Force Between Two Parallel Currents — Question 1

Section 29-2 · Physics pages 4672–4673

Question 1 The force on each of two unequal currents follows from the other wire field Two very long parallel wires carry I1=2.00 A and I2=5.00 A toward +z, separated by d=.0400 m. Consider a length ell=.300 m far from their ends; neglect return paths. Use vacuum permeability µ0 ≃4π × 10−7 T m/A where numerical values are needed. I1 I2 d x Schematic; labels, not drawing lengths, specify the data. (a) Calculate the magnetic field each wire produces at the other wire. (b) Find the force on each length ell, including direction, and explain why the forces have equal magnitudes.
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Question 1 - Solution The force on each of two unequal currents follows from the other wire field I1 I2 d x (a) Method and calculation B1→2 = µ0I1 2πd = 10.0 µT. B2→1 = µ0I2 2πd = 25.0 µT. (b) Interpretation and further calculation F2 = I2ℓB1→2 = F1 = I1ℓB2→1 = µ0I1I2ℓ 2πd . F1 = F2 = 15.0 µN ;⃗ F1 = −⃗F2 and both point toward the other wire. Physical check Although the two source fields differ, each force multiplies that field by the other current, giving the same product I1 I2.

Question 1

The force on each of two unequal currents follows from the other wire field

Two very long parallel wires carry I1=2.00 A and I2=5.00 A toward +z, separated by d=.0400 m. Consider a length ell=.300 m far from their ends; neglect return paths. Use vacuum permeability μ0≃4π×10−7Tm/A\mu_0\simeq4\pi\times10^{-7}\,\mathrm{T\,m/A} where numerical values are needed.

Diagram shown in the original SVG worksheet.

  1. Calculate the magnetic field each wire produces at the other wire.

  2. Find the force on each length ell, including direction, and explain why the forces have equal magnitudes.

Question 1 - Solution

The force on each of two unequal currents follows from the other wire field

Diagram shown in the original SVG worksheet.

(a) Method and calculation

B1→2=μ0I12πd=10.0μT.B_{1\to2}=\frac{\mu_0I_1}{2\pi d}=10.0\,\mu\mathrm T.B2→1=μ0I22πd=25.0μT.B_{2\to1}=\frac{\mu_0I_2}{2\pi d}=25.0\,\mu\mathrm T.

(b) Interpretation and further calculation

F2=I2ℓB1→2=F1=I1ℓB2→1=μ0I1I2ℓ2πd.F_2=I_2\ell B_{1\to2}=F_1=I_1\ell B_{2\to1}=\frac{\mu_0I_1I_2\ell}{2\pi d}.F1=F2=15.0μN;F→1=−F→2 and both point toward the other wire.\boxed{F_1=F_2=15.0\,\mu\mathrm N};\quad\vec F_1=-\vec F_2\text{ and both point toward the other wire}.

Physical check

Although the two source fields differ, each force multiplies that field by the other current, giving the same product I1 I2.