Power in Electric Circuits — Question 4

Section 26-6 · Physics pages 4258–4259

Question 4 A tapered conductor dissipates more power where its cross-section is smaller A wire has A(x) = A0(1 + x/L) on 0 < x < L, resistivity rho and constant current I. Use volumetric heating pv =⃗J ·⃗E. A0 2A0 I Schematic; labels, not drawing lengths, specify the data. (a) Find total power by integrating the local heating density. (b) Find the position x that divides the dissipated power into equal halves.
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Question 4 - Solution A tapered conductor dissipates more power where its cross-section is smaller A0 2A0 I (a) Method and calculation J = I/A(x), pv = ρI2/A(x)2, dP = pvA(x)dx. P = ρI2L A0 ln 2 = I2R. (b) Interpretation and further calculation P(0, x) P(0, L) = ln(1 + x/L) ln 2 . ln(1 + x/L) = 1 2 ln 2 ⇒x = ( √ 2 −1)L. Physical check Integrating power density requires the local volume element A(x) dx, not just dx.

Question 4

A tapered conductor dissipates more power where its cross-section is smaller

A wire has A(x)=A0(1+x/L)A(x)=A_0(1+x/L) on 0<x<L0<x<L, resistivity rho and constant current I. Use volumetric heating pv=J→⋅E→p_v=\vec J\cdot\vec E.

Diagram shown in the original SVG worksheet.

  1. Find total power by integrating the local heating density.

  2. Find the position x that divides the dissipated power into equal halves.

Question 4 - Solution

A tapered conductor dissipates more power where its cross-section is smaller

Diagram shown in the original SVG worksheet.

(a) Method and calculation

J=I/A(x),pv=ρI2/A(x)2,dP=pvA(x)dx.J=I/A(x),\quad p_v=\rho I^2/A(x)^2,\quad dP=p_vA(x)dx.P=ρI2LA0ln⁡2=I2R.P=\frac{\rho I^2L}{A_0}\ln2=I^2R.

(b) Interpretation and further calculation

P(0,x)P(0,L)=ln⁡(1+x/L)ln⁡2.\frac{P(0,x)}{P(0,L)}=\frac{\ln(1+x/L)}{\ln2}.ln⁡(1+x/L)=12ln⁡2⇒x=(2−1)L.\ln(1+x/L)=\tfrac12\ln2\Rightarrow x=(\sqrt2-1)L.

Physical check

Integrating power density requires the local volume element A(x) dx, not just dx.