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首页> 外文期刊>Nonlinear Processes in Geophysics Discussions >On the spectral distribution of kinetic energy in large-scale atmospheric flow
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On the spectral distribution of kinetic energy in large-scale atmospheric flow

机译:大尺度大气流动中动能的频谱分布

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A one-dimensional form of the equation of motion with forcing and dissipation is formulated in the spectral domain and used to make long term integrations from which the spectral distribution of the kinetic energy is determined The forcing in the wave number domain is determined in advance and kept constant for the duration of the time integrations. The dissipation is proportional to the second derivative of the velocity. The applied equation is made non-dimensional by selecting a length scale from which the time scale and the velocity scale may be determined. The resulting equation contains no parameters apart from the forcing. The integrations use a large number of spectral components and no approximation is made with respect to the non-linear interaction among the spectral components. Starting from an initial state in which all the velocity components are set to zero the equation is integrated for a long time to see if it reaches a steady state. The spectral distribution of the kinetic energy is determined in the steady state, and it is found that the distribution, in agreement with observational studies, may be approximated by a power law of the form n-3 within certain wave number regions. The wave numbers for which the -3 power law applies is found between the region of maximum forcing and the dissipation range. The intensity of the maximum forcing is varied to see how the resulting steady state varies. In addition, the maximum number of spectral components is varied. However, the available computing power sets an upper limit to the number of components.
机译:在谱域中公式化了带有强迫和耗散的运动方程的一维形式,并用于进行长期积分,从而确定了动能的频谱分布。预先确定了波数域中的强迫,并且在时间积分期间保持恒定。耗散与速度的二阶导数成正比。通过选择可以确定时间标度和速度标度的长度标度,使应用的方程成为无量纲的。所得方程除强制外不包含任何参数。积分使用了大量的光谱分量,并且在光谱分量之间的非线性相互作用方面未做任何近似。从所有速度分量均设为零的初始状态开始,对方程进行长时间积分,以查看其是否达到稳定状态。动能的频谱分布是在稳态下确定的,发现与观察研究一致,该分布可以在某些波数区域内以n-3形式的幂定律近似。在最大受力区域和耗散范围之间找到了-3幂定律适用的波数。改变最大强迫的强度,以查看最终的稳态如何变化。另外,频谱分量的最大数量是变化的。但是,可用的计算能力为组件数量设置了上限。

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