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Physics HL · Chapter 19: Motion in Electric and Magnetic Fields

19.5 Beam Applications, Charge-to-Mass Ratio, and Cyclotron Logic

Connect field-motion equations to beam diagnostics: acceleration by potential difference, magnetic bending, q/m extraction, and cyclotron frequency control.

Estimated time: 34 minutes

Two-Stage Beamline Reasoning

Many instruments use two regions in sequence: first accelerate with electric potential difference, then bend in magnetic field. Stage 1 sets speed from energy gain. Stage 2 maps that speed and particle identity into trajectory radius. Keeping these stages separate makes multi-step exam problems much easier to organize.

qV = rac{1}{2}mv^2Rightarrow v = sqrt{ rac{2qV}{m}}

This non-relativistic relation is valid when speed is well below c.

Substitute this speed into magnetic radius relation to get direct parameter dependence. For fixed V and B, lighter ions bend more than heavier ones if charge state is the same. This is the core principle behind isotopic separation by magnetic analyzers.

Deriving the Charge-to-Mass Ratio Formula

Eliminate speed by combining qV = (1/2)mv^2 with r = mv/(|q|B). Rearranging gives the classic q/m expression used in electron q/m experiments. This relation is one of the clearest examples of why electric and magnetic stages are paired experimentally.

rac{|q|}{m} = rac{2V}{B^2r^2}

Measure V, B, and r experimentally, then infer q/m from geometry.

When q is known (for example singly ionized ions), the same formula gives mass. Conversely, if mass is known, it gives charge state. This dual use is why field-motion chapters are foundational for instrumentation topics later in physics and chemistry.

Cyclotron Frequency and the Relativistic Limit

In a cyclotron, particles gain energy from electric fields while magnetic fields keep them in near-circular paths. The drive frequency is matched to the magnetic revolution frequency f = |q|B/(2pi m). At high speeds relativity increases effective inertia, so synchronization drifts and simple non-relativistic cyclotron operation breaks down unless design modifications are introduced.

f = rac{|q|B}{2pi m}

Frequency depends on q/m and B, and is speed-independent only in the non-relativistic regime.

Simulation: Beam-Tuning and Radius Sensitivity

Use selector and magnetic modes together to see how tiny changes in q/m shift accepted speed and bend radius.

········································v (green), Fe (mint), Fm (pink), Fnet (yellow)

Selector speed E/B

2.00e+5 m/s

Speed mismatch

-2.50 %

Electric force

2.88e-16 N

Magnetic force

-2.81e-16 N

Net force

7.21e-18 N

Vertical acceleration

1.08e+9 m/s^2

Deflection at exit

0.08 cm

Force relation

Net force upward

Test Yourself

In a q/m experiment, V = 490 V, B = 1.2 mT, and semicircle radius R = 6.1 cm. Enter |q|/m.

Hint: Use |q|/m = 2V/(B^2 R^2).