Force Between Two Parallel Currents — Question 3

Section 29-2 · Physics pages 4676–4677

Question 3 Three parallel currents reveal a force balance that is unstable along their line Two fixed wires at x=-a and x=+a carry current I toward +z. A third wire of mass per length lambda carries i toward +z and can slide along x between them. Let its displacement from the midpoint be x; neglect gravity along x. Use vacuum permeability µ0 ≃4π × 10−7 T m/A where numerical values are needed. I i I −a x +a x Schematic; labels, not drawing lengths, specify the data. (a) Find the net force per unit length and its leading term for small x. (b) Classify the midpoint stability. Repeat the linear stability analysis if only i is reversed.
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Question 3 - Solution Three parallel currents reveal a force balance that is unstable along their line I i I −a x +a x (a) Method and calculation fx = µ0Ii 2π ( 1 a −x − 1 a + x ) . fx = µ0Ii x π(a2 −x2) ≃µ0Ii πa2 x. (b) Interpretation and further calculation λ¨x = +µ0Ii πa2 x ⇒x = 0 is unstable. i →−i : ¨x = −Ω2x, Ω= √ µ0Ii πλa2 . Physical check An attractive displacement favors the nearer fixed wire and grows; repulsion reverses that linear response when motion is confined to x.

Question 3

Three parallel currents reveal a force balance that is unstable along their line

Two fixed wires at x=-a and x=+a carry current I toward +z. A third wire of mass per length lambda carries i toward +z and can slide along x between them. Let its displacement from the midpoint be x; neglect gravity along x. 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. Find the net force per unit length and its leading term for small x.

  2. Classify the midpoint stability. Repeat the linear stability analysis if only i is reversed.

Question 3 - Solution

Three parallel currents reveal a force balance that is unstable along their line

Diagram shown in the original SVG worksheet.

(a) Method and calculation

fx=μ0Ii2π(1a−x−1a+x).f_x=\frac{\mu_0Ii}{2\pi}\left(\frac1{a-x}-\frac1{a+x}\right).fx=μ0Iixπ(a2−x2)≃μ0Iiπa2x.f_x=\frac{\mu_0Ii\,x}{\pi(a^2-x^2)}\simeq\frac{\mu_0Ii}{\pi a^2}x.

(b) Interpretation and further calculation

λẍ=+μ0Iiπa2x⇒x=0 is unstable.\lambda\ddot x=+\frac{\mu_0Ii}{\pi a^2}x\Rightarrow x=0\text{ is unstable}.i→−i:ẍ=−Ω2x,Ω=μ0Iiπλa2.i\to-i:\quad\ddot x=-\Omega^2x,\quad\boxed{\Omega=\sqrt{\frac{\mu_0Ii}{\pi\lambda a^2}}}.

Physical check

An attractive displacement favors the nearer fixed wire and grows; repulsion reverses that linear response when motion is confined to x.