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Formulas/physics/Moving Charges/Force Per Unit Length Between Parallel Wires

Force Per Unit Length Between Parallel Wires

Two parallel wires separated by d attract for same-direction currents, repel for opposite. This result defines the SI ampere (pre-2019 definition).
Class 12
Derivation

Setup

Two long parallel wires separated by distance dd, carrying currents I1I_1 and I2I_2.

Step 1 — Field of Wire 1 at Wire 2

From mc10:

B1=μ0I12πdB_1 = \frac{\mu_0 I_1}{2\pi d}

Step 2 — Force on Wire 2

From the force on a current-carrying conductor (F=IL×B\vec{F} = I\vec{L} \times \vec{B}), with B1I2B_1 \perp I_2:

F=I2LB1=I2Lμ0I12πdF = I_2 L B_1 = I_2 L \cdot \frac{\mu_0 I_1}{2\pi d}

Force per unit length:

FL=μ0I1I22πd\boxed{\frac{F}{L} = \frac{\mu_0 I_1 I_2}{2\pi d}}

Direction

  • Same-direction currents: F\vec{F} directed toward the other wire. Attraction.
  • Opposite-direction currents: Repulsion.
Warning
Like currents attract, unlike repel — opposite to the rule for electric charges.

Definition of the Ampere

Substituting I1=I2=1AI_1 = I_2 = 1\,\text{A}, d=1md = 1\,\text{m}:

FL=4π×107×1×12π×1=2×107N/m\frac{F}{L} = \frac{4\pi \times 10^{-7} \times 1 \times 1}{2\pi \times 1} = 2 \times 10^{-7}\,\text{N/m}

This was the pre-2019 SI definition of the ampere. The 2019 redefinition fixes ee numerically; the formula remains exact.