D.1.4—Gravitational field strength

Syllabus
First assessment 2025
Objective
Level
SL

Calculate Gravitational Field Strength

Define the field

Gravitational field strength is force per unit test mass. For a point or spherical source of mass MM, it depends on distance rr from the source centre. It is a vector directed toward the source, with unit Nkg1\mathrm{N\,kg^{-1}}, numerically equivalent to ms2\mathrm{m\,s^{-2}}.

g=\frac{F}{m}=\frac{GM}{r^2}

Worked example — surface field

For M=4.87×1024kgM=4.87\times10^{24}\,\mathrm{kg} and r=6.05×106mr=6.05\times10^6\,\mathrm{m}, g=(6.67×1011)(4.87×1024)/(6.05×106)2=8.87Nkg1g=(6.67\times10^{-11})(4.87\times10^{24})/(6.05\times10^6)^2=8.87\,\mathrm{N\,kg^{-1}}. The result is the force per kilogram at the surface, directed inward.

Read the scaling

At a fixed distance, gg is proportional to MM. At a fixed source mass, doubling rr reduces gg to one quarter. The field direction is toward the source mass; the scalar expression gives the magnitude. Near a surface, the weight of a mass mm is W=mgW=mg.

Common trap

Do not use the object’s own mass in g=GM/r2g=GM/r^2 as MM, and do not use altitude alone for rr: use distance from the source centre.

D.1.4 Exam Analysis

Assessment in practice

1–2 marks
How it is assessed

Questions calculate weight near an asteroid or compare surface field strengths when source masses and radii change.

Command terms

Calculate / What is

What earns marks

Identify the source mass M and centre-to-point distance r, apply g=GM/r² for magnitude, include the direction toward the source, and use W=mg only when calculating a test object’s weight.

Watch for

Using the test mass in place of source mass M, or scaling g with radius rather than inverse-square radius.

Representative question

Question 1

[Maximum number: 1]

State the SI unit for gravitational field strength.

Retrieve the Core D.1 Gravitational Fields Model

D.1 core gravitational fields is secure when you can connect source mass, distance and field representation.

  • Kepler’s three laws describe orbital geometry and period
  • F=Gm1m2/r² for point-mass interactions
  • Point-mass approximation requires suitable size or symmetry conditions
  • g=F/m=GM/r² is a vector field strength
  • Field lines point toward mass and spread as the field weakens