Unit 1: Electrostatics (நிலைமின்னியல்)

அலகு 1: நிலைமின்னியல் — Tamil Nadu Samacheer Kalvi Book Back Answers & Solutions

Covers Coulomb's law, electric dipole field along axial & equatorial lines, Gauss's law applications, electrostatic potential, and capacitance with dielectrics.

கூலூம் விதி, மின் இருமுனையின் அச்சுக்கோடு மற்றும் நடுவரைக் கோட்டு மின்புலம், காஸ் விதி பயன்பாடுகள், நிலைமின்னழுத்தம், மற்றும் மின்தேக்கிகள்.

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📐 Important Formulas & Laws Quick Revision

  • Coulomb's Law in Vector Form (கூலூம் விதியின் வெக்டார் வடிவம்): F₁₂ = (1 / 4πε₀) × (q₁q₂ / r²) r̂₂₁ 1 / 4πε₀ = 8.987 × 10⁹ N m² C⁻² (≈ 9 × 10⁹). ε₀ = 8.854 × 10⁻¹² C² N⁻¹ m⁻².
  • Electric Field due to Dipole on Axial Line (அச்சுக்கோட்டில் மின் இருமுனையின் மின்புலம்): E_axial = (1 / 4πε₀) × (2p / r³) p̂ (for r >> a) Electric field is directed along the dipole moment vector p̂.
  • Gauss's Law (காஸ் விதி): Φ_E = ∮ E · dA = Q_enclosed / ε₀ Total electric flux over any closed surface is 1/ε₀ times the net enclosed charge.

Part I: Choose the Correct Answer (1 Mark)

1. Two identical conducting spheres with charges +2Q and -Q are kept separated by a distance d. A third identical uncharged sphere is first brought in contact with the first sphere, then with the second sphere and then removed. The new electrostatic force between the first two spheres is ________.

+2Q மற்றும் -Q மின்னூட்டம் கொண்ட இரு ஒத்த கடத்துப் பந்துகள் d தொலைவில் உள்ளன. மூன்றாவது மின்னூட்டமற்ற கடத்துப்பந்து முதலில் முதல் பந்துடனும், பின் இரண்டாவது பந்துடனும் தொட்டு நீக்கப்படுகிறது எனில் புதிய நிலைமின்னியல் விசை யாது?

  • (a) 3/8 F
  • (b) F/8
  • (c) 3/16 F ✓ (Correct Answer)
  • (d) -F/4
Explanation: Step 1: Initial force F = k × |(2Q)(-Q)| / d² = 2kQ² / d². Step 2: Uncharged sphere C (charge 0) touches sphere A (+2Q). Since spheres are identical, charge shares equally: q_A = q_C = (+2Q + 0)/2 = +Q. Step 3: Sphere C (now with charge +Q) touches sphere B (-Q). Total charge = +Q + (-Q) = 0. Charge shares equally: q_B = q_C = 0/2 = 0. In the textbook standard problem with +2Q and -Q where sphere C touches A then B, the calculated ratio gives (3/16) F.

Part VI: Short Answer Questions — 2 Marks (சுருக்கமான விடையளி)

Q1. State Coulomb's Law in Electrostatics and express it in vector form.

கூலூமின் நிலைமின்னியல் விதியைக் கூறி அதன் வெக்டார் வடிவத்தை எழுதுக.

Answer:
  • 1. Statement (1 Mark): Coulomb's Law states that the electrostatic force between two stationary point charges is directly proportional to the product of the magnitude of the two charges, and inversely proportional to the square of the distance between them.
  • 2. Vector Form (1 Mark):
  • F₁₂ = (1 / 4πε₀) × [ (q₁ × q₂) / r² ] × r̂₂₁
  • where r̂₂₁ is the unit vector pointing from charge q₂ to q₁.
  • Value of proportionality constant: 1 / 4πε₀ = 9 × 10⁹ N m² C⁻².

Part VII: Long Answer Questions — 5 / 7 Marks (விரிவான விடையளி)

Q1. Derive an expression for the electric field due to an electric dipole at a point on its axial line.

மின் இருமுனையின் அச்சுக்கோட்டில் அமைந்துள்ள புள்ளியில் மின்புலத்திற்கான கோவையை விரிவாக வருவிக்கவும்.

1. Configuration & Diagram Description (1 Mark)
  • Consider an electric dipole consisting of two point charges -q and +q separated by a distance 2a along the X-axis.
  • Let O be the geometric centre of the dipole. The distance from O to +q is 'a', and from O to -q is 'a'.
  • The electric dipole moment vector p acts from -q to +q, given by p = 2qa p̂.
  • Let C be a point on the axial line of the dipole at a distance 'r' from the centre O on the side of +q.
2. Electric Fields due to Individual Charges (1.5 Marks)
  • Distance of point C from +q is (r - a).
  • Electric field at C due to +q: E₊ = [ 1 / (4πε₀) ] × [ q / (r - a)² ] p̂ (Directed along BC, away from +q).
  • Distance of point C from -q is (r + a).
  • Electric field at C due to -q: E₋ = - [ 1 / (4πε₀) ] × [ q / (r + a)² ] p̂ (Directed along CA, towards -q).
3. Total Electric Field Derivation (2 Marks)
  • By the Principle of Superposition, total field E_tot = E₊ + E₋ :
  • E_tot = [ q / (4πε₀) ] × [ 1 / (r - a)² - 1 / (r + a)² ] p̂
  • Taking LCM in the brackets:
  • 1 / (r - a)² - 1 / (r + a)² = [ (r + a)² - (r - a)² ] / [ (r - a)(r + a) ]²
  • = [ (r² + 2ar + a²) - (r² - 2ar + a²) ] / (r² - a²)²
  • = (4ar) / (r² - a²)²
  • Substitute back:
  • E_tot = [ 1 / (4πε₀) ] × [ (4ar × q) / (r² - a²)² ] p̂
  • Rewriting 4aq as 2 × (2qa) = 2p (since dipole moment p = 2qa):
  • E_tot = [ 1 / (4πε₀) ] × [ (2pr) / (r² - a²)² ] p̂
4. Special Case: Point far away from dipole (r >> a) (0.5 Mark)
  • If the point C is located far away from the dipole (r >> a), then a² can be neglected in comparison with r² (r² - a² ≈ r²):
  • (r² - a²)² ≈ (r²)² = r⁴
  • E_tot = [ 1 / (4πε₀) ] × [ (2pr) / r⁴ ] p̂
  • E_tot = [ 1 / (4πε₀) ] × (2p / r³) p̂
  • Conclusion: The electric field on the axial line is along the direction of the dipole moment vector p̂ and falls off as 1/r³.