Physics 2: Electricity and Magnetism: cram pack

Formula sheets, the key method steps for every topic and 10 practice problems, with full solutions at the back.

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1Formulas and methods

Coulomb’s law & electric fields

Coulomb’s law: F = k·|q₁q₂|/r²
Field of a point charge: E = k·|q|/r²
Constant: k = 8.99 × 10⁹ N·m²/C²
Force on a charge: F = q·E

Series & parallel resistors

Resistors in series: R_eq = R₁ + R₂ + …
Resistors in parallel: 1/R_eq = 1/R₁ + 1/R₂ + …
Two in parallel: R_eq = R₁R₂ / (R₁ + R₂)
Ohm's law: V = I·R
Power: P = V·I = I²R = V²/R

Method

Start at the end of the network furthest from the terminals.
Combine resistors in series by adding them, and resistors in parallel with 1/R = 1/R₁ + 1/R₂ + …
Redraw the circuit after each step.
Repeat until one resistor is left between the terminals.

RC & RL transients

Time constant: τ = RC | τ = L/R
Response: x(t) = x(∞) + [x(0) − x(∞)]·e^−t/τ
Capacitor at DC: open circuit; v_C cannot jump
Inductor at DC: short circuit; i_L cannot jump
Settled: t ≈ 5τ

Method

Find the initial value just after switching: a capacitor voltage and an inductor current cannot jump.
Find the final value long after switching: a capacitor acts as an open circuit, an inductor as a short circuit.
Find the time constant: τ = RC or τ = L/R, using the resistance seen by the capacitor or inductor.
Use x(t) = x(∞) + [x(0) − x(∞)]·e^−t/τ.

Magnetic fields & induction

Long straight wire: B = μ₀I/(2πr)
Centre of a flat coil: B = μ₀NI/(2R)
Long solenoid: B = μ₀nI, n = N/L
Constant: μ₀ = 4π × 10⁻⁷ T·m/A
Force on a wire: F = BIL·sin θ
Force on a charge: F = |q|vB·sin θ
Circular motion: r = mv/(|q|B), T = 2πm/(|q|B)
Parallel wires: F/L = μ₀I₁I₂/(2πd)
Flux: Φ = BA·cos θ
Faraday’s law: ε = −N·ΔΦ/Δt
Moving rod: ε = BLv
Generator: E₀ = NBAω, E_rms = E₀/√2
Inductance: ε = L·ΔI/Δt, L = μ₀N²A/l, W = ½LI²
Mutual inductance: ε₂ = M·di₁/dt, M = k√(L₁L₂)
Velocity selector and spectrometer: v = E/B, r = √(2mV/|q|)/B

Method

Convert every quantity to SI units: cm to m, cm² to m², mT and µT to T.
Pick the right formula: B = μ₀I/(2πr) for a wire, μ₀NI/(2R) for the centre of a coil, μ₀nI inside a solenoid; F = BIL·sin θ or |q|vB·sin θ for forces.
For induction, find the change of flux ΔΦ = Δ(BA·cos θ) and use ε = N·ΔΦ/Δt, or ε = BLv for a moving rod and NBAω for a rotating coil.
Find directions separately with the right-hand rules, and Lenz’s law for induced currents.

AC impedance & phasors

Impedances: Z_R = R, Z_L = jωL, Z_C = 1/(jωC)
Angular frequency: ω = 2πf
Magnitude and angle: |Z| = √(R² + X²), φ = atan(X/R)
Phasor Ohm’s law: V = I·Z

Method

Convert the frequency: ω = 2πf.
Find each reactance: X_L = ωL and X_C = 1/(ωC).
Add impedances like resistors, with Z = R + jX.
Find the magnitude |Z| = √(R² + X²) and the angle φ = atan(X/R), then use Ohm’s law with phasors.

2Practice problems

1.Coulomb’s law & electric fieldsMedium

A charge of +4 µC and a charge of +4 µC are 10 cm apart. Point P lies on the line between them, 7.5 cm from the first charge. Find the magnitude of the electric field E at P.

q₁ = +4 µCq₂ = +4 µCr₁ = 7.5 cmr₂ = 2.5 cm

E = N/C

2.Coulomb’s law & electric fieldsHard

Three positive point charges sit at the corners of a right triangle: q₃ = 5 µC is at the right-angle corner, q₁ = 5 µC is 3 cm from it along one side and q₂ = 6 µC is 3 cm from it along the other side. Find the magnitude of the net electric force F on q₃.

q₁ = 5 µCq₂ = 6 µCq₃ = 5 µCr₁₃ = 3 cmr₂₃ = 3 cm

F = N

3.Series & parallel resistorsMedium

Find the current I_R1 delivered by the source, which flows through R₁.

V₁ = 9 VR₁ = 12 ΩR₂ = 6 ΩR₃ = 3 ΩR₄ = 12 Ω

I_R1 = A

4.Series & parallel resistorsHard

Find the current I_R1 delivered by the source, which flows through R₁.

V₁ = 10 VR₁ = 5 ΩR₂ = 12 ΩR₃ = 25 ΩR₄ = 10 ΩR₅ = 6 ΩR₆ = 30 Ω

I_R1 = A

5.RC & RL transientsMedium

The inductor carries a steady current of 3 A. At t = 0 the switch closes the loop through R and the source is removed, so the inductor current decays through R. Find the voltage v_R across R at t = 2 ms.

i(0) = 3 AR = 100 ΩL = 150 mHt = 2 ms

v_R = V

6.RC & RL transientsHard

A timer starts charging an uncharged capacitor through a resistor from a 5 V supply at t = 0. It must trigger when the capacitor voltage reaches 4.5 V, exactly 500 ms after the start. With R = 2.2 kΩ, find the capacitance C needed.

V_s = 5 VV_th = 4.5 VT = 500 msR = 2.2 kΩ

C = µF

7.Magnetic fields & inductionMedium

A proton moves down the page through a uniform magnetic field pointing out of the page. Click the direction of the magnetic force on it.

v: down the pageB: out of the page

1up the page
2to the right
3down the page
4to the left

8.Magnetic fields & inductionHard

The current in a 5 mH inductor changes steadily from 0.5 A to 5.5 A in 1 ms. Find the magnitude of the self-induced emf ε.

L = 5 mH0.5 A → 5.5 AΔt = 1 ms

ε = V

9.AC impedance & phasorsMedium

A resistor and an inductor are connected in parallel across a 120 V (rms), 200 Hz supply. Find the rms current I.

V = 120 V (rms)f = 200 HzR = 20 ΩL = 20 mH

I = A

10.AC impedance & phasorsHard

A series RLC circuit is connected to a 24 V (rms), 60 Hz supply. Find the rms voltage V_C across the capacitor.

V = 24 V (rms)f = 60 HzR = 20 ΩL = 150 mHC = 10 µF

V_C = V

3Solutions

1.Coulomb’s law & electric fields

Answer: E = 5.114 × 10⁷ N/C

Coulomb’s law: two point charges attract or repel with F = k·|q₁·q₂|/r², with k = 8.99 × 10⁹ N·m²/C². The field of a point charge is E = k·|q|/r², pointing away from a positive charge and towards a negative one. Forces and fields from several charges add as vectors.

Field of each charge

E₁ = k·4 × 10⁻⁶/0.075² = 6.393 × 10⁶ N/C

E₂ = k·4 × 10⁻⁶/0.025² = 5.754 × 10⁷ N/C

Directions and sum

Both charges are positive: at P their fields point away from each charge, so in opposite directions.

E = |6.393 × 10⁶ − 5.754 × 10⁷| = 5.114 × 10⁷ N/C

Answer

E = 5.114 × 10⁷ N/C

2.Coulomb’s law & electric fields

Answer: F = 390.1 N

Each force on q₃

F₁ = k·5·5 × 10⁻¹²/0.03² = 249.7 N

F₂ = k·6·5 × 10⁻¹²/0.03² = 299.7 N

Vector sum

F = √(249.7² + 299.7²) = 390.1 N

Answer

F = 390.1 N

3.Series & parallel resistors

Answer: I_R1 = 0.5526 A

Series and parallel resistors: in series the same current flows through each resistor and R = R₁ + R₂ + …. In parallel each resistor has the same voltage and 1/R = 1/R₁ + 1/R₂ + …. A ladder network is reduced one pair at a time until a single equivalent resistance remains.

Combine resistors from the far end

Start at the end farthest from the source and work back towards it. Resistors carrying the same current are in series; resistors across the same two nodes are in parallel.

R₃ + R₄ = 3 + 12 = 15 Ω

R₂ ∥ 15 = 6·15/(6+15) = 4.286 Ω

R_eq = R₁ + 4.286 = 12 + 4.286 = 16.29 Ω

Current from the source

The source sees only R_eq, so Ohm’s law gives the current it delivers. That current flows through R₁.

I_R1 = V₁/R_eq = 9/16.29 = 0.5526 A

Answer

I_R1 = 0.5526 A

4.Series & parallel resistors

Answer: I_R1 = 0.7253 A

Combine resistors from the far end

Start at the end farthest from the source and work back towards it. Resistors carrying the same current are in series; resistors across the same two nodes are in parallel.

R₅ + R₆ = 6 + 30 = 36 Ω

R₄ ∥ 36 = 7.826 Ω

R₃ + 7.826 = 32.83 Ω

R₂ ∥ 32.83 = 8.788 Ω

R_eq = R₁ + 8.788 = 5 + 8.788 = 13.79 Ω

Current from the source

The source sees only R_eq, so Ohm’s law gives the current it delivers. That current flows through R₁.

I_R1 = V₁/R_eq = 10/13.79 = 0.7253 A

Answer

I_R1 = 0.7253 A

5.RC & RL transients

Answer: v_R = 79.08 V

First-order transients: in a circuit with one capacitor or one inductor, every voltage and current moves exponentially from its initial value to its final value: x(t) = x(∞) + [x(0) − x(∞)]·e^−t/τ, with τ = RC or τ = L/R. After about 5τ the circuit has settled.

Time constant

τ = L/R = 150 mH / 100 Ω = 1.5 ms

Decay of the current

i(t) = 3·e^−2/1.5 = 0.7908 A

v_R = R·i = 100·0.7908 = 79.08 V

Answer

v_R = 79.08 V

6.RC & RL transients

Answer: C = 98.7 µF

Required time constant

4.5 = 5·(1 − e^−500/τ) → τ = 500/ln(5/(5 − 4.5))

τ = 500/2.303 = 217.1 ms

Capacitance

kΩ times µF gives milliseconds.

C = τ/R = 217.1/2.2 = 98.7 µF

Answer

C = 98.7 µF

7.Magnetic fields & induction

Answer: to the left

Magnetic forces: a straight wire carrying I in a field B feels F = BIL·sin θ, and a moving charge F = |q|vB·sin θ, where θ is the angle between the current (or velocity) and B. The force is perpendicular to both: point the fingers of the right hand along I or v, curl them towards B, and the thumb gives F for a positive charge; reverse it for a negative charge. Because F is perpendicular to v, a charge moving across a uniform field moves on a circle: |q|vB = mv²/r gives r = mv/(|q|B) and the period T = 2πm/(|q|B), which does not depend on the speed. Two parallel wires attract for currents in the same direction: F/L = μ₀I₁I₂/(2πd).

Right-hand rule

Point the fingers along the current or velocity and curl them towards B; the thumb gives the force on a positive charge.

v: down the page, B: out of the page

Direction of the force

to the left

Answer

F: to the left

8.Magnetic fields & induction

Answer: ε = 25 V

Electromagnetic induction: the flux through a loop is Φ = BA·cos θ, with θ between B and the normal of the loop. Faraday's law: a change of flux induces emf = −N·dΦ/dt in a coil of N turns, and Lenz's law says the induced current flows so that its own field opposes the change. A rod moving across a field gives emf = BLv. A coil rotating at ω gives e = NBAω·sin ωt, peak NBAω. Self-inductance: emf = −L·di/dt, with L = μ₀N²A/l for a long solenoid, and the energy stored is W = ½LI². Two coupled coils: emf₂ = −M·di₁/dt with M = k√(L₁L₂).

Self-induced emf

The emf opposes the change of current (Lenz), so its sign is opposite to ΔI; the size is L·|ΔI|/Δt.

ε = L·ΔI/Δt = 0.005·5/0.001 = 25 V

Answer

ε = 25 V

9.AC impedance & phasors

Answer: I = 7.668 A

AC circuits with phasors: resistors, inductors and capacitors have impedances R, jωL and 1/(jωC), with ω = 2πf. In series, impedances add like resistances, but as complex numbers. Rms current and voltage follow Ohm’s law with |Z|.

Reactance

X_L = ωL = 2π·200·0.02 = 25.13 Ω

Branch currents

Both branches are connected straight across the supply, so each sees the full voltage V.

I_R = V/R = 120/20 = 6 A

I_X = V/X_L = 120/25.13 = 4.775 A

Total current

The resistor current is in phase with V and the reactive current is 90° out of phase, so they add like the sides of a right triangle.

I = √(I_R² + I_X²) = √(6² + 4.775²) = 7.668 A

Answer

I = 7.668 A

10.AC impedance & phasors

Answer: V_C = 30.36 V

Reactances

ω = 2πf = 2π·60 = 377 rad/s

X_L = ωL = 377·0.15 = 56.55 Ω

X_C = 1/(ωC) = 1/(377·10·10⁻⁶) = 265.3 Ω

Impedance

In series the impedances add as complex numbers: Z = R + j(X_L − X_C).

|Z| = √(R² + (X_L − X_C)²) = √(20² + (−208.7)²) = 209.7 Ω

Current

The same current flows through every element of a series circuit.

I = V/|Z| = 24/209.7 = 0.1145 A

Voltage across the capacitor

V_C = I·X_C = 0.1145·265.3 = 30.36 V

Answer

V_C = 30.36 V

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