Revision Notes
OCR A Level Physics A: Electric fields, Coulomb's law, potential and uniform fields (H556) – Revision Notes
Condensed formulae, methods, distinctions and a self-test on Coulomb's law, uniform fields, potential and energy for OCR A Level Physics A (H556).
- Subject
- Physics
- Level
- A LEVELS
- Topic
- Electric fields, Coulomb's law, potential and uniform fields
- Author
- Marlbridge Academic Team
- Updated
Aligned to OCR A Level Physics (H556), Version 3.0 (March 2026), for first assessment in 2017. Official specification .
Syllabus page (what it covers and how it is assessed): OCR A Level Physics.
Syllabus points this page covers
H556
- 6.2 Electric fields
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Condensed notes for section 6.2 (Electric fields) of OCR A Level Physics A (H556), Version 3.0 (March 2026), first assessment 2017. Use the full study guide for explanations and worked examples, then try the practice questions. Links: OCR A Level Physics hub, printable checklist and free diagnostics.
Definitions
- Electric field strength, E: force per unit positive charge, E = F/q. Unit N C⁻¹ (= V m⁻¹). A vector; direction of the force on a positive charge. (6.2.1(d))
- Field line: a line whose tangent gives the direction of the force on a small positive charge. Lines start on positive, end on negative; closer lines mean a stronger field; lines never cross. (6.2.1(c))
- Electric potential at a point: work done bringing unit positive charge from infinity to that point. Zero at infinity. Scalar. Unit V = J C⁻¹. (6.2.4(a))
- Permittivity, ε: property of the material between plates, ε = εᵣε₀. Relative permittivity εᵣ is at least 1. (6.2.3(b))
- Point-charge model: a uniformly charged sphere acts, for points outside, as if its charge were at its centre. (6.2.1(b))
Formulae
| Result | Equation | Spec |
|---|---|---|
| Field strength | E = F/q | 6.2.1(d) |
| Coulomb’s law | F = Qq/(4πε₀r²) | 6.2.2(a) |
| Field of a point charge | E = Q/(4πε₀r²) | 6.2.2(b) |
| Uniform field | E = V/d | 6.2.3(a) |
| Capacitor, vacuum or air | C = ε₀A/d | 6.2.3(b) |
| Capacitor with material | C = εA/d, ε = εᵣε₀ | 6.2.3(b) |
| Potential of a point charge | V = Q/(4πε₀r) | 6.2.4(b) |
| Isolated sphere | C = 4πε₀R | 6.2.4(c) |
| Potential energy | E_p = Vq = Qq/(4πε₀r) | 6.2.4(e) |
Data used in the examples: ε₀ = 8.85 × 10⁻¹² F m⁻¹; elementary charge 1.60 × 10⁻¹⁹ C; masses of electron (9.11 × 10⁻³¹ kg) and proton (1.67 × 10⁻²⁷ kg).
Methods in steps
Force between two charges
- Convert units (nC to 10⁻⁹ C, cm to m).
- Use the sizes of Q and q in F = Qq/(4πε₀r²).
- State direction in words: repel (like), attract (unlike).
Field from two charges at a point
- Find the size and direction of each field separately.
- Add as vectors: along a line, subtract if opposite directions; at right angles, use Pythagoras.
- Zero-field point between like charges: equate Q₁/x² and Q₂/(d − x)².
Charged particle in a uniform field
- E = V/d, F = qE, a = F/m.
- Along the field from rest: qV = ½mv².
- Entering across the field: horizontal speed constant, time t = length/speed, sideways displacement y = ½at².
Work done and potential energy
- V = Q/(4πε₀r) at each radius, keeping the sign of Q.
- W = qΔV (or the change in Qq/(4πε₀r)).
- Positive work done on the charge when like charges are pushed together.
Must-know distinctions
| Compare | Point or spherical charge | Parallel plates |
|---|---|---|
| Field pattern | radial lines | parallel, evenly spaced lines |
| Field strength | E ∝ 1/r², varies with r | E = V/d, same at every point in the gap |
| Equation | E = Q/(4πε₀r²) | E = V/d |
| Compare | Gravitational | Electric |
|---|---|---|
| Force | F = Gm₁m₂/r², always attractive | F = Qq/(4πε₀r²), attractive or repulsive |
| Field strength | force per unit mass | force per unit charge |
| Common ground | inverse square of distance, radial field, potential zero at infinity | same |
Field E and potential V: E is a vector, V is a scalar. Add fields with direction; add potentials as numbers with signs.
Fields as forms of field (6.2.2(d)): gravitational, electric and magnetic fields each give rise to a force on the right kind of object. Link to section 5.4 and, for magnetic, section 6.3.
Area under a force-distance graph (6.2.4(d)): work done moving the charge between the two distances. Estimate by trapezia (over-estimates on this curve) or squares.
Worked reminders
Isolated sphere derivation: V = Q/(4πε₀R) at the surface, C = Q/V, so C = 4πε₀R. For R = 0.10 m, C = 1.1 × 10⁻¹¹ F.
Dielectric: inserting material with εᵣ = 2.5 raises C by a factor 2.5. Plates of area 5.0 × 10⁻³ m² and gap 1.0 mm: C = 4.4 × 10⁻¹¹ F (air), 1.1 × 10⁻¹⁰ F with material.
Potential energy sign: two protons 1.0 × 10⁻¹⁴ m apart store e²/(4πε₀r) = 2.3 × 10⁻¹⁴ J, positive because they repel.
Fields from two opposite charges: +4.0 nC and −4.0 nC, 0.10 m apart. At the midpoint each charge is 0.050 m away and each gives E = 1.44 × 10⁴ N C⁻¹. Both point towards the negative charge, so they add: 2.9 × 10⁴ N C⁻¹. Between like charges at the midpoint they would cancel.
Uniform field and an electron: plates 1.8 cm apart with 450 V. E = 450/0.018 = 2.5 × 10⁴ V m⁻¹, F = eE = 4.0 × 10⁻¹⁵ N, and a = F/m = 4.4 × 10¹⁵ m s⁻², directed towards the positive plate (opposite to E).
V against r: for a +6.0 nC point charge V = 270 V at 0.20 m and 135 V at 0.40 m. Doubling r halves V (V ∝ 1/r) but quarters E (E ∝ 1/r²).
Graph and diagram reminders
- Radial field of a positive point charge: straight lines directed outwards, equally spaced around the charge; lines get further apart as r increases.
- Two opposite charges: curved lines from the positive to the negative charge; none cross.
- Two charged plates: parallel lines at right angles to the plates in the middle; draw them bending outwards near the edges.
- F against r (point charge): a curve that falls steeply then flattens, never touching the axis. Doubling r quarters F.
- V against r (positive charge): a similar but less steep curve, V ∝ 1/r. For a negative charge V is negative and rises towards zero at infinity.
Links to other sections
- Section 3.1 to 3.3 (motion, forces, Newton’s laws): a charged particle in a uniform field has constant force, so use constant-acceleration equations and resolve motion into two perpendicular components.
- Section 5.4 (gravitational fields): the same structure of ideas; compare inverse square laws, field strength as force per unit property, and potential zero at infinity.
- Section 6.1 (capacitors): Q = VC links charge, p.d. and capacitance; C = εA/d tells you how the plate geometry and material set C.
- Section 6.3 (electromagnetism): moving charges in magnetic fields complete the set of fields giving rise to forces.
Quick self-test
- Define electric field strength and give its unit.
- Find the force between two point charges of 1.0 µC, 0.30 m apart.
- Find E at 0.20 m from a point charge of +2.0 nC.
- By what factor does E change if r is tripled?
- Plates 0.80 cm apart have a p.d. of 240 V. Find E.
- Plates of area 5.0 × 10⁻³ m² are 1.0 mm apart in air. Find C.
- Find the potential 0.30 m from a point charge of +5.0 nC.
- Find C for an isolated sphere of radius 0.10 m.
- Find the potential energy of two protons 1.0 × 10⁻¹⁴ m apart.
- An electron is accelerated from rest through 500 V. Find its final speed.
- State what the area under a force-distance graph represents.
- Give one way in which gravitational and electric fields are alike and one way they differ.
Answers
- Force per unit positive charge, E = F/q; N C⁻¹ (or V m⁻¹).
- 0.10 N, repulsive.
- 4.5 × 10² N C⁻¹, directed away from the charge.
- Divided by 9 (E ∝ 1/r²).
- 240/0.0080 = 3.0 × 10⁴ V m⁻¹.
- 8.85 × 10⁻¹² × 5.0 × 10⁻³ / 1.0 × 10⁻³ = 4.4 × 10⁻¹¹ F.
- 1.5 × 10² V.
- 1.1 × 10⁻¹¹ F.
- 2.3 × 10⁻¹⁴ J.
- v = √(2eV/m) = 1.3 × 10⁷ m s⁻¹.
- Work done moving the charge between the two distances.
- Alike: both follow an inverse square law for a point source. Different: gravity only attracts, but electric forces can attract or repel.
Where marks are usually lost
- Measuring r from the surface of a sphere instead of from its centre.
- Leaving nC, µC, cm or mm unconverted.
- Quoting a force or field without a direction when the question asks for one.
- Adding fields from two charges as plain numbers when they point in different directions.
- Using the sign of a charge inconsistently in V = Q/(4πε₀r) so that the change in potential has the wrong sign.
- Using E = V/d for a radial field, or the inverse square law between plates.
- Writing C = ε₀A/d when a material with εᵣ is present.
- Deriving C = 4πε₀R without stating that V = Q/(4πε₀R) applies at the surface, or without starting from C = Q/V.
- Ignoring the sideways displacement limit: checking whether a charged particle actually leaves the plates.
Official syllabus
OCR Level 3 Advanced GCE in Physics A (H556), Version 3.0 (March 2026), published by OCR: section 6.2 (Electric fields), learning outcomes 6.2.1(a)-(d), 6.2.2(a)-(d), 6.2.3(a)-(c) and 6.2.4(a)-(e).
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