Hi Ben,
Thank you for the response.
When the sample is illuminated by a laser impulse, the sample surface is displaced via thermoelastic expansion. In this case, the effects of the thermal diffusion were neglected because of the time scale for stress relaxationis much more rapid compared to the time scale for thermal diffusion. The trace of the sample displacement can be functions of the optical/mechenical properties of the sample. The corresponding wave equation is expressed as:
diff(u,z,2) - 1/c^2*diff(u,t,2) = -(B*K*T0)/(rho*c^2*D)*exp(-z/D)
where
(1) diff(u,z,2) is double partial derivative of u with respect to z
(2) u displacement of the sample surface
(3) c longitudinal speed of sound
(4) B thermal expansion coef.
(5) T0 relative surface temperature at z=0
(6) rho density
(7) D effectilve optical attenuation depth
(8) K bulk modulus
initial B.C. when the semi-infinite sample is surrounded by air environment.
u=0 at t=0, diff(u,t)=0 at t=0, stress=0 at z=0, u=0 at z->infinite
I think this belongs to photoacoustic regime.
Thank you.
Seongjun Park.