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
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.
1Formulas and methods
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
- 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; vC cannot jump
- Inductor at DC
- short circuit; iL 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, 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
- 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
- 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
- Convert the frequency: ω = 2πf.
- Find each reactance: XL = ωL and XC = 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
Two identical small metal spheres carry charges of +6 µC and +8 µC. They are touched together and then put back 10 cm apart. Find the magnitude of the force F between them now. Use k = 8.99 × 10⁹ N·m²/C².
q1 = +6 µCq2 = +8 µCr = 10 cm
F = N
2.Coulomb’s law & electric fieldsHard
Three positive point charges sit at the corners of a right triangle: q₃ = 6 µC is at the right-angle corner, q₁ = 5 µC is 10 cm from it along one side and q₂ = 2 µC is 4 cm from it along the other side. Find the magnitude of the net electric force F on q₃.
q1 = 5 µCq2 = 2 µCq3 = 6 µCr13 = 10 cmr23 = 4 cm
F = N
3.Series & parallel resistorsMedium
Find the equivalent resistance Req seen by the source V1.
V1 = 6 VR1 = 15 ΩR2 = 15 ΩR3 = 3 ΩR4 = 3 Ω
Req = Ω
4.Series & parallel resistorsHard
Find the equivalent resistance Req seen by the source V1.
V1 = 15 VR1 = 5 ΩR2 = 4 ΩR3 = 12 ΩR4 = 20 ΩR5 = 30 ΩR6 = 6 Ω
Req = Ω
5.RC & RL transientsMedium
The inductor carries no current before the switch closes at t = 0. How long after the switch closes does the current reach 75% of its final value? Find t.
Vs = 5 VR = 22 ΩL = 33 mH
t = ms
6.RC & RL transientsHard
A timer starts charging an uncharged capacitor through a resistor from a 9 V supply at t = 0. It must trigger when the capacitor voltage reaches 5.69 V, exactly 1000 ms after the start. With C = 47 µF, find the resistance R needed.
Vs = 9 VVth = 5.69 VT = 1000 msC = 47 µF
R = kΩ
7.Magnetic fields & inductionMedium
An electron moving at 6 × 10⁶ m/s enters a uniform magnetic field at right angles and moves on a circle of radius 0.3412 cm. Find the magnetic flux density B.
m = 9.109 × 10⁻³¹ kg|q| = 1.602 × 10⁻¹⁹ Cv = 6 × 10⁶ m/sr = 0.3412 cm
B = mT
8.Magnetic fields & inductionHard
An alpha particle passes undeflected through a velocity selector with crossed fields E = 4 × 10⁴ V/m and B₁ = 0.25 T. It then enters a second region with only a magnetic field B₂ = 0.25 T, at right angles. Find the radius r of its path there.
E = 4 × 10⁴ V/mB1 = 0.25 TB2 = 0.25 Tm = 6.645 × 10⁻²⁷ kg|q| = 3.204 × 10⁻¹⁹ C
r = cm
9.AC impedance & phasorsMedium
A series RLC circuit is connected to a 230 V (rms), 200 Hz supply. Find the rms current I.
V = 230 V (rms)f = 200 HzR = 10 ΩL = 200 mHC = 2.2 µF
I = A
10.AC impedance & phasorsHard
A series RLC circuit is connected to a 24 V (rms), 500 Hz supply. Find the resonant frequency f0 of the circuit.
V = 24 V (rms)f = 500 HzR = 20 ΩL = 150 mHC = 1 µF
f0 = Hz
3Solutions
1.Coulomb’s law & electric fields
Answer: F = 44.05 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.
Charge after touching
q′ = (6 + 8)/2 = 7 µC
New force
F = 8.99 × 10⁹·(7 × 10⁻⁶)²/0.1² = 44.05 N
Answer
F = 44.05 N
Both spheres now carry the same sign, so they repel.
2.Coulomb’s law & electric fields
Answer: F = 72.62 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·5·6 × 10⁻¹²/0.1² = 26.97 N
F2 = k·2·6 × 10⁻¹²/0.04² = 67.42 N
Vector sum
F = √(26.97² + 67.42²) = 72.62 N
Answer
F = 72.62 N
3.Series & parallel resistors
Answer: Req = 19.29 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.
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 + 3 = 6 Ω
R2 ∥ 6 = 15·6/(15+6) = 4.286 Ω
Req = R1 + 4.286 = 15 + 4.286 = 19.29 Ω
Answer
Req = 19.29 Ω
4.Series & parallel resistors
Answer: Req = 8.446 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.
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 = 30 + 6 = 36 Ω
R4 ∥ 36 = 12.86 Ω
R3 + 12.86 = 24.86 Ω
R2 ∥ 24.86 = 3.446 Ω
Req = R1 + 3.446 = 5 + 3.446 = 8.446 Ω
Answer
Req = 8.446 Ω
5.RC & RL transients
Answer: t = 2.079 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.
Time constant and final current
Long after the switch closes the inductor behaves like a short circuit, so the final current is set by R alone.
τ = L/R = 33 mH / 22 Ω = 1.5 ms
i(∞) = Vs/R = 5/22 = 0.2273 A
Solve for the time
0.75 = 1 − e−t/τ → t = −τ·ln(1 − 0.75)
t = −1.5·ln(0.25) = 2.079 ms
Answer
t = 2.079 ms
6.RC & RL transients
Answer: R = 21.27 kΩ
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.
Required time constant
5.69 = 9·(1 − e−1000/τ) → τ = 1000/ln(9/(9 − 5.69))
τ = 1000/1 = 999.7 ms
Resistance
kΩ times µF gives milliseconds.
R = τ/C = 999.7/47 = 21.27 kΩ
Answer
R = 21.27 kΩ
7.Magnetic fields & induction
Answer: B = 9.999 mT
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).
Field from the radius
B = mv/(|q|r) = 9.109 × 10⁻³¹·6 × 10⁶/(1.602 × 10⁻¹⁹·0.003412) = 9.999 mT
Answer
B = 9.999 mT
8.Magnetic fields & induction
Answer: r = 1.327 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).
Selected speed
Undeflected: the electric force qE balances the magnetic force qvB.
v = E/B1 = 4 × 10⁴/0.25 = 160000 m/s
Radius in the second field
r = mv/(|q|B2) = 0.01327 m = 1.327 cm
Answer
r = 1.327 cm
9.AC impedance & phasors
Answer: I = 2.075 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|.
Reactances
ω = 2πf = 2π·200 = 1257 rad/s
XL = ωL = 1257·0.2 = 251.3 Ω
XC = 1/(ωC) = 1/(1257·2.2·10⁻⁶) = 361.7 Ω
Impedance
In series the impedances add as complex numbers: Z = R + j(XL − XC).
|Z| = √(R² + (XL − XC)²) = √(10² + (−110.4)²) = 110.8 Ω
Current
The same current flows through every element of a series circuit.
I = V/|Z| = 230/110.8 = 2.075 A
Answer
I = 2.075 A
10.AC impedance & phasors
Answer: f0 = 410.9 Hz
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|.
Resonance
At resonance the inductive and capacitive reactances cancel: ωL = 1/(ωC). The supply frequency does not matter.
f0 = 1/(2π√(LC)) = 1/(2π·√(0.15·1·10⁻⁶)) = 410.9 Hz
Answer
f0 = 410.9 Hz
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