### Abstract

We analyze the linear stability of the edge of a thin liquid metal layer subject to a transverse high-frequency ac magnetic field. The layer is treated as a perfectly conducting liquid sheet that allows us to solve the problem analytically for both a semi-infinite geometry with a straight edge and a thin disk of finite radius. It is shown that the long-wave perturbations of a straight edge are monotonically unstable when the wave number exceeds the critical value kc = F0 /(γ l0), which is determined by the linear density of the electromagnetic force F0 acting on the edge, the surface tension γ, and the effective arclength of edge thickness l0. Perturbations with wavelength shorter than critical are stabilized by the surface tension, whereas the growth rate of long-wave perturbations reduces as ∼k for k→0. Thus, there is the fastest growing perturbation with the wave number kmax =2/3 kc. When the layer is arranged vertically, long-wave perturbations are stabilized by the gravity, and the critical perturbation is characterized by the capillary wave number kc = gρ/γ, where g is the acceleration due to gravity and ρ is the density of metal. In this case, the critical linear density of electromagnetic force is F0,c =2 kc l0 γ, which corresponds to the critical current amplitude I0,c =4 π kc l0 Lγ/ μ0 when the magnetic field is generated by a straight wire at the distance L directly above the edge. By applying the general approach developed for the semi-infinite sheet, we find that a circular disk of radius R0 placed in a transverse uniform high-frequency ac magnetic field with the induction amplitude B0 becomes linearly unstable with respect to exponentially growing perturbation with the azimuthal wave number m=2 when the magnetic Bond number exceeds Bmc = B02 R02 /(2 μ0 l0 γ)=3π. For Bm> Bmc, the wave number of the fastest growing perturbation is mmax =[2Bm/(3π)]. These theoretical results agree well with the experimental observations.

Original language | English |
---|---|

Article number | 066303 |

Journal | Physical Review E - Statistical, Nonlinear, and Soft Matter Physics |

Volume | 73 |

Issue number | 6 |

DOIs | |

Publication status | Published - 7 Jun 2006 |

Externally published | Yes |

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### ASJC Scopus subject areas

- Statistical and Nonlinear Physics
- Statistics and Probability
- Condensed Matter Physics

### Cite this

*Physical Review E - Statistical, Nonlinear, and Soft Matter Physics*,

*73*(6), [066303]. https://doi.org/10.1103/PhysRevE.73.066303

**Edge pinch instability of liquid metal sheet in a transverse high-frequency ac magnetic field.** / Priede, Janis; Etay, Jacqueline; Fautrelle, Yves.

Research output: Contribution to journal › Article

*Physical Review E - Statistical, Nonlinear, and Soft Matter Physics*, vol. 73, no. 6, 066303. https://doi.org/10.1103/PhysRevE.73.066303

}

TY - JOUR

T1 - Edge pinch instability of liquid metal sheet in a transverse high-frequency ac magnetic field

AU - Priede, Janis

AU - Etay, Jacqueline

AU - Fautrelle, Yves

PY - 2006/6/7

Y1 - 2006/6/7

N2 - We analyze the linear stability of the edge of a thin liquid metal layer subject to a transverse high-frequency ac magnetic field. The layer is treated as a perfectly conducting liquid sheet that allows us to solve the problem analytically for both a semi-infinite geometry with a straight edge and a thin disk of finite radius. It is shown that the long-wave perturbations of a straight edge are monotonically unstable when the wave number exceeds the critical value kc = F0 /(γ l0), which is determined by the linear density of the electromagnetic force F0 acting on the edge, the surface tension γ, and the effective arclength of edge thickness l0. Perturbations with wavelength shorter than critical are stabilized by the surface tension, whereas the growth rate of long-wave perturbations reduces as ∼k for k→0. Thus, there is the fastest growing perturbation with the wave number kmax =2/3 kc. When the layer is arranged vertically, long-wave perturbations are stabilized by the gravity, and the critical perturbation is characterized by the capillary wave number kc = gρ/γ, where g is the acceleration due to gravity and ρ is the density of metal. In this case, the critical linear density of electromagnetic force is F0,c =2 kc l0 γ, which corresponds to the critical current amplitude I0,c =4 π kc l0 Lγ/ μ0 when the magnetic field is generated by a straight wire at the distance L directly above the edge. By applying the general approach developed for the semi-infinite sheet, we find that a circular disk of radius R0 placed in a transverse uniform high-frequency ac magnetic field with the induction amplitude B0 becomes linearly unstable with respect to exponentially growing perturbation with the azimuthal wave number m=2 when the magnetic Bond number exceeds Bmc = B02 R02 /(2 μ0 l0 γ)=3π. For Bm> Bmc, the wave number of the fastest growing perturbation is mmax =[2Bm/(3π)]. These theoretical results agree well with the experimental observations.

AB - We analyze the linear stability of the edge of a thin liquid metal layer subject to a transverse high-frequency ac magnetic field. The layer is treated as a perfectly conducting liquid sheet that allows us to solve the problem analytically for both a semi-infinite geometry with a straight edge and a thin disk of finite radius. It is shown that the long-wave perturbations of a straight edge are monotonically unstable when the wave number exceeds the critical value kc = F0 /(γ l0), which is determined by the linear density of the electromagnetic force F0 acting on the edge, the surface tension γ, and the effective arclength of edge thickness l0. Perturbations with wavelength shorter than critical are stabilized by the surface tension, whereas the growth rate of long-wave perturbations reduces as ∼k for k→0. Thus, there is the fastest growing perturbation with the wave number kmax =2/3 kc. When the layer is arranged vertically, long-wave perturbations are stabilized by the gravity, and the critical perturbation is characterized by the capillary wave number kc = gρ/γ, where g is the acceleration due to gravity and ρ is the density of metal. In this case, the critical linear density of electromagnetic force is F0,c =2 kc l0 γ, which corresponds to the critical current amplitude I0,c =4 π kc l0 Lγ/ μ0 when the magnetic field is generated by a straight wire at the distance L directly above the edge. By applying the general approach developed for the semi-infinite sheet, we find that a circular disk of radius R0 placed in a transverse uniform high-frequency ac magnetic field with the induction amplitude B0 becomes linearly unstable with respect to exponentially growing perturbation with the azimuthal wave number m=2 when the magnetic Bond number exceeds Bmc = B02 R02 /(2 μ0 l0 γ)=3π. For Bm> Bmc, the wave number of the fastest growing perturbation is mmax =[2Bm/(3π)]. These theoretical results agree well with the experimental observations.

UR - http://www.scopus.com/inward/record.url?scp=33745013739&partnerID=8YFLogxK

U2 - 10.1103/PhysRevE.73.066303

DO - 10.1103/PhysRevE.73.066303

M3 - Article

VL - 73

JO - Physical Review E

JF - Physical Review E

SN - 1539-3755

IS - 6

M1 - 066303

ER -