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How much work is needed to move a charge through an electric field, and how does this compare with gravity?

Absolute electric potential and potential energy in a radial field, the potential gradient, equipotentials, and the work done moving a charge.

A focused answer to AQA A-Level Physics 3.7.3.3, covering absolute electric potential in a radial field, electric potential energy, the potential gradient and its link to field strength, equipotentials, and the work done moving a charge.

Generated by Claude Opus 4.89 min answer

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

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  1. What this dot point is asking
  2. Electric potential
  3. Electric potential energy
  4. Potential gradient and field strength
  5. Equipotentials
  6. Try this

What this dot point is asking

AQA specification point 3.7.3.3 wants you to define absolute electric potential, calculate it in a radial field, relate the potential gradient to field strength, describe equipotential surfaces, and calculate the work done moving a charge.

Electric potential

The potential is positive around a positive charge (work must be done against repulsion to bring a positive test charge in) and negative around a negative charge (the test charge is attracted, so work is done by the field). The zero of potential is taken at infinity, where the charges are infinitely far apart and no longer interact. Note the 1r\dfrac{1}{r} dependence: potential falls off more slowly than the field, which falls as 1r2\dfrac{1}{r^2}.

Electric potential energy

The potential energy of a charge qq at a point of potential VV is the energy stored by virtue of its position in the field:

This work is independent of the path taken between the two points (the electric force is conservative), so only the start and end potentials matter.

Potential gradient and field strength

Field strength is the negative potential gradient: the field points in the direction of decreasing potential, from high to low. The steeper the potential changes with distance, the stronger the field. This is why field lines are closely spaced where the potential changes rapidly. In a uniform field the potential changes linearly, giving E=VdE = \dfrac{V}{d} as a special case.

Equipotentials

The spacing of equally-spaced equipotentials reveals the field strength: closely spaced equipotentials mean a steep potential gradient and a strong field.

Try this

Q1. State the relationship between electric field strength and electric potential. [1 mark]

  • Cue. Field strength is the negative potential gradient, E=ΔVΔrE = -\dfrac{\Delta V}{\Delta r}.

Q2. Calculate the work done moving a charge of +3.0 nC+3.0 \text{ nC} through a potential difference of 500 V500 \text{ V}. [2 marks]

  • Cue. W=qΔV=3.0×109×500=1.5×106 JW = q\Delta V = 3.0 \times 10^{-9} \times 500 = 1.5 \times 10^{-6} \text{ J}.

Q3. State where the zero of electric potential is taken. [1 mark]

  • Cue. At infinity.

Exam-style practice questions

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

AQA 20194 marksAn isolated metal sphere of radius 5.0 cm5.0 \text{ cm} carries a charge of +8.0 nC+8.0 \text{ nC}. Calculate the electric potential at its surface. Take 14πε0=8.99×109 N m2 C2\dfrac{1}{4\pi\varepsilon_0} = 8.99 \times 10^9 \text{ N m}^2 \text{ C}^{-2}.
Show worked answer →

Outside (and at the surface of) a charged sphere the field and potential are those of a point charge at its centre, so use V=14πε0QrV = \dfrac{1}{4\pi\varepsilon_0}\dfrac{Q}{r} with rr the radius.

V=(8.99×109)8.0×1095.0×102=(8.99×109)(1.6×107)V = (8.99 \times 10^9)\dfrac{8.0 \times 10^{-9}}{5.0 \times 10^{-2}} = (8.99 \times 10^9)(1.6 \times 10^{-7}).

V=1.4×103 VV = 1.4 \times 10^{3} \text{ V}, positive because the charge is positive.

Markers reward treating the sphere as a point charge at its surface, conversion to SI units, and a positive answer.

AQA 20213 marksDefine an equipotential surface and explain why no work is done when a charge moves along it.
Show worked answer →

An equipotential surface joins all points that are at the same electric potential.

The work done moving a charge between two points is W=qΔVW = q\Delta V. Along an equipotential the potential does not change, so ΔV=0\Delta V = 0 and therefore W=0W = 0.

Equivalently, equipotentials are always perpendicular to the field lines, so a charge moving along one has no component of the electric force in its direction of motion.

Markers reward defining the surface by constant potential and linking zero work to ΔV=0\Delta V = 0 (or to motion perpendicular to the field).

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