(a) Discontinuity of Normal Component of Electric Field:
Consider a small cylindrical Gaussian surface (pillbox) straddling a charged surface with uniform surface charge density σ. Let the flat faces of the cylinder be parallel to the surface, one face (Area A) just inside the surface (region 1) and the other face (Area A) just outside the surface (region 2). The curved surface area is negligible. Let E₁ and E₂ be the electric fields in region 1 and region 2, respectively. Let n̂ be the unit vector normal to the surface, pointing from region 1 to region 2.
According to Gauss's Law, the total electric flux through a closed surface is equal to the total charge enclosed divided by ε₀:
∮ E ⋅ dA = Qenclosed / ε₀
The flux through the curved surface is zero because the electric field is perpendicular to the curved surface (or the curved surface is infinitesimally small).
Flux through the face in region 2 = E₂ ⋅ n̂ A
Flux through the face in region 1 = E₁ ⋅ (-n̂) A (since n̂ points from 1 to 2, the outward normal for region 1 face is -n̂)
Total flux = (E₂ ⋅ n̂ A) + (E₁ ⋅ (-n̂) A) = (E₂ ⋅ n̂ - E₁ ⋅ n̂) A = (E₂ - E₁) ⋅ n̂ A
The charge enclosed by the pillbox is Qenclosed = σA.
Applying Gauss's Law:
(E₂ - E₁) ⋅ n̂ A = σA / ε₀
Dividing by A, we get:
(E₂ - E₁) ⋅ n̂ = σ/ε₀
This shows that the normal component of the electric field is discontinuous across a charged surface, and the discontinuity is equal to σ/ε₀.
Special Case: If region 1 is inside a conductor, E₁ = 0. Then, E₂ ⋅ n̂ = σ/ε₀, which means the electric field just outside a conductor is σ/ε₀, normal to the surface.
(b) Continuity of Tangential Component of Electric Field:
Consider a small rectangular closed loop (Amperian loop) placed across the charged surface. Let the length of the loop parallel to the surface be L, and the width perpendicular to the surface be infinitesimally small (approaching zero). Let the loop be oriented such that two sides of length L are parallel to the surface, one just above (region 2) and one just below (region 1) the surface. Let E₁ and E₂ be the electric fields in region 1 and region 2, respectively.
For a conservative field like the electrostatic field, the line integral of the electric field around any closed loop is zero:
∮ E ⋅ dl = 0
Let E₁t and E₂t be the tangential components of the electric field in region 1 and region 2, respectively, along the length L of the loop.
The line integral along the loop can be broken into four parts:
∫₁ E ⋅ dl + ∫₂ E ⋅ dl + ∫₃ E ⋅ dl + ∫₄ E ⋅ dl = 0
Where:
∫₁ E ⋅ dl = E₂t L (along the side in region 2)
∫₂ E ⋅ dl = 0 (along the infinitesimally small side perpendicular to the surface, as its length approaches zero)
∫₃ E ⋅ dl = -E₁t L (along the side in region 1, in the opposite direction)
∫₄ E ⋅ dl = 0 (along the other infinitesimally small side perpendicular to the surface)
So, E₂t L - E₁t L = 0
(E₂t - E₁t) L = 0
Since L ≠ 0, we must have:
E₂t - E₁t = 0
E₂t = E₁t
This shows that the tangential component of the electric field is continuous across a charged surface. In other words, the tangential component of the electric field just above the surface is equal to the tangential component just below the surface.
NEET Relevance
While the full derivation is more common for board exams, the *results* (boundary conditions for normal and tangential components of E-field) are very important for NEET. MCQs often test the understanding of these conditions, especially for conductors (where E_tangential = 0 and E_normal = σ/ε₀ just outside).
This question has appeared in previous NEET exams.