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Pol Grasland-Mongrain edited When_a_laser_beam_of__1.tex
over 8 years ago
Commit id: 8a5c7f42a5e9ed8e4cde5ad6376b035b36332698
deletions | additions
diff --git a/When_a_laser_beam_of__1.tex b/When_a_laser_beam_of__1.tex
index 1b5621d..d47bdca 100644
--- a/When_a_laser_beam_of__1.tex
+++ b/When_a_laser_beam_of__1.tex
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T = T_0 + \frac{\gamma}{S \rho C} E \exp(-\gamma r)
\label{eq:eqTemperature}
\end{equation}
where $T_0$ is the initial temperature of the medium.
The local increase of temperature can lead to two main effects creating elastic waves: (1) thermoelastic expansion and (2) ablation of medium. In metals, transition from first to second regime occurs approximately about 10$^7$ W.cm$^{-2}$. This is equal to the energy of the laser we used, so the predominant regime in our experiment cannot be determined yet.
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