Residual stress measurements that correlate fatigue and fracture behavior Residual Stress Summit 26 September, 2010 Tahoe City, CA
←
→
Page content transcription
If your browser does not render page correctly, please read the page content below
Residual stress measurements that correlate fatigue and fracture behavior Residual Stress Summit 26 September, 2010 Tahoe City, CA Michael R. Hill Professor Mechanical and Aeronautical Engineering University of California, Davis mrhill@udavis.edu President Hill Engineering, LLC McClellan, CA
Acknowledgements Development of laser shock peening (LSP) (1999 to present) LLNL and MIC (Lloyd Hackel) Boeing and Lockheed-Martin (Jim Pillers, Jeff Bunch, Tom Brussat, Dale Ball) FAA Rotorcraft Damage Tolerance (RCDT) Program (2006 - Pres) John Bakuckas, Traci Stadtmueller, Felix Abali, Dy Le NAVAIR SBIR Phase I and II (established Hill Engineering, LLC) “Design Tools for Fatigue Life Prediction in Surface Treated Aerospace Components”, 2004 to 2009 Ravi Ravindranath (NAVAIR) Mike Shepard (AFRL) Pratt & Whitney (Bob Morris) USAF SBIR Phase I and Phase III “Design/Life Prediction Tools for Aircraft Structural Components with Engineered Residual Stresses”, 2008 – Pres) Kristina Langer (AFRL) NRC/EPRI joint program on weld residual stress Al Csontos, Howard Rathbun, Matthew Kerr Paul Crooker, Eric Willis My graduate students Makarenko, Lin, Yau, McKenna, Meith, Rankin, Demma, DeWald, Truong, Bhoon, Lee, Cuellar, Boyd, Chandra, Pistochini, Liu, Hopkins, Luong, VanDalen, Stuart, Minotti 2
Presented at the 2nd Int’l Laser Peening Conf (19Apr10) Presented by David Jensen, Boeing Glass bead peening = Durability Small number of aircraft 3
Presented at the 2nd Int’l Laser Peening Conf (19Apr10) Presented by David Jensen, Boeing Laser shock peening = DT and Durability Small number of aircraft Process matured on test airframe “Current capability is on track for implementation in 2011” 4
Residual stress engineering methods for sustainment Sustainment: assuring structural safety in presence of degradation Sub-critical cracking (fatigue, SCC, creep) Residual strength (fracture) Characterize residual stress fields in parts Residual stress measurements More complicated than Residual stress predictions determining applied stress field Combine applied and residual stress fields (linear or non-linear) Correlate performance under combined stress fields Remove effects of residual stress in property measurements (fatigue crack growth and fracture properties) the “reverse problem” (ref: Dale Ball, RS Summit 2007, ASIP Con 2008) Forecast effects of residual stress on performance (fatigue crack growth, stress corrosion cracking, residual strength) the “forward problem” Objectives for today’s session Describe residual stress measurement methods Describe coupon-scale experiments Show correlation of fatigue and fracture data Is behavior as expected from combined stress fields? 5
Residual stress background Residual stresses play a significant role in many failure mechanisms Examples: fatigue, fracture, stress corrosion cracking Tensile RS decrease performance Compressive RS increase performance Subsurface 1 mm • Often provided by surface treatments initiation From: M. J. Shepard, P. S. Prevéy, N. Jayaraman, Residual stresses satisfy equilibrium “Effects of surface treatment on fretting fatigue performance of Ti-6Al-4V”, Proceedings of the 8th Residual stresses in all parts are both National Turbine Engine High Cycle Fatigue Tensile and Compressive Conference, April 14-16, Monterey, CA, 2003. Example: compressive stress treatments • Compressive in treatment zone • Tensile outside treatment zone Need to understand through- thickness residual stress • Can lead to, e.g., sub-surface crack variations in coupons and initiation (> 1 mm depth) components 6
Slitting method residual stress measurement Provides a 1-D stress “profile”, through thickness Parts of arbitrary cross section, but prismatic Wide range of thickness Experimental steps Instrument with strain gage(s) Incrementally cut slit into body, measure strain release vs depth of cut Solve for initial residual stress from measured strain (elastic inverse) Representative slitting measurement Laser peened block of material 7
Working principle (Iain Finnie and co-workers, 1971 and following) Consider a beam or plate containing residual stress Slit incrementally to a set of depths (a1, a2, …) Measure strain release at each depth (ai) at two gages (“front” and “back”) Assume Elastic stress release No stress variation out of plane (z) Released strain a function of Residual stress perpendicular to slit Elastic properties Geometry: gage sizes, positions part and slit dimensions Find stress from measured strain (elastic inversion) Assume polynomial expansion Find Aj to determine RS(y) RS (y) = A P (y)j j j= 2,m Non-polynomial alternative available (the “pulse method”) 8
Laser Shock Peening (LSP) Process Description An extension of conventional shot peening Laser peening provides High compressive surface stress Deep compressive stress Low cold work Smooth surface Process control Photo courtesy of Metal Improvement Company 9
Slitting useful in understanding effects of LSP parameters Rectangular, highly uniform laser beam intensity distribution is coupled to the part using an optical delivery system that preserves the uniform intensity Peening pulses are applied sequentially in complete rows without the need for re-coating the surface Photo and graphic courtesy of ablation layer Metal Improvement Company Key laser shock peening parameters: Irradiance (GW/cm2) (proportional to peak pressure) Pulse width (nsec) Number of layers (number of times surface is covered) Optimal parameters depend on material, geometry, and failure mode 10
Effects of LSP parameters in titanium alloy Process variations studied in 0.5 inch thick block coupons Material: BSTOA Ti6Al4V Increases in irradiance and layers increase depth of compression Key: (GW/cm2-nsec-#layers) XRD difficult in this large grained material 11
Benchmark Slitting with Contour and X-ray: Set-up Uniformly LSP entire surface of titanium alloy plate Cut into 4 block coupons Each 25 x 25 x 8.7 mm Measure residual stress Slitting, Contour, X-ray diffraction Expect good agreement Uniform microstructure, small equiaxed grains Residual stress field that meets assumptions of methods 12
Benchmark Slitting with Contour and X-ray: Results Very favorable results Some differences in near-surface behavior Good agreement in integral of stress with depth LSP Surface 13
Establish intralaboratory repeatability of Slitting: Set-up Uniformly LSP entire surface of 316L stainless steel plate Initially: 100 x 250 x 17.9 mm Cut into 10 block coupons Each 50 x 50 x 17.9 mm Each block should have similar RS • Expect low variability in LSP process, material properties • Observe variability in RS measurement Measure RS in six blocks 14
Establish intralaboratory repeatability of Slitting: Results Results in six blocks All six measurements shown along with average and deviation RMS deviation: ~40 MPa near surface ~10 MPa away from surface Demonstrated repeatability error < 5% of peak stress 15
Session objectives Describe residual stress measurement methods Describe coupon-scale experiments Show correlation of fatigue and fracture data Is behavior as expected from combined stress fields? Summary comments 16
Tests and analyses of C(T) coupons with residual stress Are residual stress data useful? YES, if they correlate mechanical performance! Without such correlation, merely “reference data” Objective: Determine the degree of correlation achieved by combination of applied and residual stresses for fracture and fatigue crack growth under (nearly) SSY conditions Approach Designed residual stress bearing C(T) coupons • 5 different residual stress levels Developed test data • Residual stress fields • Fracture data • Fatigue crack growth data Carried out companion analyses • Fracture: superposition of applied and residual K • Fatigue crack growth: superposition, LEFM, and NASGRO equation 17
Coupon design ASTM C(T) coupons Clad 7075-T6 Al sheet, 4.8 mm thick Low-energy, ductile fracture B = 3.8 mm, W = 50.8 mm, L-T Residual stress from Laser Shock Peening Repeatable, controlled, low cold work, deep compression Applied to both sides In a square region (23mm wide) • Near the front face (N) LSP Near • Far from the front face (F) front face LSP intensity varied by layers: (KRS Negative) low (1) or high in (3) Five conditions AM, LSP-1F, LSP-1N, LSP-3F, LSP-3N LSP Far from Tests performed Fracture tests (K-R and FCG) front face Measure RS (contour) (KRS Positive) Measure KRS (slitting) 18
Contour residual stress measurement Opening stress, on crack plane LSP-3N • Compression in peened area • Balancing tension and bending AM: rolling Good repeatability Material Processing Measurements 19
Contour residual stress measurement Opening stress, on crack plane LSP-3N • Compression in peened area Thickness-average residual stress • Balancing tension and bending AM: rolling Good repeatability 20
Slitting residual stress measurement: Strain data Back-face strain gage (a) High levels of strain Significant differences among coupon conditions 21
Slitting residual stress measurement: Computed stress Back-face strain gage (a) Data reduction used the unit pulse method (Schajer and Prime, JEMT 2006) 22
Validation opportunity: Stress from Slitting and Contour Slitting and Contour each use different measured quantities Comparison of results provides validation Compare Slitting with thickness-average of Contour results Thickness-average residual stress 300 LSP-3N - Slitting LSP-3N - Contour 200 AM - Contour Residual Stress (MPa) 100 0 -100 -200 0 10 20 30 40 50 60 x (mm) 23
Slitting also provides KRS(a) Schindler’s method Schindler, H.J. and P. Bertschinger. “Some Steps Towards Automation of the Crack Compliance Method to Measure Residual Stress Distributions.” in Proc. 5th Int. Conference on Res. Stress. 1997. Linköping. E d(a) (a) = K RS (a) Z(a) da Note: crack size measured from loading holes. a = x – 12.7 mm 24
Validation opportunity: KRS(a) from Slitting and Contour E d(a) a Slitting K RS (a) = Contour K RS (a) = 0 RS (x) m(x,a)dx Z(a) da Residual stress intensity factor 20 Green’s Function, or Slitting, d/da Weight Function 15 Slitting stress + GF Contour stress + GF 10 KRS (MPa m ) 0.5 5 0 Note: crack size -5 measured from loading holes. -10 a = x – 12.7 mm -15 -20 0 10 20 30 40 50 a (mm) 25
Fracture toughness tests R-curve tests to ASTM E561-98 Load vs CMOD data Initiation toughness to E399 (KQ, not sized for KIc) Results ignoring, and including residual stress KQ,Tot = KQ,App(ao) + KRS(ao) KR,Tot(ae) = KR,App(ae-ao)+KRS(ae) Details Precracking performed to E 561 • Constraint: final 0.65mm >5,000 cycles • Guideline: Kmax = 0.0001E m1/2 • Account for KRS effects • Compression-compression for LSP-1F, LSP-3F • High stress ratio tension-tension for LSP-1N, LSP-3N Valid a0 Effective crack extension, ae • Initial and final physical crack lengths measured 26
Observed load, displacement Peak load significantly affected by residual stress KRS(a0) > 0 Reduced Pmax KRS(a0) < 0 Increased Pmax Valid a0 27
Initiation toughness, KQ Ignoring residual stress: spread is 9.7 to 52 MPam0.5 28
Initiation toughness, KQ Ignoring residual stress: spread is 9.7 to 52 MPam0.5 Including residual stress: spread is 32 to 37 MPam0.5 KQ,Tot = KQ,App(ao) + KRS(ao) LSP-3F LSP-1F AM LSP-1N LSP-3N 29
R-curve, ignoring residual stress Two replicates for each condition Applied load and CMOD data only LSP Near front face (KRS Negative) LSP Far from front face (KRS Positive) 30
R-curve, including residual stress Linear superposition KR,Tot(ae) = KR,App(ae-ao)+KRS(ae) LSP Near front face (KRS Negative) LSP Far from front face (KRS Positive) 31
Fatigue crack growth prediction Constant Pmax (0.98 kN for AM, 2.22 kN for LSP) Rapp = 0.1 (K increasing) LSP-3N coupon condition (KRS < 0) LSP-3N AM LSP-3N AM 32
Fatigue crack growth data and prediction Constant Pmax (0.98 kN for AM, 2.22 kN for LSP) Rapp = 0.1 (K increasing) LSP-3N coupon condition (KRS < 0) LSP-3N AM LSP-3N AM 33
Comments on fracture toughness and FCG testing Sample design provided useful coupons for study Significant residual stress levels Range of residual stress effect (sign and magnitude) Repeatable processing Wide range of KRS(ao) -50% to 78% of as-machined KQ Residual stress measurement methods in agreement Stress distribution KRS(a) Residual stress data provided useful correlation Across all coupon conditions Initation toughness R-curve Fatigue crack growth More than merely reference data!! 34
Residual stress complicates the building block approach Sustainment engineering often uses building blocks Proof of concept data in simple, typically small, coupons Success in coupons used as gate for more complicated tests De Simple cr Develop/Optimize ea Feature Tests si Technology ng Ri sk Quantify Variation of More Complicated for Intended St Feature Tests ru Application ct ur al Fa Develop ilu KEY: Component re Analysis Tests Analysis Methodology Verified By Testing Demonstrate Technology for Full -Scale Actual Tests Application 35
Residual stress complicates the building block approach Size and shape differences between coupons and components Residual stresses must be different Benefits in coupons will not equal benefits in structure B Bair, et al, 2009 ASIP Conference Need to validate residual stress engineering tools at appropriate scales and develop methods for transferability between coupon and full scales Residual Stress (ksi) Depth from surface (in) 36
Summary Residual stress engineering is advancing Residual stress measurement Residual stress modeling Test experience with well-characterized coupons and components Measurements of full-field residual stress enable fundamental understanding of fracture and fatigue behavior Can be exploited for validation of residual stress models The majority of our work shows superposition to be adequate for many problems Coupon scale data show good correlation with expected behavior (when residual stress is known) Be aware of challenges and complications in transferring results between coupon and full scales Must have continued support for development of residual stress engineering methods Government and industry sponsorship Advanced process design and specifications Industrial use Standardization 37
Thank you. 38
Contact Information Michael R. Hill Mechanical and Aeronautical Engineering University of California One Shields Avenue Davis, CA 95616 mrhill@ucdavis.edu (530) 754-6178 Hill Engineering, LLC Adrian DeWald, Managing member atdewald@hill-engineering.com (916) 635-5706 Hill Engineering provides residual stress measurements and residual stress engineering services to industry. 39
Transition in residual stress engineering paradigm Historical Future Residual Stresses are Residual Stresses are part of managed consequences higher-order specifications that affect design performance that ensure design performance Residual stress measurements are Residual stress measurements are opportunistic or last resort routine and part of quality program Tensile residual stresses removed Tensile residual stresses limited by where possible; accounted for with specifications and improvements in high conservatism if required process design and toolsets Compressive stress treatments used Compressive stress treatments widely sparingly to assure safety & available, part of design and repair sustainability engineering Residual stress engineering methods Residual stress engineering methods and tools highly specific, developed and tools are vetted through broad for unique events consensus (Standards, Code cases) Residual stress engineering is Residual stress engineering is a expensive, time-consuming work of manageable discipline, consistent experts with economic considerations Future needs require advances in residual stress engineering methods and tools 40
Similar test program in open hole coupons Can we also achieve good correlation in more relevant geometry? Material and geometry Open hole 7075 T6 sheet a • Clad (C) or Bare (B) • 2.03mm thick Residual stresses As-machined (AM) Split-sleeve cold expanded (CX) • 3% interference Reamed after CX As Machined Cold Expanded Loading B1 C1 B1 C1 R = 0.1 Constant amplitude load B2 C2 B2 C2 Stress ratios: R=0.1, R=0.5 B1 C1 B1 C1 R = 0.5 B2 C2 B2 C2 8 test variations, 8 replicates 41
Contour residual stress measurements 2-D residual stress distribution thickness-average 3 coupons measured on both sides = 6 measurements ±10% variability in through thickness average Through thickness average stress distribution 100 0 Bare Right Residual stress (MPa) -100 Bare Left Clad Right -200 Clad Left Clad2 Right -300 Clad2 Left Average -400 -500 ±10% variability Length in (mm) -600 0 2 4 6 8 10 12 14 16 Stress in (MPa) Distance from edge of hole (mm) 42
Results for as-machined coupons, R=0.1 Low variability in crack growth history Good correlation with LEFM prediction 8 Fatigue crack growth rate (mm/cycle) B080-1NC 7 C080-1NC -4 10 C080-2NC 6 LEFM Crack size (mm) 5 4 B080-1NC 3 C080-1NC 2 C080-2NC -5 10 1 LEFM 0 0 50000 100000 150000 200000 0 1 2 3 4 5 6 7 8 Cycles Crack size (mm) 43
Results for cold-expanded coupons, R=0.1 Greater variability in crack growth history Factor of 9 spread in lifetime Good correlation with LEFM prediction (including spread) 8 Fatigue crack growth rate (mm/cycle) B080-14 -3 C080-08 10 7 C080-06 C080-14 6 LEFM LEFM 90% Crack size (mm) LEFM 110% 5 -4 10 4 B080-14 3 C080-08 C080-06 2 -5 C080-14 10 LEFM LEFM 90% 1 LEFM 110% 0 0 50000 100000 150000 200000 0 1 2 3 4 5 6 7 8 Cycles Crack size (mm) 44
You can also read