论文标题
使用时间依赖的金茨堡 - 兰道和迅捷 - 霍恩伯格随机方程的浅对流云场中的中尺度模式形成的描述
Description of mesoscale pattern formation in shallow convective cloud fields by using time-dependent Ginzburg-Landau and Swift-Hohenberg stochastic equations
论文作者
论文摘要
提出了依赖时间的Ginzburg-Landau方程和Swift-Hohenberg方程,均添加了随机术语,以描述在中尺度系统中组织的浅对流云的云模式形成和云状态相变。起点是热带降水的Hottovy-Stechmann线性时空随机模型,用于描述水蒸气和热带对流的动力学。通过考虑到浅层层云接近自组织的批评,并且水蒸气含量是顺序参数,可以观察到,方程中必须具有非线性项,以包括由于降水和蒸发而引起的动态反馈。这种非线性的包含导致了一种时间依赖性的金茨堡 - 兰道随机方程,该方程最初用于描述超导性阶段。通过进行数值模拟,可以观察到模式形成,特别是针对细胞对流阶段。与纯线性模型相比,与真实卫星观测相比,这些模式要好得多。这是通过比较真实和数值云场的空间傅立叶变换来完成的。最后,通过考虑湍流涡流扩散的波动术语,我们到达了霍恩伯格 - 旋转方程。在闭合细胞和滚动对流的情况下,获得的模式比从金茨堡 - 兰道方程中获得的模式更加有条理。
The time-dependent Ginzburg-Landau equation and the Swift-Hohenberg equation, both added with a stochastic term, are proposed to describe cloud pattern formation and cloud regime phase transitions of shallow convective clouds organized in mesoscale systems. The starting point is the Hottovy-Stechmann linear spatio-temporal stochastic model for tropical precipitation, used to describe the dynamics of water vapor and tropical convection. By taking into account that shallow stratiform clouds are close to a self-organized criticallity and that water vapor content is the order parameter, it is observed that sources must have non-linear terms in the equation to include the dynamical feedback due to precipitation and evaporation. The inclusion of this non-linearity leads to a kind of time-dependent Ginzburg-Landau stochastic equation, originally used to describe superconductivity phases. By performing numerical simulations, pattern formation is observed, specially for cellular convective phases. These patterns are much better compared with real satellite observations than the pure linear model. This is done by comparing the spatial Fourier transform of real and numerical cloud fields. Finally, by considering fluctuation terms for the turbulent eddy diffusion we arrive to a Hohenberg-Swift equation. The obtained patterns are much more organized that the patterns obtained from the Ginzburg-Landau equation in the case of closed cellular and roll convection.