Physics — Important Derivations
Step-by-step derivation outlines for the most frequently asked derivations in the TS Inter 2nd Year Physics board exam. Practise writing each derivation in full — including diagrams, numbered equations, and the final boxed result.
Optics (Ch 2 & 3)
1. Mirror formula: 1/f = 1/v + 1/u
- Draw concave mirror with pole P, centre C, focus F
- Take object AB beyond C; draw two rays — one parallel to principal axis (reflects through F), one through C (reflects back)
- Use similar triangles △APB and △APB′ to get A′B′/AB = PA′/PA
- Apply sign convention; obtain v and u in terms of f → derive 1/f = 1/v + 1/u
- Result: f = R/2
2. Lens maker's equation: 1/f = (n−1)(1/R₁ − 1/R₂)
- Apply refraction at first surface (radius R₁): n₁/u + n₂/v₁ = (n₂−n₁)/R₁
- Apply refraction at second surface (radius R₂) using v₁ as virtual object: n₂/−v₁ + n₁/v = (n₁−n₂)/R₂
- Add both equations; for n₁=1 (air), n₂=n: 1/f = (n−1)(1/R₁ − 1/R₂)
3. Young's double slit — fringe width β = λD/d
- S₁ and S₂ separated by d; screen at distance D
- Path difference Δ = S₂P − S₁P = d·y/D (for small angles)
- Bright fringe at y_n = nλD/d; Dark fringe at y_n = (2n−1)λD/2d
- Fringe width: β = y_(n+1) − y_n = λD/d
4. Prism — minimum deviation relation n = sin[(A+δₘ)/2]/sin(A/2)
- At minimum deviation: i₁ = i₂ and r₁ = r₂ = A/2
- i₁ = (A + δₘ)/2 from A = r₁ + r₂ and δₘ = 2i − A
- Apply Snell's law at first surface: sin(i₁) = n·sin(r₁)
- Substitute: n = sin[(A+δₘ)/2]/sin(A/2)
Electrostatics & Current (Ch 4–6)
1. Electric field due to an infinite sheet: E = σ/2ε₀
- Choose a Gaussian cylinder with flat ends perpendicular to the sheet
- By symmetry, E is perpendicular to the sheet on both sides
- Gauss's law: 2·E·A = σA/ε₀
- Therefore E = σ/(2ε₀)
2. Energy stored in a capacitor: U = ½CV²
- Work done dW to add charge dq against potential V = q/C is dW = (q/C)dq
- Total work: W = ∫₀^Q (q/C)dq = Q²/(2C)
- Since Q = CV: U = ½CV² = Q²/2C
3. Wheatstone bridge balance condition: P/Q = R/S
- Four resistors P, Q, R, S in a diamond; galvanometer across BD, battery across AC
- At balance: I_G = 0, so V_B = V_D
- Applying Kirchhoff: V_A − V_B = I₁P and V_B − V_C = I₁Q
- Also V_A − V_D = I₂R and V_D − V_C = I₂S
- Dividing: P/Q = R/S
Magnetic Effects (Ch 7)
1. Magnetic field at centre of circular current loop: B = μ₀I/(2R)
- Each element dl of the circular loop at distance R from centre
- Biot-Savart: dB = μ₀I dl sin90°/(4πR²) = μ₀I dl/(4πR²)
- Integrate over full circle (dl = 2πR): B = μ₀I(2πR)/(4πR²) = μ₀I/(2R)
- Direction: right-hand rule perpendicular to loop plane
2. Force on current in uniform magnetic field: F = BIL sinθ
- Current I in wire of length L; carriers each have drift velocity v_d
- Force on one carrier: f = qv_dB sinθ
- Number of carriers in length L: n·A·L (n = carrier density)
- Total force: F = nALq·v_d·B sinθ = IL·B sinθ (since I = nAqv_d)
3. Radius of circular motion in magnetic field: r = mv/(qB)
- Magnetic force provides centripetal force: qvB = mv²/r
- Solving for r: r = mv/(qB)
- Time period: T = 2πr/v = 2πm/(qB) — cyclotron frequency
EMI, AC & EM Waves (Ch 9–11)
1. Faraday's law: ε = −dΦ/dt
- Magnetic flux Φ = B·A·cosθ
- An induced EMF opposes the change in flux (Lenz's law)
- ε = −dΦ/dt; for N turns: ε = −N·dΦ/dt
2. Motional EMF: ε = Bvl
- Conducting rod of length l moving with velocity v perpendicular to field B
- Free charges experience force F = qvB along the rod
- Work done in moving charge q from one end to other: W = qvBl
- EMF = W/q = Bvl
3. LCR series circuit — impedance Z = √(R² + (X_L−X_C)²)
- V_R = IR (in phase with I)
- V_L = IX_L (leads current by 90°), V_C = IX_C (lags current by 90°)
- Phasor addition: V = √(V_R² + (V_L−V_C)²)
- Dividing by I: Z = √(R² + (X_L−X_C)²)
Modern Physics (Ch 12–14)
1. Bohr's model — radii: rₙ = n²a₀; energy: Eₙ = −13.6/n² eV
- Centripetal force = Coulomb attraction: mv²/r = e²/(4πε₀r²)
- Angular momentum quantisation: mvr = nh/(2π)
- From these two: r_n = n²ε₀h²/(πme²) = n² × 0.529 Å
- Total energy: E = KE + PE = −e²/(8πε₀r_n) = −13.6/n² eV
2. Radioactive decay law: N = N₀e^(−λt)
- Rate of disintegration: dN/dt = −λN
- Separate variables: dN/N = −λ dt
- Integrate: ln(N/N₀) = −λt
- Therefore: N = N₀e^(−λt)
- Half-life: T₁/₂ = ln2/λ = 0.693/λ
Semiconductors (Ch 15)
1. Transistor current relations: I_E = I_B + I_C; β = α/(1−α)
- Emitter current splits between base and collector: I_E = I_B + I_C
- DC current gain α = I_C/I_E (common-base, < 1)
- DC current gain β = I_C/I_B (common-emitter, large)
- Relation: α = β/(β+1); β = α/(1−α)