Respuesta :
a) E = 0
b) [tex]3.38\cdot 10^6 N/C[/tex]
Explanation:
a)
We can solve this problem using Gauss theorem: the electric flux through a Gaussian surface of radius r must be equal to the charge contained by the sphere divided by the vacuum permittivity:
[tex]\int EdS=\frac{q}{\epsilon_0}[/tex]
where
E is the electric field
q is the charge contained by the Gaussian surface
[tex]\epsilon_0[/tex] is the vacuum permittivity
Here we want to find the electric field at a distance of
r = 12 cm = 0.12 m
Here we are between the inner radius and the outer radius of the shell:
[tex]r_1 = 10 cm\\r_2 = 15 cm[/tex]
However, we notice that the shell is conducting: this means that the charge inside the conductor will distribute over its outer surface.
This means that a Gaussian surface of radius r = 12 cm, which is smaller than the outer radius of the shell, will contain zero net charge:
q = 0
Therefore, the magnitude of the electric field is also zero:
E = 0
b)
Here we want to find the magnitude of the electric field at a distance of
r = 20 cm = 0.20 m
from the centre of the shell.
Outside the outer surface of the shell, the electric field is equivalent to that produced by a single-point charge of same magnitude Q concentrated at the centre of the shell.
Therefore, it is given by:
[tex]E=\frac{Q}{4\pi \epsilon_0 r^2}[/tex]
where in this problem:
[tex]Q=15 \mu C = 15\cdot 10^{-6} C[/tex] is the charge on the shell
[tex]r=20 cm = 0.20 m[/tex] is the distance from the centre of the shell
Substituting, we find:
[tex]E=\frac{15\cdot 10^{-6}}{4\pi (8.85\cdot 10^{-12})(0.20)^2}=3.38\cdot 10^6 N/C[/tex]