Fundamentals of Plasma Physics

(C. Jardin) #1

24 Chapter 1. Basic concepts


is the relationship between Tesla and Gauss, between particles per cubiccentimeter
and particles per cubic meter? What is magneticflux? If a circular loop of wire with
a break in it links a magneticflux of 29.83 Weber which increases at a constant rate to
aflux of 30.83 Weber in one second, what voltage appears across the break?


  1. Solve Eq.(1.5) the ‘easy’ way by first proving using Gauss’ law to show thatthe solu-
    tion of
    ∇^2 φ=−


1


ε 0

δ(r)
is
φ=

1


4 πε 0 r

.


Show that this implies
∇^2

1


4 πr
=−δ(r) (1.39)
is a representation for the delta function. Then, use spherical polar coordinates and
symmetry to show that the Laplacian reduces to

∇^2 φ=

1


r^2


∂r

(


r^2
∂φ
∂r

)


.


Explicitly calculate∇^2 (1/r)and then reconcile your result with Eq.(1.39). Using
these results guess that the solution to Eq.(1.5) has the form

φ=
g(r)
4 πε 0 r

.


Substitute this guess into Eq.(1.5) to obtain a differential equation forgwhich is trivial
to solve.


  1. Solve Eq.(1.5) forφ(r)using a more general method which illustrates several im-
    portant mathematical techniques and formalisms. Begin by defining the 3D Fourier
    transform
    φ ̃(k) =



drφ(r)e−ik·r (1.40)
in which case the inverse transform is

φ(r) =

1


(2π)^3


dk ̃φ(k)eik·r (1.41)

and note that the Dirac delta function can be expressed as

δ(r) =

1


(2π)^3


dkeik·r. (1.42)

Now multiply Eq.(1.5) by∫ exp(−ik·r)and then integrate over allr, i.e. operate with
dr. The term involving∇^2 is integrated by parts, which effectively replaces the∇
operator withik.
Show that the Fourier transform of the potential is

φ ̃(k) = qT
ǫ 0 (k^2 +λ−D^2 )

. (1.43)

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