2020 A/L Physics Past Paper · Question 28 (English Medium)

A free charged sphere on a smooth table — its path

As shown in the figure, three small conducting spheres carrying charges +Q,−Q,+Q+Q, -Q, +Q are placed at the corners of an equilateral triangle ABCABC on a smooth horizontal surface. The spheres at BB and CC are fixed, while the sphere at AA is free to move. Which of the following best represents the possible path of the sphere at AA?

  1. (1) aa
  2. (2) bb
  3. (3) cc
  4. (4) dd
  5. (5) ee
Answer and explanation

Answer: (3) cc

What the question asks

We must find: the path the +Q+Q sphere at A can follow on the smooth table, starting from rest.

Relevant theory

Like charges (+, + and -, -) repel each other while unlike charges (+, -) attract each other.

The mutual force between two point electric charges is directly proportional to the product of the two charges and inversely proportionatel to the square of the distance between them

The direction of the unbalanced (resultant) force is the same as the direction of the momentum change.

Applying it to this question

Direction convention: in the figure BCBC is horizontal.

The direction from CC towards BB is "left", the direction from BCBC towards AA is "up".

A is the top vertex of the triangle; AB=AC=aAB = AC = a.

Vectors: two forces act on A.

The attraction F⃗B\vec F_B from the −Q-Q at B (from A towards B).

The repulsion F⃗C\vec F_C from the +Q+Q at C (from C towards A, continuing outward).

Since the table is smooth and horizontal, these alone determine the motion.

Reasoning and calculation

Direction rule: both forces are from charges of equal magnitude QQ at the same distance aa.

So FB=FC=kQ2a2=FF_B = F_C = \dfrac{kQ^2}{a^2} = F.

F⃗B\vec F_B is 60∘60^\circ below horizontal, towards the left.

F⃗C\vec F_C is 60∘60^\circ above horizontal, towards the left.

The vertical components Fsin⁡60∘F\sin 60^\circ cancel each other.

Fx=Fcos⁡60∘+Fcos⁡60∘F_x = F\cos 60^\circ + F\cos 60^\circ

Fx=2F×12=FF_x = 2F \times \frac{1}{2} = F

Fy=Fsin⁡60∘−Fsin⁡60∘=0F_y = F\sin 60^\circ - F\sin 60^\circ = 0

Fnet=kQ2a2 (left, horizontal)F_{net} = \frac{kQ^2}{a^2}\ \text{(left, horizontal)}

Eventual direction: starting from rest, the first velocity is in the direction of the resultant — horizontally left.

As A moves left, ABAB shrinks and ACAC grows.

FB∝1AB2F_B \propto \dfrac{1}{AB^2} grows, FCF_C shrinks, so a downward component develops.

Since the velocity turns towards the force, the path starts horizontal and gradually curves downward.

Reading the options

Comparing with the diagram's paths: only path cc starts horizontal and curves downward — option (3).

Why the other options fail

Curves upward.

Assumes the force direction stays fixed.

Considers only B's attraction.

Moves downward right from the start.

Checks

0.5∗QB−0.5∗QC0.5 * QB - 0.5 * QC

Second way (a limiting case): if B also had +Q+Q, the horizontal components of both repulsions would cancel, and A would be pushed straight upward.

Flipping one sign turns the resultant 90∘90^\circ to point left — matching our result.

Also, paths that move away from A's starting direction (dd, ee) are impossible for an object starting from rest.

Conclusion

At the start the resultant kQ2a2\dfrac{kQ^2}{a^2} points horizontally left; as A moves, B's attraction grows and the force turns downward: path cc — the answer is (3).

Assuming an object moves straight along a force line, or in the direction of the force forever.

A force changes velocity; the velocity turns slowly towards the force. Only when starting from rest is the initial direction the direction of the force.

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