Calculating the Field from the Potential — Question 6

Section 24-9 · Physics pages 3962–3963

Question 6 A fitted local potential reveals the charge density required to support it A measured three-dimensional potential is V = V0 + ax + by + c(x2 + y2 + z2) over a region. Use ∇· E = ρ/ϵ0. level surfaces Schematic; labels, not drawing lengths, specify the data. (a) Find E and the implied volume charge density. (b) If c>0, find the equilibrium position for a positive test charge q of mass m and classify its local stability.
Show solutionHide solution
Question 6 - Solution A fitted local potential reveals the charge density required to support it level surfaces (a) Method and calculation E = −(a + 2cx)ˆx −(b + 2cy)ˆy −2czˆz. ρ = ϵ0∇· E = −6ϵ0c. (b) Interpretation and further calculation req = ( −a 2c, −b 2c, 0 ) . U = qV = qc|r −req|2 + constant, ω = √ 2qc/m. For q>0 and c>0 the local equilibrium is stable if the fitted region includes it. Physical check This stable electrostatic minimum requires nonzero negative source charge density, so it is not a charge-free trap.

Question 6

A fitted local potential reveals the charge density required to support it

A measured three-dimensional potential is V=V0+ax+by+c(x2+y2+z2)V=V_0+ax+by+c(x^2+y^2+z^2) over a region. Use ∇⋅𝑬=ρ/ϵ0\nabla\cdot\mathbf E=\rho/\epsilon_0.

Diagram shown in the original SVG worksheet.

  1. Find E and the implied volume charge density.

  2. If c>0, find the equilibrium position for a positive test charge q of mass m and classify its local stability.

Question 6 - Solution

A fitted local potential reveals the charge density required to support it

Diagram shown in the original SVG worksheet.

(a) Method and calculation

𝑬=−(a+2cx)𝒙̂−(b+2cy)𝒚̂−2cz𝒛̂.\mathbf E=-(a+2cx)\hat{\mathbf x}-(b+2cy)\hat{\mathbf y}-2cz\hat{\mathbf z}.ρ=ϵ0∇⋅𝑬=−6ϵ0c.\rho=\epsilon_0\nabla\cdot\mathbf E=-6\epsilon_0c.

(b) Interpretation and further calculation

𝒓eq=(−a2c,−b2c,0).\mathbf r_{\mathrm{eq}}=\left(-\frac a{2c},-\frac b{2c},0\right).U=qV=qc|𝒓−𝒓eq|2+constant,ω=2qc/m.U=qV=q c|\mathbf r-\mathbf r_{\mathrm{eq}}|^2+\text{constant},\quad\omega=\sqrt{2qc/m}.For q>0 and c>0 the local equilibrium is stable if the fitted region includes it.

Physical check

This stable electrostatic minimum requires nonzero negative source charge density, so it is not a charge-free trap.