Electromagnetic Force Calculator

Calculate Lorentz force, magnetic force on a wire, force between parallel conductors, and solenoid pull force. Covers all key EM force equations.

Force on Wire
1.000000 N
BIL sin(90°)
Weight Equivalent
0.101937 kg
Force / 9.81 m/s²
Force (mN)
1,000.0000 mN
Millinewtons
Force (lbf)
0.224800 lbf
Pounds-force
μ₀ (permeability)
1.2566 × 10⁻⁶ T·m/A
Vacuum permeability constant
Force Magnitude Scale:
pN
nN
μN
mN
N
kN
Angle (°)sin(θ)Force% of Max
0°0.00000.0000e+0 N0.0%
15°0.25880.258819 N25.9%
30°0.50000.500000 N50.0%
45°0.70710.707107 N70.7%
60°0.86600.866025 N86.6%
75°0.96590.965926 N96.6%
90°1.00001.000000 N100.0%
Planning notes, formulas, and examples

About the Electromagnetic Force Calculator

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 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.

When This Page Helps

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.

How to Use the Inputs

  1. Select the calculation mode: Lorentz force, wire in field, parallel conductors, or solenoid.
  2. Enter the charge or current value depending on the mode selected.
  3. Enter the magnetic field strength (Tesla) or current for parallel conductor mode.
  4. Specify velocity (for Lorentz), wire length, or conductor spacing as needed.
  5. Enter the angle between the field and motion/current direction.
  6. Review the computed force and the breakdown of contributing factors.
  7. Use presets to explore common real-world scenarios.
Formula used
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.

Example Calculation

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.

Tips & Best Practices

  • Remember sin(90°) = 1 — maximum force occurs when current/velocity is perpendicular to the field.
  • μ₀ = 4π × 10⁻⁷ ≈ 1.257 × 10⁻⁶ T·m/A — memorize this constant for quick hand calculations.
  • For solenoids, doubling current quadruples pull force (F ∝ B² ∝ I²).
  • Real solenoid force drops sharply with air gap — manufacturers spec force at zero gap.
  • Parallel conductor forces are tiny in household wiring but significant in bus bars carrying thousands of amps.
  • Use right-hand rule: fingers curl from v to B, thumb points in force direction (for positive charges).

Lorentz Force and Charged Particles

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.

Force on Current-Carrying Conductors

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.

Applications in Modern Engineering

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.

Sources & Methodology

Last updated:

Frequently Asked Questions

  • 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.