"Pumping" Charges — Question 5

Section 27-1 · Physics pages 4320–4321

Question 5 A common potential shift does not alter the required pumping work A two-terminal pump moves positive charge Q from A to B. Initially VA = −40 V and VB = −25 V. The reference is then changed by adding +100 V to both potentials. low V high V positive charge non-electrostatic pump Schematic; labels, not drawing lengths, specify the data. (a) Find the pump work for Q=6.00 mC before and after the shift. (b) Express the work using a line integral of the electrostatic field and show why the reference shift disappears.
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Question 5 - Solution A common potential shift does not alter the required pumping work low V high V positive charge non-electrostatic pump (a) Method and calculation ∆V = (−25) −(−40) = 15.0 V, W = Q∆V = .0900 J. ∆V ′ = 75 −60 = 15.0 V, W′ = W. (b) Interpretation and further calculation ∆V = − ∫B A⃗ E · d⃗ℓ, Wpump = −Q ∫B A⃗ E · d⃗ℓ.⃗ E′ = −∇(V + 100 V) = −∇V =⃗E. Physical check Negative terminal potentials relative to an arbitrary reference do not prevent the source from raising charge energy.

Question 5

A common potential shift does not alter the required pumping work

A two-terminal pump moves positive charge Q from A to B. Initially VA=−40V_A=-40 V and VB=−25V_B=-25 V. The reference is then changed by adding +100 V to both potentials.

Diagram shown in the original SVG worksheet.

  1. Find the pump work for Q=6.00 mC before and after the shift.

  2. Express the work using a line integral of the electrostatic field and show why the reference shift disappears.

Question 5 - Solution

A common potential shift does not alter the required pumping work

Diagram shown in the original SVG worksheet.

(a) Method and calculation

ΔV=(−25)−(−40)=15.0V,W=QΔV=.0900J.\Delta V=(-25)-(-40)=15.0\,\mathrm V,\quad W=Q\Delta V=.0900\,\mathrm J.ΔV′=75−60=15.0V,W′=W.\Delta V\prime=75-60=15.0\,\mathrm V,\quad W\prime=W.

(b) Interpretation and further calculation

ΔV=−∫ABE→⋅dℓ→,Wpump=−Q∫ABE→⋅dℓ→.\Delta V=-\int_A^B\vec E\cdot d\vec\ell,\quad W_{\mathrm{pump}}=-Q\int_A^B\vec E\cdot d\vec\ell.E→′=−∇(V+100V)=−∇V=E→.\vec E\prime=-\nabla(V+100\,\mathrm V)=-\nabla V=\vec E.

Physical check

Negative terminal potentials relative to an arbitrary reference do not prevent the source from raising charge energy.