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Ratio of Charges on Concentric Spherical Shells with Equal Outer Charge Densities

Three concentric metallic spherical shells of radii R,2R,3RR, 2R, 3R, are given charges Q1,Q2,Q3Q_1, Q_2, Q_3, respectively. It is found that the surface charge densities on the outer surfaces of the shells are equal. Then, the ratio of the charges given to the shells, Q1:Q2:Q3Q_1 : Q_2 : Q_3, is

Options

A

1:2:31 : 2 : 3

B

1:3:51 : 3 : 5

Correct
C

1:4:91 : 4 : 9

D

1:8:181 : 8 : 18

Step-by-Step Solution

To find the ratio of the charges Q1:Q2:Q3Q_1 : Q_2 : Q_3, we analyze the distribution of charges on the inner and outer surfaces of each concentric metallic spherical shell using electrostatic induction and Gauss's law.

Let the radii of the three concentric shells be:

  • Innermost shell: r1=Rr_1 = R
  • Middle shell: r2=2Rr_2 = 2R
  • Outermost shell: r3=3Rr_3 = 3R

Let the equal surface charge density on the outer surface of each shell be σ\sigma.

  1. For the innermost shell of radius RR:
    Since there is no charge in the cavity inside the innermost shell, the charge on its inner surface is zero:
    q1,inner=0q_{1,\text{inner}} = 0
    Therefore, the entire charge Q1Q_1 resides on its outer surface:
    q1,outer=Q1q_{1,\text{outer}} = Q_1
    The surface charge density on the outer surface is:
    σ=q1,outer4πR2=Q14πR2  ⟹  Q1=4πR2σ\sigma = \frac{q_{1,\text{outer}}}{4\pi R^2} = \frac{Q_1}{4\pi R^2} \implies Q_1 = 4\pi R^2 \sigma

  2. For the middle shell of radius 2R2R:
    By Gauss's law, the electric field inside the conducting material of the middle shell must be zero. Thus, the inner surface of this shell must induce a charge equal and opposite to the total enclosed charge:
    q2,inner=−Q1q_{2,\text{inner}} = -Q_1
    Since the net charge given to the middle shell is Q2Q_2, by conservation of charge:
    q2,inner+q2,outer=Q2  ⟹  q2,outer=Q1+Q2q_{2,\text{inner}} + q_{2,\text{outer}} = Q_2 \implies q_{2,\text{outer}} = Q_1 + Q_2
    The surface charge density on its outer surface is:
    σ=q2,outer4π(2R)2=Q1+Q216πR2\sigma = \frac{q_{2,\text{outer}}}{4\pi (2R)^2} = \frac{Q_1 + Q_2}{16\pi R^2}
    Equating this to σ=Q14πR2\sigma = \frac{Q_1}{4\pi R^2}:
    Q1+Q216πR2=Q14πR2\frac{Q_1 + Q_2}{16\pi R^2} = \frac{Q_1}{4\pi R^2}
    Q1+Q2=4Q1  ⟹  Q2=3Q1Q_1 + Q_2 = 4Q_1 \implies Q_2 = 3Q_1

  3. For the outermost shell of radius 3R3R:
    Similarly, the charge enclosed by the inner surface of the outermost shell is the net charge on the inner two shells, which is Q1+Q2Q_1 + Q_2. Thus, the induced charge on its inner surface is:
    q3,inner=−(Q1+Q2)q_{3,\text{inner}} = -(Q_1 + Q_2)
    Since the net charge given to this shell is Q3Q_3, the charge on its outer surface is:
    q3,outer=Q3−q3,inner=Q1+Q2+Q3q_{3,\text{outer}} = Q_3 - q_{3,\text{inner}} = Q_1 + Q_2 + Q_3
    The surface charge density on its outer surface is:
    σ=q3,outer4π(3R)2=Q1+Q2+Q336πR2\sigma = \frac{q_{3,\text{outer}}}{4\pi (3R)^2} = \frac{Q_1 + Q_2 + Q_3}{36\pi R^2}
    Equating this to σ=Q14πR2\sigma = \frac{Q_1}{4\pi R^2}:
    Q1+Q2+Q336πR2=Q14πR2\frac{Q_1 + Q_2 + Q_3}{36\pi R^2} = \frac{Q_1}{4\pi R^2}
    Q1+Q2+Q3=9Q1Q_1 + Q_2 + Q_3 = 9Q_1
    Substituting Q1+Q2=4Q1Q_1 + Q_2 = 4Q_1:
    4Q1+Q3=9Q1  ⟹  Q3=5Q14Q_1 + Q_3 = 9Q_1 \implies Q_3 = 5Q_1

Combining the results, we find:
Q1:Q2:Q3=Q1:3Q1:5Q1=1:3:5Q_1 : Q_2 : Q_3 = Q_1 : 3Q_1 : 5Q_1 = 1 : 3 : 5

Therefore, the correct option is (B).