5.5 Normalization

Choose a typical number density n0 and a typical velocity v0, then define the electron plasma frequency ωpe and the Debye length λD as

     ∘ -----
        n0e2
ωpe =  m--𝜀-,
         e 0
(89)

and

     -v0-
λD = ωpe,
(90)

respectively. Using ωpe and λD, define the following normalized quantities:

-      --  -x- -- --eϕ-- --  v0  -    vx --   ni
t = tωpe,x = λD ,ϕ = mev20,F = n0F,vx = v0,ni = n0
(91)

In terms of these normalized quantities, equation (78) is written

 --
dF-= 0,
dt
(92)

and the Poisson equation (79) is written

 2--
d-ϕ = − ρ.
dx2
(93)

where ρ = nion −∞Fdvx.

The equations for the characteristic lines, Eq. (76) and (77), are written

 --
dx= vx,
dt
(94)

 -     --
dvx = dϕ.
 dt   dx
(95)

The electric field is given by E = dϕ∕dx, which, in terms of normalized quantities, is written

       --
E-= − dϕ,
      dx
(96)

where E = EeλD(mv02).

In terms of the normalized quantities, the evolution equation (87) of δF is written as

 --      --
dδF--= E∂-F0
dt      ∂vx
(97)

In terms of δF, Poisson’s equation is written as

  --  ∫
-dϕ     ∞  -- -
dx2 =  −∞ δF dvx,
(98)

where nion = ne0 has been assumed.