A2 · Practice questions · Gravitational potential

Zero at infinity, so every value is negative.

Six original Cambridge-style questions on the definition of gravitational potential, φ = −GM / r, potential energy E = −GMm / r and the energy needed to move a mass in a field.

Original questions All questions on this page are original work, written in the Cambridge AS & A Level style. They are not from past papers. They test the same concepts and skills the syllabus rewards.
Keep these straight

Potential is work per unit mass from infinity.

01
Analysis
[2 marks]

State the difference between gravitational potential and gravitational potential energy, and give the SI unit of each.

  • Gravitational potential is the work done per unit mass in bringing a small test mass from infinity to the point; it is a property of the point in the field, with unit J kg⁻¹. ✓
  • Gravitational potential energy is the work done in bringing a particular mass m from infinity to the point, E = mφ, so it depends on the mass as well as the point; its unit is the joule, J. ✓
02
Calculation
[3 marks]

The Earth has mass 6.0 × 10²⁴ kg and radius 6.4 × 10⁶ m. Calculate the gravitational potential at the Earth's surface, and hence the minimum energy needed to move a probe of mass 2400 kg from the surface to a point very far from the Earth.

  • φ = −GM / R = −(6.67 × 10⁻¹¹ × 6.0 × 10²⁴) / 6.4 × 10⁶ = −6.25 × 10⁷ J kg⁻¹. ✓
  • The potential at a very large distance is zero, so each kilogram must gain 6.25 × 10⁷ J of potential energy to get there. ✓
  • Minimum energy = mΔφ = 2400 × 6.25 × 10⁷ = 1.5 × 10¹¹ J. ✓
03
Calculation
[3 marks]

A meteoroid starts from rest at a very large distance from the Moon and falls freely onto the Moon's surface. The Moon has mass 7.35 × 10²² kg and radius 1.74 × 10⁶ m, and it has no atmosphere. Calculate the speed of the meteoroid as it reaches the surface.

  • Change in potential from infinity to the surface: Δφ = 0 − (−GM / R) = GM / R = (6.67 × 10⁻¹¹ × 7.35 × 10²²) / 1.74 × 10⁶ = 2.82 × 10⁶ J kg⁻¹. ✓
  • The potential energy lost per kilogram becomes kinetic energy per kilogram: ½v² = 2.82 × 10⁶. ✓
  • v = √(2 × 2.82 × 10⁶) = 2.4 × 10³ m s⁻¹. ✓
04
Analysis
[3 marks]

A student says that a space probe moving away from a planet "loses potential energy, because the potential gets smaller as the distance increases". Explain the error in this statement.

  • The potential φ = −GM / r is negative; as r increases its magnitude falls but its value rises toward zero, so the potential increases, not decreases. ✓
  • The potential energy E = mφ = −GMm / r therefore also becomes less negative, which is an increase in potential energy. ✓
  • This is consistent with work having to be done on the probe against the attractive field to move it outward; the probe gains, not loses, potential energy. ✓
05
Calculation
[2 marks]

Planet X has twice the mass and twice the radius of planet Y. Determine the ratio of the gravitational potential at the surface of X to that at the surface of Y, and state whether the surface field strengths are also in this ratio.

  • φ = −GM / R, so φX / φY = (2M / 2R) / (M / R) = 1: the surface potentials are equal. ✓
  • No: g = GM / R² gives gX / gY = 2 / 4 = ½, because potential depends on 1 / R but field strength on 1 / R². ✓
06
Calculation
[4 marks]

The Earth has mass 6.0 × 10²⁴ kg and radius 6.4 × 10⁶ m. A probe of mass 1500 kg is moved from the Earth's surface to a distance of 2.0 × 10⁷ m from the Earth's centre.

(a) Calculate the gravitational potential at the Earth's surface. (b) Calculate the gravitational potential at 2.0 × 10⁷ m from the centre. (c) Calculate the increase in gravitational potential energy of the probe. (d) Explain why using E = mgh with g = 9.81 m s⁻² would give a much larger, and incorrect, answer.

  • (a) φ1 = −GM / R = −(6.67 × 10⁻¹¹ × 6.0 × 10²⁴) / 6.4 × 10⁶ = −6.25 × 10⁷ J kg⁻¹. ✓
  • (b) φ2 = −GM / r = −4.00 × 10¹⁴ / 2.0 × 10⁷ = −2.0 × 10⁷ J kg⁻¹. ✓
  • (c) ΔE = m(φ2 − φ1) = 1500 × (−2.0 × 10⁷ + 6.25 × 10⁷) = 1500 × 4.25 × 10⁷ = 6.4 × 10¹⁰ J. ✓
  • (d) E = mgh assumes g is constant over the height h = 1.36 × 10⁷ m, giving 2.0 × 10¹¹ J, but g falls as 1 / r² and is only about 1 N kg⁻¹ at the far end, so the true work done is much less. ✓

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