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Modern Physics

Photoelectric effect, atomic structure, nuclear physics

Photoelectric EffectBohr ModelX-RaysRadioactivityNuclear ReactionsSemiconductors
📋 PYQs Available:
20242023202220212020
Expert Content

Modern Physics

Why This Chapter Matters

Modern Physics covers photoelectric effect, Bohr model, nuclear physics, and semiconductors — 8-12 marks in JEE every year. This is the last chapter of Physics but always present in the exam.

Core Concepts

1. Photoelectric Effect

When light hits a metal surface, electrons are emitted IF frequency ≥ threshold.

Einstein's equation: KE_max = hf - φ = hf - hf₀

h = 6.626×10⁻³⁴ J·s (Planck's constant)

φ = work function (energy needed to remove electron from surface)

f₀ = threshold frequency = φ/h

Key observations:

KE_max depends on frequency, NOT intensity
Intensity determines number of electrons (photocurrent)
No time delay (instantaneous emission)
Stopping potential V₀: eV₀ = KE_max = hf - φ

2. de Broglie Wavelength

Every particle has associated wavelength: λ = h/p = h/mv

For electron accelerated through V volts: λ = h/√(2meV) = 1.23/√V nm

3. Bohr Model of Hydrogen

Electrons orbit in discrete circular orbits without radiating.

Quantisation: L = mvr = nh/2π = nℏ (n = 1, 2, 3...)

Orbit radius: r_n = n²a₀ (a₀ = 0.53 Å = Bohr radius)

Energy: E_n = -13.6/n² eV (negative → bound state)

Velocity: v_n = v₁/n (v₁ = 2.2×10⁶ m/s)

Energy of emitted photon: ΔE = E_final - E_initial = hf = hc/λ

Rydberg formula: 1/λ = R_H(1/n₁² - 1/n₂²) (R_H = 1.097×10⁷ m⁻¹)

Spectral series: Lyman (n₁=1, UV), Balmer (n₁=2, visible), Paschen (n₁=3, IR)

4. X-Rays

Characteristic X-rays: from electron transitions in inner shells. Specific to element.

Continuous X-rays (Bremsstrahlung): from deceleration of electrons.

Minimum wavelength: λ_min = hc/eV (V = accelerating voltage)

Moseley's law: √f = a(Z - b) (relates characteristic X-ray frequency to atomic number Z)

5. Nuclear Physics

Mass number A = protons + neutrons. Atomic number Z = protons.

Binding energy: BE = [Zm_p + (A-Z)m_n - M_nucleus]c²

Radioactive decay: N = N₀e^(-λt) = N₀(1/2)^(t/T₁/₂)

T₁/₂ = ln2/λ = 0.693/λ (half-life)

Activity: A = λN = A₀e^(-λt)

Types: α decay (A-4, Z-2), β⁻ decay (A, Z+1), β⁺ decay (A, Z-1), γ (A,Z unchanged)

6. Semiconductors (Brief)

Intrinsic: pure semiconductor (Si, Ge). Some e-h pairs by thermal excitation.

n-type: doped with pentavalent (P, As) → excess electrons

p-type: doped with trivalent (B, Al) → excess holes

p-n junction: depletion region, forward bias (current flows), reverse bias (no current)

PYQs

2024: Metal with work function 2 eV illuminated by photons of energy 5 eV. KE_max and stopping potential?

KE_max = 5-2 = 3 eV. Stopping potential V₀ = 3V.

2023: Hydrogen electron jumps from n=3 to n=1. Wavelength of emitted photon?

1/λ = R_H(1/1² - 1/3²) = R_H(1 - 1/9) = 8R_H/9

λ = 9/(8×1.097×10⁷) = 102.6 nm (UV, Lyman series)

2022: Radioactive sample T₁/₂ = 10 days. After 30 days, fraction remaining?

Fraction = (1/2)^(30/10) = (1/2)³ = 1/8

Revision Notes

PHOTOELECTRIC:
KE_max = hf - φ = hf - hf₀
Stopping potential: eV₀ = KE_max
Photocurrent ∝ intensity (NOT frequency)

de BROGLIE: λ = h/p = h/mv
Electron: λ = 1.23/√V nm (V in volts)

BOHR MODEL:
r_n = n²a₀ (a₀ = 0.53 Å)
E_n = -13.6/n² eV
ΔE = hf (photon energy = energy difference)
Lyman(UV), Balmer(visible), Paschen(IR)

NUCLEAR:
BE = Δm × c² (mass defect × c²)
Decay: N = N₀(1/2)^(t/T½)
T½ = 0.693/λ | Activity A = λN
α: A-4, Z-2 | β⁻: A, Z+1 | γ: A,Z unchanged
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