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Formulas/physics/Moving Charges/Lorentz Magnetic Force

Lorentz Magnetic Force

Force on a point charge q moving with velocity v in field B. Always perpendicular to v — magnetic force does no work and cannot change kinetic energy.
Class 12
Derivation

Statement

A charge qq moving with velocity v⃗\vec{v} in magnetic field B⃗\vec{B} experiences:

F⃗=q (v⃗×B⃗)\boxed{\vec{F} = q\,(\vec{v} \times \vec{B})}

Direction

The cross product v⃗×B⃗\vec{v} \times \vec{B} gives a vector perpendicular to both v⃗\vec{v} and B⃗\vec{B}. For positive qq, F⃗\vec{F} is in the direction of v⃗×B⃗\vec{v} \times \vec{B}. For negative qq, it is opposite.

Use the right-hand rule: point fingers along v⃗\vec{v}, curl toward B⃗\vec{B} — thumb points along F⃗\vec{F} for positive charge.

Magnitude

F=qvBsin⁡θF = qvB\sin\theta

where θ\theta is the angle between v⃗\vec{v} and B⃗\vec{B}.

  • F=0F = 0 when v⃗∥B⃗\vec{v} \parallel \vec{B} (θ=0\theta = 0): no force.
  • F=qvBF = qvB (maximum) when v⃗⊥B⃗\vec{v} \perp \vec{B} (θ=90°\theta = 90°).

Magnetic Force Does No Work

Since F⃗⊥v⃗\vec{F} \perp \vec{v} always, the power delivered:

P=F⃗⋅v⃗=0P = \vec{F} \cdot \vec{v} = 0

Magnetic force can change the direction of motion but never the speed or kinetic energy.

Note
This is why a magnetic field cannot accelerate a particle from rest — it needs an initial velocity to exert any force at all.