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本文第一部分利用未作无旋和静压假定的线性波动方程求得了现有波动的统一解。本文的这一部分对未作静压假定的线性长波方程作了进一步讨论。求得了ω=f时的所有解。也求得了ωf时的Sverdrup波和Poincaré波的统一解,但它们代表的波动具有不同的速度铅直结构。这一组解不包含在作了静压假定的线性长波方程中,因而被看作是被静压假定滤掉的可能波动。
In the first part of this paper, the univariate solution of the existing wave is obtained by using the linear wave equation without the assumption of rotation and static pressure. This section of this paper further discusses the linear long-wave equation without assuming hydrostatic pressure. Obtain all solutions for ω = f. We also obtain a set of solutions for ω f, but the fluctuations they represent have different velocity vertical structures. This set of solutions is not included in the linear long-wave equation for which hydrostatic assumptions are made and is therefore considered as a possible fluctuation that is assumed to be filtered by hydrostatic pressure.