Gravitational fields

Physics · Fields. The idea in plain words, the rules to remember, the mistake to avoid and a worked example, written and checked by Mega Lecture.

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The idea

Every mass attracts every other mass. Newton's law says the force between two point masses is proportional to the product of the masses and inversely proportional to the square of the distance between them. A uniform sphere acts as if all its mass were at its centre, so distances are measured from centre to centre.

Gravitational field strength g at a point is the force per unit mass on a small test mass placed there. Field lines show the direction of this force. Around a sphere they are radial and point inwards. Near the surface they are parallel and equally spaced.

Kepler's laws describe orbits. For a circular orbit, gravity provides the centripetal force.

Rules to remember

Common mistake

Students use the height above the surface as r. The distance r is measured from the centre of the planet, so a height of one radius above the surface means r = 2R and g falls to one quarter, not one half.

Worked example

A planet has mass 6.4 × 1023 kg and radius 3.4 × 106 m. What is the gravitational field strength at its surface? (G = 6.67 × 10−11 N m² kg−2)

  1. Use g = GM ÷ r², with r equal to the radius of the planet.
  2. GM = 6.67 × 10−11 × 6.4 × 1023 = 4.27 × 1013.
  3. r² = (3.4 × 106)² = 1.156 × 1013 m².
  4. g = (4.27 × 1013) ÷ (1.156 × 1013) = 3.7 N kg−1.

Answer: 3.7 N kg−1

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