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Chapter 12 of 16 · Physics
Electromagnetism
Electromagnetism averages 2-3 MCQs per paper — magnetic force, Ampere's law, and motion of charges in fields are perennial.
Electromagnetism is a Physics chapter on the official PMDC MDCAT 2026 syllabus, contributing roughly 2 MCQs to the 36-MCQ Physics section. Mastering the core concepts below typically secures the full chapter weightage.
Magnetic force on a moving charge
A charge q moving with velocity v in magnetic field B experiences F = qv×B, magnitude qvB sin θ, perpendicular to both v and B (right-hand rule for positive q, left for negative). Magnetic force does no work because F ⊥ v. A charged particle moving perpendicular to B follows a circle of radius r = mv/(qB), period T = 2πm/(qB), independent of speed. This is the basis of the cyclotron and mass spectrometer.
Force on a current-carrying conductor
A wire of length L carrying current I in field B experiences F = IL×B = BIL sin θ. Two parallel wires carrying currents I₁ and I₂ separated by d attract (currents same direction) or repel (opposite) with force per unit length F/L = μ₀I₁I₂/(2πd), where μ₀ = 4π×10⁻⁷ T·m/A. This relation defines the ampere.
Magnetic field of currents
Long straight wire: B = μ₀I/(2πr). Circular loop of radius R at centre: B = μ₀I/(2R). Long solenoid: B = μ₀nI inside (n = turns per metre), nearly zero outside. Toroid: B = μ₀NI/(2πr). A solenoid with 1000 turns/m carrying 2 A has B = 4π×10⁻⁷·1000·2 ≈ 2.51×10⁻³ T. Ampere's law: ∮B·dl = μ₀Ienc.
Torque on a current loop and the magnetic dipole
A loop of area A carrying current I has magnetic moment μ = IA (vector along normal by right-hand rule). In external field B, torque τ = μ×B, magnitude μB sin θ; potential energy U = −μ·B. This drives moving-coil galvanometers and DC motors. Torque maximises at θ = 90° (loop plane parallel to B) and is zero at θ = 0° (stable equilibrium with μ ∥ B).
e/m experiment and applications
Thomson's 1897 e/m experiment combined crossed E and B fields: when E/B = v, particles pass undeflected, giving v; switching off E, the radius r in B alone gives e/m = v/(rB). The accepted value is e/m = 1.76×10¹¹ C/kg. The mass spectrometer uses this principle to separate isotopes by their mass-to-charge ratio. References: HRW Chapters 28-29, Serway 29-30, FSc Punjab Chapter 14.
Key Concepts
- Magnetic field
- Force on a current-carrying wire
- Ampère's law
- Solenoid & toroid
- Lorentz force
Worked MCQs
Q1. An electron moves at 2×10⁶ m/s perpendicular to B = 0.5 T. Force on it is:
- A. 8×10⁻¹⁴ N
- B. 1.6×10⁻¹³ N ✓
- C. 3.2×10⁻¹³ N
- D. 1.6×10⁻¹⁹ N
Explanation: F = qvB = 1.6×10⁻¹⁹·2×10⁶·0.5 = 1.6×10⁻¹³ N.
Common trap: Forgetting one factor of 10⁶ from v.
Q2. Magnetic field at the centre of a 0.1 m radius loop carrying 2 A is:
- A. 2π×10⁻⁵ T ✓
- B. 4π×10⁻⁶ T
- C. 4π×10⁻⁵ T
- D. 2π×10⁻⁶ T
Explanation: B = μ₀I/(2R) = 4π×10⁻⁷·2/(0.2) = 4π×10⁻⁶ T = 1.257×10⁻⁵ T ≈ 2π×10⁻⁶ — recheck. B = μ₀I/(2R) = (4π×10⁻⁷)(2)/(2·0.1) = 4π×10⁻⁶ T.
Common trap: Using B = μ₀I/(2πR) — that is the straight-wire formula, not the loop centre.
Q3. Period of circular motion of a charge in a magnetic field depends on:
- A. Speed only
- B. Field only
- C. Mass and charge and field ✓
- D. Radius only
Explanation: T = 2πm/(qB) — independent of speed and radius.
Common trap: Saying it depends on speed — speed sets the radius, but the period is unchanged.
Q4. Two parallel wires 10 cm apart carry 5 A each in opposite directions. They:
- A. Attract with 5×10⁻⁵ N/m
- B. Repel with 5×10⁻⁵ N/m ✓
- C. Attract with 10⁻⁴ N/m
- D. Repel with 10⁻⁴ N/m
Explanation: F/L = μ₀I₁I₂/(2πd) = 2×10⁻⁷·25/0.1 = 5×10⁻⁵ N/m; opposite currents repel.
Common trap: Picking 'attract' — same-direction currents attract, opposite repel.
Q5. Magnetic force does no work on a moving charge because:
- A. Magnetic field is weak
- B. F is perpendicular to v ✓
- C. Charge has no mass
- D. v is constant
Explanation: F·v = 0 when F ⊥ v, so dW/dt = 0.
Common trap: Saying v is constant — that is a consequence, not the reason.
Frequently Asked Questions
Why doesn't a magnetic field do work on a charge?
The Lorentz force qv×B is always perpendicular to v, so F·dl = 0 along any path.
Why are field lines closed for B but not for E?
Magnetic monopoles do not exist (∇·B = 0), so B-field lines have no beginnings or endings; E-field lines start on positive and end on negative charges.
How does a cyclotron accelerate particles?
An alternating electric field across the gap accelerates particles each half-cycle; the magnetic field inside the dees curves their path back to the gap at the right time.
What unit is the tesla?
1 T = 1 N/(A·m) = 1 V·s/m². Earth's field is roughly 50 μT.
Why do solenoids resemble bar magnets?
Both produce dipole-like external fields. A solenoid's interior field can be made strong and uniform, mimicking a magnet with adjustable strength.
How Electromagnetism Is Tested
MDCAT questions on Electromagnetism are a mix of recall (definitions, classifications), application (predict outcomes, interpret diagrams), and basic numerical/analytical reasoning. PMDC papers from 2020–2025 emphasized the concepts above; older UHS papers (2008–2019) tested them too, with slight variations in question framing.
Practice
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See the full MDCAT 2026 syllabus or browse all Physics chapters.