2021 A/L Physics Past Paper · Question 47 (English Medium)

Potential energy of two conducting spheres that shared charge

A conducting sphere of radius 2r2r is given a charge of +3Q+3Q. Another uncharged conducting sphere of radius rr is touched to the first sphere and then separated by a distance rr as shown in the figure. What is the electrical potential energy of the system now? (Assume that the charge distributions of spheres are uniform and the system is in free space.)

  1. (1) Q24πε0r\dfrac{Q^2}{4\pi\varepsilon_0 r}
  2. (2) Q28πε0r\dfrac{Q^2}{8\pi\varepsilon_0 r}
  3. (3) Q216πε0r\dfrac{Q^2}{16\pi\varepsilon_0 r}
  4. (4) 3Q28πε0r\dfrac{3Q^2}{8\pi\varepsilon_0 r}
  5. (5) 3Q216πε0r\dfrac{3Q^2}{16\pi\varepsilon_0 r}
Answer and explanation

Answer: (2) Q28πε0r\dfrac{Q^2}{8\pi\varepsilon_0 r}

Given information

We know:

The big sphere has radius 2r2r and charge +3Q+3Q. The small sphere has radius rr and no charge.

They are touched, then moved apart. The surfaces are then rr apart. The system is in free space.

What the question asks

We want: the electrical potential energy of the two spheres after they are apart.

The plan: first share the charge between the spheres, then find the distance between the centres, then use the energy of a pair of charges.

Relevant theory

When the two spheres are connected by a conductor they reach the same potential V

It is known that in this case, with respect to point P, the charge Q on the sphere acts as if it were concentrated at the centre of the sphere.

The total potential energy of a system consisting of a number of charges would be the sum of the potential energies of all positive pairs of charges in the system.

Required equations

V1=V2V_1 = V_2

V=14πε0qRV = \dfrac{1}{4\pi\varepsilon_0}\dfrac{q}{R}

U=14πε0q1q2dU = \dfrac{1}{4\pi\varepsilon_0}\dfrac{q_1q_2}{d}

Applying it to this question

q1=2q2q_1 = 2q_2

QQ

q2=3Q3q_2 = \dfrac{3Q}{3}

2Q2Q

q1=3Q−Qq_1 = 3Q - Q

4r4r

d=2r+r+rd = 2r + r + r

Q28πε0r\dfrac{Q^2}{8\pi\varepsilon_0 r}

U=14πε02Q×Q4rU = \dfrac{1}{4\pi\varepsilon_0}\dfrac{2Q \times Q}{4r}

Q2ε0r\dfrac{Q^2}{\varepsilon_0 r} has units C2C2 N−1m−2 m=N m=J\dfrac{\text{C}^2}{\text{C}^2\,\text{N}^{-1}\text{m}^{-2}\ \text{m}} = \text{N m} = \text{J}. So the answer is an energy.

Reasoning and calculation

The charge is shared as 2Q2Q and QQ. The centres are 4r4r apart.

The spheres are uniform, so each acts like a point charge at its centre. The energy of the pair is Q28πε0r\dfrac{Q^2}{8\pi\varepsilon_0 r}. This is option (2).

Checks

(a∗b)/d(a * b) / d

Does it make sense?

Both spheres are positive, so they repel, and the energy is positive.

Charge was only shared, never made: 2Q+Q=3Q2Q + Q = 3Q. The distance is between the centres, not between the surfaces.

Conclusion

U=14πε0q1q2d=Q28πε0rU = \dfrac{1}{4\pi\varepsilon_0}\dfrac{q_1q_2}{d} = \dfrac{Q^2}{8\pi\varepsilon_0 r}

The charges are 2Q2Q and QQ, and the centres are 4r4r apart.

U=14πε02Q×Q4r=Q28πε0rU = \dfrac{1}{4\pi\varepsilon_0}\dfrac{2Q \times Q}{4r} = \dfrac{Q^2}{8\pi\varepsilon_0 r}. The answer is (2).

Touching conductors reach the same potential, so the charge is shared in the ratio of the radii.

For the energy, measure the distance from centre to centre.

Exam tip

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