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One of these aspects is the shock wave interaction with a developed turbulized layer.
The experimentally obtained shock wave behaviors at initial phase are almost the same with the numerical results.
We have also investigated a behavior of a plasma boundary and a shock wave in water both experimentally and numerically.
The spall strength limit of matter at ultrahigh strain rates induced by laser shock wave.
We have compared the numerical results of shock wave velocities with experimental data.
Theoretical investigation of shock wave instability in metals.
Two photodiodes measured the time difference between the main laser pulse, generating the shock wave, and the diagnostic laser producing the hologram.
The presence of this shock wave results in a high drag coefficient compared with that of a pointed body with an attached nose shock wave.
If a wall is placed normal to the expanding flow, a shock wave will reflect from it.
As the piston continues to gain speed, the shock wave will become stronger.
When it reaches the face of the piston it will again be reflected and the shock wave will return to the closed end.
The shock wave is in general curved and the post-shock flow in general non-parallel.
The generation of a well-formed fourth shock wave is therefore even less likely.
As a result of these pressure variations, an inward facing, second shock wave exists in the spherical flow field.
At a certain critical flow rate, however, the bow shock wave begins to bulge out (see figure 8c, plate 1).
