Q . The electric field components in Fig. 1.27 are E(x) = αx 1/2 , E(y) = E(z) = 0, in which α = 800 N/C m1/2. Calculate (a) the flux through the cube, and (b) the charge within the cube. Assume that a = 0.1 m.
Solution :
(a) Since the electric field has only an x component, for faces
perpendicular to x direction, the angle between E and ΔS is ± π/2.
Therefore, the flux φ = E.ΔS is separately zero for each face
of the cube except the two shaded ones.
Now the magnitude of the electric field at the left face is E(L) = αx
1/2
= αa
1/2 (x = a at the left face).
The magnitude of electric field at the right face is
E(R) = α x
1/2
= α (2a)
1/2 (x = 2a at the right face).
The corresponding fluxes are
φ(L) = E(L) .ΔS = ΔS E(L) . n^ (L) =E(L) ΔS cosθ = –E(L) ΔS,
since θ = 180°
φ(L)= –E(L) a^2
φ(R) = E(R).ΔS = E(R) ΔS cosθ = E(R) ΔS, since θ = 0°
φ(R)= E(R) a^2
Net flux through the cube = φ(R) + φ(L) = E(R)a^2
– E(L) a^2
= a^2 [E(R) – E(L)] = αa^2
[(2a) ^1/2
– a ^1/2]
= αa ^5/2 [2^1/2 - 1] = 1.05 N m2
C–1
(b) We can use Gauss’s law to find the total charge q inside the cube.
We have φ = q/ε0
or q = φε
0
. Therefore,
q = 1.05 × 8.854 × 10–^12 C = 9.27 × 10^–12 C
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