2019 A/L Physics Past Paper · Question 05 (English Medium)

Gravitational potential of a point mass — the V(r) graph

The variation of the gravitational potential V(r)V(r) due to a point mass, with distance rr is best represented by

  1. (1) Graph (1)
  2. (2) Graph (2)
  3. (3) Graph (3)
  4. (4) Graph (4)
  5. (5) Graph (5)
Answer and explanation

Answer: (2) Graph (2)

What the question asks

We want:

The graph of the potential V(r)V(r) of a point mass MM against the distance rr.

Which of the five graphs is it?

Relevant theory

The potential at a point is the work done in bringing 1 kg from infinity to that point.

At infinity V=0V = 0.

Gravity pulls. So the field does the work.

That work is negative. So V<0V < 0 at every distance.

The negative sign above indicates that the relevant work is done by the field and not against the field.

Required equations

g=GMr2g = \frac{GM}{r^2}

V(r)=−∫∞rGMr2 drV(r) = -\int_{\infty}^{r} \frac{GM}{r^2}\,dr

V(r)=−GMrV(r) = -\frac{GM}{r}

Reasoning and calculation

The graph has two axes.

Across: the distance rr from the mass.

Up: the potential V(r)V(r).

Above the zero line VV is positive. Below it VV is negative.

Start with a small rr.

V=−GMrV = -\dfrac{GM}{r}

When rr is small, VV is a large negative number.

So the curve starts far below the zero line.

Is there a place where the rule changes?

No. Outside the mass the same rule holds for every rr.

So it is one smooth curve.

Now make rr bigger.

GMr\dfrac{GM}{r} gets smaller. So VV stays negative and rises towards zero.

Double rr and ∣V∣|V| becomes half.

What happens at the two ends?

When r→0r \to 0, V→−∞V \to -\infty.

When r→∞r \to \infty, V→0V \to 0.

But VV is not zero at any fixed distance. It only gets closer and closer to zero.

How steep is the curve?

dVdr=GMr2\dfrac{dV}{dr} = \dfrac{GM}{r^2}

This is always positive. So the curve always goes up.

It is steep when rr is small. It is flat when rr is large.

Reading the options

Look at the five graphs.

Only graph (2) starts far below zero, rises steeply, then flattens and gets close to zero.

So the answer is graph (2).

Why the other options fail

The shape is right. But VV is above zero.

VV is positive and reaches zero at a finite rr.

It is negative. But it meets the axis at a finite rr.

A constant VV means no field.

Conclusion

V(r)=−GMrV(r) = -\dfrac{GM}{r}

It is always below zero. It rises towards zero as rr grows.

So the answer is graph (2).

Drawing the potential as a positive 1/r1/r curve.

Gravity always pulls. So the potential is negative.

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