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Magnetic Force on a Moving Charge

Calculate the force on a charged particle moving through a magnetic field.
The basis of electric motors and particle accelerators.

Need to calculate, not just reference? Use the interactive version. Open Magnetic Force Calculator →

The Formula

F = qvB × sin(θ)

A charged particle moving through a magnetic field experiences a force perpendicular to both its velocity and the field. This force changes the particle's direction but not its speed.

Variables

SymbolMeaning
FMagnetic force (Newtons)
qElectric charge of the particle (Coulombs)
vVelocity of the particle (m/s)
BMagnetic field strength (Tesla)
θAngle between velocity and magnetic field

Example 1

A proton (q = 1.6 × 10⁻¹⁹ C) moves at 2 × 10⁶ m/s perpendicular to a 0.5 T field

θ = 90°, so sin(90°) = 1

F = 1.6 × 10⁻¹⁹ × 2 × 10⁶ × 0.5 × 1

F = 1.6 × 10⁻¹³ N

Example 2

An electron (q = 1.6 × 10⁻¹⁹ C) moves at 3 × 10⁵ m/s at 30° to a 0.2 T field

F = 1.6 × 10⁻¹⁹ × 3 × 10⁵ × 0.2 × sin(30°)

F = 1.6 × 10⁻¹⁹ × 3 × 10⁵ × 0.2 × 0.5

F = 4.8 × 10⁻¹⁵ N

When to Use It

Use the magnetic force formula when:

  • Calculating forces on current-carrying wires in motors
  • Understanding how particle accelerators bend charged beams
  • Analyzing the motion of charged particles in magnetic fields
  • Designing mass spectrometers and cyclotrons

Key Notes

  • Formula: F = qvB sinθ: F is the magnetic force (N), q is the charge (C), v is the speed (m/s), B is the magnetic field (T), and θ is the angle between the velocity and the field.
  • Direction from the right-hand rule: Point fingers in the direction of v, curl them toward B, and the thumb points in the direction of F for positive charges. For negative charges, the force is reversed.
  • Maximum and zero force: Force is maximum (F = qvB) when v ⊥ B (θ = 90°). Force is zero when v ∥ B (θ = 0° or 180°). A charge moving parallel to a magnetic field experiences no force.
  • Magnetic force does no work: The magnetic force is always perpendicular to the velocity, so it changes the direction of motion but never the speed or kinetic energy of a charged particle.
  • Circular motion in a uniform field: A charged particle moving perpendicular to a uniform magnetic field travels in a circle with radius r = mv/(qB). Particle accelerators and mass spectrometers use this principle.

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