Chapter 7

1. Introduction to Quantum Theory
  • Classical physics failed to explain phenomena at the atomic and subatomic level (e.g., blackbody radiation, photoelectric effect, atomic spectra).

  • Quantum theory describes matter and energy at the atomic and subatomic level, proposing that energy exists in discrete packets called quanta.

2. Electromagnetic Radiation
  • Electromagnetic radiation (EMR) consists of oscillating electric and magnetic fields that travel at the speed of light in a vacuum.

    • Wavelength (λ\lambda): Distance between two consecutive peaks or troughs of a wave (units: m, nm).

    • Frequency (ν\nu): Number of waves passing a point per unit time (units: Hz or s1s^{-1}).

    • Amplitude: Height of the wave from the origin to a crest.

    • Speed of Light (cc): 3.00×108 m/s3.00 \times 10^8 \text{ m/s} in a vacuum.

  • Relationship between cc, λ\lambda, and ν\nu: c=λνc = \lambda \nu

  • Energy of a Photon (EE):

    • Planck's equation: E=hνE = h \nu

    • Where hh is Planck's constant (6.626 \times 10^{-34} \text{ J\cdot s}).

    • Combining equations: E=hcλE = \frac{hc}{\lambda}

2.1. Photoelectric Effect
  • Emission of electrons from a metal surface when light shines on it.

  • Explained by Einstein using Planck's quantum theory: light behaves as particles (photons) with energy hνh\nu.

  • A minimum frequency (threshold frequency, ν0{\nu}_{0}) is required to eject an electron, regardless of light intensity.

3. Atomic Spectra
  • Continuous spectrum: Produced when white light passes through a prism, showing all wavelengths.

  • Line spectrum: Specific wavelengths of light emitted or absorbed by excited atoms.

    • Emission spectrum: Light emitted by excited atoms, unique to each element.

    • Absorption spectrum: Dark lines appear in a continuous spectrum where specific wavelengths are absorbed by atoms.

  • Bohr Model (Limitations):

    • Proposed electrons orbit the nucleus in fixed energy levels (quantized).

    • Electrons can transition between

    • energy levels by absorbing or emitting photons of specific energies.

    • Formula for energy levels in a hydrogen atom: E<em>n=R</em>H(1n2)E<em>n = -R</em>H \left( \frac{1}{n^2} \right), where RHR_H is the Rydberg constant and nn is the principal quantum number.

    • Failed for multi-electron atoms and did not explain fine structure of spectral lines.

4. Quantum Mechanics
4.1. Wave-Particle Duality
  • De Broglie Wavelength: Proposed that particles (like electrons) can also exhibit wave-like properties.

    • λ=hmv\lambda = \frac{h}{mv}, where mm is mass and vv is velocity.

4.2. Heisenberg Uncertainty Principle
  • It is impossible to simultaneously know precisely both the position (Δx\Delta x) and momentum (Δp\Delta p) of a particle.

    • ΔxΔph4π\Delta x \cdot \Delta p \ge \frac{h}{4\pi}

4.3. Schrödinger Equation (Conceptual)
  • A mathematical equation that describes the wave function (Ψ\Psi) of an electron in an atom.

  • Solutions to the Schrödinger equation yield atomic orbitals, which represent probability distributions of finding an electron in space.

  • Ψ2\Psi^2 (probability density) gives the probability of finding an electron at a particular point in space.

5. Quantum Numbers
  • Four quantum numbers describe the state of an electron in an atom:

    1. Principal Quantum Number (nn):

      • Values: 1,2,3,1, 2, 3, …

      • Describes the electron's main energy level (shell) and average distance from the nucleus.

      • Higher nn means higher energy and larger orbital size.

    2. Azimuthal (Angular Momentum) Quantum Number (ll):

      • Values: 0,1,2,,n10, 1, 2, …, n-1

      • Describes the shape of the orbital (subshell).

      • l=0l=0: s orbital (spherical)

      • l=1l=1: p orbital (dumbbell)

      • l=2l=2: d orbital (more complex)

      • l=3l=3: f orbital (even more complex)

    3. Magnetic Quantum Number (mlm_l):

      • Values: l,,0,,+l-l, …, 0, …, +l

      • Describes the orientation of the orbital in space.

      • For l=0l=0 (s), ml=0m_l = 0 (1 orbital).

      • For l=1l=1 (p), ml=1,0,+1m_l = -1, 0, +1 (3 orbitals).

      • For l=2l=2 (d), ml=2,1,0,+1,+2m_l = -2, -1, 0, +1, +2 (5 orbitals).

    4. Spin Quantum Number (msm_s):

      • Values: +12+\frac{1}{2} or -12\text{-}\frac{1}{2}

      • Describes the intrinsic angular momentum (spin) of an electron, either "spin up" or "spin down".

6. Atomic Orbitals and Their Shapes
  • s orbitals (l=0l=0): Spherical shape, increasing size with nn (e.g., 1s, 2s, 3s).

  • p orbitals (l=1l=1): Dumbbell shape, existing in three orientations (p<em>x,p</em>y,pzp<em>x, p</em>y, p_z) along the axes.

  • d orbitals (l=2l=2): More complex shapes, typically four cloverleaf shapes (d<em>xy,d</em>yz,d<em>xz,d</em>x2y2d<em>{xy}, d</em>{yz}, d<em>{xz}, d</em>{x^2-y^2}) and one dumbbell with a toroid (dz2d_{z^2}).

7. Electron Configurations
  • The arrangement of electrons in an atom's orbitals.

  • Governed by three main principles:

    1. Aufbau Principle: Electrons fill the lowest energy orbitals first (e.g., 1s2s2p1s \to 2s \to 2p).

    2. Pauli Exclusion Principle: No two electrons in an atom can have the same set of four quantum numbers. Therefore, an atomic orbital can hold a maximum of two electrons, and these two electrons must have opposite spins.

    3. Hund's Rule: For degenerate orbitals (orbitals of the same energy), electrons will occupy separate orbitals with parallel spins before pairing up in any one orbital.

7.1. Orbital Diagrams
  • Visual representation of electron configuration using boxes or lines for orbitals and arrows for electrons (up arrow for +12+\frac{1}{2}, down arrow for -12\text{-}\frac{1}{2}).

7.2. Notation
  • Spectroscopic notation: e.g., 1s22s22p61s^2 2s^2 2p^6 (superscript indicates number of electrons in that orbital).

  • Noble gas notation: Shorthand using the preceding noble gas symbol in brackets (e.g., for Sodium (Na): [Ne]3s1[Ne] 3s^1).