🏠 Home
FractionRush AQA A-Level Physics 7

Electric Fields

Electric fields govern everything from the structure of atoms to the operation of cathode ray tubes and inkjet printers. Understand how charges create fields and how fields act on charges — the foundation of all electromagnetism.

Define electric field strength E = F/Q and apply it to point charges and uniform fields
📐Use E = kQ/r² (radial) and E = V/d (uniform) in calculations
🌀Draw and interpret electric field line diagrams for various charge configurations
💡Define electric potential V = kQ/r and explain its sign for positive and negative charges
Describe equipotential surfaces and their relationship to field lines
↔️Compare gravitational and electric fields — similarities and differences

Electric Field Strength

An electric field is a region where a charge experiences an electric force. The electric field strength E at a point is defined as the force per unit positive charge at that point:

E = F / Q    (N C⁻¹ or V m⁻¹)

E is a vector — it points in the direction of force on a positive test charge.

For a point charge Q: By Coulomb's law, the force on a test charge q at distance r is F = kQq/r². So:

E = kQ / r²    where k = 1/(4πε₀) = 8.99 × 10⁹ N m² C⁻²

E due to a positive charge points radially outward; due to a negative charge, radially inward.

For a uniform field between parallel plates: A potential difference V across plates separated by distance d creates a uniform field:

E = V / d    (V m⁻¹ ≡ N C⁻¹)
Permittivity of free space: ε₀ = 8.85 × 10⁻¹² F m⁻¹ (or C² N⁻¹ m⁻²). In a medium with relative permittivity ε_r: k → k/ε_r, or equivalently ε₀ → ε₀ε_r. This reduces the field strength in a dielectric medium.

Electric Field Lines

Field lines represent the direction and relative strength of an electric field:

Key field line patterns:

ConfigurationField line patternField type
Isolated positive chargeRadial outward from chargeNon-uniform (radial)
Isolated negative chargeRadial inward to chargeNon-uniform (radial)
Two opposite charges (+/−)Leave + , curve to −Non-uniform (dipole)
Parallel plates (opposite charges)Uniform, parallel, perpendicular to platesUniform (between plates)
Two like chargesRepel away from each other, neutral point betweenNon-uniform
⚠️ A common misconception: electric field lines do NOT represent the path a charge would follow. A positive charge released from rest follows the field line only if E is in the direction of motion. If launched with velocity perpendicular to E, the charge follows a parabolic path (like projectile motion in a gravitational field).

Electric Potential

The electric potential V at a point is the work done per unit positive charge in bringing a small test charge from infinity to that point:

V = W / Q    (J C⁻¹ = V)

For a point charge Q at distance r:

V = kQ / r = Q / (4πε₀r)

Sign convention:

Electric potential energy: E_p = QV = kQ₁Q₂/r. For a charge Q₁ in the field of Q₂, the potential energy is positive if charges have the same sign (they repel — energy stored), and negative if opposite signs (they attract — bound system).

Relationship between field and potential:

E = −dV/dr    (or E = −ΔV/Δr for uniform fields: E = V/d)

This is analogous to the gravitational case: field points in the direction of steepest decrease in potential.

Equipotential Surfaces in Electric Fields

Equipotential surfaces (in 3D) or equipotential lines (in 2D cross-sections) are surfaces/lines of constant potential. Key properties (analogous to gravitational equipotentials):

The work done moving charge Q between two points at potentials V₁ and V₂:

W = Q(V₂ − V₁) = QΔV

If the charge moves to higher potential (for positive Q), work must be done on the charge. If it moves to lower potential, the field does positive work on the charge (KE increases).

The electron-volt (eV): 1 eV is the KE gained by an electron accelerated through a potential difference of 1 V. 1 eV = 1.6 × 10⁻¹⁹ J. Useful for atomic and nuclear energy scales: a 5 MeV alpha particle has KE = 5×10⁶ × 1.6×10⁻¹⁹ = 8×10⁻¹³ J.

Comparison: Gravitational and Electric Fields

PropertyGravitationalElectric
Force lawF = Gm₁m₂/r²F = kQ₁Q₂/r²
Field strengthg = GM/r²E = kQ/r²
PotentialV = −GM/rV = kQ/r
SignAlways attractive; V always negativeCan repel; V positive or negative
ConstantG = 6.67×10⁻¹¹ N m² kg⁻²k = 8.99×10⁹ N m² C⁻²
Source propertyMass (always positive)Charge (positive or negative)
Relative strengthWeakest force~10³⁶ times stronger than gravity

The mathematical structures are identical — this is not a coincidence but reflects deep symmetry in the laws of nature. Many results derived for one field can be adapted for the other by substituting the appropriate constants and replacing mass with charge.

Two parallel plates are separated by 8.0 mm and have a potential difference of 400 V between them. Calculate (a) the electric field strength, (b) the force on a proton (e = 1.6×10⁻¹⁹ C) between the plates, (c) the acceleration of the proton (m_p = 1.67×10⁻²⁷ kg).
1E = V/d = 400/(8.0×10⁻³) = 50 000 V m⁻¹ = 5.0 × 10⁴ N C⁻¹
2Force on proton: F = EQ = 5.0×10⁴ × 1.6×10⁻¹⁹ = 8.0 × 10⁻¹⁵ N
3Acceleration: a = F/m = 8.0×10⁻¹⁵ / 1.67×10⁻²⁷ = 4.79 × 10¹² m s⁻² ≈ 4.8 × 10¹² m s⁻²
E = 5.0×10⁴ N C⁻¹; F = 8.0×10⁻¹⁵ N; a = 4.8×10¹² m s⁻² (enormous — atomic scales!)
Calculate the electric field strength and potential at a distance of 0.20 m from a point charge of +4.0 μC. (k = 8.99×10⁹ N m² C⁻²)
1Q = 4.0×10⁻⁶ C; r = 0.20 m
2E = kQ/r² = (8.99×10⁹ × 4.0×10⁻⁶)/(0.20)² = (3.596×10⁴)/0.04 = 8.99×10⁵ N C⁻¹ ≈ 9.0×10⁵ V m⁻¹
3V = kQ/r = (8.99×10⁹ × 4.0×10⁻⁶)/0.20 = 3.596×10⁴/0.20 = 1.798×10⁵ V ≈ 1.8×10⁵ V
E = 9.0×10⁵ V m⁻¹ (directed radially outward); V = +1.8×10⁵ V (positive for positive charge)
An electron is accelerated from rest through a potential difference of 5000 V. Find (a) its kinetic energy in joules and eV, (b) its final speed. (m_e = 9.11×10⁻³¹ kg, e = 1.6×10⁻¹⁹ C)
1Work done on electron = QΔV = eV = 1.6×10⁻¹⁹ × 5000 = 8.0×10⁻¹⁶ J
2KE = 8.0×10⁻¹⁶ J = 8.0×10⁻¹⁶ / 1.6×10⁻¹⁹ eV = 5000 eV = 5 keV
3Speed: ½m_e v² = 8.0×10⁻¹⁶ → v² = 2×8.0×10⁻¹⁶/9.11×10⁻³¹ = 1.757×10¹⁵ → v = 4.19×10⁷ m s⁻¹
4v ≈ 4.2×10⁷ m s⁻¹ ≈ 0.14c — relativistic effects start to matter above ~10% of c.
KE = 8.0×10⁻¹⁶ J = 5000 eV = 5 keV; v = 4.2×10⁷ m s⁻¹ (14% speed of light)

Q1. Electric field lines indicate the direction of force on:

Q2. Parallel plates are 5.0 mm apart with 250 V across them. What is the electric field strength?

Q3. Which of the following is a key difference between electric and gravitational fields?

Q4. The electric potential due to a positive charge Q at distance r is V. At distance 2r, the potential is:

Q5. What is the work done moving a charge of +3.0 μC from a point at potential +200 V to a point at potential +800 V?

Challenge 1. An electron enters a uniform electric field horizontally with speed 3.0×10⁶ m s⁻¹. The field is 1.5×10⁴ V m⁻¹ directed vertically upward. The plates are 0.10 m long. (a) Find the vertical deflection as the electron passes through. (b) Find the angle at exit. (c) What happens to KE?

Challenge 2. Two point charges: Q₁ = +8.0 μC at the origin and Q₂ = −2.0 μC at x = 0.30 m. Find (a) the point on the x-axis where E = 0 (not between them), (b) the potential at the midpoint (x = 0.15 m).

Challenge 3 (Synoptic). Compare the ratio of electric to gravitational force between an electron and a proton in a hydrogen atom (r = 5.3×10⁻¹¹ m). Discuss why atomic structure is determined by electric forces rather than gravity.