Force Between Two Parallel Currents — Question 8

Section 29-2 · Physics pages 4686–4687

Question 8 A fixed total current has one split that maximizes the attraction Two parallel wires a distance d apart share a prescribed positive total current IT = I1 + I2, with both currents in the same direction. Neglect heating constraints and hold the geometry fixed. Use vacuum permeability µ0 ≃4π × 10−7 T m/A where numerical values are needed. IT /2 + δ IT /2 −δ d x Schematic; labels, not drawing lengths, specify the data. (a) Find the current split that maximizes the attractive force per unit length. (b) If I1 = IT /2 + δ and I2 = IT /2 −δ, find the fractional force reduction and the allowed imbalance for no more than 4.00 percent reduction.
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Question 8 - Solution A fixed total current has one split that maximizes the attraction IT /2 + δ IT /2 −δ d x (a) Method and calculation f = µ0 2πdI1(IT −I1), df dI1 = µ0 2πd(IT −2I1). I1 = I2 = IT /2, fmax = µ0I2 T 8πd ; f′′ < 0. (b) Interpretation and further calculation f = fmax ( 1 −4δ2 I2 T ) , fmax −f fmax = 4δ2 I2 T . 4δ2/I2 T ≤.0400 ⇒|δ| ≤.100IT . Physical check The maximum is broad: a small current imbalance changes the force only to second order.

Question 8

A fixed total current has one split that maximizes the attraction

Two parallel wires a distance d apart share a prescribed positive total current IT=I1+I2I_T=I_1+I_2, with both currents in the same direction. Neglect heating constraints and hold the geometry fixed. 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 current split that maximizes the attractive force per unit length.

  2. If I1=IT/2+δI_1=I_T/2+\delta and I2=IT/2−δI_2=I_T/2-\delta, find the fractional force reduction and the allowed imbalance for no more than 4.00 percent reduction.

Question 8 - Solution

A fixed total current has one split that maximizes the attraction

Diagram shown in the original SVG worksheet.

(a) Method and calculation

f=μ02πdI1(IT−I1),dfdI1=μ02πd(IT−2I1).f=\frac{\mu_0}{2\pi d}I_1(I_T-I_1),\quad\frac{df}{dI_1}=\frac{\mu_0}{2\pi d}(I_T-2I_1).I1=I2=IT/2,fmax=μ0IT28πd;f′′<0.\boxed{I_1=I_2=I_T/2,\quad f_{\max}=\frac{\mu_0I_T^2}{8\pi d}};\quad f\prime\prime<0.

(b) Interpretation and further calculation

f=fmax(1−4δ2IT2),fmax−ffmax=4δ2IT2.f=f_{\max}\left(1-\frac{4\delta^2}{I_T^2}\right),\quad\frac{f_{\max}-f}{f_{\max}}=\frac{4\delta^2}{I_T^2}.4δ2/IT2≤.0400⇒|δ|≤.100IT.4\delta^2/I_T^2\le.0400\Rightarrow\boxed{|\delta|\le.100I_T}.

Physical check

The maximum is broad: a small current imbalance changes the force only to second order.