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MotionLab
Moving charges feel a sideways push in a magnetic field — the force that makes electric motors spin.
Unlike gravity or electric forces, the magnetic force is always perpendicular to both the velocity and the magnetic field — this is why it can change a particle's direction but never its speed, causing charged particles to move in circles (or spirals) in uniform magnetic fields.
When a charge moves parallel to the field lines (θ = 0° or 180°), the magnetic force is zero — it only feels the full force when moving perpendicular (θ = 90°). This angle dependence is why particle accelerators and mass spectrometers are carefully designed to control the orientation of particles relative to the field.
Magnetic force (N)
0
F = |q|vB sin(θ)
What you entered
sin(θ)
sin(90°)= 1F = |q|vB sin(θ)
|1.60e-19| × 1000000 × 0.5 × 1= 8.0100e-14 NResult
Magnetic force (N): 0
A charge of 1.60e-19 C moving at 1.00e+6 m/s through a 0.5 T field at 90° experiences a force of 8.0100e-14 N.