2014
DOI: 10.1063/1.4855296
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Comment on “Motion of a helical vortex filament in superfluid 4He under the extrinsic form of the local induction approximation” [Phys. Fluids 25, 085101 (2013)]

Abstract: We comment on the paper by Van Gorder [“Motion of a helical vortex filament in superfluid 4He under the extrinsic form of the local induction approximation,” Phys. Fluids 25, 085101 (2013)]. We point out that the flow of the normal fluid component parallel to the vortex will often lead into the Donnelly–Glaberson instability, which will cause the amplification of the Kelvin wave. We explain why the comparison to local nonlinear equation is unreasonable, and remark that neglecting the motion in the x-direction … Show more

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Cited by 6 publications
(4 citation statements)
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“…Van Gorder 21,22 employed this formulation to study a number of special case solutions. Limitations and benefits to this type of formulation were recently a topic of discussion in the sequence, [23][24][25] where (for the helical case) the direct approach using (10) when * x xx − x * xx is not a constant in x, the solution of (10) will be an approximation to the LIA, rather than an exact solution.…”
Section: Formulationmentioning
confidence: 99%
“…Van Gorder 21,22 employed this formulation to study a number of special case solutions. Limitations and benefits to this type of formulation were recently a topic of discussion in the sequence, [23][24][25] where (for the helical case) the direct approach using (10) when * x xx − x * xx is not a constant in x, the solution of (10) will be an approximation to the LIA, rather than an exact solution.…”
Section: Formulationmentioning
confidence: 99%
“…For a helical vortex, the dimensionless product Ak is an important parameter. It appears in the dispersion relation of a Kelvin wave of arbitrary amplitude (derived using the local induction approximation) 26,27…”
Section: Methodsmentioning
confidence: 99%
“…( 1). The inclusion of mutual friction or counterflow would change the dispersion relation 27 . The motion of a helical vortex is purely rotational when Ak → 0.…”
Section: Methodsmentioning
confidence: 99%
“…For notation purposes, I assume such a filament takes the form r(x, t) = (x, A cos(kx − ωt + x 0 ), A sin(kx − ωt + x 0 )) which is equivalent to (x, t) = Ae i[kx−ωt+x 0 ] in potential form. In their comments, 2 Hietala and Hänninen give some criticisms of the work. In particular, they state (I) the local nonlinear equation (LNE) is not comparable to the LIA, since the LIA includes friction parameters α, α ; (II) the reduction of the LIA used in Ref.…”
mentioning
confidence: 99%