On the theory of internal waves of permanent form in fluids of great depth
On the theory of internal waves of permanent form in fluids of great depth
复制标题
论大深度流体中永久形式的内波理论
DOI：
--
复制
发表时间：
1994
期刊：
影响因子：
--
通讯作者：
C. Amick
中科院分区：
文献类型：
--
作者：
C. Amick
其中h > 0是给定参数。根据比例，我们可以取h = 1，由此Q = M。x（-1，oo）。流体域Q由其中密度可以被归一化为相等的单位的下部流体区域Q_、其中密度是给定常数pE（0，1）的上部区域Q+以及这两个区域之间的未知界面T组成：T = {（x，Z（x））：xE E}。这里Z是一个光滑函数，Z（±oo）= 0。n+ r ^y-^^y = z（x）· n_ ->x y = -l
where h > 0 is a given parameter. Upon scaling, we may take h = 1, whence Q = M. x (-1, oo). The fluid domain Q consists of a lower fluid region Q_ in which the density may be normalized to equal unity, an upper region Q+ in which the density is a given constant p £ (0, 1), and the unknown interface T between these two regions: T = {(x, Z(x)) : x £ E} . Here Z is a smooth function with Z(±oo) = 0. n+ r ^y—^-^-^^y = z(x) • n_ ->x y = -l