Work, Energy, and Emf — Question 3

Section 27-2 · Physics pages 4336–4337

Question 3 Equal charge in and out does not give unit energy efficiency A cell of constant emf E and resistance r is charged by quantity Q at current magnitude I, then discharged by the same Q at the same I. Assume Ir < E and no other loss. cell charge discharge Schematic; labels, not drawing lengths, specify the data. (a) Find input energy, recovered energy and total heat. (b) Find round-trip efficiency and its first-order approximation for Ir/E ≪1.
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Question 3 - Solution Equal charge in and out does not give unit energy efficiency cell charge discharge (a) Method and calculation Win = (E + Ir)Q, Wrecovered = (E −Ir)Q. Wheat = Win −Wrecovered = 2IrQ. (b) Interpretation and further calculation η = E −Ir E + Ir = 1 −x 1 + x, x = Ir/E. η = 1 −2x + O(x2). Physical check Chemical energy returns to its initial value after equal charge cycling, but irreversible heating remains.

Question 3

Equal charge in and out does not give unit energy efficiency

A cell of constant emf E and resistance r is charged by quantity Q at current magnitude I, then discharged by the same Q at the same I. Assume Ir<EIr<E and no other loss.

Diagram shown in the original SVG worksheet.

  1. Find input energy, recovered energy and total heat.

  2. Find round-trip efficiency and its first-order approximation for Ir/E≪1Ir/E\ll1.

Question 3 - Solution

Equal charge in and out does not give unit energy efficiency

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Win=(E+Ir)Q,Wrecovered=(E−Ir)Q.W_{\mathrm{in}}=(E+Ir)Q,\quad W_{\mathrm{recovered}}=(E-Ir)Q.Wheat=Win−Wrecovered=2IrQ.W_{\mathrm{heat}}=W_{\mathrm{in}}-W_{\mathrm{recovered}}=2IrQ.

(b) Interpretation and further calculation

η=E−IrE+Ir=1−x1+x,x=Ir/E.\eta=\frac{E-Ir}{E+Ir}=\frac{1-x}{1+x},\quad x=Ir/E.η=1−2x+O(x2).\eta=1-2x+O(x^2).

Physical check

Chemical energy returns to its initial value after equal charge cycling, but irreversible heating remains.