⚡ Gauss's Theorem:
Basic Statement, Mathematical Formulation & Electric Flux
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1. Gauss's Theorem — Basic Statement
Gauss's theorem states that the total electric flux through any closed
surface is equal to 1/ε₀ times the net charge enclosed
by that surface.
ΦE = Qenc/ε₀
The important point is:
Only the charge enclosed inside the closed surface contributes to
the net flux.
Charges outside the Gaussian surface may produce electric field through
the surface, but their net flux is zero.
2. Mathematical Formulation
For a small surface element dA:
dΦ = E⃗ · dA⃗
Since:
dΦ = E dA cos θ
For a complete closed surface:
Φ = ∮ E⃗ · dA⃗
According to Gauss's theorem:
∮ E⃗ · dA⃗ = Qenc/ε₀
3. 🔬 Interactive Gaussian Surface Simulator
Change charge, surface size and field direction
q =
5
μC
R =
5
m
E =
5
+
Gaussian Surface
Enclosed charge
Enclosed Charge:
0 C
Net Electric Flux: 0 N·m²/C
Surface Radius: 5 m
Observation: Increasing the Gaussian surface size does not change the total flux if the enclosed charge remains unchanged.
Net Electric Flux: 0 N·m²/C
Surface Radius: 5 m
Observation: Increasing the Gaussian surface size does not change the total flux if the enclosed charge remains unchanged.
4. What is Electric Flux?
Electric flux measures the number of electric field lines passing through
a surface.
For a uniform electric field:
E = electric field
A = area of surface
θ = angle between electric field and area vector.
Φ = EA cos θ
where:
E = electric field
A = area of surface
θ = angle between electric field and area vector.
⚠️ Important:
The angle θ is measured between E and the
area vector, not directly with the plane.
If the angle is given between E and the plane itself, use: Φ = EA sin θ
If the angle is given between E and the plane itself, use: Φ = EA sin θ
5. ⭐ Important Flux Cases
| Condition | θ | Flux |
|---|---|---|
| E parallel to area vector | 0° | EA |
| E perpendicular to area vector | 90° | 0 |
| E opposite to area vector | 180° | −EA |
6. Flux Due to a Point Charge
For a point charge q at the centre of a spherical Gaussian surface:
Electric field at radius R:
E = (1/4πε₀) q/R²
Area of sphere:
A = 4πR²
Therefore:
Φ = EA
Substituting:
Φ =
(q/4πε₀R²)(4πR²)
Hence:
Φ = q/ε₀
Notice that R² cancels.
Therefore the total flux is independent of the radius of the Gaussian
surface.
7. Why Gaussian Surface is Useful?
Point Charge
Use a spherical Gaussian surface.
E is same at every point of the sphere.
Φ = E(4πR²)
Use a spherical Gaussian surface.
E is same at every point of the sphere.
Φ = E(4πR²)
Infinite Line Charge
Use a cylindrical Gaussian surface.
E is same on the curved surface.
Φ = E(2πRL)
Use a cylindrical Gaussian surface.
E is same on the curved surface.
Φ = E(2πRL)
Infinite Plane Sheet
Use a pillbox Gaussian surface.
Flux passes through both flat faces.
Φ = 2EA
Use a pillbox Gaussian surface.
Flux passes through both flat faces.
Φ = 2EA
8. ⭐ Standard Applications of Gauss's Law
| Charge Distribution | Gaussian Surface | Electric Field |
|---|---|---|
| Point charge | Sphere | q/(4πε₀R²) |
| Infinite line charge | Cylinder | λ/(2πε₀R) |
| Infinite plane sheet | Pillbox | σ/(2ε₀) |
| Conducting surface | Pillbox | σ/ε₀ |
9. Infinite Line Charge — Flux Calculation
Let linear charge density be λ.
For a cylindrical Gaussian surface:
Enclosed charge:
Q = λL
Curved surface area:
A = 2πRL
Since E is constant on the curved surface:
Φ = E(2πRL)
Using Gauss's law:
E(2πRL) = λL/ε₀
Therefore:
E = λ/(2πε₀R)
10. Infinite Plane Sheet
For surface charge density σ, choose a pillbox Gaussian surface.
Charge enclosed:
Q = σA
Flux passes through two faces:
Φ = EA + EA = 2EA
Gauss's law gives:
2EA = σA/ε₀
Hence:
E = σ/(2ε₀)
11. Electric Field Just Outside a Conductor
For a conductor in electrostatic equilibrium:
Electric field inside the conductor = 0
Take a small Gaussian pillbox.
Flux:
Φ = EA
Enclosed charge:
Q = σA
Therefore:
EA = σA/ε₀
Hence:
E = σ/ε₀
12. ⭐ Most Important JEE Concept
Charge inside Gaussian surface → contributes to net flux.
Charge outside Gaussian surface → contributes zero net flux.
However, an external charge can still create electric field at points on the Gaussian surface.
Charge outside Gaussian surface → contributes zero net flux.
However, an external charge can still create electric field at points on the Gaussian surface.
13. 📝 30 JEE-Level MCQs with Solutions
1. According to Gauss's theorem, total electric flux through a closed
surface is:
A. Qε₀
B. Q/ε₀
C. ε₀/Q
D. Zero always
Answer: B
Φ = Qenc/ε₀.
Φ = Qenc/ε₀.
2. Electric flux is a:
A. Scalar quantity
B. Vector quantity
C. Tensor quantity
D. Dimensionless quantity
Answer: A. Scalar
3. Electric flux through a surface is maximum when θ is:
A. 0°
B. 45°
C. 90°
D. 180°
Answer: A. 0°
Φ = EA cosθ.
Φ = EA cosθ.
4. Flux is zero when electric field is parallel to the surface.
A. True
B. False
Answer: A. True
E is perpendicular to area vector, so θ = 90°.
E is perpendicular to area vector, so θ = 90°.
5. SI unit of electric flux is:
A. N/C
B. N·m²/C
C. C/N
D. J/C
Answer: B
6. A closed surface encloses charge 5 μC. Flux is approximately:
A. 5ε₀
B. 5/ε₀ μC
C. 5 × 10⁻⁶/ε₀
D. Zero
Answer: C
Φ = Q/ε₀.
Φ = Q/ε₀.
7. A charge outside a closed Gaussian surface produces:
A. Positive net flux
B. Negative net flux
C. Zero net flux
D. Infinite flux
Answer: C
8. For a point charge, the suitable Gaussian surface is:
A. Cube
B. Sphere
C. Cylinder
D. Plane
Answer: B
9. For an infinite line charge, the suitable Gaussian surface is:
A. Sphere
B. Cube
C. Cylinder
D. Cone
Answer: C
10. For an infinite plane sheet, the suitable Gaussian surface is:
A. Sphere
B. Pillbox
C. Cylinder along the sheet
D. Cube only
Answer: B
11. Electric field due to an infinite line charge is:
A. λ/(4πε₀R²)
B. λ/(2πε₀R)
C. λ/(ε₀R²)
D. λR/(2πε₀)
Answer: B
12. Electric field due to an infinite non-conducting sheet is:
A. σ/ε₀
B. σ/(2ε₀)
C. 2σ/ε₀
D. Zero
Answer: B
13. Electric field just outside a charged conductor is:
A. σ/(2ε₀)
B. σ/ε₀
C. 2σ/ε₀
D. Zero
Answer: B
14. Electric field inside a conductor in electrostatic equilibrium is:
A. σ/ε₀
B. σ/(2ε₀)
C. Zero
D. Infinite
Answer: C
15. If the radius of a spherical Gaussian surface is doubled, flux due to
a fixed enclosed charge becomes:
A. Double
B. Four times
C. Half
D. Same
Answer: D. Same
Flux depends only on enclosed charge.
Flux depends only on enclosed charge.
16. If enclosed charge is doubled, flux becomes:
A. Half
B. Same
C. Double
D. Four times
Answer: C
17. If net enclosed charge is zero, total flux through a closed surface is:
A. Zero
B. Infinite
C. Always positive
D. Always negative
Answer: A
18. A closed surface contains +q and −q. Net flux is:
A. q/ε₀
B. 2q/ε₀
C. Zero
D. −q/ε₀
Answer: C
Net enclosed charge = 0.
Net enclosed charge = 0.
19. Flux through a closed surface depends on:
A. Surface shape only
B. Surface area only
C. Enclosed charge
D. Radius only
Answer: C
20. The outward area vector of a closed surface points:
A. Inward
B. Tangentially
C. Outward normal
D. Randomly
Answer: C
21. Flux through a sphere containing charge q is:
A. q/(4πε₀R²)
B. q/ε₀
C. qR²/ε₀
D. Zero
Answer: B
22. A Gaussian surface must necessarily be:
A. Spherical
B. Cylindrical
C. Closed
D. Planar
Answer: C
23. Gauss's law is most useful when the charge distribution has:
A. No symmetry
B. High symmetry
C. Random distribution
D. Zero charge only
Answer: B
24. Dimension of electric flux is:
A. ML³T⁻³A⁻¹
B. ML²T⁻³A⁻¹
C. MLT⁻²
D. ML²T⁻²
Answer: A
25. If the angle between E and area vector is 60°, flux is:
A. EA
B. EA/2
C. √3EA/2
D. Zero
Answer: B
Φ = EA cos60° = EA/2.
Φ = EA cos60° = EA/2.
26. If electric field is parallel to the surface, flux is:
A. EA
B. EA/2
C. Zero
D. 2EA
Answer: C
27. A point charge is placed outside a closed surface. Its contribution to
net flux is:
A. q/ε₀
B. −q/ε₀
C. Zero
D. qε₀
Answer: C
28. For an isolated positive charge, net flux through a surrounding
closed surface is:
A. Positive
B. Negative
C. Zero
D. Depends only on radius
Answer: A
29. For an isolated negative charge, net electric flux is:
A. Positive
B. Negative
C. Zero
D. Infinite
Answer: B
30. Gauss's law is mathematically represented by:
A. ∮E·dA = 0
B. ∮E·dA = Q/ε₀
C. E = q/r
D. Φ = qε₀
Answer: B
14. ⭐ JEE Quick Revision
Electric Flux:
Φ = ∫ E⃗ · dA⃗
Uniform Field: Φ = EA cosθ
Gauss's Law: ∮ E⃗ · dA⃗ = Qenc/ε₀
Point Charge: Φ = q/ε₀
Infinite Line: E = λ/(2πε₀r)
Infinite Sheet: E = σ/(2ε₀)
Conductor Surface: E = σ/ε₀
Key Rule: Only net enclosed charge determines the total flux through a closed surface.
Uniform Field: Φ = EA cosθ
Gauss's Law: ∮ E⃗ · dA⃗ = Qenc/ε₀
Point Charge: Φ = q/ε₀
Infinite Line: E = λ/(2πε₀r)
Infinite Sheet: E = σ/(2ε₀)
Conductor Surface: E = σ/ε₀
Key Rule: Only net enclosed charge determines the total flux through a closed surface.