient reliability formulafor cyclic loading- simplified version

}]]...

....]]

)([[[...[4V{-exp)(

211

210

11,

20

,)2(

)2(

20

,

2

0

max,,in

1=i

1

1

1

1

)2(

)2(

iN

m

VNBV

NIeq

j

VjNBVj

jN

jIeqNm

Nm

kVk

NBVk

kN

kIeq

N

BVk

TkIeqkSV

dB

tZ

B

tZ

B

tZ

tP

V

V

V

V

VjNVim

ViNVjm

vj

Vj

VkVj

VjVk

Vk

Vk

Vk

TT

2T ZT

load

time

}]dB

tZ)R1(A

Af1

...

...B

tZ)R1(A

Af1

B

tZ)R1(A

Af1

[[...[4V{-exp)t(P

i

)2N(

m

1

1V2N

1BV0

1Q

1V1

2c

N

1,Ieq

T,1,IeqN1,Ieq

)2N(m

)2N(m

j

Vj

2N

BVj0

j

Q

Vj1

2c

N

j,Ieq

T,j,IeqN

j,Ieq

)2N(m

)2N(m

k

Vk2N

BVk0

kQ

Vk1

2c

N

k,Ieq

T,k,IeqNk,Ieq2N

BVk0

T,k,Ieq

in

1=ikSV

1V

1V

1V

1V

1V

Max1V

VjVi

ViVj

Vj

Vj

Vj

MaxVj

VkVj

VjVk

Vk

Vk

Vk

MaxVk

Vk

Max

Combined Walker Law & Power Law for cyclic fatigue- Computationally efficient version with Z factor multiple

Combined Walker Law & Power Law for cyclic fatigue- Computationally efficient version with Z factor multiple

10 step transient uniaxial loading for a single load block – single element problem

Time step #

Time Ieq Temp

1 25 100 100

2 50 90 200

3 75 80 300

4 100 70 400

5 125 60 500

6 150 70 600

7 175 80 700

8 200 90 800

9 225 95 900

10 250 100 1000

Temp m o N B

100 5 230 40 0.0021

500 9 226 36 0.021

1000 14 221 31 0.21

Temperature vs: material properties

Example – Tradeoff Between Accuracy

and Computational Efficiency For a Cyclic Load

Exact solution versus the Z approximation method for one solution increment (n = 1)• The results for one solution increment represent the least accurate but most computationally efficient answer.

Number of cycles

Pf ,

Exact solution

Pf ,

Z method

% Error

1 4.6620E-3 4.6620E-3 0.0

10 6.3066E-3 6.3066E-3 -2.0E-4

100 8.5288E-3 8.5288E-3 -4.0e-4

1000 0.011530 0.011530 -6.0E-4

10,000 0.015578 0.015578 -0.001

100,000 0.021032 0.021032 -0.002

1,000,000 0.028369 0.028368 -0.005

Note: Load factor is 0.5

Pf = Failure Probability

Exact solution versus the Z approximation method for one solution increment (n = 1)• The results for one solution increment represent the least accurate but most computationally efficient answer.

Number of cycles

Pf ,

Exact solution

Pf ,

Z method

% Error

1 0.16428 0.16428 0%

10 0.21701 0.21571 -0.6

100 0.28955 0.28037 -3.2

1000 0.41831 0.36997 -11.6

10,000 0.70425 0.68330 -3.0

100,000 0.96954 0.96850 -0.1

1,000,000 0.99997 9.99997 -1.0E-4

Note: Load factor is 1.0

Pf = Failure Probability

Cycles Pf

exact solution

Pf

n = 1

Pf

n = 2

Pf

n = 5

Pf

n = 10

Pf

n = 100

Pf

n = 500

Pf

n = 1000

1,000 0.41831 0.36997 0.39447 0.40958 0.41420 0.41796 0.41827 0.41831

100,000 0.96954 0.96850 0.96864 0.96877 0.96884 0.96924 0.96948 0.96951

Example of Z approximation method for various values of n. The solution increments are equally spaced (Zi = Zj= Zn).

Percent error from exactsolution versus numberof load blocks for afailure probability predictionof 1000 cycles

Percent error from exactsolution versus numberof load blocks for afailure probability predictionof 1000 cycles

n = Number of discrete load blocks

IncreasingComputational

Effort

Pf = Failure Probability

EXAMPLE: Diesel Engine Si3N4 Exhaust Valve (ORNL/Detroit Diesel)

DATA: Material: Silicon Nitride NT551Information Source: Andrews, M. A., Wereszczak, A. A., Kirkland, T. P., and Breder, K.; “Strength and Fatigue of NT551 Silicon Nitride and NT551 Diesel Exhaust Valves,” ORNL/TM1999/332. Available from the Oak Ridge National Laboratory 1999

Corum, J. M, Battiste, R. L., Gwaltney, R. C., and Luttrell, C. R.; “Design Analysis and Testing of Ceramic Exhaust Valve for Heavy Duty Diesel Engine,” ORNL/TM13253. Available from the Oak Ridge National Laboratory, 1996

MODEL: • ANSYS FEA analysis using axisymmetric elements

• Combustion cycle (0.0315 sec.) discretized into 29 load steps

• A 445 N (100 lb) spring pre-load applied to valve stem in open position. 1335 N (300 lb) on valve stem on closure. Thermal stresses superposed with mechanical stresses

• Volume flaw failure assumed

OBJECTIVE: Contrast failure probability predictions for static loadingVersus transient loading of a Diesel engine exhaust valve for the power law and a combined power & Walker law

0

500

1000

1500

2000

2500

0 0.01 0.02 0.03 0.04

Time (sec)

Pres

sure

(psi

)

Pressure load applied to face of a ceramic valve over

the combustion cycle

Pressure load applied to face of a ceramic valve over

the combustion cycle

Thermaldistribution

Thermaldistribution

First principalstress at maximum

applied pressure

(MPa)

First principalstress at maximum

applied pressure

(MPa)

Loading and Stress Solution of Diesel Engine Exhaust Valve

Silicon Nitride NT551 Fast Fracture and SCG Material Properties

T (C) m 0V

(MPa.mm3/m)

Average strength

(MPa)

N B(MPa2.sec)

Q A2A1

20 9.4 1054 806 31.6 5.44e5  3.2 0.65

700 9.6 773 593 87 1.12e4 3.2 0.65

850 8.4 790 577 19 1.13e6 3.2 0.65

Power Law Parameters (NT551): N and BCyclic Fatigue Parameters: Q and A2A1

Note: Cyclic fatigue parameters are assumed values for demonstration purposes only

Diesel Engine Si3N4 Exhaust Valve

Batdorf, SERR criterion with Griffith crack

Transient and static probability of failure versus combustion cycles(1000 hrs = 1.14E+8 cycles)

Diesel Engine Si3N4 Exhaust Valve

Transient reliability analysis with proof testing capability for combined Walker & power law

Diesel Engine Si3N4 Exhaust Valve

Transient reliability analysis with proof testing capabilityProof test: 10,000 cycles at 1.1 load level

EXAMPLE: Predict material reliability response of an alumina assumingtime varying Weibull & Fatigue Parameters

DATA: Material: AluminaSpecimen: 4-pt flexure (2.2mm x 2.8mm x 50mm -- 38mm and 19mm bearing spans)

Test Type: Static FatigueTemperature: 10000 CSource: G. D. Quinn – J. Mat. Sci. – 1987

MODEL: • Single element model of specimen inner load span (2.8mm x 19mm)

with uniform uniaxial stress state (surface flaw analysis)

• Loading is static (non-varying) over time

• Weibull and fatigue parameters vary with the log of the time

PROCEDURE: A single element CARES neutral file is constructed withdiscrete time steps (10 steps per decade on a log scale)spanning 8 orders of magnitude. Applied load is constantbut Weibull and fatigue parameters allowed to vary with each time step.

EXAMPLE: Time Dependent Weibull & Fatigue Parameters

G. D. Quinn, “Delayed Failure of a Commercial Vitreous Bonded Alumina”; J. of Mat. Sci., 22, 1987, pp 2309-2318.

Static Fatigue Testing of Alumina (4-Point Flexure)

10000 C

t = 1.6 sec., m = 29.4, 0= 165.8, N = 6.7, B = 2711.1

t = 31.6 sec., m = 15.8, 0= 152.7, N = 13.2, B = 9707.7

t = 1.0E+5 sec., m = 13.1, 0= 127.3, N = 36.4, B = 2276.2

Parameters interpolatedwith log of time -No extrapolationoutside of range

t = 1.6 sec., m = 29.4, 0= 165.8, N = 6.7, B = 2711.1

t = 31.6 sec., m = 7.4, 0= 263.3, N = 8.0, B = 2395.9

t = 316.2 sec., m = 4.5, 0= 870.1, N = 9.0, B = 10,389.0

Parameters interpolatedwith log of time -No extrapolationoutside of range

Conclusions

A computationally efficient methodology for computing the transient reliability in ceramic components subjected to cyclic thermomechanical loading was developed for power law (SCG), and combined power & Walker law (SCG & cyclic fatigue).

This methodology accounts for varying stresses as well as varying Weibull and fatigue parameters with time/temperature.

FORTRAN routines have been coded for the CARES/Life (version 6.0), and examples demonstrating the program viability & capability were presented.

Future Plans

Goal to release CARES/Life 6.0 to engine companies for evaluation/beta testing by 9/30/02

- Continuing benchmarking activities - Continue developing GUI - Complete ANSYS and ABAQUS interfaces - User guide with example problems ?? (FY’02 - FY’03)

CARES/MEMS - Single crystal reliability - Edge recognition macro within ANSYS - Edge flaw reliability model