F/l = μ0·I1·I2/(2π·a)
Conductors carrying current in the same direction attract; force per length grows with both currents and falls with conductor spacing.
Conductors carrying current in the same direction attract; force per length grows with both currents and falls with conductor spacing.
Select a target and calculate.
Conductors carrying current in the same direction attract; force per length grows with both currents and falls with conductor spacing.
I1=I2=10 A at 1 cm spacing give F/l=2 mN/m.
Infinitely long, thin, parallel conductors in vacuum or air (μr≈1); real conductor cross-sections, finite length and ferromagnetic surroundings are excluded.
This calculator determines the force per unit length between two parallel current-carrying conductors, the basic magnetic force effect that once underpinned the definition of the ampere.
Two parallel conductors spaced a apart carrying currents I1 and I2 exert force per length F/l=μ0·I1·I2/(2π·a) on each other. They attract when currents flow the same direction and repel when opposite.
F/l = μ0·I1·I2/(2π·a)
F/l = μ0·I1·I2/(2π·a)| Symbol / input | Meaning |
|---|---|
| Force per length F/l | Attractive (same current direction) or repulsive force per metre of conductor length. |
| Current in first conductor I1 | Current magnitude in the first of the two parallel conductors. |
| Current in second conductor I2 | Current magnitude in the second of the two parallel conductors. |
| Conductor spacing a | Distance between the two conductors' centre axes. |
I1 and I2 are the currents in the two conductors, a is the distance between their centre axes.
Take currents and spacing from the actual wiring layout; for multi-core cables use the spacing of the cores considered.
I1=I2=10 A at 1 cm spacing give F/l=2 mN/m.
Force grows with the product of both currents and falls inversely with spacing; at fault currents this can produce substantial mechanical loading on busbars.
I1 and I2 are currents, a a length. F/l is output as force per length.
Estimating mechanical short-circuit forces on parallel busbars and conductors, and illustrating magnetic force effects in teaching.
Ideal infinitely long, thin, parallel conductors in vacuum or air; finite conductor length, real cross-sections and ferromagnetic surroundings are excluded.
Common mistake: Do not forget that opposite current direction produces a repulsive rather than attractive force; the formula's magnitude is unchanged.
Estimating mechanical short-circuit forces on parallel busbars and conductors, and illustrating magnetic force effects in teaching.
I1 and I2 are the currents in the two conductors, a is the distance between their centre axes.
Ideal infinitely long, thin, parallel conductors in vacuum or air; finite conductor length, real cross-sections and ferromagnetic surroundings are excluded.