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Chapter 20
physics • intermediate 12th

Chapter 20: Atomic Spectra

Comprehensive notes for Chapter 20 Atomic Spectra. Covers Atomic Spectra types, Bohr's Model of Hydrogen Atom, X-rays production and properties, and Lasers (He-Ne).

Atomic Spectra

Continuous Spectrum: Continuous range of frequencies (e.g., Black body).

Line Spectrum: Discrete lines characteristic of an element (e.g., Atomic Hydrogen).

Spectral Series of Hydrogen:

  • Lyman Series (UV): $$ \frac{1}{\lambda} = R_H (\frac{1}{1^2} - \frac{1}{n^2}) $$ where n=2,3...
  • Balmer Series (Visible): $$ \frac{1}{\lambda} = R_H (\frac{1}{2^2} - \frac{1}{n^2}) $$ where n=3,4...
  • Paschen (IR), Brackett (IR), Pfund (IR): Corresponding to p=3, 4, 5.

$$ R_H = 1.0974 \times 10^7 m^{-1} $$

Bohr's Model of Hydrogen Atom

Postulates: 1. Circular orbits without radiating. 2. Angular momentum quantization $$ mvr = \frac{nh}{2\pi} $$. 3. Energy emission/absorption on transition $$ hf = E_n - E_p $$.

Radius: $$ r_n = n^2 r_1 $$ where $$ r_1 = 0.53 \mathring{A} $$.

Energy: $$ E_n = -\frac{E_0}{n^2} $$ where $$ E_0 = 13.6 eV $$.

Inner Shell Transitions and Characteristic X-Rays

X-rays: High frequency EM radiation ($$ \lambda \approx 10^{-10} m $$). Produced by reverse photoelectric effect.

Characteristic X-rays: Due to inner shell transitions. $$ K_{\alpha} $$ (L to K), $$ K_{\beta} $$ (M to K). Energy depends on target material.

Continuous X-rays (Bremsstrahlung): Due to deceleration of electrons hitting the target. Min wavelength $$ \lambda_{min} = \frac{hc}{Ve} $$.

Lasers

LASER: Light Amplification by Stimulated Emission of Radiation.

Principle: 1. Population Inversion (More atoms in excited state). 2. Stimulated Emission (Incident photon triggers emission of identical photon). 3. Metastable State (Longer lifetime $$ 10^{-3} s $$).

He-Ne Laser: Most common gas laser. Neon provides laser action (Red light $$ 632.8 nm $$).

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