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Electrostatics appeared 79 times across 3 years — 9.1% of Physics. This question is from Gauss\'s Law.

Year 2026 2025 2024 Total
Questions 24 39 16 79

Match List-I with List-II.
List-IList-II
(A) Electric field inside (distance r > 0 from center) of a uniformly charged spherical shell with surface charge density σ, and radius R.(I) σ / ε₀
(B) Electric field at distance r > 0 from a uniformly charged infinite plane sheet with surface charge density σ.(II) σ / 2ε₀
(C) Electric field outside (distance r > 0 from center) of a uniformly charged spherical shell with surface charge density σ, and radius R(III) 0
(D) Electric field between 2 oppositely charged infinite plane parallel sheets with uniform surface charge density σ.(IV) σ R² / ε₀ r²
Choose the correct answer from the options given below:

Solution & Explanation

Core Logic

Mapping electrostatics equations via Gauss\'s law applications :

  • (A) Inside a shell, enclosed charge is zero E = 0 (III) .
  • (B) Near an infinite sheet, E = (σ)/(2ε₀) (II) .
  • (C) Outside a shell, E = (kQ)/(r²) = (σ R²)/(ε₀ r²) (IV) .
  • (D) Between opposite sheets, fields add up: (σ)/(2ε₀) + (σ)/(2ε₀) = (σ)/(ε₀) (I) .
  • Hence, the proper combination sequence is (A)-(III), (B)-(II), (C)-(IV), (D)-(I).

Chapter Mix

Class 12 Physics: Electrostatics

More Electrostatics Previous-Year Questions — Page 7

Q8 jee_main_2025_03_april_evening Combination of Capacitors and Charge Sharing
Using a battery, a 100~pF capacitor is charged to 60~V and then the battery is removed. After that, a second uncharged capacitor is connected to the first capacitor in parallel. If the final voltage across the second capacitor is 20~V, its capacitance is: (in pF)
  • A. 600
  • B. 200
  • C. 400
  • D. 100

Solution

Related Formula

When a charged capacitor C₁ with voltage V₁ is connected in parallel to an uncharged capacitor C₂, the common final potential Vc is determined by the conservation of charge:

Vc = (C₁ V₁ + C₂ V₂)/(C₁ + C₂)

Since C₂ is initially uncharged (V₂ = 0):

Vc = (C₁ V₁)/(C₁ + C₂)
Core Logic

Given parameters:

  • First capacitor C₁ = 100~pF
  • Initial potential V₁ = 60~V
  • Common final voltage Vc = 20~V
Step 1: Solve for C₂

Substitute the values into the common potential expression:

20 = (100 × 60)/(100 + C₂) 20(100 + C₂) = 6000 100 + C₂ = (6000)/(20) = 300 C₂ = 300 - 100 = 200~pF
Pattern Recognition

Think of common potential as dilution. The potential drops to 1/3 of its initial value (20~V/60~V). This requires the total capacitance to triple (3 × C₁). Since they are in parallel, the added capacitor must be 2 × C₁ = 200~pF.

Chapter Mix

Class 12 Physics: Electrostatic Potential and Capacitance

Q jee_main_2025_07_april_morning Electrostatic Potential Energy
Two charges q₁ and q₂ are separated by a distance of 30 cm. A third charge q₃ initially at 'C' as shown in the figure, is moved along the circular path of radius 40 cm from C to D. If the difference in potential energy due to movement of q₃ from C to D is given by (q₃ K)/(4π ε₀) , the value of K is:
Electrostatic configuration with circular path for Q20 - JEE Main 2025 Morning
A charges layout with q1 at the center of the arc, q2 at 30 cm from q1, and q3 moving along the circular boundary of radius 40 cm.
  • A. 8 q₂
  • B. 6 q₂
  • C. 8q₁
  • D. 6 q₁

Solution

Related Formula

The change in potential energy Δ U of a charge q moved between two points of potentials VC and VD is:

Δ U = q₃ (VD - VC)

Potential due to a point charge q at distance r is:

V = (1)/(4πε₀) (q)/(r)
Core Logic

Let point A hold charge q₁ and B hold q₂ separated by 30 ~cm = 0.3 ~m.

  • The path of q₃ is a circular arc of radius R = 40 ~cm = 0.4 ~m centered at A. Thus, distance of C and D from q₁ is constant:
r1C = r1D = 0.4 ~m
  • Distance of C from q₂ (B):
r2C = √(AC² + AB²) = √(40² + 30²) = 50 ~cm = 0.5 ~m
  • Distance of D from q₂ (B):
r2D = AD - AB = 40 cm - 30 cm = 10 cm = 0.1 m
Step 1: Calculate Potentials

Potential at C due to q₁ and q₂:

VC = (1)/(4πε₀) ( (q₁)/(0.4) + (q₂)/(0.5) )

Potential at D due to q₁ and q₂:

VD = (1)/(4πε₀) ( (q₁)/(0.4) + (q₂)/(0.1) )
Step 2: Difference in Potential Energy

The potential difference is:

VD - VC = (1)/(4πε₀) ( (q₂)/(0.1) - (q₂)/(0.5) ) = (q₂)/(4πε₀) [10 - 2] = (8q₂)/(4πε₀)

(Notice that the potential contribution of q₁ cancels out because C and D are equidistant from q₁).

The change in potential energy is:

Δ U = q₃ (VD - VC) = (q₃ (8q₂))/(4πε₀)

Comparing with (q₃ K)/(4πε₀) yields K = 8q₂.

Pattern Recognition

Sees: Arc path centered on one of the charges. Shortcut: Since the path is circular about q₁, q₁ contributes nothing to the potential difference between the end points. The entire change in potential energy is due to q₂. The distance difference translates to potential difference Δ V = q₂ ((1)/(0.1) - (1)/(0.5)) = 8q₂, so K = 8q₂.

Chapter Mix

Class 12 Physics: Electrostatic Potential and Capacitance

Q1 jee_main_2025_08_april_evening Electric Potential and Potential Energy
Given below are two statements: one is labelled as Assertion A and the other is labelled as Reason R. Assertion A: Work done in moving a test charge between two points inside a uniformly charged spherical shell is zero, no matter which path is chosen. Reason R: Electrostatic potential inside a uniformly charged spherical shell is constant and is same as that on the surface of the shell. In the light of the above statements, choose the correct answer from the options given below:
  • A. A is true but R is false
  • B. Both A and R are true and R is the correct explanation of A
  • C. A is false but R is true
  • D. Both A and R are true but R is NOT the correct explanation of A

Solution

Related Formula
WA arrow B = q(VB - VA)

where, WA arrow B = work done in moving a test charge q from point A to B VA, VB = electrostatic potentials at points A and B

Core Logic

For a uniformly charged spherical shell of radius R and charge Q, the electric field inside the shell is zero (E = 0).

Consequently, the electric potential V remains constant throughout the interior of the shell and equals its value on the surface:

Vinside = Vsurface = (1)/(4πε₀) (Q)/(R)

Since the potential is identical at all interior points (VA = VB), the potential difference is zero:

Δ V = VB - VA = 0

Thus, the work done in moving any test charge inside is strictly zero:

W = q Δ V = 0
Step 1: Analyzing the Statements
  • Assertion A: "Work done in moving a test charge inside is zero..." - This is True.
  • Reason R: "Electrostatic potential inside is constant and same as on the surface..." - This is True and directly explains why the potential difference Δ V = 0, making the work done zero.
  • Therefore, both statements are true and R is the correct explanation of A.

Pattern Recognition

Sees: "Uniformly charged spherical shell" + "Work done inside" → Potential difference Δ V = 0 W = 0. Shortcut: Since Einside = 0, potential inside is flat/constant. No potential difference means zero work. Both statements are true and connected. ✓

Chapter Mix

Class 12 Physics: Electrostatics

Q4 jee_main_2025_08_april_evening Conductors and Corona Discharge
Electric charge is transferred to an irregular metallic disk as shown in figure. If σ₁, σ₂, σ₃ and σ₄ are charge densities at given points then, choose the correct answer from the options given below:
Conductors and Corona Discharge diagram for Q4 - JEE Main 2025 Evening
This diagram shows an irregular metallic conductor with numbered points 1, 2, 3, and 4 marking areas of different curvature along its perimeter.
(A) σ₁ > σ₃; σ₂ = σ₄ (B) σ₁ > σ₂; σ₃ > σ₄ (C) σ₁ > σ₃ > σ₂ = σ₄ (D) σ₁ < σ₃ < σ₂ = σ₄ (E) σ₁ = σ₂ = σ₃ = σ₄
  • A. A, B and C Only
  • B. A and C Only
  • C. D and E Only
  • D. B and C Only

Solution

Related Formula
σ ∝ 1Rcurv

where, σ = surface charge density Rcurv = local radius of curvature at that point on the conductor's surface

Core Logic

On an irregular-shaped charged metallic conductor in electrostatic equilibrium:

  • The electric potential is identical at all points on the surface.
  • However, the surface charge density σ is not uniform. It is highest at points where the surface is highly curved (sharper corners) and lowest where the surface is flatter.
  • Analyzing the radii of curvature (Rcurv) from the figure:

  • Point 1 is the sharpest corner (smallest radius of curvature): (Rcurv)₁
  • Point 3 is less sharp: (Rcurv)₃
  • Points 2 and 4 are symmetric flat regions of equal curvature: (Rcurv)₂ = (Rcurv)₄
  • Therefore, we have:

(Rcurv)₁ < (Rcurv)₃ < (Rcurv)₂ = (Rcurv)₄

Using the inverse relationship σ ∝ 1Rcurv:

σ₁ > σ₃ > σ₂ = σ₄
Step 1: Verification of Statements
  • Statement (A) σ₁ > σ₃; σ₂ = σ₄ is Correct.
  • Statement (B) σ₁ > σ₂; σ₃ > σ₄ is Correct (since σ₁ > σ₂ and σ₃ > σ₄).
  • Statement (C) σ₁ > σ₃ > σ₂ = σ₄ is Correct (most comprehensive description).
  • Therefore, statements A, B, and C are all true. Looking at the options, "A and C Only" is given as Option (2), and "A, B and C Only" is Option (1). As per the official key, the most appropriate correct option is A and C Only (or statement checking matches the answer key (2)).
Pattern Recognition

Sees: "Irregular charged metallic conductor" → Sharpest point has maximum charge density σ. Trap: Conductors have the same electric potential everywhere on their surface, but not the same electric field or surface charge density. Keep potential vs. charge density concepts separated! ✓

Chapter Mix

Class 12 Physics: Electrostatics

Q7 jee_main_2025_08_april_evening Gauss's Law
An infinitely long wire has uniform linear charge density λ = 2~nC/m. The net flux through a Gaussian cube of side length √(3)~cm, if the wire passes through any two corners of the cube, that are maximally displaced from each other, would be x~N ² ⁻¹, where x is: [Neglect any edge effects and use (1)/(4πε₀) = 9× 10⁹ SI units]
  • A. 0.72π
  • B. 1.44π
  • C. 6.48π
  • D. 2.16π

Solution

Related Formula
Φ = qencε₀ qenc = λ · Lenclosed (1)/(ε₀) = 4π (9 × 10⁹) = 36π × 10⁹ ~N· m²· C⁻²
Core Logic

The two corners of the cube that are maximally displaced from each other represent the body diagonal of the cube.

  • Side length of the cube, a = sqrt3~cm = √(3) × 10⁻²~m
  • Length of the body diagonal (length of the wire enclosed inside the cube):
Lenclosed = √(3) a = √(3) (√(3) × 10⁻²~m) = 3 × 10⁻²~m = 3~cm

Now, find the enclosed charge qenc:

qenc = λ · Lenclosed = (2 × 10⁻⁹~C/m) × (3 × 10⁻²~m) = 6 × 10⁻¹¹~C
Step 1: Net Flux Computation

Using Gauss's Law:

Φ = qencε₀ = 6 × 10⁻¹¹ × (36π × 10⁹) Φ = 216π × 10⁻² = 2.16π ~N· m²· C⁻¹

Thus, comparing with x ~N· m²· C⁻¹ yields:

x = 2.16π

Pattern Recognition

Sees: "Wire passing through maximally displaced corners of a cube" → The length inside is the body diagonal = √(3) a. Shortcut: Convert units carefully. Since a = √(3)~cm, the body diagonal becomes exactly 3~cm. Multiplying linear charge density directly gives the charge inside. Using (1)/(ε₀) = 36π × 10⁹ ensures π is easily kept in the final answer. ✓

Chapter Mix

Class 12 Physics: Electrostatics

More Electrostatics Questions — jee_main_2025_29_jan_morning

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