Module 1 :Atomic Structure and Periodicity of Elements Chemistry Semester 1 Notes

Module 1 :Atomic Structure and Periodicity of Elements Chemistry Semester 1 Notes



Atomic Structure – Introduction


1. Rutherford’s Atomic Model (1911)

Experiment:

  • Gold Foil Experiment (Geiger–Marsden).

  • Alpha (α) particles shot at thin gold foil.

Observations:

  1. Most α-particles passed straight → atom mostly empty space.

  2. Few deflected → presence of dense positive center (nucleus).

  3. Very few bounced back → nucleus is very small.

Model:

  • Atom has small, dense, positively charged nucleus containing protons (and later neutrons).

  • Electrons revolve around nucleus in circular paths.

  • Most of atom is empty space.

Limitations:

  • Could not explain why electrons don’t spiral into nucleus.

  • Could not explain line spectra of atoms.


2. Failure of Classical Physics

Classical theory predicted:

  • Accelerating electrons lose energy continuously as radiation.

  • Atom would collapse → not observed.

  • Spectra should be continuous, but experiments showed line spectra.


3. Blackbody Radiation Problem

  • Blackbody: Perfect absorber and emitter of radiation.

  • Observed: Energy distribution curve → intensity rises with wavelength, peaks, then falls.

  • Classical Rayleigh–Jeans law failed at short wavelengths (predicted infinite energy → UV catastrophe).


4. Planck’s Quantum Hypothesis (1900)

  • Energy is not continuous; it is emitted or absorbed in small packets called quanta.

  • Formula:

E=nhνE = n h \nu

where:
nn = integer,
hh = Planck’s constant = 6.626×1034 J
s
6.626 \times 10^{-34} \ \text{J·s}
,
ν\nu = frequency.

  • Explained blackbody radiation successfully.


5. Photoelectric Effect (Einstein, 1905)

Observation:

  • When light of certain frequency hits a metal surface, electrons are emitted instantly.

Laws:

  1. No electrons if ν<ν0\nu < \nu_0 (threshold frequency).

  2. Kinetic energy of electrons depends on frequency, not intensity.

  3. Number of electrons ∝ light intensity (for ν>ν0\nu > \nu_0).

Einstein’s Equation:

hν=hν0+12mvmax2h\nu = h\nu_0 + \frac{1}{2}mv_{\text{max}}^2

6. Compton Effect (1923)

  • X-rays scattered by electrons have greater wavelength than incident rays.

  • Explained by photon concept of light.

  • Wavelength change:

Δλ=hmec(1cosθ)\Delta\lambda = \frac{h}{m_e c} (1 - \cos\theta)

where mem_e = electron mass, θ\theta = scattering angle.


7. Bohr’s Theory of Atom (1913)

Postulates:

  1. Electrons revolve in fixed circular orbits (stationary states) without radiating energy.

  2. Angular momentum is quantized:

mvr=nh2π,n=1,2,3...mvr = \frac{nh}{2\pi}, \quad n = 1, 2, 3...
  1. Radiation emitted/absorbed only when electron jumps between orbits:

ΔE=hν\Delta E = h\nu

Energy of nth orbit (Hydrogen atom):

En=13.6n2 eVE_n = -\frac{13.6}{n^2} \ \mathrm{eV}

Rydberg Formula (spectral lines):

1λ=RH(1n121n22)\frac{1}{\lambda} = R_H \left( \frac{1}{n_1^2} - \frac{1}{n_2^2} \right)

where RH=1.097×107 m1R_H = 1.097 \times 10^7 \ \mathrm{m^{-1}}.


8. Limitations of Bohr’s Theory

  • Works only for hydrogen-like atoms.

  • Cannot explain:

    • Fine structure of spectral lines.

    • Zeeman effect (in magnetic field).

    • Stark effect (in electric field).

    • Intensities of lines.

    • Wave nature of electrons.


9. de Broglie’s Matter Waves (1924)

  • Particles have wave-like properties:

λ=hmv\lambda = \frac{h}{mv}
  • Supported Bohr’s quantization — electron waves fit perfectly in allowed orbits.


10. Heisenberg’s Uncertainty Principle (1927)

  • Impossible to know exact position (Δx\Delta x) and exact momentum (Δp\Delta p) of a particle at the same time:

ΔxΔph4π\Delta x \cdot \Delta p \ge \frac{h}{4\pi}
  • For electrons: Only probability distribution can be known → led to concept of orbitals instead of fixed paths.


All points are included, but in a condensed, easy-to-revise format so you can score full marks.


📘 MODULE – 2 : ATOMIC STRUCTURE & CHEMICAL BONDING (Short Notes)


🔹 Bohr’s Atom Model

Postulates:

  1. Electrons revolve around nucleus in fixed circular orbits (stationary states).

  2. Energy of electron is constant in a given orbit → called energy level.

  3. Allowed orbits satisfy:
    mvr=nh2πmvr = \dfrac{nh}{2\pi}
    (n = principal quantum number).

  4. Energy ↑ when orbit is farther from nucleus.

  5. Electron jumps between orbits:

    • Low → High: absorbs energy.

    • High → Low: emits energy.

    • Frequency: ν=E2E1h\nu = \dfrac{E_2 - E_1}{h} (Bohr frequency rule).

  6. n = 1,2,3,4… = K, L, M, N shells.


🔹 Hydrogen Spectrum

  • Heated atoms/electric discharge → line spectrum (discontinuous).

  • Series:

Series n₁ n₂ Region
Lyman 1 2,3,4… UV
Balmer 2 3,4,5… Visible
Paschen 3 4,5,6… IR
Brackett 4 5,6,7… IR
Pfund 5 6,7,8… IR
  • Formula (Rydberg):
    1λ=R(1n121n22)\dfrac{1}{\lambda} = R \left( \dfrac{1}{n_1^2} - \dfrac{1}{n_2^2} \right)
    R=1.097×107m1R = 1.097 \times 10^7 \, m^{-1}.

  • Bohr explains H and H-like ions (He⁺, Li²⁺).

Limitations:
❌ Cannot explain fine spectrum, multi-electron atoms, bonding & shapes, Zeeman/Stark effects, against de Broglie & Heisenberg.


🔹 de Broglie Equation

  • Matter has wave-particle duality.

  • Wavelength:
    λ=hmv=hp\lambda = \dfrac{h}{mv} = \dfrac{h}{p}

  • Significance:

    • Macroscopic objects → λ negligible.

    • Microscopic particles (electrons) → λ large (wave nature significant).

Derivation (short):
Photon energy: E=hν=hc/λE = h\nu = hc/\lambda.
Einstein: E=mc2E = mc^2.
λ=h/mc\lambda = h/mc.
For matter: replace c with v → λ=h/mv\lambda = h/mv.


🔹 Heisenberg’s Uncertainty Principle

  • Impossible to know position & momentum of electron simultaneously.

  • ΔxΔpxh4π\Delta x \cdot \Delta p_x \geq \dfrac{h}{4\pi}

  • Rules out definite electron paths (unlike Bohr).


🔹 Schrödinger Wave Equation

  • Describes electron as a standing wave.

  • Solution = wave function (Ψ).

  • Ψ → no meaning; Ψ² → probability of finding electron.

  • Energy of electron → quantized.


🔹 Orbitals

  • Region in space where probability of finding electron is maximum.

  • s orbital → spherical.

  • p, d, f → directional.


🔹 Quantum Numbers

  1. Principal (n): main shell, distance from nucleus (n=1,2,3…).

  2. Azimuthal (l): subshell (0 to n-1).

    • l=0 (s), l=1 (p), l=2 (d), l=3 (f).

  3. Magnetic (m): orientation (values: -l to +l).

  4. Spin (s): spin ±½ (↑ or ↓).


🔹 Electron Arrangement

  1. Pauli Exclusion: one orbital max 2 e⁻ with opposite spins.

  2. Aufbau Principle: electrons fill in increasing energy order:
    1s < 2s < 2p < 3s < 3p < 4s < 3d < 4p < 5s < 4d < 5p < 6s < 4f < 5d < 6p …

  3. Hund’s Rule:

    • Each orbital gets 1 electron before pairing.

    • Unpaired electrons → parallel spins.


🔹 Stability of Configurations

  • Half-filled & fully filled orbitals = extra stable.

  • Reasons:
    i) Symmetry.
    ii) Exchange energy (parallel spin exchange releases energy).

  • Examples:

    • Cr (24): [Ar] 4s¹ 3d⁵

    • Cu (29): [Ar] 4s¹ 3d¹⁰


🔹 Chemical Bonding

Ionic (Electrovalent) Bond

  • Electrostatic attraction between +ve and -ve ions (formed by transfer of electrons).

  • Examples: NaCl, MgCl₂.

Favourable conditions:

  1. Low ionization energy of donor atom.

  2. High electron affinity of acceptor atom.

  3. High (negative) lattice energy.


✅ This is your entire Module-2 in short form, all points covered.

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