Calculate Lorentz force, magnetic force on a wire, force between parallel conductors, and solenoid pull force. Covers all key EM force equations.
The Electromagnetic Force Calculator computes the mechanical force exerted on charged particles and current-carrying conductors in magnetic fields. It covers four fundamental scenarios: the Lorentz force on a moving charge, the force on a current-carrying wire in a field, the force between two parallel conductors, and the pull force of a solenoid/electromagnet. That makes it a practical first-pass check for motors, relays, bus bars, coils, and other real electromagnetic devices. It is useful when you want one force estimate before committing to a more detailed field model.
Electromagnetic forces are the foundation of motors, generators, relays, speakers, and countless other devices. Understanding these forces helps engineers design efficient actuators, select appropriately sized electromagnets, and predict mechanical behavior of circuits in strong magnetic fields.
Enter your parameters for any of the four calculation modes to instantly see the resulting force, along with component breakdowns and practical context for the magnitude of force produced. It is a quick way to compare the same magnetic idea across charges, wires, conductors, and solenoids.
Use this calculator when you want one place to compare the common electromagnetic force formulas instead of treating each case as a separate problem. It is useful for actuator sizing, motor intuition, and quick checks on whether a current-and-field combination is mechanically meaningful in wires, coils, and solenoids. That makes it easier to sanity-check a force before building hardware or choosing a different geometry.
Lorentz: F = qvB sin(θ). Wire: F = BIL sin(θ). Parallel Conductors: F/L = μ₀I₁I₂ / (2πd). Solenoid: F = B²A / (2μ₀). Where q = charge (C), v = velocity (m/s), B = magnetic field (T), I = current (A), L = length (m), d = spacing (m), A = area (m²), μ₀ = 4π×10⁻⁷ T·m/A.
Result: 5.0 N
A 1m wire carrying 10A perpendicular to a 0.5T field: F = 0.5 × 10 × 1 × sin(90°) = 5.0 N. This is roughly the weight of a 500g object — enough to drive a small DC motor.
The Lorentz force F = qvB sin(θ) governs particle accelerators, mass spectrometers, and CRT displays. A charged particle entering a uniform magnetic field perpendicular to its velocity follows a circular path with radius r = mv/(qB). This principle separates isotopes by mass, focuses electron beams, and confines plasma in fusion reactors.
When a straight conductor of length L carrying current I sits in a uniform magnetic field B, it experiences force F = BIL sin(θ). This is the operating principle of every electric motor. In practice, motors use many turns (N) of wire, so the total force multiplies by N. The resulting torque τ = NBIA sin(θ) drives the rotor.
Electromagnetic forces power everything from hard drive actuators (voice coil motors) to maglev trains (repulsive levitation at 500+ km/h). Relay coils use solenoid force to switch high-current circuits with low-power control signals. Electromagnetic brakes on roller coasters and trains use eddy-current forces for smooth, frictionless deceleration. Understanding these forces enables efficient design across industries.
The Lorentz force is the force on a charged particle moving through electric and magnetic fields: F = q(E + v×B). The magnetic component is F = qvB sin(θ), where θ is the angle between velocity and field vectors.
Parallel wires carrying current in the same direction attract each other. Wires carrying current in opposite directions repel. This is Ampère's force law and is how the ampere was historically defined.
One Tesla is very strong — an MRI machine is 1.5–3T. Earth's magnetic field is about 50 μT. Refrigerator magnets are about 5 mT. Neodymium magnets reach 1–1.4T at their surface.
Solenoid force depends on current (more turns × more amps = stronger field), core material (ferromagnetic cores multiply field 100-1000×), air gap (force drops rapidly with gap), and cross-sectional area. F = B²A / (2μ₀).
The force is maximum when the motion/current is perpendicular to the field (sin 90° = 1) and zero when parallel (sin 0° = 0). This is why motor windings are oriented to maximize the perpendicular component at all rotor positions.
DC motors use F = BIL on rotor conductors to produce torque. The commutator reverses current direction every half turn to maintain rotation. Brushless motors use electronic switching instead, varying the field to keep force perpendicular.