Q.The electric field components in Fig. 1.24 are Ex=αx1/2, Ey=Ez=0, in which α=800N/C m1/2. Calculate
Concept understanding — Gauss Law
Gauss's Law is a shortcut. Instead of adding up the Coulomb contribution of every charge — a nightmare of vectors and integrals — it lets you read the field straight off the symmetry of a problem. The whole idea rests on one quantity: electric flux.
Flux — field-lines counted through a surface. For a uniform field E crossing a flat area A, the flux is Φ = E·A = EA cosθ, where θ is the angle between the field and the normal to the surface. Picture the field as a bundle of lines; flux is how many pierce the surface. When E is edge-on (θ = 90°) nothing passes through and Φ = 0; when E is ⊥ to the surface (θ = 0) the count is maximal. For a closed surface, Φ is the net number of lines leaving it — lines that enter and exit cancel.
The law itself. Gauss's law states that the net flux out of any closed surface depends only on the charge trapped inside:
Φ = q_enclosed / ε₀.
Two consequences do most of the work. First, only enclosed charge counts — a charge outside sends as many lines in as out, so its net contribution is exactly zero. Second, the surface's shape is irrelevant; move the charge around inside or deform the surface, and Φ never changes.
Why symmetry makes it powerful. By itself Φ = q/ε₀ has E buried in an integral. It becomes a tool only when you pick a Gaussian surface matched to the symmetry — one where E is constant and everywhere either ⊥ to the surface (so Φ = EA) or ∥ to it (contributing nothing). Then E slides out and you solve in one line. This works for exactly three geometries:
1 — Infinite line charge (linear density λ). Use a coaxial cylinder: E = λ / 2πε₀r, falling off as ∝ 1/r.
2 — Infinite sheet (surface density σ). Use a pillbox pierced through the sheet: E = σ / 2ε₀ — uniform and completely independent of distance. The field near a large charged plane simply doesn't weaken as you step back.
3 — Spherical shell / sphere. For a thin shell of charge Q, a Gaussian sphere inside encloses nothing, so E = 0 everywhere within; outside, the charge acts as if concentrated at the centre, E = kQ/r² — indistinguishable from a point charge. For a solid uniformly charged sphere, an interior surface encloses only the charge within radius r, giving E ∝ r (rising linearly from zero at the centre) up to the surface, then 1/r² beyond.
Field just outside a conductor. A charged conductor holds all its charge on the surface with E = 0 inside, so a straddling pillbox gives E = σ / ε₀ just outside — twice the sheet result, because all the flux escapes on the one outer face.
How it's examined. JEE questions test whether you can spot the symmetry, pick the right surface, and recall which result scales as 1/r, which is flat, and which is 1/r². The physics is always the one line Φ = q_enclosed / ε₀, and the skill is knowing that only the enclosed charge — never the far-off one — ever matters.
"Gauss law class 12 physics derivation" and "electric field due to infinite sheet using Gauss law" are heavily searched terms, since this is one of the core results of the Electrostatics chapter in the NCERT/CBSE Class 12 Physics curriculum. Gauss's law applications for spheres, sheets, and line charges are near-guaranteed questions in JEE Main, NEET, and state CETs.
Why this formula?
Gauss's Law: Why It Holds
Gauss's Law is one of the four Maxwell's equations and a cornerstone of electromagnetism. Let's build the understanding from the ground up — not just the formula, but the why.
1. The Core Idea: Flux as "Flow" of Field
Imagine an electric field E passing through a small patch of area dA. The electric flux through that patch is:
dΦE=E⋅dA=EdAcosθ
where θ is the angle between E and the outward normal to the surface.
Why this definition?
- If E is perpendicular to the surface (θ=0), maximum field "flows through".
- If E is parallel (θ=90∘), no flux — the field just slides along the surface.
Total flux through a closed surface S is:
ΦE=∮SE⋅dA
2. The Key Insight: Flux Depends Only on Enclosed Charge
Consider a single point charge +q at the centre of a spherical surface of radius r.
- By Coulomb's law, at every point on the sphere: E=4πε01r2q, radially outward.
- The area vector dA is also radially outward.
- So E⋅dA=EdA everywhere.
The total flux:
ΦE=∮EdA=E∮dA=(4πε01r2q)(4πr2)=ε0q
Notice: The r2 cancels! The flux is independent of the radius.
3. Why Shape Doesn't Matter
Now, what if the surface is not spherical but any closed shape enclosing the charge?
- Draw a small cone from the charge to the surface.
- The flux through a patch dA at distance r is dΦ=4πε01r2qcosθdA.
- But r2cosθdA is exactly the solid angle dΩ subtended by dA at the charge.
So dΦ=4πε0qdΩ.
Integrating over the entire closed surface: ∮dΩ=4π (total solid angle around a point).
Hence:
ΦE=4πε0q⋅4π=ε0q
Result: For any closed surface enclosing q, the flux is ε0q.
4. Multiple Charges: Superposition
If there are many charges q1,q2,…,qn inside the surface, the total electric field is the vector sum of individual fields:
E=E1+E2+⋯+En
Flux is linear:
∮E⋅dA=∮E1⋅dA+∮E2⋅dA+⋯=ε0q1+ε0q2+⋯=ε0Qenc
Charges outside the surface contribute zero net flux — their field lines enter and exit the surface, cancelling out.
5. The Final Law
∮SE⋅dA=ε0Qenc
Why it's profound:
- It relates a global property (flux through a surface) to a local source (charge inside).
- It's true for any closed surface, not just symmetric ones.
- It's a direct consequence of Coulomb's inverse-square law — the 1/r2 dependence is essential for the cancellation.
6. Quick Exam Tip
| Situation | What to remember |
|---|---|
| Point charge | Flux = q/ε0 through any enclosing surface |
| Dipole inside | Net flux = 0 (equal + and -) |
| Charge outside | Flux contribution = 0 |
| Symmetric surfaces | Use Gauss's law to find E easily |
Key takeaway: Gauss's law holds because the electric field from a point charge obeys the inverse-square law, making the flux through any closed surface independent of the surface's shape — it depends only on the total charge enclosed.
Only the two faces perpendicular to the x‑axis carry flux, since Ey=Ez=0 and Ex=αx1/2 is constant on each such face.
Left face (x=a, outward normal −x^): ΦL=−αa1/2a2=−αa5/2.
Right face (x=2a, outward normal +x^): ΦR=+α(2a)1/2a2=2αa5/2.
- Net flux:
With α=800N/C⋅m1/2 and a=0.1m, a5/2=3.16×10−3:
Φ=ΦL+ΦR=αa5/2(2−1).
Φ=800(3.16×10−3)(0.414)≈1.05N⋅m2/C.
- Enclosed charge (Gauss's law):
q=ε0Φ=(8.854×10−12)(1.05)≈9.27×10−12C.
✓Final answerNet flux Φ≈1.05N⋅m2/C; enclosed charge q≈9.27×10−12C.
Only the two faces ⊥ to the x‑axis carry flux; with Ex=αx1/2 the net flux is Φ=αa5/2(2−1)≈1.05N⋅m2/C, and by Gauss's law the enclosed charge is q=ε0Φ≈9.27×10−12C.
The field points only along x, so flux passes only through faces whose normal has an x‑component. For the axis‑aligned cube, those are the left face at x=a and the right face at x=2a; the four faces parallel to the x‑axis contribute nothing because E⋅dA=0 there.
Left face (x=a). Here Ex=αa1/2 is uniform over the face of area a2, and the outward normal points in −x^:
ΦL=−(αa1/2)a2=−αa5/2.
Right face (x=2a). Now Ex=α(2a)1/2=2αa1/2, and the outward normal points in +x^:
ΦR=+(2αa1/2)a2=2αa5/2.
- Net flux.
With α=800N/C⋅m1/2 and a=0.1m,
Φ=ΦL+ΦR=αa5/2(2−1).
a5/2=(0.1)5/2=3.162×10−3,2−1=0.4142,
Φ=800×3.162×10−3×0.4142≈1.05N⋅m2/C.
Watch outNote a5/2=a2a, not a3/2 — the extra a2 is the face area. Keep the minus sign on the left face, or the two contributions wrongly add.
- Enclosed charge. Gauss's law Φ=q/ε0 gives
q=ε0Φ=(8.854×10−12)(1.05)≈9.27×10−12C.
✓Final answer- Net flux Φ≈1.05N⋅m2/C.
- Enclosed charge q≈9.27×10−12C.
Method: Gauss's Law Flux Calculation via Surface Integration
This problem uses Gauss's Law in integral form:
ΦE=∮E⋅dA=ε0qenc
Step 1: Identify the non-zero field contribution
Given:
- Ex=αx1/2, where α=800 N/C m1/2
- Ey=Ez=0
- Cube side length a=0.1 m, placed with one corner at origin
Since only Ex is non-zero, flux only passes through faces perpendicular to the x-axis — the left face (at x=0) and the right face (at x=a).
Step 2: Calculate flux through each x-face
Right face (x=a=0.1 m):
- Area vector: dA=i^dydz (outward normal is +i^)
- Field at this face: Ex=αa1/2 (constant over the face)
- Flux:
Φright=∫ExdA=αa1/2×a2=αa5/2
Left face (x=0):
- Area vector: dA=−i^dydz (outward normal is −i^)
- Field at this face: Ex=α(0)1/2=0
- Flux: Φleft=0
Step 3: Total flux through the cube
ΦE=Φright+Φleft=αa5/2+0
Substitute values:
ΦE=800×(0.1)5/2=800×(0.1)2×(0.1)1/2
Since (0.1)1/2=0.1≈0.3162:
ΦE=800×0.01×0.3162=8×0.3162
ΦE=2.53 N m2/C
Step 4: Find enclosed charge using Gauss's Law
qenc=ε0ΦE
ε0=8.85×10−12 C2/N m2
qenc=(8.85×10−12)×2.53
qenc=2.24×10−11 C
Final Answer Summary
| Quantity | Value |
|---|---|
| Flux through cube | 2.53 N m2/C |
| Charge inside cube | 2.24×10−11 C |
Common Mistakes Students Make with This Gauss Law Problem
Mistake 1: Forgetting That Flux Depends Only on the Perpendicular Component
The error: Students often try to integrate Ex over all six faces of the cube, including faces where the field is parallel to the surface.
Why it's wrong: Flux through a surface is Φ=∫E⋅dA. Since Ey=Ez=0, only the two faces perpendicular to the x-axis contribute. The four side faces (parallel to the x-axis) have zero flux because E⋅dA=0 there.
How to avoid: Always check which field components are non-zero. If Ey=Ez=0, only faces with normals along i^ matter. Draw the cube and label each face's normal vector.
Mistake 2: Using the Same x Value for Both Faces
The error: Plugging x=a into Ex=αx1/2 for both the left and right faces.
Why it's wrong: The left face is at x=0, the right face is at x=a. The field strength is different at each location:
- Left face: Ex(0)=α⋅01/2=0
- Right face: Ex(a)=αa1/2
How to avoid: Write the coordinates explicitly:
- Left face: x=0, area vector dA=−dAi^
- Right face: x=a, area vector dA=+dAi^
Then compute each flux separately.
Mistake 3: Ignoring the Direction of the Area Vector
The error: Treating both faces as having +dAi^ and getting zero net flux.
Why it's wrong: By convention, the area vector points outward from the closed surface:
- Left face: outward normal is −i^, so dA=−dAi^
- Right face: outward normal is +i^, so dA=+dAi^
The flux through the left face is:
Φleft=∫E⋅dA=∫(Exi^)⋅(−dAi^)=−∫ExdA
How to avoid: Always draw outward normals on each face before computing dot products.
Mistake 4: Forgetting That Ex Varies Over the Face
The error: Treating Ex as constant over the entire right face and writing Φ=Ex⋅A.
Why it's wrong: Ex=αx1/2 depends on x. On the right face, x=a is constant, so this actually works here — but only because the face is perpendicular to the x-axis. Students often carry this habit to problems where the field varies across the face.
How to avoid: Check if the field component is constant over the surface. Here, since the right face is at fixed x=a, Ex is uniform across it. But be cautious — this is a special case.
Mistake 5: Incorrectly Computing the Net Flux
The error: Adding magnitudes without signs, e.g., Φnet=αa1/2⋅a2+0=αa5/2.
Why it's wrong: The left face contributes negative flux because E points inward there (field enters the cube). The correct calculation:
Φnet=Φleft+Φright=−α(0)1/2⋅a2+αa1/2⋅a2=αa5/2
The left face has Ex=0, so its flux is zero. The net flux is just from the right face: Φnet=αa5/2.
How to avoid: Compute each face's flux with its correct sign, then sum. Don't shortcut.
Mistake 6: Using the Wrong Formula for Charge from Flux
The error: Writing q=Φ⋅ε0 instead of q=Φε0.
Why it's wrong: Gauss's law states:
Φ=ε0qenc⇒qenc=Φε0
How to avoid: Memorize the exact form: flux = charge enclosed divided by epsilon-zero. Rearrange carefully.
Mistake 7: Unit Errors in the Final Answer
The error: Reporting flux in N/C or charge in C without checking dimensions.
Why it's wrong: Flux has units N⋅m2/C. With α=800N/C⋅m1/2 and a=0.1m:
Φ=αa5/2=800⋅(0.1)5/2=800⋅(0.1)2⋅(0.1)1/2=800⋅0.01⋅0.316=2.53N⋅m2/C
Then q=Φε0=2.53×8.85×10−12=2.24×10−11C.
How to avoid: Track units at every step. Write the unit of each quantity before substituting numbers.
Quick Checklist to Avoid These Mistakes
| Step | What to Check |
|---|---|
| 1 | Which field components are non-zero? |
| 2 | Which faces have flux? (Only those with E⊥ face) |
| 3 | What is the x-coordinate of each contributing face? |
| 4 | What is the outward normal direction for each face? |
| 5 | Is the field constant over the face? |
| 6 | Did I include the correct sign in the dot product? |
| 7 | Did I use q=Φε0 correctly? |
| 8 | Are the final units consistent? |
- KEAM 2026Set eng-2026-04194 marksMCQQ.If a spherical conductor of 10 cm radius contains 5×106 electrons, then the electric field on its surface (in NC−1) is (A) 0.86 (B) 0.36 (C) 0.45 (D) 1.44 (E) 0.72
›Reveal solutionSolution
Find the surface charge, then use E=kQ/r2 at the sphere's surface.
Total charge:
Q=ne=(5×106)(1.6×10−19)=8×10−13 C.
Field at the surface of a conducting sphere of radius r=0.1 m:
E=r2kQ=(0.1)2(9×109)(8×10−13)=0.017.2×10−3=0.72 N C−1.
✓Final answerThe correct option is (E).
- KEAM 2026Set eng-2026-04214 marksMCQQ.If an infinitely long uniformly charged wire produces an electric field of intensity E at a distance of d from it, then the linear charge density λ of the wire is (A) πϵ0Ed (B) 2πϵ0Ed (C) 21ϵ0Ed (D) 2πϵ0Ed (E) ϵ0Ed
›Reveal solutionSolution
Invert E=2πϵ0dλ to get λ=2πϵ0Ed.
For an infinite line charge, Gauss's law gives E=2πϵ0dλ at perpendicular distance d.
Rearranging: λ=2πϵ0Ed.
✓Final answerThe correct option is (D).
- KEAM 2026Set eng-2026-04224 marksMCQQ.A uniformly charged cube of side one cm having surface charge density of 8.85 μC cm−2 is placed inside a hollow metal sphere. The total flux emerging out of the sphere in Nm2C−1 is (ε0=8.85×10−12 C2N−1m−2) (A) 8.85×106 (B) 12×106 (C) 19.7×106 (D) 3×106 (E) 6×106
›Reveal solutionSolution
By Gauss's law the flux out of the enclosing sphere is the total charge divided by ε0.
The cube (side 1 cm) has 6 faces of 1cm2 each, total area 6cm2.
Total charge Q=σA=8.85μC cm−2×6cm2=53.1μC=53.1×10−6C.
Flux =ε0Q=8.85×10−1253.1×10−6=6×106Nm2C−1.
✓Final answerThe correct option is (E).
- KEAM 2026Set pha-2026-0420F4 marksMCQQ.Electric-flux through a closed surface depends on the (A) shape of the surface (B) area of the surface (C) volume of the surface (D) electric field outside the surface (E) charge enclosed by the surface
›Reveal solutionSolution
Gauss's law: Φ=qenc/ε0 — only the enclosed charge matters.
Gauss's law states
ΦE=∮E⋅dA=ε0qenclosed.
The net electric flux through a closed surface depends only on the total charge enclosed by it — not on the shape, area or volume of the surface, nor on charges lying outside it. Hence (E).
✓Final answerThe correct option is (E).
- KEAM 2025Set eng-2025-04234 marksMCQQ.The inward and outward electric flux from a closed surface are 6×104 NM2C−1 and 3×104 NM2C−1. Then the net charge (in coulomb) inside the closed surface is (A) −6×104ε0 (B) 6×104ε0 (C) 3×104ε0 (D) 9×104ε0 (E) [AMBIGUOUS]
›Reveal solutionSolution
[!TLDR]
Using Gauss's law with net flux =ϕout−ϕin=−3×104 gives an enclosed charge of −3×104ε0 C, which matches option (E).
Concept
Gauss's law states that the net electric flux through a closed surface equals the enclosed charge divided by the permittivity of free space: ϕnet=ε0qenc. Outward flux is taken positive and inward flux negative — the standard NCERT/CBSE electrostatics convention the KEAM syllabus is aligned with.
Solution
The net flux through the surface is the outward flux minus the inward flux:
ϕnet=ϕout−ϕin=3×104−6×104=−3×104 Nm2C−1.
By Gauss's law the enclosed charge is
qenc=ε0ϕnet=−3×104ε0 C.
The negative sign correctly reflects that more flux enters than leaves, so the enclosed charge is negative. This value, −3×104ε0, is not any of the printed options (A)–(D) (−6×104ε0, 6×104ε0, 3×104ε0, 9×104ε0), so by elimination it corresponds to option (E).
[!ANSWER]
(E) qenc=−3×104ε0 C
- KEAM 2025Set eng-2025-04274 marksMCQQ.The electric field inside a uniformly charged spherical shell of radius R is: (A) directly proportional to the charge within the shell (B) inversely proportional to R2 (C) same as that outside the shell (D) zero (E) maximum at the centre
›Reveal solutionSolution
A Gaussian surface inside a uniformly charged spherical shell encloses no charge, so E=0 everywhere inside.
For a uniformly charged spherical shell, apply Gauss's law to a concentric spherical surface of radius r<R. It encloses zero net charge, so
∮E⋅dA=ε0qenc=0⇒E=0.
The electric field is zero at every point inside the shell.
✓Final answerThe correct option is (D).
- KEAM 2024Set eng-2024-06094 marksMCQQ.The electric field due to a an infinitely long thin wire with linear charge density λ at a radial distance r is proportional to (A) rλ2 (B) rλ (C) r2λ (D) rλ (E) rλ
›Reveal solutionSolution
By Gauss's law the field of an infinite line charge is E=2πε0rλ, i.e. proportional to λ/r.
Using a cylindrical Gaussian surface of radius r:
E=2πε0rλ∝rλ.
✓Final answerThe correct option is (B).
- KEAM 2023Set eng-2023-P1-A14 marksMCQQ.A hollow sphere of radius 'r' encloses an electric dipole composed of two charges +q and −q. The net flux of electric field through the surface of the sphere due to the enclosed dipole is: (A) ε02q (B) ε02q⋅4πr2 (C) infinite (D) zero (E) ε0q
›Reveal solutionSolution
The net electric flux through the sphere is zero.
Concept and Intuition
By Gauss's law the flux depends only on the enclosed net charge. A dipole encloses +q and −q, whose sum is zero.
Step-by-Step Solution
- Enclosed charge =+q+(−q)=0.
- Gauss's law: Φ=ε0Qenc=ε00.
- Φ=0.
Common Mistakes
- Thinking the strong dipole field near the surface implies non-zero flux.
- Adding the magnitudes of the charges instead of their signed sum.
✓Final answerThe correct option is (D) — zero.
ANSWER: D
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