Potential Difference Between Two Points — Question 8

Section 27-5 · Physics pages 4406–4407

Question 8 Potential gradients inside conducting wires reconcile nonzero current with small voltage drop A straight uniform wire of length L, area A and resistivity rho carries steady current I toward +x. Let V(0)=V0 and assume local Ohm behavior. A +x tap 1 tap 2 Wire cross-section and reference direction; dimensions are schematic. (a) Find V(x) and its electric field. (b) For two taps separated by distance ell, find their voltage difference; explain the ideal-wire limit at fixed current.
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Question 8 - Solution Potential gradients inside conducting wires reconcile nonzero current with small voltage drop A +x tap 1 tap 2 (a) Method and calculation J = I/A, Ex = ρJ = ρI/A, dV/dx = −Ex. V (x) = V0 −ρIx/A. (b) Interpretation and further calculation V (x + ℓ) −V (x) = −ρIℓ/A. ρ →0 at fixed I : Ex →0, ∆V →0. Physical check A real resistive wire needs a small field for steady current; an ideal zero-resistance wire is a limiting model.

Question 8

Potential gradients inside conducting wires reconcile nonzero current with small voltage drop

A straight uniform wire of length L, area A and resistivity rho carries steady current I toward +x. Let V(0)=V0 and assume local Ohm behavior.

Diagram shown in the original SVG worksheet.

  1. Find V(x) and its electric field.

  2. For two taps separated by distance ell, find their voltage difference; explain the ideal-wire limit at fixed current.

Question 8 - Solution

Potential gradients inside conducting wires reconcile nonzero current with small voltage drop

Diagram shown in the original SVG worksheet.

(a) Method and calculation

J=I/A,Ex=ρJ=ρI/A,dV/dx=−Ex.J=I/A,\quad E_x=\rho J=\rho I/A,\quad dV/dx=-E_x.V(x)=V0−ρIx/A.V(x)=V_0-\rho Ix/A.

(b) Interpretation and further calculation

V(x+ℓ)−V(x)=−ρIℓ/A.V(x+\ell)-V(x)=-\rho I\ell/A.ρ→0 at fixed I:Ex→0,ΔV→0.\rho\to0\text{ at fixed }I:\quad E_x\to0,\quad\Delta V\to0.

Physical check

A real resistive wire needs a small field for steady current; an ideal zero-resistance wire is a limiting model.