Moving Charges and Magnetism

Physics · Class 12

Lesson 12 of 12 · 18 min

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Must-know facts

18 facts

  1. 1Magnetic force F = qvB sin θ: zero for a charge at rest or moving along B, largest at right angles.
  2. 2The magnetic force is perpendicular to v, so it does no work: the speed and kinetic energy never change.
  3. 3Circle in a uniform field: r = mv/qB. The period T = 2πm/qB does not depend on the speed.
  4. 4Helix when v has a part along B: pitch p = v∥ × 2πm/qB.
  5. 5Force on a wire: F = I l × B; zero when the wire lies along B.
  6. 6Biot–Savart: dB = (μ₀/4π) I dl sin θ/r²; no field along the line of the element.
  7. 7μ₀ = 4π × 10⁻⁷ T m A⁻¹, and μ₀ε₀ = 1/c².
  8. 8Centre of a coil: B = μ₀NI/2R. On its axis: B = μ₀NIR²/2(x² + R²)^(3/2).
  9. 9Long straight wire: B = μ₀I/2πr, field lines are closed circles.
  10. 10Thick wire with uniform current: B ∝ r inside, B ∝ 1/r outside, largest at the surface.
  11. 11Long solenoid: B = μ₀nI inside, uniform, independent of radius; about zero outside.
  12. 12Parallel wires: f = μ₀I₁I₂/2πd per metre; same direction attract, opposite repel.
  13. 131 A is the current giving 2 × 10⁻⁷ N per metre between wires 1 m apart.
  14. 14Current loop: m = NIA; τ = m × B; net force zero in a uniform field.
  15. 15Stable equilibrium when m is along B, unstable when opposite.
  16. 16Far field of a loop: (μ₀/4π)(2m/x³) on the axis, half that in the plane of the loop.
  17. 17MCG: kφ = NIAB in a radial field; current sensitivity NAB/k.
  18. 18Ammeter = galvanometer + small shunt in parallel; voltmeter = galvanometer + large resistance in series.

Common traps

Where marks are lost

Using the left-hand or right-hand rule for a positive charge when the particle is an electron.

Work out v × B for a positive charge, then reverse the force for a negative one.

Thinking a magnetic field speeds up or slows down a charge.

F ⟂ v, so no work is done; only the direction changes. Energy can change only through an electric field.

Believing a faster particle takes longer to go round its circle.

r ∝ v but the path length grows with it; T = 2πm/qB is independent of speed.

Using B = μ₀I/2πr for the centre of a loop, or μ₀I/2R for a straight wire.

Straight wire: μ₀I/2πr. Loop centre: μ₀I/2R (times N for a coil). The π sits only in the wire formula.

Taking n in B = μ₀nI as the total number of turns.

n is turns per metre: n = N/L. Stacked layers add their turns before dividing by length.

Expecting like currents to repel, as like charges do.

Parallel currents attract, antiparallel currents repel: the reverse of electrostatics.

Measuring θ in τ = NIAB sin θ from the plane of the coil.

θ is between B and the normal (the area vector). With B in the plane of the coil, θ = 90° and the torque is greatest.

Connecting the shunt in series or the large resistance in parallel.

Ammeter: small resistance in parallel (it carries the extra current). Voltmeter: large resistance in series (it limits the current).

Assuming more turns always make a meter more sensitive to voltage.

Doubling N doubles φ/I but also doubles the coil's resistance, so φ/V can stay the same.

Formulas

17 to know

Lorentz force

F = q(E + v × B)

Magnetic part qvB sin θ, perpendicular to v and B.

Force on a straight wire

F = I l × B, |F| = IlB sin θ

l points along the current; B is the external field.

Radius of circular path

r = mv/(qB)

v perpendicular to B; r ∝ momentum.

Cyclotron frequency

ν = qB/(2πm), T = 2πm/(qB)

Independent of speed and radius.

Pitch of the helix

p = v∥T = 2πm v∥/(qB)

v∥ is the velocity component along B.

Biot–Savart law

dB = (μ₀/4π) I dl sin θ/r²

μ₀/4π = 10⁻⁷ T m A⁻¹; direction of dl × r.

Axis of a circular loop

B = μ₀IR²/[2(x² + R²)^(3/2)]

Multiply by N for N turns.

Centre of a circular coil

B = μ₀NI/(2R)

A semicircle gives half of a full loop.

Ampere's circuital law

∮B·dl = μ₀I

Simple form BL = μ₀Iₑ when symmetry allows.

Long straight wire

B = μ₀I/(2πr)

Inside a thick wire with uniform current: B = μ₀Ir/(2πa²).

Long solenoid

B = μ₀nI

n = turns per unit length.

Force between parallel wires

f = μ₀I₁I₂/(2πd)

Per unit length; like currents attract.

Torque on a coil

τ = m × B, τ = NIAB sin θ

m = NIA; θ between m and B.

Dipole field of a loop

B = (μ₀/4π)(2m/x³) axial, (μ₀/4π)(m/x³) in plane

Valid for x ≫ R.

Galvanometer

kφ = NIAB, φ/I = NAB/k, φ/V = NAB/(kR)

k = torsional constant of the spring.

Ammeter shunt

rₛ = I_G R_G/(I − I_G)

Follows from equal voltage across G and the shunt; I_G is the full-scale current of G.

Voltmeter series resistance

R = V/I_G − R_G

V is the full-scale voltage wanted.

Key terms

17 terms

Magnetic field (B)
A vector field set up by currents and moving charges, measured by the force it puts on a moving charge; unit tesla.
Tesla
The field that exerts 1 N on 1 C moving at 1 m/s at right angles to it; 1 gauss = 10⁻⁴ T.
Lorentz force
The total force q(E + v × B) on a charge in electric and magnetic fields.
Cyclotron frequency
The rate qB/2πm at which a charge circles in a uniform magnetic field, the same at every speed.
Pitch
The distance a charge moves along B during one turn of its helical path.
Current element
A tiny length dl of wire with its current, I dl, treated as a vector source of field.
Permeability of free space (μ₀)
The constant in the Biot–Savart law, 4π × 10⁻⁷ T m A⁻¹.
Amperian loop
A closed path chosen so that B is tangential and constant, or normal, or zero along its parts, making Ampere's law easy to apply.
Solenoid
A long, closely wound helical coil whose inside field is uniform and along its axis.
Ampere (unit)
The steady current that gives 2 × 10⁻⁷ N per metre between two long parallel wires 1 m apart in vacuum.
Magnetic moment (m)
NIA for a current loop, along its area vector; unit A m².
Magnetic dipole
A current loop seen from far away; its field has the same form as an electric dipole's.
Radial field
A field whose lines point along radii of the coil's axis, so the coil's plane always lies along B.
Torsional constant (k)
The restoring torque of the galvanometer spring per unit angle of twist.
Shunt
A small resistance put in parallel with a galvanometer so it can measure large currents as an ammeter.
Current sensitivity
Deflection per unit current, φ/I = NAB/k.
Voltage sensitivity
Deflection per unit voltage, φ/V = NAB/(kR).
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