Lecture Notes: CHEM 410A - Physical Chemistry

Lecture 5.2: Physical Chemistry - CHEM 410A

Basic Information

  • Instructor: Yuezhi Mao
  • Course: CHEM 410A (Physical Chemistry)
  • Semester: Spring 2026
  • Institution: San Diego State University (SDSU)

Recap of 1-D Harmonic Oscillator and Energy Levels

  • Harmonic Potential:
    • A potential energy function typically represented in physical chemistry.
    • Configured as a parabolic curve which describes the restorative force experienced by a particle displaced from its equilibrium position.
  • Schrödinger Equation (S.E.):
    • Fundamental equation in quantum mechanics that describes how the quantum state of a physical system changes over time.
  • Results from Solving the Schrödinger Equation:
    • Derives the energy levels of a quantum system.
  • Energy Levels:
    • Defined by the vibrational quantum number (ν).
    • Levels are evenly spaced.
    • Represented mathematically as:
      Ev=(<br/>ν+12)hˉ<br/>νE_v = \bigg( <br />\nu + \frac{1}{2} \bigg) \bar{h}<br />\nu
  • Zero-Point Energy:
    • The lowest energy state (ν = 0) of the quantum oscillator which is not zero; it includes the value given by:
      E0=12hˉ<br/>νE_0 = \frac{1}{2} \bar{h}<br />\nu

1-D Harmonic Oscillator Wavefunctions

Key Characteristics and Components
  • Wavefunctions:
    • Depict the probability amplitude of a particle's position.
  • Normalization Constant:
    • Ensure that the total probability across all space equals one.
    • This constant changes with the quantum number ν.
  • Hermite Polynomials:
    • A set of orthogonal polynomials crucial for the solutions of the wavefunctions of the harmonic oscillator.
    • Their highest power corresponds directly to ν, and the polynomials will either exclusively represent odd or even powers depending on ν.
  • Complete Set of Orthonormal Functions:
    • The H.O. wavefunctions can represent functions such that:
    • They are orthogonal to one another.
    • They can be normalized to 1.
  • Ground-State Wavefunction (ν = 0):
    • Expressed as a standard Gaussian function given by:
      extψ0(x)=Aex22a2ext{ψ}_0(x) = A e^{-\frac{x^2}{2a^2}}
    • Where A is the normalization constant, and a is the characteristic length scale of the oscillator.

Features of Harmonic Oscillator Wavefunctions

  • Even/Odd Functionality:
    • The wavefunction behaves as an even function when ν is even and as an odd function when ν is odd.
  • Number of Nodes:
    • The number of nodes in the wavefunction corresponds to the vibrational quantum number ν.
  • Behavior Between Classical Turning Points:
    • The wavefunction oscillates between the classical turning points but decays to 0 beyond those limits.
  • Effect of Higher Quantum Numbers (ν):
    • As ν increases, the Hermite polynomial dimensions grow substantially before the Gaussian function rapidly decreases to zero.
    • This phenomenon leads to wavefunctions that spread out over a wider range, resulting in maxima of probability density moving towards classical turning points.
  • Classical Turning Points:
    • These points are defined where energy levels intersect with the potential energy curve, given by the equation:
      E=V,extthus,xtp=(2ν+1)hˉ<br/>νE = V, ext{ thus, } x_{tp} = \bigg(2ν + 1 \bigg) \frac{\bar{h}}{<br />\nu}
    • Expresses the classical turning points of oscillator behavior, where
      xtp=((2ν+1)hˉmωˉ)1/2x_{tp} = \bigg( \frac{\bigg( 2ν + 1 \bigg) \bar{h}}{m\bar{ω}} \bigg)^{1/2}
  • Implications of Intrinsic Properties of the Oscillator:
    • Heavier Particles: This leads to smaller energy spacings:
      ωˉ=km\bar{ω} = \frac{k}{m}
    • Stiffer Spring (Higher k): Results in larger energy spacings and produces narrower wavefunctions.

Evaluating Quantities from H.O. Wavefunctions

  1. Normalization:
    • The process of ensuring the total probability of finding a particle in all space is equal to 1.
  2. Expectation Values:
    • Measured averages of physical quantities derived from wavefunctions, useful in quantum mechanics to describe particle behavior.
  3. Probability in Classically Forbidden Regions (Tunneling Probability):
    • Specifically discussed for the ground state (ν = 0) and includes cases where:
    • Probability beyond classical limits (i.e., for x > x{max} and x<x</em>maxx < -x</em>{max}).
    • Additionally provided a Python program to calculate tunneling probability for states where ν > 0.