Gravitational Fields

What is a Gravitational Field?

A gravitational field is a region of space where a mass experiences a gravitational force. All objects with mass create a gravitational field around them.

Gravitational field strength g is defined as the force per unit mass at a point in the field.

g = F / m    (N kg−1)

For a point mass or outside a uniform sphere:

g = GM / r²

where G = 6.67 × 10−11 N m² kg−2, M is the mass creating the field, and r is the distance from the centre of the mass.

Radial Gravitational Field

Around a spherical mass like the Earth, the gravitational field is radial — field lines point inward towards the centre of mass.

Earth

Radial gravitational field around Earth — field lines point inward towards the centre

Worked Example

Calculate the gravitational field strength at a height of 400 km above the Earth's surface. (RE = 6.4 × 106 m, ME = 6.0 × 1024 kg)

Step 1: r = RE + h = 6.4 × 106 + 400 × 103 = 6.8 × 106 m

Step 2: g = GM/r² = (6.67 × 10−11 × 6.0 × 1024) / (6.8 × 106

Step 3: g = 4.0 × 1014 / 4.624 × 1013 = 8.7 N kg−1

Key Facts

  • Gravitational fields are always attractive — masses always attract each other
  • Field strength follows an inverse-square law: doubling the distance quarters the field strength
  • Near Earth's surface, g ≈ 9.81 N kg−1 and is approximately uniform

Exam Tip

Always check whether the question gives the distance from the surface or from the centre of the Earth. You need the distance from the centre for g = GM/r².

Gravitational Potential

Gravitational Potential (V)

The gravitational potential at a point is the work done per unit mass in bringing a test mass from infinity to that point.

V = −GM / r    (J kg−1)

Gravitational potential is always negative (zero at infinity) because work must be done against gravity to move a mass away.

Orbits & Kepler's Third Law

For a circular orbit, gravitational force provides the centripetal force:

GMm/r² = mv²/r   ⇒   v = √(GM/r)

Kepler's third law relates orbital period T to orbital radius r:

T² ∝ r³     specifically: T² = (4π²/GM) r³

Worked Example

Calculate the orbital period of a satellite at height 400 km above the Earth.

Step 1: r = 6.4 × 106 + 4.0 × 105 = 6.8 × 106 m

Step 2: T² = (4π²/GM) r³ = (4π² / (6.67 × 10−11 × 6.0 × 1024)) × (6.8 × 106

Step 3: T² = (9.87 × 10−14) × 3.14 × 1020 = 3.10 × 107

Step 4: T = 5570 s ≈ 93 minutes

Key Facts

  • Gravitational potential energy: Ep = mV = −GMm/r
  • Escape velocity: vesc = √(2GM/r)
  • Field strength is the negative potential gradient: g = −dV/dr

Electric Fields

Electric Field Strength

An electric field is a region where a charged particle experiences a force. Electric field strength E is the force per unit positive charge:

E = F / Q    (N C−1 or V m−1)

Uniform Electric Field

Between parallel plates with potential difference V and separation d:

E = V / d
+ E = V/d (uniform field)

Uniform electric field between parallel plates — equally spaced field lines from + to −

Radial Electric Field & Coulomb's Law

For a point charge or spherical charge Q, the field is radial:

E = Q / (4πε0r²)

Coulomb's law gives the force between two point charges:

F = Q1Q2 / (4πε0r²)

where ε0 = 8.85 × 10−12 F m−1. The constant 1/(4πε0) ≈ 9.0 × 109 N m² C−2.

Worked Example

Calculate the force between charges of +3.0 μC and −5.0 μC separated by 0.10 m.

Step 1: F = Q1Q2 / (4πε0r²)

Step 2: F = (9.0 × 109) × (3.0 × 10−6 × 5.0 × 10−6) / (0.10)²

Step 3: F = 9.0 × 109 × 1.5 × 10−11 / 0.01 = 13.5 N (attractive)

Exam Tip

Electric fields can be attractive OR repulsive (unlike gravity which is always attractive). Always state the direction and nature of the force in your answer.

Electric Potential

Electric Potential (V)

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

V = Q / (4πε0r)

Unlike gravitational potential, electric potential can be positive (near positive charges) or negative (near negative charges).

Comparing Gravitational & Electric Fields

Property Gravitational Electric
SourceMassCharge
Force typeAlways attractiveAttractive or repulsive
Field strengthg = GM/r²E = Q/(4πε0r²)
PotentialV = −GM/r (always −ve)V = Q/(4πε0r) (+ve or −ve)

Key Facts

  • Both gravitational and electric fields obey inverse-square laws
  • Field strength equals the negative potential gradient: E = −dV/dr
  • Equipotential surfaces are perpendicular to field lines

Capacitance

Capacitance & Energy Storage

Capacitance is the charge stored per unit potential difference:

C = Q / V    (farads, F)

Energy stored in a capacitor:

E = ½QV = ½CV² = ½Q²/C

Worked Example

A 470 μF capacitor is charged to 12 V. Calculate the energy stored.

Step 1: E = ½CV²

Step 2: E = 0.5 × 470 × 10−6 × 12²

Step 3: E = 0.5 × 470 × 10−6 × 144 = 0.034 J

Charging & Discharging

The time constant τ = RC determines how quickly a capacitor charges or discharges.

τ = RC    (seconds)

Discharging: Q = Q0e−t/RC    V = V0e−t/RC    I = I0e−t/RC

After one time constant, the value falls to 1/e ≈ 37% of its initial value.

Time (t) Charge (Q) Q0 Charging Discharging τ=RC

Capacitor charging and discharging curves — exponential approach to final value

Exam Tip

To find the time constant from a graph, read off the time at which the value has fallen to 37% of its initial value (discharging) or risen to 63% of its final value (charging).

Magnetic Fields

Magnetic Flux & Flux Density

Magnetic flux density B (tesla, T) is the force per unit length per unit current on a conductor perpendicular to the field.

Magnetic flux Φ through an area A:

Φ = BA cosθ    (webers, Wb)

Flux linkage for a coil of N turns:

Flux linkage = NΦ = BAN cosθ

Force on a Current-Carrying Conductor

A wire of length L carrying current I in a magnetic field B experiences a force:

F = BIL sinθ

Direction given by Fleming's left-hand rule (thuMb = Motion, First finger = Field, seCond finger = Current).

Force on a Moving Charge

A charge Q moving at velocity v perpendicular to a magnetic field B experiences:

F = BQv

This force is always perpendicular to the velocity, causing circular motion. The radius of the circular path is r = mv/(BQ).

Worked Example

A wire of length 0.30 m carries a current of 4.0 A perpendicular to a field of 0.50 T. Find the force.

F = BIL sinθ = 0.50 × 4.0 × 0.30 × sin 90°

F = 0.60 N

Transformers

A transformer changes alternating voltage using electromagnetic induction between two coils on a shared iron core:

Ns / Np = Vs / Vp

For an ideal transformer: VsIs = VpIp (power is conserved).

Key Facts

  • 1 tesla = 1 Wb m−2
  • A charged particle moving parallel to a magnetic field experiences no force
  • Step-up transformers increase voltage (Ns > Np); step-down transformers decrease it

Electromagnetic Induction

Faraday's Law

The magnitude of the induced EMF is equal to the rate of change of magnetic flux linkage:

ε = −N dΦ/dt

The negative sign reflects Lenz's law: the induced EMF acts in a direction to oppose the change in flux that produces it.

Lenz's Law

The direction of the induced current is such that it opposes the change producing it. This is a consequence of conservation of energy.

Worked Example

The flux through a 200-turn coil changes from 0.05 Wb to 0.01 Wb in 0.02 s. Find the induced EMF.

Step 1: ΔΦ = 0.05 − 0.01 = 0.04 Wb

Step 2: ε = N × ΔΦ/Δt = 200 × 0.04 / 0.02

Step 3: ε = 400 V

Key Facts

  • An EMF is induced whenever the flux linkage through a circuit changes
  • Moving a magnet into a coil induces a current; moving it out induces a current in the opposite direction
  • Faster motion or more turns produces a larger EMF

Exam Tip

Lenz's law questions are common. Remember: the induced effect always opposes the cause. If flux is increasing, the induced current creates a field to reduce the flux.

Fields Flashcards

Click to flip. Use arrow keys to navigate, space to flip.

Fields Quiz

Test your knowledge of fields and their consequences.

Fields - Mock Exam Questions

Practice exam-style questions. Write your answer, then check the mark scheme.