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arXiv 2510.18436cond-mat.soft
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任意外势中的颗粒流体:自发对流与自泳动

Granular fluid in an arbitrary external potential: spontaneous convection, self-phoresis

Alvaro Domínguez, Nagi Khalil

AI总结:

该研究理论分析任意外势下受驱颗粒流体的定态,证明非对称条件下静止态不存在并自发形成对流,同时将其与活性颗粒自扩散泳动联系起来,指出决定最大诱导流动尺度的状态相关特征长度。

摘要:

本文从理论上研究颗粒流体在受到能量注入以及一个不随时间变化、但在其他方面任意的外势力作用时的流体力学定态。当后者在某种明确定义的意义上不那么对称时,我们证明静止定态并不存在,而不仅仅是不稳定;相应地,会自发出现一种稳定的对流态。我们还揭示了该特征与催化活性颗粒的自扩散泳动之间一种出人意料的联系:如果颗粒流体中的一个侵入体是该势的源,它将按照最近提出的一种机制实现自推进;该机制超出线性响应理论,并突显颗粒浴状态内在非平衡性质的作用。在这两种情形中,都识别出颗粒流体的一个依赖于状态的特征长度,它设定了诱导流动最强的尺度。

英文摘要:

The hydrodynamic stationary states of a granular fluid are addressed theoretically when subject to energy injection and a time-independent, but otherwise arbitrary external potential force. When the latter is not too symmetrical in a well defined sense, we show that a quiescent stationary state does not exist, rather than simply being unstable and, correspondingly, a steady convective state emerges spontaneously. We also unveil an unexpected connection of this feature with the self-diffusiophoresis of catalytically active particles: if an intruder in the granular fluid is the source of the potential, it will self-propel according to a recently proposed mechanism that lies beyond linear response theory, and that highlights the role of the intrinsic nonequilibrium nature of the state of the granular bath. In both scenarios, a state-dependent characteristic length of the granular fluid is identified which sets the scale at which the induced flow is the largest.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

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