TY - JOUR

T1 - Pulsatile instability in rapid directional solidification

T2 - strongly-nonlinear analysis

AU - Merchant, G. J.

AU - Braun, R. J.

AU - Brattkus, K.

AU - Davis, S. H.

PY - 1992/1/1

Y1 - 1992/1/1

N2 - In the rapid directional solidification of a dilute binary alloy, analysis reveals that, in addition to the cellular mode of Mullins and Sekerka [J. Appl. Phys., 35 (1964), pp. 444-451] there is an oscillatory instability. For the model analyzed by Merchant and Davis [Acta Metallurgica et Materialia 38 (1990), pp. 2683-2693], the preferred wavenumber is zero; the mode is one of pulsation. Two strongly nonlinear analyses are performed that describe this pulsatile mode. In the first case, nonequilibrium effects that alter solute rejection at the interface are taken asymptotically small. A nonlinear oscillator equation governs the position of the solid-liquid interface at leading order, and amplitude and phase evolution equations are derived for the uniformly pulsating interface. The analysis provides a uniform description of both subcritical and supercritical bifurcation and the transition between the two. In the second case, nonequilibrium effects that alter solute rejection are taken asymptotically large, and a different nonlinear oscillator equation governs the location of the interface to leading order. A similar analysis allows for the derivation of an amplitude evolution equation for the uniformly pulsating interface. In this case, the bifurcation is always supercritical. The results are used to make predictions about the characteristics of solute bands that would be frozen into the solid.

AB - In the rapid directional solidification of a dilute binary alloy, analysis reveals that, in addition to the cellular mode of Mullins and Sekerka [J. Appl. Phys., 35 (1964), pp. 444-451] there is an oscillatory instability. For the model analyzed by Merchant and Davis [Acta Metallurgica et Materialia 38 (1990), pp. 2683-2693], the preferred wavenumber is zero; the mode is one of pulsation. Two strongly nonlinear analyses are performed that describe this pulsatile mode. In the first case, nonequilibrium effects that alter solute rejection at the interface are taken asymptotically small. A nonlinear oscillator equation governs the position of the solid-liquid interface at leading order, and amplitude and phase evolution equations are derived for the uniformly pulsating interface. The analysis provides a uniform description of both subcritical and supercritical bifurcation and the transition between the two. In the second case, nonequilibrium effects that alter solute rejection are taken asymptotically large, and a different nonlinear oscillator equation governs the location of the interface to leading order. A similar analysis allows for the derivation of an amplitude evolution equation for the uniformly pulsating interface. In this case, the bifurcation is always supercritical. The results are used to make predictions about the characteristics of solute bands that would be frozen into the solid.

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U2 - 10.1137/0152074

DO - 10.1137/0152074

M3 - Article

AN - SCOPUS:0026931440

VL - 52

SP - 1279

EP - 1302

JO - SIAM Journal on Applied Mathematics

JF - SIAM Journal on Applied Mathematics

SN - 0036-1399

IS - 5

ER -