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.
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).