Application of Gauss' Theorem Electric Field near Charged Infinite
E Field Of Infinite Sheet. (1.6.12) (1.6.12) e = σ 2 ϵ 0. For an infinite sheet of charge, the electric field will be perpendicular to the surface.
Web all we have to do is to put α = π/2 α = π / 2 in equation 1.6.10 to obtain. For an infinite sheet of charge, the electric field will be perpendicular to the surface. (1.6.12) (1.6.12) e = σ 2 ϵ 0.
(1.6.12) (1.6.12) e = σ 2 ϵ 0. (1.6.12) (1.6.12) e = σ 2 ϵ 0. Web all we have to do is to put α = π/2 α = π / 2 in equation 1.6.10 to obtain. For an infinite sheet of charge, the electric field will be perpendicular to the surface.
