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Physics · Ch 4 — Moving Charges and Magnetism

Magnetic Force

4.2

Magnetic Force

Magnetic Force: The Lorentz Force

Magnetism is a force that acts on moving charges. A stationary charge experiences no magnetic force. The magnetic force on a charge depends on three things: the charge itself, its velocity, and the magnetic field it moves through.

The Lorentz Force Law

The total force on a charged particle in an electric field E⃗\vec{E} and a magnetic field B⃗\vec{B} is the Lorentz force:

F⃗=q(E⃗+v⃗×B⃗)\vec{F} = q(\vec{E} + \vec{v} \times \vec{B})

Here:

  • qq is the charge of the particle.
  • v⃗\vec{v} is its velocity.
  • E⃗\vec{E} is the electric field.
  • B⃗\vec{B} is the magnetic field.
  • ×\times denotes the vector cross product.

The electric part qE⃗q\vec{E} is independent of velocity. The magnetic part q(v⃗×B⃗)q(\vec{v} \times \vec{B}) depends on velocity and is always perpendicular to both v⃗\vec{v} and B⃗\vec{B}.

Direction of Magnetic Force

The magnetic force F⃗m\vec{F}_m on a moving charge is given by:

F⃗m=q(v⃗×B⃗)\vec{F}_m = q(\vec{v} \times \vec{B})

Its direction is given by the right-hand rule:

  • Point your fingers in the direction of v⃗\vec{v}.
  • Curl them toward B⃗\vec{B}.
  • Your thumb points in the direction of v⃗×B⃗\vec{v} \times \vec{B}.
  • For a positive charge (q>0q > 0), the force is along the thumb.
  • For a negative charge (q<0q < 0), the force is opposite to the thumb.
Magnitude of Magnetic Force

The magnitude of the magnetic force is:

Fm=∣q∣vBsin⁡θF_m = |q| v B \sin\theta

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

  • If v⃗\vec{v} is parallel to B⃗\vec{B} (θ=0∘\theta = 0^\circ or 180∘180^\circ), sin⁡θ=0\sin\theta = 0, so Fm=0F_m = 0. No magnetic force acts.
  • If v⃗\vec{v} is perpendicular to B⃗\vec{B} (θ=90∘\theta = 90^\circ), sin⁡θ=1\sin\theta = 1, so Fm=∣q∣vBF_m = |q| v B — the maximum possible force.
Key Properties of Magnetic Force
  • Always perpendicular to both velocity and magnetic field: F⃗m⊥v⃗\vec{F}_m \perp \vec{v} and F⃗m⊥B⃗\vec{F}_m \perp \vec{B}. …