Force Between Two Parallel Currents — Question 7

Section 29-2 · Physics pages 4684–4685

Question 7 Quasistatic separation of attractive currents requires logarithmic mechanical work Two parallel long wires carry constant currents I1 and I2 in the same direction. One wire is fixed; an external agent slowly moves the other from separation d1 to d2, with d2 > d1. Current supplies maintain both currents; end effects are neglected. 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) Find the external mechanical work per unit length. (b) Evaluate for I1=4.00 A, I2=6.00 A and d2=3d1, and state why this is not the full electrical-source energy balance.
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Question 7 - Solution Quasistatic separation of attractive currents requires logarithmic mechanical work I1 I2 d x (a) Method and calculation fext(d) = µ0I1I2 2πd , Wext ℓ = ∫d2 d1 fext(d) dd. Wext ℓ = µ0I1I2 2π ln d2 d1 . (b) Interpretation and further calculation Wext/ℓ= (4.80 × 10−6) ln 3 = 5.27334 × 10−6 J/m . Wmagnetic,mechanical = −Wext. Maintaining the currents during motion also involves the current supplies; the mechanical integral alone does not determine their energy transfer. Physical check The logarithm is dimensionless and the mechanical work is positive when attractive wires are separated quasistatically.

Question 7

Quasistatic separation of attractive currents requires logarithmic mechanical work

Two parallel long wires carry constant currents I1 and I2 in the same direction. One wire is fixed; an external agent slowly moves the other from separation d1 to d2, with d2>d1d_2>d_1. Current supplies maintain both currents; end effects are neglected. 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 external mechanical work per unit length.

  2. Evaluate for I1=4.00 A, I2=6.00 A and d2=3d1, and state why this is not the full electrical-source energy balance.

Question 7 - Solution

Quasistatic separation of attractive currents requires logarithmic mechanical work

Diagram shown in the original SVG worksheet.

(a) Method and calculation

fext(d)=μ0I1I22πd,Wextℓ=∫d1d2fext(d)dd.f_{\mathrm{ext}}(d)=\frac{\mu_0I_1I_2}{2\pi d},\quad\frac{W_{\mathrm{ext}}}\ell=\int_{d_1}^{d_2}f_{\mathrm{ext}}(d)\,dd.Wextℓ=μ0I1I22πln⁡d2d1.\boxed{\frac{W_{\mathrm{ext}}}\ell=\frac{\mu_0I_1I_2}{2\pi}\ln\frac{d_2}{d_1}}.

(b) Interpretation and further calculation

Wext/ℓ=(4.80×10−6)ln⁡3=5.27334×10−6J/m.W_{\mathrm{ext}}/\ell=(4.80\times10^{-6})\ln3=\boxed{5.27334\times10^{-6}\,\mathrm{J/m}}.Wmagnetic,mechanical=−Wext.W_{\mathrm{magnetic,mechanical}}=-W_{\mathrm{ext}}.Maintaining the currents during motion also involves the current supplies; the mechanical integral alone does not determine their energy transfer.

Physical check

The logarithm is dimensionless and the mechanical work is positive when attractive wires are separated quasistatically.