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Resistive ballooning mode

The resistive ballooning mode (RBM) is an instability occurring in magnetized plasmas, particularly in magnetic confinement devices such as tokamaks, when the pressure gradient is opposite to the effective gravity created by a magnetic field.

Linear growth rate

The linear growth rate γ of the RBM instability is given as

\gamma^2 = -\vec{g_{eff}}\cdot\frac{\nabla p}{p}

where |\nabla p|\sim \frac{p}{L_p} is the pressure gradient g_{eff}=c_s|\frac{\nabla B}{B}|\sim 1/R_0 is the effective gravity produced by a non-homogeneous magnetic field, R0 is the major radius of the device, Lp is a characteristic length of the pressure gradient, and cs is the plasma sound speed.

Similarity with the Rayleigh-Taylor instability

The RBM instability is similar to the Rayleigh-Taylor instability (RT), with Earth gravity \vec g replaced by the effective gravity \vec g_{eff}, except that for the RT instability, \vec g acts on the mass density ρ of the fluid, whereas for the RBM instability, \vec g_{eff} acts on the pressure p of the plasma.

This article is licensed under the GNU Free Documentation License. It uses material from the Wikipedia article "Resistive_ballooning_mode". A list of authors is available in Wikipedia.
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