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Question: A conducting sphere of radius $R = 1.0$ m is charged to a potential $V_i = 1000$ V. A thin metal dis...

A conducting sphere of radius R=1.0R = 1.0 m is charged to a potential Vi=1000V_i = 1000 V. A thin metal disc of radius r=1.0r = 1.0 cm mounted on an insulating handle is touched with the sphere making contact with one of its flat faces and then separated. After separation the disc is earthed and the process is repeated until the potential of the sphere becomes Vf=999V_f = 999 V. Approximately how many times has this process been repeated?

A

10

B

20

C

30

D

40

Answer

40

Explanation

Solution

Let RR be the radius of the sphere and rr be the radius of the disc. The capacitance of the conducting sphere is Cs=4πϵ0RC_s = 4 \pi \epsilon_0 R.

Let VnV_n be the potential of the sphere after the nn-th repetition of the process. Initially, the potential of the sphere is V0=Vi=1000V_0 = V_i = 1000 V.

When the disc is touched to the sphere, it samples the potential at the contact point. The charge transferred ΔQ\Delta Q is proportional to the potential VV and can be expressed as ΔQ=CV\Delta Q = C'V, where CC' is an effective capacitance.

The potential of the sphere after one contact is V=QΔQCs=VΔQCs=VCVCs=V(1CCs)V' = \frac{Q - \Delta Q}{C_s} = V - \frac{\Delta Q}{C_s} = V - \frac{C'V}{C_s} = V \left(1 - \frac{C'}{C_s}\right). Thus, each contact reduces the potential by a factor of (1CCs)\left(1 - \frac{C'}{C_s}\right).

After NN repetitions, the potential is Vf=Vi(1CCs)NV_f = V_i \left(1 - \frac{C'}{C_s}\right)^N.

We have Vi=1000V_i = 1000 V and Vf=999V_f = 999 V, so 9991000=(1CCs)N\frac{999}{1000} = \left(1 - \frac{C'}{C_s}\right)^N.

The key is to estimate CCs\frac{C'}{C_s}. The charge density on the sphere is σ=Q4πR2=CsV4πR2=4πϵ0RV4πR2=ϵ0VR\sigma = \frac{Q}{4 \pi R^2} = \frac{C_s V}{4 \pi R^2} = \frac{4 \pi \epsilon_0 R V}{4 \pi R^2} = \frac{\epsilon_0 V}{R}.

The charge transferred to the disc might be proportional to its area multiplied by the charge density. So ΔQσ×(area of disc)=ϵ0VR×(πr2)\Delta Q \sim \sigma \times (\text{area of disc}) = \frac{\epsilon_0 V}{R} \times (\pi r^2). Thus, CVϵ0VRπr2C' V \sim \frac{\epsilon_0 V}{R} \pi r^2, which gives Cϵ0πr2RC' \sim \frac{\epsilon_0 \pi r^2}{R}.

Then CCsϵ0πr2/R4πϵ0R=r24R2\frac{C'}{C_s} \sim \frac{\epsilon_0 \pi r^2 / R}{4 \pi \epsilon_0 R} = \frac{r^2}{4 R^2}.

Given R=1.0R = 1.0 m and r=0.01r = 0.01 m, we have CCs=(0.01)24(1)2=0.00014=0.000025\frac{C'}{C_s} = \frac{(0.01)^2}{4 (1)^2} = \frac{0.0001}{4} = 0.000025.

So, 9991000=(10.000025)N\frac{999}{1000} = (1 - 0.000025)^N, which means 0.999=(0.999975)N0.999 = (0.999975)^N.

Taking the natural logarithm of both sides, we have ln(0.999)=Nln(0.999975)\ln(0.999) = N \ln(0.999975). Thus, N=ln(0.999)ln(0.999975)N = \frac{\ln(0.999)}{\ln(0.999975)}.

Using a calculator, ln(0.999)0.0010005\ln(0.999) \approx -0.0010005 and ln(0.999975)0.0000250003\ln(0.999975) \approx -0.0000250003.

Therefore, N0.00100050.000025000340.019840N \approx \frac{-0.0010005}{-0.0000250003} \approx 40.0198 \approx 40.

The number of repetitions is approximately 40.