Lorentz Force Calculator
Find magnetic force on a charge moving perpendicular to B: F = |q|vB
Parameters
Controls
Calculated Values
Examples
Electron in 0.5 T
v = 10⁶ m/s perpendicular to B.
Proton in 1 T
Compare heavier mass, same speed.
Visualization
Lorentz Force on a Moving Charge
The Lorentz force is the magnetic force on a point charge q moving with velocity v in a magnetic field B: F⃗ = q(v⃗ × B⃗). The cross product means F is perpendicular to both v and B. Magnitude F = |q|vB sin θ, where θ is the angle between v and B. The most important case for circular motion is θ = 90°, giving F = |q|vB.
Direction is found with the right-hand rule for positive charge: point thumb along v, curl fingers toward B — palm pushes in the direction of F. Electrons (q < 0) curve the opposite way. In a uniform B field with v ⊥ B, the particle moves in a circle of radius r = mv/(|q|B) because qvB supplies centripetal force mv²/r.
Crucially, magnetic force does no work on the particle because F ⊥ v at every instant (W = ∫F·v dt = 0). Speed |v| stays constant in a pure magnetic field; only direction changes. If v has a component parallel to B, the path is a helix: circular motion in the perpendicular plane plus uniform drift along B.
The full electromagnetic Lorentz force includes the electric part: F⃗ = q(E⃗ + v⃗ × B⃗). Velocity selectors in mass spectrometers use crossed E and B so only particles with v = E/B pass straight through; all others are deflected.
Typical magnitudes: an electron (|q| = 1.6×10⁻¹⁹ C) at v = 10⁶ m/s in B = 0.5 T feels F ≈ 8×10⁻¹⁴ N — small but enough for tight curvature in particle detectors. Earth's field (~50 μT) gently steers cosmic rays; auroras come from charged solar wind in the magnetosphere.
Class 12 NCERT Moving Charges and Magnetism covers Lorentz force, circular motion in B, and cyclotron frequency ω = |q|B/m. JEE problems often combine energy conservation (electric) with magnetic deflection.
Key Concepts
- F⃗ = q(v⃗ × B⃗)
- F = |q|vB when v ⊥ B
- Right-hand rule for direction
- No work: F ⊥ v
- Circular path r = mv/(|q|B)
- Helix if v∥B ≠ 0
Real-World Applications
- Cyclotron and mass spectrometer
- Cloud chamber / bubble chamber tracks
- Magnetic confinement (fusion research)
- Aurora and Van Allen belts
- Class 12–JEE moving charge problems
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Physics Equations
Step-by-Step Solution
See how the main results are calculated.
Step 1: Vector Form
Equation:
Explanation:
Lorentz force is a cross product; magnitude depends on angle between v and B.
Step 2: Perpendicular Case
Equation:
Explanation:
When v ⊥ B, sin θ = 1 so F = |q|vB.
Step 3: Substitute Values
Calculation:
Explanation:
Charge is positive; use |q| for magnitude.
Step 4: Numerical Result
Calculation:
Result:
Step 5: Direction (Right-Hand Rule)
Thumb → v, fingers → B, palm → F (for q > 0).
Explanation:
Negative charge deflects opposite to the RHR result.
Step 6: Physical Check
F ⊥ v ⇒ magnetic force does no work; speed unchanged in pure B.
Explanation:
Particle moves in circle or helix; F provides centripetal acceleration.
Frequently Asked Questions (FAQ)
Why does magnetic force do no work?
F is always perpendicular to v, so F·v = 0. Kinetic energy stays constant in a static B field; only momentum direction changes.
Relativistic speeds?
Use relativistic momentum p = γmv and F = dp/dt; radius becomes r = p/(|q|B).
What if v is parallel to B?
Magnetic force is zero (sin 0° = 0). Particle moves along field lines at constant speed.
Units check for F = qvB?
C × (m/s) × T = C·m/s × (N·s)/(C·m) = N. Tesla is defined so field relations are SI-consistent.
How to remember direction?
Use RHR for positive charge; reverse for electrons. Alternatively use vector cross product with unit vectors.
Practice MCQs
- Lorentz force magnitude (v ⊥ B):
- Magnetic force on stationary charge:
- Work done by magnetic force on particle:
- Positive charge in B into page, v right:
- Units of B:
- Helical path when v has component || B:
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