SUMMARY The Van Leer method for the computation of convective fluxes is extended to two-phase flow. By preventing spurious undershoots and overshoots, the scheme preserves physical realism while maintaining high-order accuracy. This is particularly important for two-phase flows, since phase exchange terms are typically a function of volume fraction products and numerical diffusion can incorrectly mix the two phases. The scheme described here is constructed to guarantee that the sum of the volume fractions is always unity and that the volume fiactions are always greater than or equal to zero. Various test problems are computed to demonstrate the accuracy of the method and to show how the scheme might be incorporated in existing computational methods. In addition to multiphase flow applications, setting equal phase velocities results in a volume marker scheme that is well suited to single-phase interface tracking problems. There are few known exact solutions of the governing equations of two-phase flow and those that are known represent simple physical systems that have limited practical application. Consequently, investigators of two-phase flow fall back on experimentally determined correlations and more recently solutions of the governing equations obtained by computer. This paper addresses the problem of minimizing numerical diffusion associated with numerical representation of the convective terms in the two-phase governing equations. It is well known that numerical schemes that discretize the convective terms with an upwind procedure suffer from excessive numerical diffusion; the use of a higher-order scheme can substantially reduce this problem but can also lead to oscillations causing non-physical undershoots or overshoots. The implication of these results for two-phase flow calculations is particularly significant for the computation of the convection of phase volume fraction (mass). If an upwind procedure is used for volume fraction advection, then numerical diffusion tends to smear gradients of volume fraction. Typical two-phase exchange terms involve the product of volume fractions, so smearing produces finite values in those exchange terms, leading to numerically induced source terms and consequent inaccuracies throughout the calculation. If a naive higher-order scheme is used for volume fraction advection, then non-physical oscillations might appear in the volume fraction profiles, as well as overshoots or undershoots, so that volume fractions may be less than zero or greater than unity, which again would produce unphysical phase exchange source terms. This paper describes the use of the Van Leer method' for the computation of convective fluxes as applied to the convective transport of phase volume fraction (mass) and phase momentum in two-phase flow. The Van Leer scheme prevents spurious oscillations while maintaining a high order of numerical
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