5.5 Bounce frequency of barely trapped particles

Let us analytically estimate the bounce frequency of barely trapped particles, i.e., particle satisfying the critical condition (76),

( v∥)2       B        R0 − r
  v-  = 1 − B----≈ 1− R--+-r ≈ 2𝜀,
             max        0
(97)

i.e., v = √ --
  2𝜀v, where v is the parallel velocity on the low-field-side midplane.

The distance along the magnetic field line travelled in half an orbit is about 2πR0q, then the time needed is then given by

    2πR0q    2πR0q   2πR0q
tb ≈--v∥--≈  √2-𝜀v-≈ √2-𝜀v--
                         th
(98)

The above approximation is rough since v changes between zero and √2𝜀v and we still use a constant value, √--
 2𝜀v, in approximating it.

Then the bounce (angular) frequency is given by

               √ --         ∘--
ωb = 2π-= --2π--- 2𝜀vth = -vth-  𝜀,
     2tb   4πR0q         R0q   2
(99)

which turns out to be take the same form as Eq. (95). very strange!