# Solution - Solar Physics at MSU ```–1–
Solution to HW Problems
56. Griffiths 4.24 In this problem, there is no volume charge ρ anywhere in the space, so we’ll solve
Laplace’s equation in spherical coordinates to determine the electric potential in the material and
outside the sphere. Inside the metal sphere, r &lt; a, the potential is a constant which we may take
as zero. The general solution to the Laplace’s equation is a Legendre polynomial series.
Inside the material, a &lt; r &lt; b, the general solution is Vin = ΣAl r l Pl + ΣBl r −l−1 Pl , where Pl ≡
Pl (cosθ) is the l-th order Legendre polynomial. Note that in this solution, both r l and r −l−1
solutions exist, since r does not go to zero in this region.
~ out (r &gt;&gt;
Outside the material, r &gt; b, at r &gt;&gt; b, the solution approaches the external field E
R
~
~
b) = E0 ẑ, or Vout (r &gt;&gt; b) = − E &middot; dl = −E0 rcosθ. So we may write the solution for Vout as
Vout (r &gt; b) = ΣCl r −l−1 Pl − E0 rcosθ, so that as r &gt;&gt; b, the r −l−1 solution vanishes.
The boundary condition has to be satisfied at both boundaries r = a and r = b. At r = a, the
potential becomes zero. At r = b, Vin = Vout |r=b . Also, at r = b, since there is no free charge, the
normal component of the displacement field is continuous, or ǫr ∂Vin /∂rr=b = ∂Vout /∂r|r=b . These
boundary conditions give rise to the following equations to determine the relationship between Al ,
Bl , and Cl :
Al al + Bl a−l−1 = 0
Al bl + Bl b−l−1 = Cl b−l−1 (l 6= 1)
A1 b + B1 b−2 = C1 b−2 − E0 b
ǫr (lAl bl−1 + (−l − 1)Bl b−l−2 ) = (−l − 1)Cl b−l−2 (l 6= 1)
ǫr (A1 − 2B1 b−3 ) = −2C1 b−3 − E0
Solving these equations, it is seen that Al = Bl = Cl = 0 when l 6= 1; namely, only l = 1
terms are left. From above equations concerning l = 1 terms, it’s found that B1 = −A1 a3 ,
C1 = A1 (b3 − a3 ) + E0 b3 , and ǫr (A1 b3 + 2A1 a3 ) = −2A1 (b3 − a3 ) − 3E0 b3 , leading to the expressions
of A1 and B1 :
−3E0
A1 =
(ǫr + 2)(1 − a3 /b3 ) + 3ǫr a3 /b3
B1 =
3E0 a3
(ǫr + 2)(1 − a3 /b3 ) + 3ǫr a3 /b3
The potential inside the material is therefore
Vin = A1 rP1 + B1 r −2 P1 =
−3E0
a3
(r
−
)cosθ
(ǫr + 2)(1 − a3 /b3 ) + 3ǫr a3 /b3
r2
To simplify the solution, we may define k =
3
(ǫr +2)(1−a3 /b3 )+3ǫr a3 /b3 ,
Vin = −kE0 (r −
a3
)cosθ
r2
so the potential is written as
–2–
Note that k = (ǫr3+2) if a goes to zero, i.e., no metal sphere at the center, then the solution would
be exactly the same as in book Example 4.7.
The above solution looks like a superposition of a modified constant external field (the rcosθ
term) and a dipole field. The modified constant external field is the contribution of the original
~ ′ ∝ −E0 ẑ by the bound charges at r = b, and the dipole field is
external field E0 ẑ and the field E
the contribution of the induced charges at r = a, which generates a dipole field outside the metal
sphere.
And the electric field
3
3
~ in = −∇V
~ in = kE0 (1 + 2a )cosθr̂ − kE0 (1 − a )sinθ θ̂
E
r3
r3
```