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首页> 外文期刊>Journal of the Atmospheric Sciences >A New Interpretation of Vortex-Split Sudden Stratospheric Warmings in Terms of Equilibrium Statistical Mechanics
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A New Interpretation of Vortex-Split Sudden Stratospheric Warmings in Terms of Equilibrium Statistical Mechanics

机译:均衡统计力学方面的涡旋分裂突然平流层幽默的新解释

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摘要

Vortex-split sudden stratospheric warmings (S-SSWs) are investigated by using the Japanese 55-year Reanalysis, a spherical barotropic quasigeostrophic (QG) model, and equilibrium statistical mechanics. The statistical mechanics theory predicts a large-scale steady state as the most probable outcome of turbulent stirring, and such a state can be computed without describing all the details of the dynamics. The theory is applied to a disk domain that is modeled on the polar cap north of 45 degrees N in the stratosphere. The equilibrium state is obtained by computing the maximum of an entropy functional. In the range of parameters relevant to the winter stratosphere, this state is anticyclonic. By contrast, cyclonic states are quasi-stationary states corresponding to saddle points of the entropy functional. These results indicate that the mean state of the stratosphere associated with the polar vortex is not close to an equilibrium state but to a quasi-stationary state. The theoretical calculations are compared with the results of a quasi-static experiment in which a wavenumber-2 topographic amplitude is increased linearly and slowly with time. The results suggest that the S-SSW can be qualitatively interpreted as the transition from the cyclonic quasi-stationary state toward the anticyclonic equilibrium state. The polar vortex splits during the transition toward the equilibrium state.
机译:通过使用日本55年的重新分析,球形波奇喹啉代滴(QG)模型和均衡统计力学来研究涡旋分裂突然平流层泥浆(SSWH)。统计力学理论预测大规模稳态,作为湍流搅拌的最可能结果,并且可以计算这种状态而不描述动态的所有细节。该理论应用于磁盘域,该磁盘域在平流层中为45摄氏度的极性帽。通过计算熵功能的最大值来获得均衡状态。在与冬季平流层相关的参数范围内,这种状态是反气旋。相反,循环状态是对应于熵功能的马鞍点的准静止状态。这些结果表明与极性涡流相关的平流层的平均状态不接近平衡状态,而是对准静止状态。将理论计算与准静态实验的结果进行了比较,其中波数-2地形幅度随时间线性和缓慢增加。结果表明,S-SSW可以定性地解释为从循环准静止状态朝向反气旋平衡状态的转变。在过渡到平衡状态期间极性涡旋分裂。

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