Question
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=1.0 m is charged to a potential Vi=1000 V. A thin metal disc of radius r=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=999 V. Approximately how many times has this process been repeated?

10
20
30
40
40
Solution
Let R be the radius of the sphere and r be the radius of the disc. The capacitance of the conducting sphere is Cs=4πϵ0R.
Let Vn be the potential of the sphere after the n-th repetition of the process. Initially, the potential of the sphere is V0=Vi=1000 V.
When the disc is touched to the sphere, it samples the potential at the contact point. The charge transferred ΔQ is proportional to the potential V and can be expressed as ΔQ=C′V, where C′ is an effective capacitance.
The potential of the sphere after one contact is V′=CsQ−ΔQ=V−CsΔQ=V−CsC′V=V(1−CsC′). Thus, each contact reduces the potential by a factor of (1−CsC′).
After N repetitions, the potential is Vf=Vi(1−CsC′)N.
We have Vi=1000 V and Vf=999 V, so 1000999=(1−CsC′)N.
The key is to estimate CsC′. The charge density on the sphere is σ=4πR2Q=4πR2CsV=4πR24πϵ0RV=Rϵ0V.
The charge transferred to the disc might be proportional to its area multiplied by the charge density. So ΔQ∼σ×(area of disc)=Rϵ0V×(πr2). Thus, C′V∼Rϵ0Vπr2, which gives C′∼Rϵ0πr2.
Then CsC′∼4πϵ0Rϵ0πr2/R=4R2r2.
Given R=1.0 m and r=0.01 m, we have CsC′=4(1)2(0.01)2=40.0001=0.000025.
So, 1000999=(1−0.000025)N, which means 0.999=(0.999975)N.
Taking the natural logarithm of both sides, we have ln(0.999)=Nln(0.999975). Thus, N=ln(0.999975)ln(0.999).
Using a calculator, ln(0.999)≈−0.0010005 and ln(0.999975)≈−0.0000250003.
Therefore, N≈−0.0000250003−0.0010005≈40.0198≈40.
The number of repetitions is approximately 40.