Skip to main content
WalesPhysicsSyllabus dot point

How are electric and gravitational fields alike, and how do field strength and potential vary with distance?

Coulomb's law and Newton's law of gravitation, electric and gravitational field strength and potential, and the inverse-square nature of both fields.

A focused answer to WJEC A-Level Physics Unit 4 electrostatic and gravitational fields, covering Coulomb's law and Newton's law of gravitation, electric and gravitational field strength and potential, and the inverse-square nature shared by both fields.

Generated by Claude Opus 4.811 min answer

Reviewed by: AI editorial process; not yet individually human-reviewed

Have a quick question? Jump to the Q&A page

Jump to a section
  1. What this dot point is asking
  2. The answer
  3. Examples in context
  4. Try this

What this dot point is asking

WJEC wants you to apply Coulomb's law and Newton's law of gravitation, define and use electric and gravitational field strength and potential, and recognise the shared inverse-square structure of the two fields. The parallel between the two fields is one of the most elegant ideas in the course, and the examiners reward students who can map a result from one field onto the other.

The answer

The two force laws

Both are inverse-square laws with the same mathematical form. Gravity is always attractive; the electric force can be attractive or repulsive. The constants differ enormously in strength: gravity is extraordinarily weak between everyday objects, which is why we only notice it when one mass is planet-sized.

Field strength

Potential

The change in potential energy moving between two points is charge (or mass) times the potential difference.

Examples in context

Example 1. An ink-jet printer. Tiny ink droplets are given a charge and then deflected by a uniform electric field between two plates, where the field strength E=F/QE = F/Q determines the sideways force on each drop. Varying the charge steers each droplet to the right spot on the page. The same field concept that describes a point charge governs this everyday device.

Example 2. Weighing the Earth. Because g=GM/r2g = GM/r^2 at the surface, measuring the known g=9.81N kg1g = 9.81\,\text{N kg}^{-1} together with the Earth's radius lets you solve for the mass MM of the Earth. This is how the planet's mass of about 6×1024kg6 \times 10^{24}\,\text{kg} is found without ever placing it on a scale, using only the inverse-square gravitational field.

Try this

Q1. Two charges of +2.0μC+2.0\,\mu\text{C} and +3.0μC+3.0\,\mu\text{C} are 0.10m0.10\,\text{m} apart. Find the force between them. Take 14πε0=9.0×109N m2C2\frac{1}{4\pi\varepsilon_0} = 9.0\times10^9\,\text{N m}^2\text{C}^{-2}. [3 marks]

  • Cue. F=9.0×109×2.0×106×3.0×1060.102=5.4NF = \frac{9.0\times10^9\times2.0\times10^{-6}\times3.0\times10^{-6}}{0.10^2} = 5.4\,\text{N} (repulsive).

Q2. State one similarity and one difference between gravitational and electric fields. [2 marks]

  • Cue. Both are inverse-square fields; gravity is always attractive while the electric force can attract or repel.

Exam-style practice questions

Practice questions written in the style of WJEC exam questions on this dot point, with worked answer explainers. The year tag is the paper they imitate, not the source.

WJEC 20205 marksCalculate the gravitational field strength at the surface of the Earth, given its mass 6.0×1024kg6.0 \times 10^{24}\,\text{kg} and radius 6.4×106m6.4 \times 10^{6}\,\text{m}. Take G=6.67×1011N m2kg2G = 6.67 \times 10^{-11}\,\text{N m}^2\,\text{kg}^{-2}. Hence determine the gravitational potential at the surface.
Show worked answer →

Field strength from g=GM/r2g = GM/r^2:

g=6.67×1011×6.0×1024(6.4×106)2=4.0×10144.1×1013=9.8N kg1g = \dfrac{6.67 \times 10^{-11} \times 6.0 \times 10^{24}}{(6.4 \times 10^{6})^2} = \dfrac{4.0 \times 10^{14}}{4.1 \times 10^{13}} = 9.8\,\text{N kg}^{-1}.

This matches the familiar gg at the surface.

Gravitational potential from V=GM/rV = -GM/r:

V=6.67×1011×6.0×10246.4×106=6.3×107J kg1V = -\dfrac{6.67 \times 10^{-11} \times 6.0 \times 10^{24}}{6.4 \times 10^{6}} = -6.3 \times 10^{7}\,\text{J kg}^{-1}.

Markers reward the field from the inverse-square law giving 9.8N kg19.8\,\text{N kg}^{-1}, and the negative potential from V=GM/rV = -GM/r.

WJEC 20183 marksState two similarities and one difference between the electric field of a point charge and the gravitational field of a point mass.
Show worked answer →

Similarity one: both field strengths obey an inverse-square law with distance, E1/r2E \propto 1/r^2 and g1/r2g \propto 1/r^2.

Similarity two: both potentials vary as 1/r1/r from the source, and both fields are radial, pointing along the line joining to the source.

Difference: the gravitational force is always attractive, whereas the electric force between charges can be attractive or repulsive depending on the signs of the charges. Markers reward two genuine structural similarities and the attractive-only nature of gravity as the difference.

Related dot points

Sources & how we know this