Class 11 & 12 CBSE Physics Handbook

Class 11 & 12 CBSE Physics Handbook
CBSE NEET JEE

Electrostatics of Conductors, Electrostatic shielding, Voltage inside a spherical shell, E perpendicular to the surface, E at the surface. Quiz1

 

Worksheet:  Electrostatics of Conductors, Electrostatic shielding, Voltage inside a spherical shell, E perpendicular to the surface, E at the surface. Quiz1

🔹 Section A: Theory (Conceptual Questions)

Q1. What happens to excess charge placed on a conductor? Where does it reside?

Q2. Define electrostatic equilibrium.

Q3. What is the electric field inside a conductor in electrostatic equilibrium? Why?

Q4. Explain why electric field lines are always perpendicular to the surface of a conductor.

Q5. What is electrostatic shielding?

Q6. Why is the potential constant throughout a conductor?

Q7. What happens to the electric field at sharp edges of a conductor?

Q8. What is the electric field just outside a charged conductor?

Q9. What is the potential inside a charged spherical shell?

Q10. Give one real-life application of electrostatic shielding.


🔹 Section B: Numerical Problems

Q11. A conductor carries a charge of 5×106C5 \times 10^{-6}\,C. What is the electric field inside it?

Q12. The electric field just outside a conductor is 2×105N/C2 \times 10^5\,N/C. Find the surface charge density.
ε0=8.85×1012F/m\varepsilon_0 = 8.85 \times 10^{-12}\,F/m

👉 Use:
E=σε0E = \frac{\sigma}{\varepsilon_0}


Q13. A spherical conductor of radius 0.2m0.2\,m carries a charge 2×106C2 \times 10^{-6}\,C. Find potential at the surface.

👉 Use:
V=14πε0QRV = \frac{1}{4\pi\varepsilon_0}\frac{Q}{R}


Q14. What is the potential at the center of the above sphere?

Q15. A hollow spherical conductor is charged. What is the electric field at a point inside the cavity?

Q16. A conductor has surface charge density 4×106C/m24 \times 10^{-6}\,C/m^2. Find electric field just outside.

Q17. If electric field at surface is 106N/C10^6\,N/C, find surface charge density.

Q18. A conductor is placed in an external electric field. What is the field inside it?

Q19. A charged spherical shell has potential 100V100\,V. What is the potential at any point inside?

Q20. A Gaussian surface lies entirely inside a conductor. What is the flux through it?


✅ Answer Key

Section A

  1. On surface
  2. No net motion of charges
  3. Zero
  4. Otherwise charges move
  5. Protection from external fields
  6. No electric field inside
  7. Field is high
  8. E=σ/ε0E = \sigma/\varepsilon_0
  9. Constant (same as surface)
  10. Faraday cage, cable shielding

Section B

  1. E=0E = 0
  2. 1.77×106C/m21.77 \times 10^{-6}\,C/m^2
  3. 9×104V9 \times 10^4\,V
  4. 9×104V9 \times 10^4\,V
  5. Zero
  6. 4.52×105N/C4.52 \times 10^5\,N/C
  7. 8.85×106C/m28.85 \times 10^{-6}\,C/m^2
  8. Zero
  9. 100V100\,V
  10. Zero

✏️ Detailed Solutions

Q3. Why electric field inside conductor is zero?

Free electrons rearrange themselves such that they cancel any internal field → equilibrium → E=0E = 0.


Q4. Why E is perpendicular to surface?

If there were a tangential component → charges would move → violates equilibrium → hence perpendicular.


Q8. Electric field just outside conductor

E=σε0E = \frac{\sigma}{\varepsilon_0}

Q11.

Inside conductor:

E=0E = 0

Q12.

σ=ε0E=(8.85×1012)(2×105)=1.77×106C/m2\sigma = \varepsilon_0 E = (8.85 \times 10^{-12})(2 \times 10^5) = 1.77 \times 10^{-6}\,C/m^2

Q13.

V=14πε0QR=9×1092×1060.2=9×104VV = \frac{1}{4\pi\varepsilon_0}\frac{Q}{R} = 9 \times 10^9 \cdot \frac{2 \times 10^{-6}}{0.2} = 9 \times 10^4\,V

Q14.

Inside spherical conductor:

V=constant=Vsurface=9×104VV = \text{constant} = V_{\text{surface}} = 9 \times 10^4\,V

Q15.

Electric field inside cavity:

E=0E = 0

Q16.

E=σε0=4×1068.85×1012=4.52×105N/CE = \frac{\sigma}{\varepsilon_0} = \frac{4 \times 10^{-6}}{8.85 \times 10^{-12}} = 4.52 \times 10^5\,N/C

Q17.

σ=ε0E=8.85×1012×106=8.85×106C/m2\sigma = \varepsilon_0 E = 8.85 \times 10^{-12} \times 10^6 = 8.85 \times 10^{-6}\,C/m^2

Q18.

Field inside conductor:

E=0E = 0

Q19.

Potential inside shell:

V=constant=100VV = \text{constant} = 100\,V

Q20.

Using Gauss law:

Φ=Qenclosedε0=0\Phi = \frac{Q_{\text{enclosed}}}{\varepsilon_0} = 0

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