First adiabatic invariant

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The first adiabatic invariant, μ, is the action integral over a cyclotron frequency . It is usually written:

\mu=\frac{mv_\perp^2}{2B}

The action integral is written:

\oint p\,dq=\oint_{\mathrm{gyro}}m v_\perp\,ds

We can define the length as ds = ρdθ, and use the gyro radius \rho=v_\perp mc/qB:

\oint p\,dq=\oint_0^{2\pi}\frac{m^2 c v_\perp^2}{qB}\,d\theta

Over one orbit, if we are adiabatic then B and v_\perp change much more slowly than the gyro period Ωc. This gives:

\oint p\,dq=\frac{2\pi m^2 c v_\perp^2}{qB}=\frac{4\pi mc}{q}\mu

This page was recovered in October 2009 from the Plasmagicians page on First_adiabatic_invariant dated 01:25, 19 October 2006.

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