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~
E h
a
Hint: Think about the total flux through the pyramid first, before you do a lot of unnecessary work!
The total electric flux through the pyramid vanishes since the electric field is constant. Thus the flux
through the four slanted surfaces is, up to the sign, the same as through the square base:
Nm2
ΦE = EA ≃ 1.872 · 103 = 1.872 · 103 Vm.
C
Problem 3 (30 points)
l ξ
x
60◦
h
~
E
~ = 7.8 · 104 N/C~iy (see figure).
Consider a closed triangular box resting within a horizontal electric field E
Calculate the electric flux, Φ, through
Note that the order of the parameters, ξ and x, has been chosen such that we get the right orientation
of the surface vector, namely pointing upwards! The flux is
Z l Z 2h
E
Z
~
ΦE,S = dS · E =~ dx dξ = lhE.
0 0 2
R
x
Hint: Use cylinder coordinates, (ρ, ϕ, z)! The following integrals are needed to solve the problem:
ρ 1
Z
dρ 2 2 3/2
= −p ,
(ρ + z ) ρ2 + z 2
(2)
1 z
Z
dz 2 2 3/2
= p .
(ρ + z ) ρ2 ρ2 + z 2
Solution
(a) According to Gauss’s Law the flux through the cylinder is the enclosed charge ×1/ǫ0 :
q
ΦE = .
ǫ0
(b) To evaluate the flux we have to parametrize the three surfaces of the cylinder, i.e., the top and
bottom caps and the envelope. This is most easily done in our standard cylinder coordinates ρ, φ,
and z. In these coordinates the electric field reads
~ = 1 ~r = q
E ρ~iρ + z~iz . (3)
4πǫ0 r3 4πǫ0 (ρ2 + z 2 )3/2
For the upper cap the parameters are ρ ∈ (0, R) and φ ∈ (0, 2π), and z = h/2 = const. The
~ = ρ dρ dφ ~iz . Plugging all this into the flux integral, gives
surface-normal vector is dA
2π R
ρh q
Z Z
Φupper = dφ dρ , (4)
0 0 2 4πǫ0 (ρ + h2 /4)3/2
2
and using the first of the integrals, given in Eq. (2), leads to
" #
q h
Φupper = 2− p . (5)
4ǫ0 R2 + h2 /4
The lower cap gives the same result due to symmetry:
For the envelope of the cylinder the right parametrization is given by z ∈ (−h/2, h/2), φ ∈ (0, 2π),
while ρ = R = const, and the surface-normal vector is given by dA ~ = R dφ dz ~iρ . With help of the
second integral, given in Eq. (2), we find
2π h/2
q R2 q h
Z Z
Φenv = dφ dz = p . (7)
0 −h/2 4πǫ0 (R + z )
2 2 3/2 2ǫ0 R + h2 /4
2