Electricity and Magnetism: Fields, Induction and Magnetic Circuits
Magnetic field and magnetic circuits
Biot–Savart and Ampere answer different versions of the same practical question: what magnetic field does current create? Ampere is the shortcut only when symmetry makes ∮H·dl easy. In a magnetic circuit, mmf NI drives flux through reluctance, much like voltage drives current through resistance. The analogy is helpful, but remember that leakage flux and nonlinear B-H behaviour make the magnetic circuit imperfect.
Faraday, Lorentz force and Maxwell equations
Faraday law is the bridge from magnetism to instrumentation: changing flux creates induced emf, while Lorentz force explains the force on a moving charge. Maxwell’s equations unify the static and dynamic cases. For exam problems, first identify whether the source is charge, current or time-varying flux; that choice usually tells you which equation to start with.
| Law | Differential idea | Use |
|---|---|---|
| Gauss electric | Divergence of D follows charge density | Charge-field relation |
| Faraday | Curl E follows changing B | Induced emf |
| Ampere-Maxwell | Curl H follows current and changing D | Dynamic magnetic field |
Boundary conditions and electromagnetic energy
At an interface, normal flux density is controlled by free surface charge, while tangential magnetic field is controlled by surface current. These conditions are often faster to use than re-solving the full field equations. Electromagnetic power flow is represented by the Poynting vector S = E × H; its direction tells you where energy is flowing.
Key takeaways
- Choose Gauss or Ampere from symmetry, not from keywords.
- Keep E, D, B, H and flux conceptually separate; constitutive relations connect them.
- A changing magnetic flux can induce emf; this is central to inductive sensing and transformers.
- Use boundary conditions and the Poynting vector when the question is about interfaces or energy flow.
Practice questions (8)
Attempt each one before opening the answer. Every explanation names the tempting wrong option as well as the right one, because that is where marks are lost.
For a point charge in a homogeneous medium, the magnitude of electric field varies with distance r as:
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Answer: C — 1/r²
Coulomb’s law gives E proportional to 1/r².Which law is generally the most convenient for finding the electric field of a uniformly charged infinite plane?
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Answer: A — Gauss law
Planar symmetry makes a Gaussian pillbox reduce the flux calculation to a simple algebraic relation.A magnetic circuit has N = 200 turns carrying 0.5 A. Its magnetomotive force is:
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Answer: B — 100 AT
MMF = NI = 200 × 0.5 = 100 ampere-turns.Which statements about electromagnetic quantities are correct?
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Answer: A — D = εE in a linear isotropic medium; C — E = −∇V in an electrostatic field; D — B is flux density, while magnetic flux is its surface integral
The constitutive relation depends on the medium; B and H are not universally equal. Electric potential gives E through its negative gradient in electrostatics, and flux is the surface integral of B.If magnetic flux through a single-turn loop changes from 0.02 Wb to 0.01 Wb in 0.005 s, the magnitude of average induced emf is:
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Answer: C — 2 V
Faraday's law gives |e| = |ΔΦ|/Δt. The flux changed by 0.01 − 0.02 = −0.01 Wb, so |e| = 0.01/0.005 = 2 V. The 4 V option comes from using the initial flux 0.02 Wb in place of the change in flux, which is the usual slip: an induced emf responds to how much the flux moved, never to how much of it there was.The Poynting vector represents:
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Answer: B — Electromagnetic power flow per unit area
S = E × H gives electromagnetic power flow density and its direction.For a boundary with no free surface charge, which normal-component condition follows from Gauss law?
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Answer: A — Dn1 = Dn2
The normal component of D changes by the free surface charge density, so with zero free surface charge it is continuous.An air-core solenoid has 1000 turns and carries 2 A. If its ideal magnetic-circuit length is 0.5 m, what is NI/l in A/m?
Numerical answer — type the value.
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Answer: 4000
For an ideal magnetic circuit the magnetic field intensity is H = NI/l, so H = (1000 × 2)/0.5 = 4000 A/m. The quantity in the denominator is the mean magnetic path length in metres, not the number of turns — dividing by N instead is the common error and yields 2 A/m.