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Pol Grasland-Mongrain edited Simu disp maps.tex
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To determine if the thermoelastic or the ablative regime %This affirmation is
dominant, we can look at the displacements patterns, which is different between the two regimes \cite{Davies_1993}. As the thermoelastic regime acts mainly as local dipolar forces parallel to the surface, the medium stretches locally parallel to confirmed by the
surface, resulting in observation of a
weak displacement \textit{outside} the medium along Z axis, disk of paler color of the same size as
calculated previously. In the ablative regime, the point force in the medium displaces the
surface \textit{inside} the medium along Z axis. Initial displacement along Z axis, as seen beam diameter at
$t$=0.8 ms in Figure \ref{Figure2}, is inside the
medium along Z axis%; moreover, impact location of the
displacement along Y axis (approx. 1.5 $\mu$m) is quite smaller than laser on the
one along Z axis (approx. 3 $\mu$m)
: dominant phenomenon is probably phantom, which could correspond to a vaporization of a fraction of the
ablative regime. material.
This affirmation is confirmed by the observation of a disk of paler color of the same size as the beam diameter at the impact location of the laser on the phantom, which could correspond to a vaporization of a fraction of the material. The
ablative regime can be thermal dilatation was simulated by calculating the displacement created by
a force positive then negative over a disk two opposite forces, of
5 linear amplitude from 0 to 2.5 mm
in diameter and (respectively 0 to -2.5 mm), 100 $\mu$m in
depth, depth. Propagation as
shown on Figure \ref{Figure3} which represents displacement maps along Y and Z axis 0.8, 1.6, 2.4, 3.2 and 4.0 ms after force application. It a shear wave was calculated
in a three-dimensional simulation with spatial steps of 10 $\mu$m and temporal steps of 50 $\mu$s using Green operator
\cite{aki1980quantitative} with \cite{aki1980quantitative}, using a medium density $\rho$ of 1000 kg.m$^{-3}$, a compression wave speed of 1500 m.s$^{-1}$ and a shear wave speed of 4 m.s$^{-1}$.
Results are shown on Figure \ref{Figure3} which represents displacement maps along Y and Z axis 0.8, 1.6, 2.4, 3.2 and 4.0 ms after force application. The displacement maps present many similarities with the experimental results of the Figure
\ref{Figure2}, which support the conclusion of an ablative regime. \ref{Figure2}.