2014
DOI: 10.1007/s00033-014-0450-5
|View full text |Cite
|
Sign up to set email alerts
|

Waves on a vortex filament: exact solutions of dynamical equations

Abstract: In this paper, we take into account the dynamical equations of a vortex filament in superfluid helium at finite temperature (1 K < T < 2.17 K) and at very low temperature, which is called Biot-Savart law. The last equation is also valid for a vortex tube in a frictionless, unbounded, and incompressible fluid. Both the equations are approximated by the Local Induction Approximation (LIA) and Fukumoto's approximation. The obtained equations are then considered in the extrinsic frame of reference, where exact sol… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1
1

Citation Types

1
2
0

Year Published

2014
2014
2019
2019

Publication Types

Select...
5

Relationship

1
4

Authors

Journals

citations
Cited by 5 publications
(3 citation statements)
references
References 28 publications
(34 reference statements)
1
2
0
Order By: Relevance
“…Note that in Fig. 4 the amount of vortex line grows, because of the appearance of Kelvin waves along the straight vortices, induced by the growth of sc (a similar phenomenon has been studied by Brugarino, Mongiovì & Sciacca 2015) for He II. At q = 1, the straight vortex regime ceases, because the topology of the vortex lines changes: the vortex tangle takes part in the superfluid, and the vortex line density undergoes a sudden increase at q = 1, as shown in Fig. 6.…”
Section: A P P L I C At I O N To T H E V E L a P U L S A Rsupporting
confidence: 59%
“…Note that in Fig. 4 the amount of vortex line grows, because of the appearance of Kelvin waves along the straight vortices, induced by the growth of sc (a similar phenomenon has been studied by Brugarino, Mongiovì & Sciacca 2015) for He II. At q = 1, the straight vortex regime ceases, because the topology of the vortex lines changes: the vortex tangle takes part in the superfluid, and the vortex line density undergoes a sudden increase at q = 1, as shown in Fig. 6.…”
Section: A P P L I C At I O N To T H E V E L a P U L S A Rsupporting
confidence: 59%
“…After a reconnection, two waves run along each vortex line (in opposite direction one to each other, as in Figure 3 in [14]), but Kelvin waves can be also triggered in the waves cascade, if it starts. The propagation speed of Kelvin waves along a vortex line can be approximated by v g ∝ K (K being the wave number) quite well for K < 500 cm −1 as shown in Figure 3 of [28]. The time a Kelvin wave needs to run for a length aλ (a being a constant of the order of unity and the wavelength…”
Section: Range Of Validity Of the Modelmentioning
confidence: 99%
“…[7,42]. The former interpreted the steep increase of L at Re 2 as the beginning of vortex reconnection, namely, to the production of a high number of free vortex loops as a consequence of the crossing and cutting and recombining of vortex lines that in turbulence T I were most of them pinned to the walls [43]. The increase of L in turbulence T I, instead, is basically due to Kelvin wave excitations in pinned vortex lines.…”
Section: Quantum Turbulence: Explicit Evaluationmentioning
confidence: 99%