TAYLOR INSTABILITY IN SHOCK ACCELERATION OF COMPRESSIBLE FLUIDS
TAYLOR INSTABILITY IN SHOCK ACCELERATION OF COMPRESSIBLE FLUIDS
复制标题
DOI：
10.1002/cpa.3160130207
复制
发表时间：
1960-01-01
影响因子：
3
通讯作者：
RICHTMYER, RD
中科院分区：
文献类型：
--
作者：
RICHTMYER, RD
GI Taylor发展了一个理论，当两种不同密度的流体加速运动时，它们之间的界面上的不规则性增长。假设流体是不可压缩的，并且界面具有正弦波纹，使得界面在适当取向的笛卡尔坐标系中的位置由下式给出：（1）在某个时刻z= a cos kx，其中a和k是常数，并且其中（2）ka<< 1。
GI Taylor developed a theory of the growth of irregularities on the interface between two fluids of different densities when they are in accelerated motion. The fluids are assumed incompressible and the interface to have sinusoidal corrugations, so that the position of the interface in a suitably oriented Cartesian coordinate system is given by (1) z= a cos kx at some instant, where a and k are constants and where (2) ka<< 1.