首页> 外文期刊>Physics of fluids >Response to 'Comment on 'Motion of a helical vortex filament in superfluid 4He under the extrinsic form of the local induction approximation'' [Phys. Fluids 26, 019101 (2014)]
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Response to 'Comment on 'Motion of a helical vortex filament in superfluid 4He under the extrinsic form of the local induction approximation'' [Phys. Fluids 26, 019101 (2014)]

机译:对“关于在局部感应近似的外在形式下超流体4He中的螺旋涡旋丝运动的评论”的回应。流体26,019101(2014)]

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摘要

I agree with the authors regarding their comments on the Donnelly-Glaberson instability for such helical filaments as those obtained in my paper. I also find merit in their derivation of the quantum LIA (local induction approximation) in the manner of the LIA of Boffetta et al. However, I disagree with the primary criticisms of Hietala and H?nninen. In particular, though they suggest LIA and local nonlinear equation modes are not comparable since the former class of models contains superfluid friction parameters, note that since these parameters are small one may take them to zero and consider a qualitative comparison of the models (which is what was done in my paper). Second, while Hietala and H?nninen criticize certain assumptions made in my paper (and the paper of Shivamoggi where the model comes from) since the results break-down when Ak→∞, note that in my paper I state that any deviations from the central axis along which the filament is aligned must be sufficiently bounded in variation. Therefore, it was already acknowledged that Ak(=|φ_x|) should be sufficiently bounded, precluding the Ak→∞case. I also show that, despite what Hietala and H?nninen claim, the dispersion relation obtained in my paper is consistent with LIA, where applicable. Finally, while Hietala and H?nninen claim that the dispersion parameter should be complex valued, I showthat their dispersion relation iswrong, since it was derived incorrectly (they assume the complex modulus of the potential function is constant, yet then use this to obtain a potential functionwith non-constant modulus).
机译:我同意作者对Donnelly-Glaberson螺旋状细丝不稳定性的评论,就像我在论文中获得的那样。我也发现它们以Boffetta等人的LIA方式推导量子LIA(局部感应近似)的优点。但是,我不同意Hietala和H?nninen的主要批评。特别是,尽管他们认为LIA和局部非线性方程模式不具有可比性,因为前一类模型包含超流体摩擦参数,但请注意,由于这些参数较小,可能会将它们设为零,并考虑对模型进行定性比较(这是我的论文做了什么)。其次,虽然Hietala和H?nninen批评了我的论文(以及模型所来自的Shivamoggi的论文)中做出的某些假设,因为当Ak→∞时结果崩溃,但请注意,我在论文中指出与细丝排列所沿的中心轴必须有足够的变化范围。因此,已经认识到,Ak(= |φ_x|)应该有足够的界,而排除了Ak→∞情况。我还表明,尽管有Hietala和H?nninen的主张,但在适用的情况下,本文中得出的色散关系与LIA一致。最后,尽管Hietala和H?nninen声称色散参数应为复数值,但我证明了它们的色散关系是错误的,因为它的推导是不正确的(他们假设势函数的复数模量是常数,然后使用它来获得具有非恒定模量的势函数)。

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