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Helicity within the vortex filament model

机译:涡流丝模型内的螺旋度

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摘要

Kinetic helicity is one of the invariants of the Euler equations that is associated with the topology of vortex lines within the fluid. In superfluids, the vorticity is concentrated along vortex filaments. In this setting, helicity would be expected to acquire its simplest form. However, the lack of a core structure for vortex filaments appears to result in a helicity that does not retain its key attribute as a quadratic invariant. By defining a spanwise vector to the vortex through the use of a Seifert framing, we are able to introduce twist and henceforth recover the key properties of helicity. We present several examples for calculating internal twist to illustrate why the centreline helicity alone will lead to ambiguous results if a twist contribution is not introduced. Our choice of the spanwise vector can be expressed in terms of the tangential component of velocity along the filament. Since the tangential velocity does not alter the configuration of the vortex at later times, we are able to recover a similar equation for the internal twist angle to that of classical vortex tubes. Our results allow us to explain how a quasi-classical limit of helicity emerges from helicity considerations for individual superfluid vortex filaments.
机译:动力学螺旋是欧拉方程的不变量之一,其与流体中的涡旋线的拓扑有关。在超流体中,涡度沿着涡流丝聚集。在这种情况下,螺旋将有望获得其最简单的形式。但是,缺少涡流丝的核心结构似乎会导致无法保留其作为二次不变性的关键属性的螺旋线。通过使用Seifert框架为旋涡定义展向矢量,我们能够引入扭曲,从而恢复螺旋的关键特性。我们提供了一些用于计算内部扭曲的示例,以说明如果不引入扭曲贡献,为什么仅中心线螺旋度会导致模棱两可的结果。我们对翼展方向矢量的选择可以用沿着细丝的速度的切向分量表示。由于切向速度在以后不会改变涡旋的构型,因此我们能够恢复与传统涡旋管类似的内部扭转角方程。我们的结果使我们能够解释螺旋度的准经典极限是如何从单个超流体涡旋丝的螺旋度考虑因素产生的。

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