PhysEduc › Class 12 Physics › Chapter 4: Moving Charges and Magnetism

Motion in a magnetic field

NCERT Class 12 Physics, Chapter 4: Moving Charges and Magnetism, §4.3. A short visual lesson: 2 narrated 3D videos, 1 interactive simulation and 2 quiz questions.

Going round in circles

Narrated video. Transcript:

Fire a proton into a uniform magnetic field, at right angles to the field. Here the field points into the screen, shown by the crosses.

The magnetic force q v × B is always perpendicular to the velocity. So it never speeds the proton up or slows it down. It only turns it.

A force perpendicular to the motion does no work. So the speed, and the kinetic energy, stay exactly the same. Only the direction keeps changing.

A force of constant size that always acts at right angles to the velocity: that is just what makes uniform circular motion. The proton goes round a circle.

The magnetic force supplies the centripetal force. So m v² over r equals q v B, which gives the radius: r equals m v over q B.

A faster particle moves in a bigger circle. A stronger field, or a larger charge, bends it into a smaller one.

The angular frequency is ω equals v over r, which is q B over m. The frequency is ν equals q B over 2πm, and the time for one turn is T equals 2πm over q B.

Look closely: v has cancelled out! A fast proton runs round a big circle, a slow one round a small circle, and both take exactly the same time.

Some numbers. A proton at 2 × 10⁶ metres per second in a field of 0.5 tesla: r equals 1.67 × 10⁻²⁷ times 2 × 10⁶, over 1.6 × 10⁻¹⁹ times 0.5. That is about 4.2 centimetres.

Its period is 2π times 1.67 × 10⁻²⁷, over 1.6 × 10⁻¹⁹ times 0.5: about 1.3 × 10⁻⁷ seconds. An electron in the same field would circle the other way round.

Helical paths

Narrated video. Transcript:

What if the velocity is not perpendicular to the field? Split it into two parts: v parallel, along B, and v perpendicular, across B.

The parallel part feels no force, since sin 0 is zero. So the particle keeps drifting along the field at a steady speed v cos θ.

The perpendicular part, v sin θ, is turned round in a circle of radius m v sin θ over q B, exactly as before.

Put the two together: the particle goes round and round while drifting along the field. Its path is a helix, like the thread of a screw.

The distance it moves along B in one turn is the pitch: p equals v parallel times T, which is 2πm v cos θ over q B.

Example: our proton, at 2 × 10⁶ metres per second, now enters the 0.5 tesla field at 60° to it. v perpendicular is 1.73 × 10⁶, so the radius is 0.866 times 4.2, about 3.6 centimetres.

v parallel is 1 × 10⁶ metres per second, and T is still 1.3 × 10⁻⁷ seconds. So the pitch is about 0.13 metres: 13 centimetres per turn.

Now an electron. It moves at 3 × 10⁷ metres per second, perpendicular to a field of 6 × 10⁻⁴ tesla. Take its mass as 9 × 10⁻³¹ kilogram.

r equals 9 × 10⁻³¹ times 3 × 10⁷, over 1.6 × 10⁻¹⁹ times 6 × 10⁻⁴. That is 2.7 × 10⁻²³ over 9.6 × 10⁻²³: 0.28 metre, or 28 centimetres.

Its frequency is v over 2πr: 3 × 10⁷ over 2π times 0.28, about 1.7 × 10⁷ hertz, or 17 megahertz. And its energy, ½ m v², is 4 × 10⁻¹⁶ joule, about 2.5 kilo electron volts.

Try it: circles and helices

Interactive simulation. Things to try:

  • At θ = 90° the proton goes round a circle. Press “Look along B” to see it face on.
  • Double the speed: the circle doubles in size, but the period T does not change.
  • Double the field: the circle halves and each turn takes half the time.
  • Set θ = 60°: the path becomes a helix. Compare the pitch with p = v cos θ × T.
  • Switch to the electron: it circles the opposite way.

Twice as fast

A proton moves in a circle in a uniform magnetic field. Its speed is doubled, with the field unchanged. What happens to the radius r of its path and its period T?

  1. r doubles; T doubles
  2. r doubles; T stays the same
  3. r doubles; T halves
  4. r stays the same; T halves
Answer

B. r = m v / q B, so r is proportional to v and doubles. But T = 2πm / q B has no v in it. The proton travels twice as far each turn at twice the speed, so T stays the same.

An electron’s circle

An electron (mass 9 × 10⁻³¹ kg, charge 1.6 × 10⁻¹⁹ C) moves at 3 × 10⁷ m/s perpendicular to a magnetic field of 6 × 10⁻⁴ T. What is the radius of its path?

  1. 2.8 cm
  2. 28 cm
  3. 2.8 m
  4. 520 m
Answer

B. r = m v / q B = (9 × 10⁻³¹ × 3 × 10⁷)/(1.6 × 10⁻¹⁹ × 6 × 10⁻⁴) = (2.7 × 10⁻²³)/(9.6 × 10⁻²³) ≈ 0.28 m = 28 cm. Using the proton’s mass by mistake gives about 520 m.

Summary

  • Radius (v ⊥ B): r = m v / q B
  • Angular frequency and period: ω = q B / m, T = 2πm / q B
  • Helix (v at θ to B): r = m v sin θ / q B, p = v cos θ × T
  • The magnetic force is perpendicular to v, so it does no work: speed and kinetic energy stay constant.
  • With v ⊥ B the path is a circle. Its period does not depend on the speed.
  • A velocity component along B is not affected, so the general path is a helix around the field lines.
  • Positive and negative charges circle in opposite senses.