The Lorentz Force: A Moving Charge in a Magnetic Field
1 · Predict
A charged particle moves through a uniform magnetic field region. Does the magnetic force on it depend on the particle's speed, or only on the field strength?
- The force depends only on the field strength, not speed.
- The magnetic force doesn't depend on either quantity in a simple way.
- The force depends on both the field strength and the particle's speed — faster particles feel a stronger magnetic force.
2 · Set Up
- Open the qv-cross-b preset and press Reset. The field region has a fixed Bz = 0.12 T; the test charge is q = 3×10⁻¹⁰ C.
- Enable the force-magnitude readout on the test charge.
- Set the test charge's velocity components for each trial and record the force magnitude.
3 · Collect Data
| Velocity x-component v_x (m/s) | Velocity y-component v_y (m/s) | Force magnitude F (µN) |
|---|---|---|
| 200000.00 | 150000.00 | |
| 100000.00 | 200000.00 | |
| 300000.00 | 0.00 |
Plot force magnitude F (y-axis) against speed |v| = √(v_x² + v_y²) (x-axis) for your three trials.
4 · Analyze
- For one trial, compute |F| = |q|·|B|·|v| using q = 3×10⁻¹⁰ C, B = 0.12 T, |v| = √(v_x² + v_y²). Compare to the table.
- Explain why the magnetic force magnitude depends on the particle's total speed |v|, not on the direction of its velocity — even though the force's direction does depend on which way it's moving.
5 · Extend
- The magnetic force is always perpendicular to the velocity (F = qv×B), so it can change a particle's direction but never its speed. Explain why a magnetic field alone can never speed up or slow down a charged particle, only steer it.
- A charged particle moving perpendicular to a uniform magnetic field travels in a circle, because the magnetic force always points toward the circle's center. Explain, using F = qvB, why a faster particle in the same field traces a bigger circle.
The Physics Behind This Experiment
Lorentz Force (Magnetic)
A charge q moving with velocity v through a magnetic field B experiences a force F = qv×B, perpendicular to both its velocity and the field. Its magnitude is |F| = |q||v||B| when v is perpendicular to B.
Electromagnetism
- Coulomb's Law: The Field Around a Point Charge
- Electric Dipole: Superposing Two Opposite Charges
- Field of a Finite Line of Charge
- Parallel-Plate Capacitor: Charge and Energy Storage
- An Isolated Charged Sphere
- A Real Capacitor Matching a Circuit Component
- Magnetic Field of a Current-Carrying Wire
- Magnetic Field Inside a Solenoid
- Faraday's Law: EMF from a Changing Field
- Faraday's Law: EMF from a Changing Area
- Faraday's Law: Both Field and Area Changing at Once
- RLC Impedance vs. Drive Frequency: Finding Resonance