Laser shock peening (LSP) is a surface treatment process to improve the surface integrity of metallic components. The nearly pure mechanical process of LSP results in favorable surface integrity such as compressive residual stress and improved surface material properties. Since LSP is a transient process with laser pulse duration time on the order of 40 ns, real time in-situ measurement of laser/material interaction is very challenging, if not impossible. A fundamental understanding of laser/material interactions is essential for LSP planning. Previous finite element simulations of LSP have been limited to a single laser shock location for both two and three dimensional modeling. However, actual LSP are performed in a massively parallel mode which involves almost simultaneous multi-laser/material interactions in order to induce uniform compressive residual stress across the entire surface of the workpiece. The massively parallel laser/material interactions have a significant compound/interfering effect on the resulting surface integrity of the workpiece. The numerical simulation of shock pressure as a function of time and space during LSP is another critical problem. The purpose of this paper is to investigate the effects of parallel multiple laser/material interactions on the stress/strain distributions in the workpiece during LSP of AISI 52100 steel. FEA simulations of LSP in single and multiple passes were performed with the developed spatial and temporal shock pressure model via a subroutine. The simulated residual stresses agree with the measured data in nature and trend, while magnitude can be influenced by the interactions between neighboring peening zones and the locations of residual stress measurement. Design-of-experiment (DOE) based simulations of massive parallel LSP were also performed to determine the effects of laser intensity, laser spot size, and peening spacing on stresses and strains. Increasing the laser intensity increases both the stress magnitude and affected depth. The use of smaller laser spot sizes decreases the largest magnitude of residual stress and also decreases the depth affected by LSP. Larger spot sizes have less energy attenuation and cause more plastic deformation. Spacing between peening zones is critical for the uniformity of mechanical properties across the surface. The greatest uniformity and largest stress magnitudes are achieved by overlapping of the laser spots.

1.
A.H. Clauer, C.T. Ford, S.C. Ford, 1983, “The effects of laser shock processing on the fatigue properties of T-3 aluminum,” In: Lasers in materials processing, Metals Park (OH): American Society for Metals, pp. 7–22.
2.
Clauer
A. H.
,
Koucky
J. R.
,
1991
, “
Laser shock processing increases the fatigue life of metal parts
,”
Materials and Processing
,
6
, pp.
3
5
.
3.
Peyre
P.
,
Fabbro
R.
,
Merrien
P.
,
Lieurade
H. P.
,
1996
, “
Laser shock processing of aluminum alloys. Application to high cycle fatigue behavior
,”
Materials Science and Engineering
,
A210
, pp.
102
113
.
4.
J.A. Vaccari, 1992, “Laser shocking extends fatigue life,” American Machinist, July, pp. 62–64.
5.
Ashley
S.
,
1998
, “
Powerful laser means better peening
,”
Mechanical Engineering
,
120
, p.
12
12
.
6.
A.S. Brown, 1998, “A shocking way to strengthen metal,” In: Aerospace America, pp. 21–23.
7.
Banas
G.
,
Elsayed-Ali
H. E.
,
Lawrence
F. V.
,
Rigsbee
J. M.
,
1990
, “
Laser shock-induced mechanical and microstructural modification of welded maraging steel
,”
Journal of Applied Physics
,
67
, pp.
2380
2384
.
8.
A.H. Clauer, J.H. Holbrook, B.P. Fairand, 1981, “Effects of laser induced shock waves on metals,” In: M.A. Meyers, L.E. Murr, editors, Shock Waves and High-Strain-Rate Phenomena in Metals, New York: Plenum Publishing Corporation, pp. 675–702.
9.
Yakimets
I.
,
Richard
C.
,
Be´ranger
G.
,
Peyre
P.
,
2004
, “
Laser peening processing effect on mechanical and tribological properties of rolling steel 100Cr6
,”
Wear
,
256
(
3–4
), pp.
311
320
.
10.
Fabbro
R.
,
Peyre
P.
,
Berthe
L.
,
Sherpereel
X.
,
1998
, “
Physics and application of laser- shock processing
,”
Journal of Laser Applications
,
10
, pp.
265
279
.
11.
Peyre
P.
,
Berthe
L.
,
Scherpereel
X.
,
Fabbro
R.
,
1998
, “
Laser-shock processing of aluminum coated 55C1 steel in water-confinement regime, characterization and application to high-cycle fatigue behavior
,”
Journal of Materials Science
,
33
, pp.
1421
1429
.
12.
Ruschau
J. J.
,
John
R.
,
Thompson
S. R.
,
Nicholas
T.
,
1999
, “
Fatigue crack nucleation and growth rate behavior of laser shock peened titanium
,”
International Journal of Fatigue
,
21
, pp.
S199–S209
S199–S209
.
13.
Zhang
W.
,
Yao
Y. L.
,
Noyan
I. C.
,
2004
, “
Microscale laser shock peening of thin films, Part 1: Experiment modeling and simulation
,”
Journal of Manufacturing Science and Engineering
,
126
, pp.
10
17
.
14.
A.H. Clauer, J.H. Holbrock, 1981, “Effects of laser induced shock waves on metals,” Shock Waves and High Strain Phenomena in Metals-Concepts and Applications, New York, Plenum, pp. 675–702.
15.
Fabbro
R.
,
Fournier
J.
,
Ballard
P.
,
Devaux
D.
,
Virmont
J.
,
1990
, “
Physical study of laser-produced plasma in confined geometry
,”
Journal of Applied Physics
,
68
(
2
), pp.
775
784
.
16.
Braisted
W.
,
Brockman
R.
,
1999
, “
Finite element simulation of laser shock peening
,”
International Journal of Fatigue
,
21
, pp.
719
724
.
17.
Ding
K.
,
Ye
L.
,
2003
, “
Three-dimensional dynamic finite element analysis of multiple laser shock peening process
,”
Surface Engineering
,
19
, pp.
351
358
.
18.
Zhang
W.
,
Yao
Y. L.
,
2002
, “
Micro scale laser shock processing of metallic components
,”
Journal of Manufacturing Science and Engineering
,
124
, pp.
369
378
.
19.
ABAQUS, Inc., ABAQUS User’s Manual, Ver. 6.4, Pawtucket, RI, 2003.
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