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Home
JEE Physics
Gaussian Surface

Gaussian Surface

A Gaussian surface is a theoretical, closed surface used in electromagnetism to apply Gauss’s Law. It plays a crucial role in calculating the electric flux through a surface and greatly simplifies the determination of electric fields, especially for systems with symmetrical charge distributions. By selecting a Gaussian surface that aligns with the symmetry of the charge configuration—such as spherical, cylindrical, or planar symmetry—complex field calculations become more manageable.

1.0Gaussian Surface Definition

A Gaussian surface is an imaginary, closed surface used in the application of Gauss’s Law to analyze electric fields. It is not a physical object but a conceptual tool that encloses electric charge and helps calculate the electric flux through that surface. By choosing a Gaussian surface that matches the symmetry of the charge distribution (spherical, cylindrical, or planar), the electric field can be determined more easily and efficiently.

2.0Types of Gaussian Surface And Shapes

The choice of a Gaussian surface depends on the symmetry of the charge distribution.

Type

Shape

Symmetry

Example

Spherical

Sphere

Spherical symmetry

Point charge, charged sphere

Cylindrical

Cylinder

Cylindrical symmetry

Charged wire, cylindrical shell

Planar

Plane/Box

Planar symmetry

Infinite sheet of charge

3.0Shapes of Gaussian Surface

Shapes of Gaussian Surface

4.0Choosing a Gaussian Surface

  1. Match the Symmetry: The Gaussian surface should reflect the symmetry of the charge distribution. This alignment simplifies electric field calculations by making the electric field uniform or zero in parts.
    (a) Planar Symmetry: For infinite plane charges, use a pillbox-shaped surface. This shape works because the electric field is uniform and perpendicular to the surface on both sides.
    (b) Cylindrical Symmetry: For long charged wires or cylindrical distributions, choose a cylindrical Gaussian surface. Here, the electric field is radial and constant along the curved surface, making calculations easier.
    (c) Spherical Symmetry: For point charges or uniformly charged spheres, select a spherical surface centered on the charge. The electric field is radial and has the same magnitude at every point on this surface.

2.Align with the Electric Field: Ensure the Gaussian surface is oriented so the electric field is either perpendicular or parallel to the surface, which simplifies the dot product in Gauss’s Law.

Charge Distribution

Direction of Electric Field 

Gaussian Surface

Point charge

Radial (along the radius of sphere)

Concentric surface

Spherical charge

Radial (along the radius of sphere)

Concentric surface

Line charge

Radial (along the radius of sphere)

Coaxial cylinder

Planar charge or Charged sheets

Normal to surface

Parallel planes

5.0Gauss Law

Net electric flux passing through any closed imaginary surface (Gaussian surface) is 10 (ε0​1​) times of the total charge enclosed by it.

ϕNet​=ε0​Qenclosed​​

To understand this concept, consider a closed surface as shown                                      

Gauss Law

ϕNet​=ε0​(q1​−q2​+q3​)​

Charges present outside the closed surface –q4 and +q5 do not play any role in net flux passing through the surface (also called gaussian surface).

ϕNet​=∮E⋅ds=ε0​Qenclosed​​

Key Points:

  1. Flux through Gaussian surface is independent of location of charges within Gaussian surface.

Flux through Gaussian surface is independent of location of charges within Gaussian surface.

  1. Flux through Gaussian surface is independent of shape and size of Gaussian surface provided the net charge enclosed remains same.

Flux through Gaussian surface is independent of shape and size of Gaussian surface provided the net charge enclosed remains same.

  1. When net flux is going out then the positive charge is enclosed by the Gaussian surface.

When net flux is going out then the positive charge is enclosed by the Gaussian surface.

  1. When net flux is coming in then negative charge is enclosed by the Gaussian surface.

When net flux is coming in then negative charge is enclosed by the Gaussian surface.

  1. In Gauss’s theorem

E→due to all the charges, but ϕclosed​→due to enclosed charges only.

In Gauss’s theorem


Gauss’s theorem

  1. When an imaginary closed surface is placed in an external electric field, net flux passing through it will be zero.

When an imaginary closed surface is placed in an external electric field, net flux passing through it will be zero.

  1. Gauss’s theorem is applicable for all the forces following inverse square law.
  2. For a Gaussian surface Φ = 0 does not imply E = 0, but E = 0 implies Φ = 0.

6.0Limitations of Gaussian surface

  1. Lack of Symmetry: Gauss’s Law is difficult to apply when the charge distribution is irregular or asymmetric.
  2. Multiple Charges: Complex charge arrangements can make it hard to choose a suitable Gaussian surface.
  3. Finite Geometries: Real-world objects often lack the ideal symmetry (infinite planes, lines, etc.) assumed in Gauss’s Law.

7.0Applications of Gaussian Surface

  1. Capacitors:Used to calculate the electric field between parallel plates using planar Gaussian surfaces.
  2. Transmission Lines: Helps determine the field around charged wires with cylindrical surfaces.
  3. Atomic Models: Analyzes electric fields around nuclei using spherical Gaussian surfaces.
  4. Electrostatic Shielding: Assists in designing materials that block external fields by applying Gauss’s Law inside conductors.

Table of Contents


  • 1.0Gaussian Surface Definition
  • 2.0Types of Gaussian Surface And Shapes
  • 3.0Shapes of Gaussian Surface
  • 4.0Choosing a Gaussian Surface
  • 5.0Gauss Law
  • 6.0Limitations of Gaussian surface
  • 7.0Applications of Gaussian Surface

Frequently Asked Questions

A Gaussian surface is an imaginary closed surface used in Gauss’s Law to calculate the electric flux and analyze electric fields around charge distributions.

A closed surface is required because Gauss’s Law relates the net electric flux through a surface to the total charge enclosed within it.

Spherical, cylindrical, or planar symmetry is required to simplify the electric field and use Gauss’s Law effectively.

The electric field inside a conductor is zero, and a Gaussian surface placed inside it encloses no net charge.

Symmetric surfaces allow us to take the electric field outside the integral, simplifying the calculation of electric flux.

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