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Shock-induced Mechanical Excitations

Extending Eqs. (6) and (7) one step further, Jindal and Dlott [20] introduced a uniaxial mode-GrUneisen parameter, [Pg.149]

The uniaxial mode-Griineisen parameter is a direct measure of how much energy is transferred from a shock propagating along a particular direction to a particular mode. For instance in Eq. (8), is the Griineisen parameter for [Pg.149]


The laser-induced breakdowns are caused by three consequent mechanisms [22] (i) tiie excitation of electrons in tiie conduction band by impact and multiphoton ionization (MPI), (ii) radiation-induced heating of tiie conduction-band electrons, and (iii) transfer of the plasma energy to the lattice. The key benefit of ultia-short femtosecond laser pulses lies in their ability to deposit energy in materials in a very short time interval. Heat diffusion is frozen during the interaction and the shock-like energy deposition leads to ablation for ultra-short pulses. This is because tiie pulse... [Pg.296]


See other pages where Shock-induced Mechanical Excitations is mentioned: [Pg.148]    [Pg.148]    [Pg.148]    [Pg.36]    [Pg.219]    [Pg.296]    [Pg.180]    [Pg.72]    [Pg.217]    [Pg.355]    [Pg.48]   


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