D.2.13 (HL)—Electric potential as scalar

Syllabus
First assessment 2025
Objective
Level
HL

Treat Electric Potential as a Scalar

HL only

Define electric potential

Electric potential VeV_e at a point is the work done per unit positive test charge in bringing it from infinity to that point. Its unit is JC1\mathrm{J\,C^{-1}}, equivalent to volts. Set Ve=0V_e=0 at infinity.

Add potentials algebraically

Electric potential is a scalar, so contributions from several point charges add with their signs:
Ve=ikQiriV_e=\sum_i k\frac{Q_i}{r_i}
There is no vector-angle calculation when combining potential values.

Interpret the result

A positive source contributes positive potential and a negative source contributes negative potential. A point can have zero net potential because positive and negative contributions cancel, even though the electric field there is not necessarily zero.

Common trap

Do not add electric field magnitudes as though they were scalar, and do not infer zero electric field from zero potential. Potential and field are different quantities.

D.2.13 (HL) Exam Analysis

HL only

Assessment in practice

1–2 marks
How it is assessed

Questions define potential or determine whether a point’s net potential is zero from several source charges.

Command terms

Outline

What earns marks

Define potential per unit charge with zero at infinity, add source contributions algebraically, and keep potential distinct from vector field strength.

Watch for

Confusing scalar potential with vector field strength, or omitting “per unit positive test charge” from the definition.

Representative question

Question 1

[Maximum number: 2]

Outline, without calculation, whether or not the electric potential at P is zero.

Retrieve the HL D.2 Electric and Magnetic Fields Model

HL only

The HL extension is secure when you can connect electric energy, potential and field geometry.

  • Electric potential energy is assembly work from infinity
  • Ep=kq1q2/r and Ve=kQ/r are signed/scalar quantities
  • E=−ΔVe/Δr and W=qΔVe require careful sign conventions
  • Equipotentials have constant potential and zero work along them
  • Electric field lines cross equipotentials at right angles