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Latitudinal libration driven flows in triaxial ellipsoids

机译:三轴椭球体中纬向自由运动

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Motivated by understanding the liquid core dynamics of tidally deformed planets and moons, we present a study of incompressible flow driven by latitudinal libration within rigid triaxial ellipsoids. We first derive a laminar solution for the inviscid equations of motion under the assumption of uniform vorticity flow. This solution exhibits a resonance if the libration frequency matches the frequency of the spin-over inertial mode. Furthermore, we extend our model by introducing a reduced model of the effect of viscous Ekman layers in the limit of low Ekman number (Noir & Cebron, J. Fluid Mech., vol. 737, 2013, pp. 412-439). This theoretical approach is consistent with the results of Chan et al. (Phys. Earth Planet. Inter., vol. 187, 2011, pp. 404-415) and Zhang et al. (J. Fluid Mech., vol. 692, 2012, pp. 420-445) for spheroidal geometries. Our results are validated against systematic three-dimensional numerical simulations. In the second part of the paper, we present the first linear stability analysis of this uniform vorticity flow. To this end, we adopt different methods (Lifschitz & Hameiri, Phys. Fluids A, vol. 3, 1991, p. 2644; Gledzer & Ponomarev, Acad. Sci., USSR, Izv., Atmos. Ocean. Phys., vol. 13, 1977, pp. 565-569) that allow us to deduce upper and lower bounds for the growth rate of an instability. Our analysis shows that the uniform vorticity base flow is prone to inertial instabilities caused by a parametric resonance mechanism. This is confirmed by a set of direct numerical simulations. Applying our results to planetary settings, we find that neither a spin-over resonance nor an inertial instability can exist within the liquid core of the Moon, Io and Mercury.
机译:通过理解潮汐变形的行星和卫星的液体核心动力学,我们提出了在刚性三轴椭球体中由纬度自由度驱动的不可压缩流的研究。我们首先在均匀涡流假设下为不粘运动方程式得出层流解。如果释放频率与旋转惯性模式的频率匹配,则该解决方案会产生共振。此外,我们通过引入在低Ekman数限制内的粘性Ekman层效应的简化模型来扩展模型(Noir&Cebron,J。Fluid Mech。,第737卷,2013年,第412-439页)。这种理论方法与Chan等人的结果一致。 (Phys.Earth Planet.Inter。,第187卷,2011年,第404-415页)和Zhang等人。 (J.Fluid Mech。,vol.692,2012,pp.420-445)中的球面几何形状。我们的结果通过系统的三维数值模拟得到了验证。在本文的第二部分,我们介绍了这种均匀涡流的第一线性稳定性分析。为此,我们采用了不同的方法(Lifschitz和Hameiri,《流体物理学》 A,第3卷,1991年,第2644页; Gledzer和Ponomarev,苏联科学技术学院,Izv。,Atmos.Ocean.Phys。 (1977年13月13日,第565-569页)中,我们可以推导出不稳定增长速度的上限和下限。我们的分析表明,均匀的涡旋基流易于由参数共振机制引起的惯性不稳定性。一组直接数值模拟证实了这一点。将我们的结果应用于行星环境,我们发现在月球,艾奥和水星的液核中既不存在自旋共振也不存在惯性不稳定性。

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