Respuesta :
Answer:
a) 0 < r < R: E = 0, R < r < 2R: E = KQ/r^2, r > 2R: E = 2KQ/r^2
b) See the picture
Explanation:
We can use Gauss's law to find the electric field in all the regions:
EA = qen/e0 where qen is the enclosed charge
Remember that the electric field everywhere outside a sphere is:
E(r) = q/(4*pi*eo*r^2) = Kq/r^2
a)
- For 0 < r < R: There is not enclosed charge because all of it remains on the outer layer of the conducting sphere, therefore E = 0 EA = 0/e0 = 0 E = 0
- For R < r < 2R: Here the enclosed charge is equal Q E = Q/(4*pi*eo*r^2) = KQ/r^2
- For r > 2R: Here the enclosed charge is equal 2Q E = Q/(4*pi*eo*r^2) + Q/(4*pi*eo*r^2) = 2Q/(4*pi*eo*r^2) = 2KQ/r^2
b) At the beginning there is no electric field this is why you see a line in zero, In R the electric field is maximum and then it starts to decrease exponentially with the distance and finally in 2R the field increase a little due to the second sphere to then continue decreasing exponentially with the distance


(a) According to Gauss law, when 0 < r < R, the electric field is [tex]E(r) = 0[/tex].
When R < r < 2R, the electric field is [tex]E = \frac{1}{4 \pi r^2} \frac{Q}{\epsilon _0} =\frac{1}{4 \pi \epsilon _0} \frac{Q}{r^2}[/tex].
When R < r < 2R, the electric field is [tex]E = \frac{1}{4 \pi r^2} \frac{Q}{\epsilon _0} =\frac{1}{4 \pi \epsilon _0} \frac{Q}{r^2}[/tex].
(b) Electric field inside the conducting sphere is zero, maximum at 'R' then undergoes an exponential decrease. At '2R' there is again a maximum and then afterwards it has an exponential decrease.
Gauss' Law
(a) According to Gauss' law, the electric flux through a close surface with an enclosed charge 'Q' is given by;
[tex]\Phi = \frac{Q}{\epsilon _0}[/tex]
ie; [tex]E. A = \frac{Q}{\epsilon _0}[/tex]
Case 1: When 0 < r < R, the charge enclosed inside is zero.
Therefore, from Gauss law electric field in that area is also zero.
[tex]E(r) = 0[/tex]
Case 2: When R < r < 2R, here the charge enclosed is Q.
Therefore applying Gauss law;
[tex]E \times (4 \pi r^2) = \frac{Q}{\epsilon _0}[/tex]
[tex]E = \frac{1}{4 \pi r^2} \frac{Q}{\epsilon _0} =\frac{1}{4 \pi \epsilon _0} \frac{Q}{r^2}[/tex]
Case 3: When r > 2R, here the charge enclosed is 2Q.
Therefore applying Gauss law;
[tex]E \times (4 \pi r^2) = \frac{2Q}{\epsilon _0}[/tex]
[tex]E = \frac{1}{4 \pi r^2} \frac{2Q}{\epsilon _0} =\frac{1}{4 \pi \epsilon _0} \frac{2Q}{r^2}[/tex]
(b) There is no electric field inside the conducting sphere. Then at the surface, the electric field is maximum and undergoes an exponential decrease. At 2R there is again a maximum and then afterwards it has an exponential decrease.
(See the graph attached below)
Learn more about Gauss'law here:
https://brainly.com/question/13872115
