Abstract
A study is made of the nonlinear spatial evolution of an externally
excited instability
wave in a mixing layer of nearly perfectly conducting fluid with a large
Reynolds
number in a weak parallel magnetic field.It is shown that the evolution pattern bears a resemblance to that of
disturbances
in a weakly stratified shear flow with the Prandtl number less than unity
which was
studied in our earlier publication (Shukhman & Churilov 1997): a weak
magnetic
field, like a weak stratification when Pr<1,
has a stabilizing effect on the nonlinear
development of disturbances and in the case when the linear growth rate
of the wave
is not too large leads either to the instability saturation in the viscous
critical layer
regime or to the establishment of a unsteady nonlinear critical layer regime
where the
wave amplitude oscillates without exceeding a certain maximum value. In
this case
the regime of the quasi-steady nonlinear critical layer is not attained
evolutionarily.
When the linear growth rate is large enough the magnetic field has no dynamical
effect
on evolution and the quasi-steady nonlinear critical layer regime with
the well-known
power-law growth of amplitude (A∝x2/3)
is eventually attained.Also, the critical layer structure and the evolution behaviour in the
case of a strong
difference of dissipation coefficients (i.e. ordinary viscosity and magnetic
viscosity) are
considered.
Publisher
Cambridge University Press (CUP)
Subject
Mechanical Engineering,Mechanics of Materials,Condensed Matter Physics
Cited by
4 articles.
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