Numerical hydrodynamic simulations of the growth and collapse of a 10 μm air bubble in water were performed. Both the air and the water are treated as compressible fluids. The calculations show that the collapse is nearly isentropic until the final 10 ns, after which a strong spherically converging shock wave evolves and creates enormous temperatures and pressures in the inner 0.02 μm of the bubble. The reflection of the shock from the center of the bubble produces a diverging shock wave that quenches the high temperatures (≳30 eV) and pressures in less than 10 ps (full width at half maximum). The picosecond pulse widths are due primarily to spherical convergence/divergence and nonlinear stiffening of the air equation of state that occurs at high pressures. The results are consistent with recent measurements of sonoluminescence that had optical pulse widths less than 50 ps and 30 mW peak radiated power in the visible.
Hydrodynamic simulations of bubble collapse and picosecond sonoluminescence
William C. Moss, Douglas B. Clarke, John W. White, David A. Young; Hydrodynamic simulations of bubble collapse and picosecond sonoluminescence. Physics of Fluids 1 September 1994; 6 (9): 2979–2985. https://doi.org/10.1063/1.868124
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