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residual compressive stress on the surface increases first and then decreases. When τ is set to be around 360 ns, the residual compressive stress reach maximum.


In the case that the time interval τ is fixed to be 320 ns, the calculated radial residual stresses distributing on the surface with respect to different η are shown in Figure 7. It can be seen from Figure 6 that in general the residual compressive stress on the surface increases with the rising of the attenuation factor η, but the stress nearby the edge of spot varies oppositely due to the aggregation of the stress wave. When η is 0.9, there are small residual tensile stresses appearing near the edge of the spot. When η is too small, the composite shock wave no longer plays a significant role. These results indicate that an appropriate value of η should be set for the effective composite shock wave.


The simulations show that the main parameters of the composite shock wave, formed in the cavity, have an important influence on the strengthening effect. In order to provide guidance for the design of the cavity, further theoretical research needs to be


Figure 7. The calculated radial residual stresses distributed on the surface of the workpiece with respect to different η (τ=320 ns)


carried out. The experimental work is also under way, and the new progress will be reported soon.


The authors are with Ningbo Institute of Materials Technology & Engineering (NIMTE).


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A-121401 Motion LMP-IDL-XY-LIA hfpg.indd 1 12 LIATODAY FOCUS: SCIENCE & RESEARCH SEPTEMBER/OCTOBER 2016


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