Applying Gauss' Law: Planar Symmetry — Question 5

Section 23-7 · Physics pages 3760–3761

Question 5 A triangular slab density concentrates most of its field buildup near the midplane An infinite insulating slab has even density ρ(x) = ρ0(1 −|x|/a) for |x| < a, and zero outside, with ρ0 > 0. No external field is present. x −a a ρ(x) Edge-on view of an infinite planar slab; its transverse dimensions are unbounded. (a) Find the field for 0 ≤x ≤a and outside, using odd symmetry to cover negative x. (b) Find the positive position where the field reaches half its exterior magnitude. Compare that position with the result for a uniformly charged slab of the same half-width.
Show solutionHide solution
Question 5 - Solution A triangular slab density concentrates most of its field buildup near the midplane x −a a ρ(x) (a) Method and calculation Ex(x) = 1 ϵ0 ∫x 0 ρ0(1 −u/a) du = ρ0 ϵ0 ( x −x2 2a ) . Eout = ρ0a/(2ϵ0), Ex(−x) = −Ex(x). (b) Interpretation and further calculation u = x/a : u −u2/2 = 1/4 ⇒u = 1 −1/ √ 2 ≈.292893. x1/2,uniform = a/2 > .292893a. The triangular profile accumulates charge more rapidly near the midplane relative to its total. Physical check The second algebraic root exceeds a and is not inside the density profile used in the derivation.

Question 5

A triangular slab density concentrates most of its field buildup near the midplane

An infinite insulating slab has even density ρ(x)=ρ0(1−|x|/a)\rho(x)=\rho_0(1-|x|/a) for |x|<a|x|<a, and zero outside, with ρ0>0\rho_0>0. No external field is present.

Diagram shown in the original SVG worksheet.

  1. Find the field for 0≤x≤a0\le x\le a and outside, using odd symmetry to cover negative x.

  2. Find the positive position where the field reaches half its exterior magnitude. Compare that position with the result for a uniformly charged slab of the same half-width.

Question 5 - Solution

A triangular slab density concentrates most of its field buildup near the midplane

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Ex(x)=1ϵ0∫0xρ0(1−u/a)du=ρ0ϵ0(x−x22a).E_x(x)=\frac1{\epsilon_0}\int_0^x\rho_0(1-u/a)\,du=\frac{\rho_0}{\epsilon_0}\left(x-\frac{x^2}{2a}\right).Eout=ρ0a/(2ϵ0),Ex(−x)=−Ex(x).E_{\mathrm{out}}=\rho_0a/(2\epsilon_0),\quad E_x(-x)=-E_x(x).

(b) Interpretation and further calculation

u=x/a:u−u2/2=1/4⇒u=1−1/2≈.292893.u=x/a:\quad u-u^2/2=1/4\Rightarrow u=1-1/\sqrt2\approx.292893.x1/2,uniform=a/2>.292893a.x_{1/2,\mathrm{uniform}}=a/2>.292893a.The triangular profile accumulates charge more rapidly near the midplane relative to its total.

Physical check

The second algebraic root exceeds a and is not inside the density profile used in the derivation.