2022 A/L Physics Past Paper · Question 25 (English Medium)

Speed of a ball that just touches the top of a circular track

A ball released at point AA travels on a frictionless track as shown in the figure. Then the ball just touches point BB on the inner surface of the circular part of the track of radius RR. What is the velocity of the ball at point BB?

  1. (1) 00
  2. (2) gR\sqrt{gR}
  3. (3) 2gR2\sqrt{gR}
  4. (4) 5gR\sqrt{5gR}
  5. (5) 4gR4\sqrt{gR}
Answer and explanation

Answer: (2) gR\sqrt{gR}

Given information

What we know:

The track is frictionless. The circular part has radius RR, and BB is the highest point of the circle.

At BB the ball is on the inner surface of the track, so the track pushes it towards the centre of the circle, which is downwards.

"Just touches" means the ball only touches the track. It does not press on it, so the force from the track is N=0N = 0.

The question gives no numbers. So we keep symbols, and check with sample values g=10 m s−2g = 10\ \text{m s}^{-2} and R=0.4 mR = 0.4\ \text{m}.

What the question asks

We want: the speed vv of the ball at the point BB.

What each letter means:

mm (kg\text{kg}): the mass of the ball.

RR (m\text{m}): the radius of the circular part.

vv (m s−1\text{m s}^{-1}): the speed of the ball at BB.

NN (N\text{N}): the force the track exerts on the ball at BB.

gg (m s−2\text{m s}^{-2}): the acceleration due to gravity.

Relevant theory

Since a body is moving with an acceleration only under the action of an external force, a body performing circular motion is doing so under the action of an external force acting in the direction of the centripetal acceleration. This force is thus known as "centripetal force" and is given by. F=maF = ma F=mv2r=mrω2F = \frac{mv^2}{r} = mr\omega^2

For example, swing a bucket of water round in a vertical circle. At the top the water stays in the bucket if the bucket moves fast enough. Swing it just slowly enough and the bucket stops pressing on the water at the top. The weight of the water alone is then exactly what keeps it on the circle. That is the slowest swing that still goes round.

At BB two forces point towards the centre: the weight mgmg and the push NN of the track. Together they supply the centripetal force.

mg+N=mv2Rmg + N = \dfrac{mv^2}{R}

In words: the two forces towards the centre add up to mv2R\dfrac{mv^2}{R}.

The ball just touches, so N=0N = 0.

mg=mv2Rmg = \dfrac{mv^2}{R}

In words: the weight alone supplies the centripetal force.

Required equations

mg+N=mv2Rmg + N = \dfrac{mv^2}{R}

N=0N = 0

v=gRv = \sqrt{gR}

Applying it to this question

m s−2×m=m s−1\sqrt{\text{m s}^{-2} \times \text{m}} = \text{m s}^{-1}, which is a speed. The mass mm cancels, so the answer does not depend on it.

1010

a=v2R=ga = \dfrac{v^2}{R} = g

44

v2=gR=10×0.4v^2 = gR = 10 \times 0.4

22

v=gR=4v = \sqrt{gR} = \sqrt{4}

Reasoning and calculation

The speed does not depend on the mass of the ball. It depends only on gg and RR.

So the speed at BB is v=gRv = \sqrt{gR}. That is option (2).

Checks

v∗v/rv * v / r

Does it make sense?

At this speed the acceleration towards the centre equals gg, exactly what the weight alone can give.

A smaller speed would need less than gg. The ball would drop away from the track. A larger speed would need more than gg, and the track would have to push on the ball.

Conclusion

v=gRv = \sqrt{gR}

At BB the weight alone supplies the centripetal force, so mg=mv2Rmg = \dfrac{mv^2}{R} and v=gRv = \sqrt{gR}.

The answer is (2).

"Just touches" means the force from the track is zero. Only the weight is left to supply the centripetal force.

Put mg=mv2Rmg = \dfrac{mv^2}{R} at the top of the circle.

Exam tip

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