Calculating the Potential from the Field — Question 5

Section 24-4 · Physics pages 3860–3861

Question 5 A screened radial field integrates by recognizing a total derivative For r>0 a prescribed field is Er = Ce−r/ℓ(r−2 + 1/(ℓr)), where C and ℓare positive. Set V(infinity)=0. ℓ 2ℓ Schematic; labels, not drawing lengths, specify the data. (a) Find V(r) and verify it by differentiation. (b) Find the quasistatic external work moving charge q from r=ℓto r=2ℓ.
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Question 5 - Solution A screened radial field integrates by recognizing a total derivative ℓ 2ℓ (a) Method and calculation d dr ( e−r/ℓ r ) = −e−r/ℓ ( 1 r2 + 1 ℓr ) . V (r) = Ce−r/ℓ r , −V ′(r) = Er. (b) Interpretation and further calculation ∆V = C ℓ ( e−2 2 −e−1 ) . Wext = q∆V ≈−.300212qC ℓ. Physical check The infinity reference fixes the integration constant; for positive q the external agent extracts energy during outward motion.

Question 5

A screened radial field integrates by recognizing a total derivative

For r>0 a prescribed field is Er=Ce−r/ℓ(r−2+1/(ℓr))E_r=C e^{-r/\ell}(r^{-2}+1/(\ell r)), where C and ℓ\ell are positive. Set V(infinity)=0.

Diagram shown in the original SVG worksheet.

  1. Find V(r) and verify it by differentiation.

  2. Find the quasistatic external work moving charge q from r=ℓ\ell to r=2ℓ2\ell.

Question 5 - Solution

A screened radial field integrates by recognizing a total derivative

Diagram shown in the original SVG worksheet.

(a) Method and calculation

ddr(e−r/ℓr)=−e−r/ℓ(1r2+1ℓr).\frac d{dr}\left(\frac{e^{-r/\ell}}r\right)=-e^{-r/\ell}\left(\frac1{r^2}+\frac1{\ell r}\right).V(r)=Ce−r/ℓr,−V′(r)=Er.V(r)=\frac{C e^{-r/\ell}}r,\quad -V\prime(r)=E_r.

(b) Interpretation and further calculation

ΔV=Cℓ(e−22−e−1).\Delta V=\frac C\ell\left(\frac{e^{-2}}2-e^{-1}\right).Wext=qΔV≈−.300212qCℓ.W_{\mathrm{ext}}=q\Delta V\approx-.300212\frac{qC}{\ell}.

Physical check

The infinity reference fixes the integration constant; for positive q the external agent extracts energy during outward motion.