Flux of an Electric Field — Question 2

Section 23-2 · Physics pages 3654–3655

Question 2 A triangular aperture samples a linear field at its centroid A triangular surface lies in z = 0 with vertices (0, 0), (a, 0) and (0, b). Its normal is positive z. The field on it is Ez = E0 + αx + βy. a b centroid Schematic; labels, not drawing lengths, specify the data. (a) Integrate the flux over the triangle in terms of the given parameters. (b) Show that the same result equals area times field at the centroid, and explain why that shortcut is not generally exact for a quadratic field.
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Question 2 - Solution A triangular aperture samples a linear field at its centroid a b centroid (a) Method and calculation Φ = ∫a 0 ∫b(1−x/a) 0 (E0 + αx + βy) dy dx. Φ = abE0 2 + αa2b 6 + βab2 6 . (b) Interpretation and further calculation A = ab/2, (xc, yc) = (a/3, b/3). Φ = A ( E0 + αa 3 + βb 3 ) = AEz(xc, yc). A linear field depends only on the first area moments; a quadratic profile also depends on second moments. Physical check If both gradients vanish, the expression reduces to E0ab/2.

Question 2

A triangular aperture samples a linear field at its centroid

A triangular surface lies in z=0z=0 with vertices (0,0)(0,0), (a,0)(a,0) and (0,b)(0,b). Its normal is positive z. The field on it is Ez=E0+αx+βyE_z=E_0+\alpha x+\beta y.

Diagram shown in the original SVG worksheet.

  1. Integrate the flux over the triangle in terms of the given parameters.

  2. Show that the same result equals area times field at the centroid, and explain why that shortcut is not generally exact for a quadratic field.

Question 2 - Solution

A triangular aperture samples a linear field at its centroid

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Φ=∫0a∫0b(1−x/a)(E0+αx+βy)dydx.\Phi=\int_0^a\!\int_0^{b(1-x/a)}(E_0+\alpha x+\beta y)\,dy\,dx.Φ=abE02+αa2b6+βab26.\Phi=\frac{abE_0}{2}+\frac{\alpha a^2b}{6}+\frac{\beta ab^2}{6}.

(b) Interpretation and further calculation

A=ab/2,(xc,yc)=(a/3,b/3).A=ab/2,\quad(x_c,y_c)=(a/3,b/3).Φ=A(E0+αa3+βb3)=AEz(xc,yc).\Phi=A\left(E_0+\frac{\alpha a}{3}+\frac{\beta b}{3}\right)=AE_z(x_c,y_c).A linear field depends only on the first area moments; a quadratic profile also depends on second moments.

Physical check

If both gradients vanish, the expression reduces to E0ab/2E_0ab/2.