"Pumping" Charges — Question 1

Section 27-1 · Physics pages 4312–4313

Question 1 A source raises positive charge in potential without raising its kinetic energy Inside an ideal source, a positive charge q = 4.00 mC moves quasistatically from terminal A at 2.00 V to terminal B at 14.0 V. Neglect internal dissipation. low V high V positive charge non-electrostatic pump Schematic; labels, not drawing lengths, specify the data. (a) Find the electric force work and the non-electrostatic work. (b) Find the energy transferred to an external load if the same charge returns from B to A, and explain why the source is necessary.
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Question 1 - Solution A source raises positive charge in potential without raising its kinetic energy low V high V positive charge non-electrostatic pump (a) Method and calculation ∆U = q(VB −VA) = (.00400)(12.0) = .0480 J. WE = −∆U = −.0480 J, Wpump = +.0480 J. (b) Interpretation and further calculation WE,return = q(VB −VA) = .0480 J. WE,closed = WE + WE,return = 0. The source supplies the energy dissipated by the load, while the electrostatic field has zero net loop work. Physical check The name charge pump describes energy conversion, not creation of net electric charge.

Question 1

A source raises positive charge in potential without raising its kinetic energy

Inside an ideal source, a positive charge q=4.00q=4.00 mC moves quasistatically from terminal A at 2.00 V to terminal B at 14.0 V. Neglect internal dissipation.

Diagram shown in the original SVG worksheet.

  1. Find the electric force work and the non-electrostatic work.

  2. Find the energy transferred to an external load if the same charge returns from B to A, and explain why the source is necessary.

Question 1 - Solution

A source raises positive charge in potential without raising its kinetic energy

Diagram shown in the original SVG worksheet.

(a) Method and calculation

ΔU=q(VB−VA)=(.00400)(12.0)=.0480J.\Delta U=q(V_B-V_A)=(.00400)(12.0)=.0480\,\mathrm J.WE=−ΔU=−.0480J,Wpump=+.0480J.W_E=-\Delta U=-.0480\,\mathrm J,\quad W_{\mathrm{pump}}=+.0480\,\mathrm J.

(b) Interpretation and further calculation

WE,return=q(VB−VA)=.0480J.W_{E,\mathrm{return}}=q(V_B-V_A)=.0480\,\mathrm J.WE,closed=WE+WE,return=0.W_{E,\mathrm{closed}}=W_E+W_{E,\mathrm{return}}=0.The source supplies the energy dissipated by the load, while the electrostatic field has zero net loop work.

Physical check

The name charge pump describes energy conversion, not creation of net electric charge.