Added mass effect in coupled Brownian particles

The added mass effect is the contribution to a Brownian particle's effective mass arising from the hydrodynamic flow its motion induces. For a spherical particle in an incompressible fluid, the added mass is half the fluid's displaced mass, but in a compressible fluid its value depends on a competition between timescales. Here we illustrate this behavior with a solvable model of two harmonically coupled Brownian particles of mass m, one representing the sphere and the other representing the immediately surrounding fluid. The measured distribution of the Brownian particle's velocity, P(v[over ¯]), follows a Maxwell-Boltzmann distribution with an effective mass m^{*}. Solving analytically for m^{*}, we find that its value is determined by three relevant timescales: the momentum relaxation time, t_{p}; the harmonic oscillation period, τ; and the velocity measurement time resolution, Δt. In limiting cases of large timescale separations, m^{*} reduces to m or 2m. The model exhibits similar behavior when generalized to the case of unequal masses.