Abstract:Propagation of three dimensional magnetosonic waves is considered for a homogeneous shear flow of an incompressible fluid. The analytical solutions for all magnetohydrodynamic variables are presented by confluent Heun functions. The problem is reduced to finding a solution of an effective Schrodinger equation. The amplification of slow magnetosonic waves is analyzed in great details. A simple formula for the amplification coefficient is derived. The velocity shear primarily affects the incompressible limit of … Show more
“…This saturation simulates strong turbulence for small wave-vectors, but definitely for large wave-vectors |K y | ≫ 1 at τ → ∞ we have a wave type turbulence with a given frequency. We have to mention that the linearized case of pure shear is exactly integrable in terms of the Heun functions [1,5]. Investigating numerically this case with ω C = 0 and B z = 0 in his Ph.D. thesis [6] T. Hristov discovered in 1990 the amplification of slow magnetosonic waves (SMWs) by shear flows.…”
Section: Lyapunov Analysis Of the Linearized Set Of Equations In Lagrmentioning
Abstract. We have derived the full set of MHD equations for incompressible shear flow of a magnetized fluid and considered their solution in the wave-vector space. The linearized equations give the famous amplification of slow magnetosonic waves and describe the magnetorotational instability. The nonlinear terms in our analysis are responsible for the creation of turbulence and self-sustained spectral density of the MHD (Alfvén and pseudo-Alfvén) waves. Perspectives for numerical simulations of weak turbulence and calculation of the effective viscosity of accretion disks are shortly discussed in k-space.
“…This saturation simulates strong turbulence for small wave-vectors, but definitely for large wave-vectors |K y | ≫ 1 at τ → ∞ we have a wave type turbulence with a given frequency. We have to mention that the linearized case of pure shear is exactly integrable in terms of the Heun functions [1,5]. Investigating numerically this case with ω C = 0 and B z = 0 in his Ph.D. thesis [6] T. Hristov discovered in 1990 the amplification of slow magnetosonic waves (SMWs) by shear flows.…”
Section: Lyapunov Analysis Of the Linearized Set Of Equations In Lagrmentioning
Abstract. We have derived the full set of MHD equations for incompressible shear flow of a magnetized fluid and considered their solution in the wave-vector space. The linearized equations give the famous amplification of slow magnetosonic waves and describe the magnetorotational instability. The nonlinear terms in our analysis are responsible for the creation of turbulence and self-sustained spectral density of the MHD (Alfvén and pseudo-Alfvén) waves. Perspectives for numerical simulations of weak turbulence and calculation of the effective viscosity of accretion disks are shortly discussed in k-space.
We have analyzed the amplification of slow magnetosonic (or pseudo-Alfvénic) waves (SMW) in incompressible shear flow. As found here, the amplification depends on the component of the wave-vector perpendicular to the direction of the shear flow. Earlier numerical results are consistent with the general analytic solution for the linearized magnetohydrodynamic equations, derived here for the model case of pure homogeneous shear (without Coriolis force). An asymptotically exact analytical formula for the amplification coefficient is derived for the case when the amplification is sufficiently large.
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