In fluid mechanics, the Rayleigh–Plesset equation or Besant–Rayleigh–Plesset equation is a nonlinear ordinary differential equation which governs the dynamics of a spherical bubble in an infinite body of incompressible fluid. Its general form is usually written aswhere
ρ L {\displaystyle \rho _{L}} is the density of the surrounding liquid, assumed to be constant
R ( t ) {\displaystyle R(t)} is the radius of the bubble
ν L {\displaystyle \nu _{L}} is the kinematic viscosity of the surrounding liquid, assumed to be constant
σ {\displaystyle \sigma } is the surface tension of the bubble-liquid interface
Δ P ( t ) = P ∞ ( t ) − P B ( t ) {\displaystyle \Delta P(t)=P_{\infty }(t)-P_{B}(t)} , in which, P B ( t ) {\displaystyle P_{B}(t)} is the pressure within the bubble, assumed to be uniform and P ∞ ( t ) {\displaystyle P_{\infty }(t)} is the external pressure infinitely far from the bubble Provided that P B ( t ) {\displaystyle P_{B}(t)} is known and P ∞ ( t ) {\displaystyle P_{\infty }(t)} is given, the Rayleigh–Plesset equation can be used to solve for the time-varying bubble radius R ( t ) {\displaystyle R(t)} . The Rayleigh–Plesset equation can be derived from the Navier–Stokes equations under the assumption of spherical symmetry. It can also be derived using an energy balance.
History Neglecting surface tension and viscosity, the equation was first derived by W. H. Besant in his 1859 book with the problem statement stated as An infinite mass of homogeneous incompressible fluid acted upon by no forces is at rest, and a spherical portion of the fluid is suddenly annihilated; it is required to find the instantaneous alteration of pressure at any point of the mass, and the time in which the cavity will be filled up, the pressure at an infinite distance being supposed to remain constant (in fact, Besant attributes the problem to Cambridge Senate-House problems of 1847). Besant predicted the time required to fill an empty cavity of initial radius R 0 {\displaystyle R_{0}} to be
… excerpt ends here. Continue reading the full article.




