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

Method

  1. Start at the end of the network furthest from the terminals.
  2. Combine resistors in series by adding them, and resistors in parallel with 1/R = 1/R₁ + 1/R₂ + …
  3. Redraw the circuit after each step.
  4. 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; vC cannot jump
Inductor at DC
short circuit; iL cannot jump
Settled
t ≈ 5τ

Method

  1. Find the initial value just after switching: a capacitor voltage and an inductor current cannot jump.
  2. Find the final value long after switching: a capacitor acts as an open circuit, an inductor as a short circuit.
  3. Find the time constant: τ = RC or τ = L/R, using the resistance seen by the capacitor or inductor.
  4. 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, Erms = 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

  1. Convert every quantity to SI units: cm to m, cm² to m², mT and µT to T.
  2. 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.
  3. 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.
  4. Find directions separately with the right-hand rules, and Lenz’s law for induced currents.

AC impedance & phasors

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

Method

  1. Convert the frequency: ω = 2πf.
  2. Find each reactance: XL = ωL and XC = 1/(ωC).
  3. Add impedances like resistors, with Z = R + jX.
  4. 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
−−5 µC−−2 µC−−3 µC22.5 cm + 7.5 cm

Three point charges lie on a straight line: −5 µC on the left, −3 µC on the right 30 cm away, and −2 µC between them, 22.5 cm from the left charge. Find the magnitude of the net electric force F on the middle charge. Use k = 8.99 × 10⁹ N·m²/C².

qL = −5 µCqR = −3 µCqM = −2 µCrL = 22.5 cmrR = 7.5 cm
F = N
2.Coulomb’s law & electric fieldsHard
10 cm6 cm+q1​ = +10 µC+q3​ = +2 µC+q2​ = +3 µC

Three positive point charges sit at the corners of a right triangle: q₃ = 2 µC is at the right-angle corner, q₁ = 10 µC is 10 cm from it along one side and q₂ = 3 µC is 6 cm from it along the other side. Find the magnitude of the net electric force F on q₃.

q1 = 10 µCq2 = 3 µCq3 = 2 µCr13 = 10 cmr23 = 6 cm
F = N
3.Series & parallel resistorsMedium
R1​ = 3 ΩR3​ = 4 Ω+−V1​18 VR2​2 ΩAR4​8 ΩB

Find the equivalent resistance Req seen by the source V1.

V1 = 18 VR1 = 3 ΩR2 = 2 ΩR3 = 4 ΩR4 = 8 Ω
Req = Ω
4.Series & parallel resistorsHard
R1​ = 5 ΩR3​ = 8 ΩR5​ = 2 Ω+−V1​5 VR2​25 ΩIR2​AR4​6 ΩBR6​10 Ω

Find the current IR2 through R2.

V1 = 5 VR1 = 5 ΩR2 = 25 ΩR3 = 8 ΩR4 = 6 ΩR5 = 2 ΩR6 = 10 Ω
IR2 = A
5.RC & RL transientsMedium
+−Vs​24 Vt = 0R1​ = 1 kΩR2​ = 1 kΩC68 µF+−vC​

The source Vₛ charges the capacitor through R₁, and R₂ is connected in parallel with C. The capacitor is uncharged when the switch closes at t = 0. Find the capacitor voltage vC at t = 15 ms.

Vs = 24 VR1 = 1 kΩR2 = 1 kΩC = 68 µFt = 15 ms
vC = V
6.RC & RL transientsHard
+−Vs​6 Vt = 0R = 1 kΩC33 µF+−vC​vC​(0) = 5 V

Just before the switch closes at t = 0, the capacitor holds 5 V with the polarity shown. How long does it take for vC to reach 5.7 V? Find t.

Vs = 6 VR = 1 kΩC = 33 µFvC(0) = 5 V
t = ms
7.Magnetic fields & inductionMedium
+v = 4 × 10⁵ m/sB = 0.5 T

A proton moves on a circle in a uniform magnetic field of 0.5 T. Find the time T it takes for one revolution.

m = 1.673 × 10⁻²⁷ kg|q| = 1.602 × 10⁻¹⁹ CB = 0.5 T
T = ns
8.Magnetic fields & inductionHard
V = 1000 VB = 0.4 Tr = ?

A deuteron starts from rest, is accelerated through a potential difference of 1000 V and then enters a uniform magnetic field of 0.4 T at right angles. Find the radius r of its path in the field.

m = 3.344 × 10⁻²⁷ kg|q| = 1.602 × 10⁻¹⁹ CV = 1000 VB = 0.4 T
r = cm
9.AC impedance & phasorsMedium
12 V100 HzR = 25 ΩL = 250 mHC = 10 µF

A series RLC circuit is connected to a 12 V (rms), 100 Hz supply. Find the phase angle φ of the impedance, in degrees (positive when the current lags the voltage).

V = 12 V (rms)f = 100 HzR = 25 ΩL = 250 mHC = 10 µF
φ = °
10.AC impedance & phasorsHard
VfR = 20 ΩL = 10 mHC = 0.47 µF

A series RLC circuit has R = 20 Ω, L = 10 mH and C = 0.47 µF. Find its quality factor Q at resonance.

R = 20 ΩL = 10 mHC = 0.47 µF
Q =

3Solutions

1.Coulomb’s law & electric fields

Answer: F = 7.814 N

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.

Force from each charge

Right is positive.

FL = +k·5·2 × 10⁻¹²/0.225² = 1.776 N
FR = −k·3·2 × 10⁻¹²/0.075² = −9.589 N

Net force

F = 1.776 + (−9.589) = −7.814 N → |F| = 7.814 N

Answer

F = 7.814 N

The net force points to the left.

2.Coulomb’s law & electric fields

Answer: F = 23.4 N

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.

Each force on q₃

F1 = k·10·2 × 10⁻¹²/0.1² = 17.98 N
F2 = k·3·2 × 10⁻¹²/0.06² = 14.98 N

Vector sum

F = √(17.98² + 14.98²) = 23.4 N

Answer

F = 23.4 N
3.Series & parallel resistors

Answer: Req = 4.714 Ω

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.

R1​ = 3 ΩR3​ = 4 Ω+−V1​18 VR2​2 ΩAR4​8 ΩB

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 = 4 + 8 = 12 Ω
R2 ∥ 12 = 2·12/(2+12) = 1.714 Ω
Req = R1 + 1.714 = 3 + 1.714 = 4.714 Ω

Answer

Req = 4.714 Ω
4.Series & parallel resistors

Answer: IR2 = 0.1237 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.

R1​ = 5 ΩR3​ = 8 ΩR5​ = 2 Ω+−V1​5 VR2​25 ΩAR4​6 ΩBR6​10 Ω

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 = 2 + 10 = 12 Ω
R4 ∥ 12 = 4 Ω
R3 + 4 = 12 Ω
R2 ∥ 12 = 8.108 Ω
Req = R1 + 8.108 = 5 + 8.108 = 13.11 Ω

Current from the source

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

IR1 = V1/Req = 5/13.11 = 0.3814 A

Current through R₂

Subtract the drop across R₁ to get the voltage at node A, which is the voltage across R₂.

VA = V1 − IR1·R1 = 5 − 0.3814·5 = 3.093 V
IR2 = VA/R2 = 3.093/25 = 0.1237 A

Answer

IR2 = 0.1237 A
5.RC & RL transients

Answer: vC = 4.281 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.

Thévenin equivalent seen by the capacitor

Short the source to find Rth; open the capacitor to find the voltage it will settle at.

Rth = R1 ∥ R2 = 1·1/(1 + 1) = 0.5 kΩ
vC(∞) = 24·1/(1 + 1) = 12 V

Time constant

τ = Rth·C = 0.5·68 = 34 ms

Charging curve

vC(t) = 12·(1 − e−15/34) = 4.281 V

Answer

vC = 4.281 V
6.RC & RL transients

Answer: t = 39.73 ms

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.

Initial value, final value, time constant

The capacitor voltage cannot jump, so it starts at its stored value and heads for the source voltage.

vC(0) = 5 V, vC(∞) = Vs = 6 V
τ = R·C = 1 kΩ · 33 µF = 33 ms
vC(t) = 6 + (5 − 6)·e−t/τ

Solve for the time

5.7 = 6 + (−1)·e−t/τ → e−t/τ = (5.7 − 6)/(5 − 6) = 0.3
t = τ·ln((5 − 6)/(5.7 − 6)) = 33·ln(3.333) = 39.73 ms

Answer

t = 39.73 ms
7.Magnetic fields & induction

Answer: T = 131.2 ns

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).

Period of the circular motion

A faster particle moves on a larger circle, so the time per turn stays the same.

T = 2πm/(|q|B) = 2π·1.673 × 10⁻²⁷/(1.602 × 10⁻¹⁹·0.5) = 131.2 ns

Answer

T = 131.2 ns

The speed is not needed: this is why a cyclotron can use one fixed frequency.

8.Magnetic fields & induction

Answer: r = 1.615 cm

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).

Speed after the acceleration

v = √(2|q|V/m) = √(2·1.602 × 10⁻¹⁹·1000/(3.344 × 10⁻²⁷)) = 309537 m/s

Radius in the field

r = mv/(|q|B) = 0.01615 m = 1.615 cm

Answer

r = 1.615 cm

Combined: r = √(2mV/|q|)/B, so heavier ions of the same charge move on larger circles; this separates isotopes.

9.AC impedance & phasors

Answer: φ = −4.745 °

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|.

Reactances

ω = 2πf = 2π·100 = 628.3 rad/s
XL = ωL = 628.3·0.25 = 157.1 Ω
XC = 1/(ωC) = 1/(628.3·10·10⁻⁶) = 159.2 Ω

Impedance

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

|Z| = √(R² + (XL − XC)²) = √(25² + (−2.075)²) = 25.09 Ω

Phase angle

φ = arctan((XL − XC)/R) = arctan(−2.075/25) = −4.745°

Answer

φ = −4.745°
10.AC impedance & phasors

Answer: Q = 7.293

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|.

Resonant frequency

f0 = 1/(2π·√(0.01·0.47·10⁻⁶)) = 2322 Hz

Quality factor

Q compares the reactance at resonance with the resistance: Q = ω₀L/R.

Q = (1/R)·√(L/C) = (1/20)·√(0.01/(0.47·10⁻⁶)) = 7.293

Answer

Q = 7.293

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