Calculating the Potential from the Field — Question 8

Section 24-4 · Physics pages 3866–3867

Question 8 An infinite charged sheet gives a continuous cusp in potential An infinite sheet at x=0 produces Ex = Es sgn(x) with Es > 0. Set V(0)=0; there is no ideal dipole layer. sheet Schematic; labels, not drawing lengths, specify the data. (a) Find V(x) on both sides and check continuity. (b) Find the voltage between x=-a and x=2a and the work on positive charge q between these points.
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Question 8 - Solution An infinite charged sheet gives a continuous cusp in potential sheet (a) Method and calculation x > 0 : V = −Esx; x < 0 : V = +Esx. V (x) = −Es|x|, V (0−) = V (0+) = 0. (b) Interpretation and further calculation V (2a) −V (−a) = −2Esa + Esa = −Esa. We = −q∆V = qEsa. Physical check The cusp means the normal field jumps; it does not mean the potential jumps.

Question 8

An infinite charged sheet gives a continuous cusp in potential

An infinite sheet at x=0 produces Ex=Essgn⁡(x)E_x=E_s\operatorname{sgn}(x) with Es>0E_s>0. Set V(0)=0; there is no ideal dipole layer.

Diagram shown in the original SVG worksheet.

  1. Find V(x) on both sides and check continuity.

  2. Find the voltage between x=-a and x=2a and the work on positive charge q between these points.

Question 8 - Solution

An infinite charged sheet gives a continuous cusp in potential

Diagram shown in the original SVG worksheet.

(a) Method and calculation

x>0:V=−Esx;x<0:V=+Esx.x>0:\ V=-E_sx;\qquad x<0:\ V=+E_sx.V(x)=−Es|x|,V(0−)=V(0+)=0.V(x)=-E_s|x|,\quad V(0^-)=V(0^+)=0.

(b) Interpretation and further calculation

V(2a)−V(−a)=−2Esa+Esa=−Esa.V(2a)-V(-a)=-2E_sa+E_sa=-E_sa.We=−qΔV=qEsa.W_e=-q\Delta V=qE_sa.

Physical check

The cusp means the normal field jumps; it does not mean the potential jumps.