Lecture Notes: CHEM 410A - Physical Chemistry
Lecture 5.2: Physical Chemistry - CHEM 410A
- 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:
E_v = igg(
u + rac{1}{2} igg) ar{h}
u
- Zero-Point Energy:
- The lowest energy state (ν = 0) of the quantum oscillator which is not zero; it includes the value given by:
E_0 = rac{1}{2} ar{h}
u
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:
ext{ψ}_0(x) = A e^{-rac{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, ext{ thus, } x_{tp} = igg(2ν + 1 igg) rac{ar{h}}{
u} - Expresses the classical turning points of oscillator behavior, where
x_{tp} = igg( rac{igg( 2ν + 1 igg) ar{h}}{mar{ω}} igg)^{1/2}
- Implications of Intrinsic Properties of the Oscillator:
- Heavier Particles: This leads to smaller energy spacings:
ar{ω} = rac{k}{m} - Stiffer Spring (Higher k): Results in larger energy spacings and produces narrower wavefunctions.
Evaluating Quantities from H.O. Wavefunctions
- Normalization:
- The process of ensuring the total probability of finding a particle in all space is equal to 1.
- Expectation Values:
- Measured averages of physical quantities derived from wavefunctions, useful in quantum mechanics to describe particle behavior.
- 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{max} ).
- Additionally provided a Python program to calculate tunneling probability for states where ν > 0.