A solid conducting sphere with radius R that carries positive charge Q is concentric with a very thin insulating shell of radius 2R that also carries charge Q. The charge Q is distributed uniformly over the insulating shell.
(a) Find the electric field (magnitude and direction) in each of the regions 0 < r < R, R < r < 2R, and r > 2R.
(b) Graph the electric-field magnitude as a function of r.

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)

  1. 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
  2. For R < r < 2R: Here the enclosed charge is equal Q                                      E =  Q/(4*pi*eo*r^2) = KQ/r^2      
  3. 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

Ver imagen mateolara11
Ver imagen mateolara11

(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

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