Work, Energy, and Emf — Question 6

Section 27-2 · Physics pages 4342–4343

Question 6 Emf is the line integral of the non-electrostatic force per charge Along a source channel 0 < x < L, the non-electrostatic force on positive charge q is⃗ Fne = qf0(1 + x/L)ˆx. Traversal is quasistatic and internal losses are negligible. low V high V positive charge non-electrostatic pump Schematic; labels, not drawing lengths, specify the data. (a) Find the emf for travel from x=0 to x=L. (b) Find the average opposing electrostatic field component and the net electric work over an external return path.
Show solutionHide solution
Question 6 - Solution Emf is the line integral of the non-electrostatic force per charge low V high V positive charge non-electrostatic pump (a) Method and calculation E = ∫L 0 (⃗Fne/q) · d⃗ℓ= f0 ∫L 0 (1 + x/L)dx. E = 3 2f0L, V (L) −V (0) = E. (b) Interpretation and further calculation ⟨Ex⟩= −V (L) −V (0) L = −3 2f0. WE,return = qE = 3 2qf0L. Physical check The source force depends on its energy-conversion mechanism; its work is not part of the conservative electrostatic loop integral.

Question 6

Emf is the line integral of the non-electrostatic force per charge

Along a source channel 0<x<L0<x<L, the non-electrostatic force on positive charge q is F→ne=qf0(1+x/L)x̂\vec F_{\mathrm{ne}}=qf_0(1+x/L)\hat x. Traversal is quasistatic and internal losses are negligible.

Diagram shown in the original SVG worksheet.

  1. Find the emf for travel from x=0 to x=L.

  2. Find the average opposing electrostatic field component and the net electric work over an external return path.

Question 6 - Solution

Emf is the line integral of the non-electrostatic force per charge

Diagram shown in the original SVG worksheet.

(a) Method and calculation

ℰ=∫0L(F→ne/q)⋅dℓ→=f0∫0L(1+x/L)dx.\mathcal E=\int_0^L(\vec F_{\mathrm{ne}}/q)\cdot d\vec\ell=f_0\int_0^L(1+x/L)dx.ℰ=32f0L,V(L)−V(0)=ℰ.\mathcal E=\tfrac32f_0L,\quad V(L)-V(0)=\mathcal E.

(b) Interpretation and further calculation

⟨Ex⟩=−V(L)−V(0)L=−32f0.\langle E_x\rangle=-\frac{V(L)-V(0)}L=-\tfrac32f_0.WE,return=qℰ=32qf0L.W_{E,\mathrm{return}}=q\mathcal E=\tfrac32qf_0L.

Physical check

The source force depends on its energy-conversion mechanism; its work is not part of the conservative electrostatic loop integral.