WORKSHEET: GAUSS LAW & ELECTRIC FLUX QUIZ1

 

📘 WORKSHEET: GAUSS LAW & ELECTRIC FLUX QUIZ1


🔹 SECTION A: THEORY & CONCEPTUAL (Q1–Q10)

Q1. State Gauss’s Law in electrostatics.


Q2. Define electric flux. Write its SI unit.


Q3. The electric flux through a closed surface depends on:
A) Total charge inside
B) Charge outside
C) Shape of surface
D) Area only


Q4. What is a Gaussian surface? Why is it imaginary?


Q5. If no charge is enclosed inside a closed surface, what is the net flux?


Q6. Electric field inside a hollow conducting sphere is:
A) Zero
B) Maximum
C) Depends on charge
D) Infinite


Q7. Why is Gauss’s law useful only for highly symmetric charge distributions?


Q8. If a point charge is placed outside a closed surface, does it contribute to net flux?


Q9. What is the electric field due to an infinite plane sheet of charge?


Q10. Flux through a cube when a charge is placed exactly at one corner is:
A) q/ε₀
B) q/2ε₀
C) q/8ε₀
D) q/6ε₀


🔹 SECTION B: NUMERICAL PROBLEMS (Q11–Q20)


Q11.
A point charge q=4μCq = 4 \,\mu C is enclosed inside a cube.
Find total electric flux through the cube.


Q12.
A charge qq is placed at the center of a cube.
Find flux through one face.


Q13.
A charge qq is placed at one corner of a cube.
Find total flux through the cube.


Q14.
A charge qq is placed at the center of one face of a cube.
Find flux through the cube.


Q15.
Electric field E=5×103N/CE = 5 \times 10^3 \, N/C is normal to a surface of area 2m22 \, m^2.
Find flux.


Q16.
Electric field E=104N/CE = 10^4 \, N/C makes an angle 6060^\circ with surface normal.
Area = 3m23 \, m^2.
Find flux.


Q17.
Find electric field at distance rr from a long line charge using Gauss law.


Q18.
Find electric field due to an infinite plane sheet with surface charge density σ\sigma.


Q19.
Eight identical charges qq are placed at the eight corners of a cube.
Find flux through one face.


Q20.
A cube is placed in a uniform electric field. No charge inside.
Find net flux through the cube.


ANSWER KEY

Section A:

  1. Φ=qencε0\Phi = \frac{q_{enc}}{\varepsilon_0}
  2. Flux = EA\vec{E} \cdot \vec{A}, unit = Nm²/C
  3. A
  4. Imaginary closed surface for applying Gauss law
  5. Zero
  6. A
  7. Symmetry simplifies calculation
  8. No
  9. E=σ2ε0E = \frac{\sigma}{2\varepsilon_0}
  10. C

Section B:

  1. Φ=qε0\Phi = \frac{q}{\varepsilon_0}

Φoneface=q6ε0\Phi_{one\,face} = \frac{q}{6\varepsilon_0}
Φ=q8ε0\Phi = \frac{q}{8\varepsilon_0}
Φ=q2ε0\Phi = \frac{q}{2\varepsilon_0}
Φ=EA=5×103×2=104\Phi = EA = 5\times10^3 \times 2 = 10^4
Φ=EAcosθ=104×3×12=1.5×104\Phi = EA\cos\theta = 10^4 \times 3 \times \frac{1}{2} = 1.5\times10^4

E=λ2πε0rE = \frac{\lambda}{2\pi \varepsilon_0 r}


E=σ2ε0E = \frac{\sigma}{2\varepsilon_0}


Total enclosed charge = 8q8q

Φtotal=8qε0\Phi_{total} = \frac{8q}{\varepsilon_0}

Flux per face:

Φface=8q6ε0=4q3ε0\Phi_{face} = \frac{8q}{6\varepsilon_0} = \frac{4q}{3\varepsilon_0}
Φ=0\Phi = 0

🧠 DETAILED SOLUTIONS (IMPORTANT ONES)


🔸 Q12 (Charge at center of cube)

By symmetry, flux divides equally among 6 faces:

Φ=qε0q6ε0\Phi = \frac{q}{\varepsilon_0} \Rightarrow \frac{q}{6\varepsilon_0}

🔸 Q13 (Charge at corner)

8 cubes can be combined → charge at center:

Φcube=q8ε0\Phi_{cube} = \frac{q}{8\varepsilon_0}

🔸 Q14 (Charge at face center)

2 cubes form → charge at center:

Φ=q2ε0\Phi = \frac{q}{2\varepsilon_0}

🔸 Q19 (8 charges at corners)

Total charge enclosed:

8q8q

Total flux:

8qε0\frac{8q}{\varepsilon_0}

Divide among 6 faces.

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