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Question: A hollow spherical conductor of radius R has a charge Q on it. A small dent on the surface decreases...

A hollow spherical conductor of radius R has a charge Q on it. A small dent on the surface decreases the volume of the spherical conductor by 2%. Assume that the charge density on the surface does not change due to the dent and the electric field in the dent region remains same as other points on the surface. (a) AE is the electrostatic energy stored in the electric field in the shallow dent region and E is the total electrostatic energy of the spherical shell. Find the ΔΕ ratio E (b) Using the ratio obtained in part (a) calculate the percentage change in capacitance of the sphere due to the dent.

Answer

0.02 and -0.67%

Explanation

Solution

Explanation of the solution:

(a) Find the ratio ΔEE\frac{\Delta E}{E}: The original volume of the spherical conductor is V0=43πR3V_0 = \frac{4}{3}\pi R^3. The dent decreases the volume by 2%, which means the change in volume is ΔV=0.02V0\Delta V = 0.02 V_0. The problem defines ΔE\Delta E as the electrostatic energy stored in the electric field in the shallow dent region and EE as the total electrostatic energy of the spherical shell. Assuming that the energy associated with the dent region is proportional to the volume change it causes, relative to the total energy being proportional to the original volume, we can write the ratio as: ΔEE=ΔVV0\frac{\Delta E}{E} = \frac{\Delta V}{V_0} Given that the volume decreases by 2%, ΔVV0=0.02\frac{\Delta V}{V_0} = 0.02. Therefore, ΔEE=0.02\frac{\Delta E}{E} = 0.02.

(b) Calculate the percentage change in capacitance: The total electrostatic energy of a conductor with charge Q and capacitance C is given by E=Q22CE = \frac{Q^2}{2C}. Let the original capacitance be C0C_0 and the original energy be E0E_0. After the dent is made, the capacitance becomes CC' and the energy becomes EE'. Assuming the charge Q on the conductor remains constant, we have E0=Q22C0E_0 = \frac{Q^2}{2C_0} and E=Q22CE' = \frac{Q^2}{2C'}. The change in energy is EE0=Q22CQ22C0=Q22(1C1C0)E' - E_0 = \frac{Q^2}{2C'} - \frac{Q^2}{2C_0} = \frac{Q^2}{2} \left(\frac{1}{C'} - \frac{1}{C_0}\right). Let the change in capacitance be ΔC=CC0\Delta C = C' - C_0. For a small dent, ΔC\Delta C is small compared to C0C_0. EE0=Q22(C0CC0C)=Q22ΔCC0(C0+ΔC)E' - E_0 = \frac{Q^2}{2} \left(\frac{C_0 - C'}{C_0 C'}\right) = \frac{Q^2}{2} \frac{-\Delta C}{C_0 (C_0 + \Delta C)}. For small ΔC\Delta C, CC0C' \approx C_0, so EE0Q22C02(ΔC)=(Q22C0)ΔCC0=E0ΔCC0E' - E_0 \approx \frac{Q^2}{2C_0^2} (-\Delta C) = - \left(\frac{Q^2}{2C_0}\right) \frac{\Delta C}{C_0} = -E_0 \frac{\Delta C}{C_0}. So, EE0E0=ΔCC0\frac{E' - E_0}{E_0} = -\frac{\Delta C}{C_0}.

The change in total energy is also related to the work done to deform the conductor against the electrostatic pressure. The electrostatic pressure just outside the surface of a conductor is P=σ22ϵ0P = \frac{\sigma^2}{2\epsilon_0}. The work done on the conductor to reduce its volume by ΔV\Delta V is W=PΔVW = P \Delta V. This work increases the electrostatic energy of the conductor, so EE0=PΔVE' - E_0 = P \Delta V. For a spherical conductor, the total energy can be related to the pressure and volume: E0=Q28πϵ0R=(σ4πR2)28πϵ0R=16π2σ2R48πϵ0R=2πσ2R3ϵ0E_0 = \frac{Q^2}{8\pi\epsilon_0 R} = \frac{(\sigma 4\pi R^2)^2}{8\pi\epsilon_0 R} = \frac{16\pi^2 \sigma^2 R^4}{8\pi\epsilon_0 R} = \frac{2\pi \sigma^2 R^3}{\epsilon_0}. Since V0=43πR3V_0 = \frac{4}{3}\pi R^3, we have R3=3V04πR^3 = \frac{3V_0}{4\pi}. E0=2πσ2ϵ0(3V04π)=3σ2V02ϵ0E_0 = \frac{2\pi \sigma^2}{\epsilon_0} \left(\frac{3V_0}{4\pi}\right) = \frac{3 \sigma^2 V_0}{2\epsilon_0}. The pressure is P=σ22ϵ0P = \frac{\sigma^2}{2\epsilon_0}. So, E0=3PV0E_0 = 3 P V_0, or P=E03V0P = \frac{E_0}{3V_0}. The energy change is EE0=PΔV=E03V0ΔV=13E0ΔVV0E' - E_0 = P \Delta V = \frac{E_0}{3V_0} \Delta V = \frac{1}{3} E_0 \frac{\Delta V}{V_0}. So, EE0E0=13ΔVV0\frac{E' - E_0}{E_0} = \frac{1}{3} \frac{\Delta V}{V_0}.

Equating the two expressions for EE0E0\frac{E' - E_0}{E_0}: ΔCC0=13ΔVV0-\frac{\Delta C}{C_0} = \frac{1}{3} \frac{\Delta V}{V_0}. We are given ΔVV0=0.02\frac{\Delta V}{V_0} = 0.02. ΔCC0=13×0.02=0.023\frac{\Delta C}{C_0} = -\frac{1}{3} \times 0.02 = -\frac{0.02}{3}. The percentage change in capacitance is ΔCC0×100%=0.023×100%=23%\frac{\Delta C}{C_0} \times 100\% = -\frac{0.02}{3} \times 100\% = -\frac{2}{3}\%. As a decimal, 23%0.666...%-\frac{2}{3}\% \approx -0.666...\%. Rounded to two decimal places, this is 0.67%-0.67\%. The capacitance decreases due to the dent.

Answer:

(a) The ratio ΔEE\frac{\Delta E}{E} is 0.020.02. (b) The percentage change in capacitance is approximately 0.67%-0.67\%.

Subject: Physics Chapter: Electrostatic Potential and Capacitance Topic: Electrostatic energy of a conductor, Capacitance of a spherical conductor, Effect of shape on capacitance

Difficulty: Medium Question Type: Descriptive