Electric Potential
Electric Potential
- The “voltage” you have used since AS finally gets its full definition — the same work-from-infinity idea as gravitational potential, but with signs that matter.
The definition (two marks)
- The at a point is the work done per unit charge in moving a positive charge from infinity to the point. Split exactly there in three sessions (9702/41/O/N/23 Q5(a)) (9702/42/M/J/24 Q5(a)) (9702/41/O/N/25 Q5(a)) — keep “positive” and “from infinity”.
Symbols
- = potential at distance r from charge Q (V)
- = potential energy of two point charges Q and q (J)
- = distance from the charge (single power!) (m)
- Both formulas divide by , not — a one-marker has hung on exactly this (9702/42/F/M/23 Q4(b)(iii)). Unlike gravitational potential (always negative), takes the sign of the charge: positive charges make potential hills, negative charges make wells.
- Potential is a scalar. With several charges, add the values with their signs — no directions, no components. That is why examiners love mixing potential and field questions: one adds like numbers, the other like arrows.
Worked example
Along a hydrogen atom (2025 paper)
A proton and an electron sit 120 pm apart. Find the total potential 30 pm from the proton (9702/41/O/N/25 Q5(b)(ii)).
- Two signed contributions: .
- .
Answer
Because the charges have equal size, exactly at the midpoint — the figure's zero crossing at 60 pm.
Capacitance preview
A 2025 part chained an isolated sphere's capacitance into this lesson's formula: from , a sphere holding 83 pC at 1.2 V, then m (9702/42/O/N/25 Q6(b)). The capacitance chapter builds on exactly this .