1972Journal of the Physical Society of JapanRequires access

Hydromagnetic Instability of a Two-Dimensional Jet at Small Magnetic Reynolds Numbers

Kanefusa Gotoh, Isamu Nakata

Open publisher page 2 citations

Abstract

The effect of a uniform and parallel magnetic field upon the instability of a Bickley jet is investigated at small magnetic Reynolds numbers. The equation of disturbance is solved numerically and it is shown that the flow is stabilized with the magnetic field. The change of the lowest critical Reynolds number R c is shown graphically. When magnetic field is measured by the parameter S (\({=}\sqrt{MR}\)), where M is the Hartmann number and R is the Reynolds number, R c is caused by the two-dimensional disturbance provided 0≦ S <5.5. For S >5.5, R c is expressed as R c =3.3 S and the responsible disturbance is the three-dimensional one which propagates at angle cos -1 (5.5/ S ) to the direction of the basic flow.

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What this paper is about

The effect of a uniform and parallel magnetic field upon the instability of a Bickley jet is investigated at small magnetic Reynolds numbers. The equation of disturbance is solved numerically and it is shown that the flow is stabilized with the magnetic field. The change of the lowest critical Reynolds number R c is shown graphically. When magnetic field is measured by the parameter S (\({=}\sqrt{MR}\)), where M is the Hartmann number and R is the Reynolds number, R c is caused by the two-dimensional disturbance provided 0≦ S <5.5. For S >5.5, R c is expressed as R c =3.3 S and the responsible disturbance is the three-dimensional one which propagates at angle cos -1 (5.5/ S ) to the direction of the basic flow.

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Available abstract

The effect of a uniform and parallel magnetic field upon the instability of a Bickley jet is investigated at small magnetic Reynolds numbers. The equation of disturbance is solved numerically and it is shown that the flow is stabilized with the magnetic field. The change of the lowest critical Reynolds number R c is shown graphically. When magnetic field is measured by the parameter S (\({=}\sqrt{MR}\)), where M is the Hartmann number and R is the Reynolds number, R c is caused by the two-dimensional disturbance provided 0≦ S <5.5. For S >5.5, R c is expressed as R c =3.3 S and the responsible disturbance is the three-dimensional one which propagates at angle cos -1 (5.5/ S ) to the direction of the basic flow.

Key concepts: Reynolds number, Magnetic Reynolds number, Physics, Magnetic field, Jet (fluid), Instability, Hartmann number, Flow (mathematics)

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