Gauss' Law — Question 1

Section 23-3 · Physics pages 3672–3673

Question 1 Large exterior charges can change the field without changing enclosed flux Use ϵ0 = 8.854 × 10−12 C2/(N m2). A closed Gaussian surface contains charges +5.00 nC, −8.00 nC and −2.00 nC. A separate +100 nC charge is outside. None lies on the surface. +5 −8 −2 +100 nC Enclosed charge labels are in nC; the dashed boundary is a Gaussian surface. (a) Find the net outward electric flux. (b) The exterior charge doubles while all three interior charges stay fixed. Find the change in total flux and explain whether the field at individual surface points must stay fixed.
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Question 1 - Solution Large exterior charges can change the field without changing enclosed flux +5 −8 −2 +100 nC (a) Method and calculation Qenc = (5 −8 −2) nC = −5.00 × 10−9 C. Φ = Qenc ϵ0 = −5.00 × 10−9 8.854 × 10−12 ≈−564.716 N m2/C. (b) Interpretation and further calculation ∆Qenc = 0 ⇒∆Φ = 0. Etotal = Einside + Eoutside, I ∆Eoutside · dA = 0. The external source generally changes the local field, while its net closed-surface contribution remains zero. Physical check Negative total flux means net inward field flux, not inward field at every point.

Question 1

Large exterior charges can change the field without changing enclosed flux

Use ϵ0=8.854×10−12C2/(Nm2)\epsilon_0=8.854\times10^{-12}\,\mathrm{C^2/(N\,m^2)}. A closed Gaussian surface contains charges +5.00+5.00 nC, −8.00-8.00 nC and −2.00-2.00 nC. A separate +100+100 nC charge is outside. None lies on the surface.

Diagram shown in the original SVG worksheet.

  1. Find the net outward electric flux.

  2. The exterior charge doubles while all three interior charges stay fixed. Find the change in total flux and explain whether the field at individual surface points must stay fixed.

Question 1 - Solution

Large exterior charges can change the field without changing enclosed flux

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Qenc=(5−8−2)nC=−5.00×10−9C.Q_{\mathrm{enc}}=(5-8-2)\,\mathrm{nC}=-5.00\times10^{-9}\,\mathrm C.Φ=Qencϵ0=−5.00×10−98.854×10−12≈−564.716Nm2/C.\Phi=\frac{Q_{\mathrm{enc}}}{\epsilon_0}=\frac{-5.00\times10^{-9}}{8.854\times10^{-12}}\approx-564.716\,\mathrm{N\,m^2/C}.

(b) Interpretation and further calculation

ΔQenc=0⇒ΔΦ=0.\Delta Q_{\mathrm{enc}}=0\Rightarrow\Delta\Phi=0.𝑬total=𝑬inside+𝑬outside,∮Δ𝑬outside⋅d𝑨=0.\mathbf E_{\mathrm{total}}=\mathbf E_{\mathrm{inside}}+\mathbf E_{\mathrm{outside}},\quad\oint\Delta\mathbf E_{\mathrm{outside}}\cdot d\mathbf A=0.The external source generally changes the local field, while its net closed-surface contribution remains zero.

Physical check

Negative total flux means net inward field flux, not inward field at every point.