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Peter Atkins • Julio de Paula Atkins’ Physical Chemistry

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1 Peter Atkins • Julio de Paula Atkins’ Physical Chemistry
Eighth Edition Chapter 9 Quantum Theory: Techniques and Applications Copyright © 2006 by Peter Atkins and Julio de Paula

2 Chap 9 Quantum Theory: Techniques and Applications
Objectives: Solve the Schrodinger equation for: Translational motion (Particle in a box) Vibrational motion (Harmonic and anharmonic oscillator Rotational motion (Particle on a ring & on a sphere

3 Fig 9.20 Potential energy of a harmonic oscillator
Restoring force: F = -kx where k ≡ force constant Potential energy: Schrodinger equation:

4 Fig 9.21 Energy levels of a harmonic oscillator
Solving Gives: where: Zero point energy

5 Form of the harmonic oscillator wavefunctions:
Ψ(x) = N · (polynomial in x) · (Gaussian function) Fig Graph of Gaussian function:

6 Form of the harmonic oscillator wavefunctions:
Ψ(x) = N · (polynomial in x) · (Gaussian function) Precisely: where: and

7 When the Schrodinger equation for the harmonic oscillator
is solved, the solutions contain this set of polynomials, named the Hermite polynomials.

8 Fig 9.23 Normalized Ψ and Ψ2 for the v = 0 state
of a harmonic oscillator

9 Fig 9.24 Normalized Ψ and Ψ2 for the v=1 state
of a harmonic oscillator

10 Interpretation of Harmonic Oscillator Wavefunctions
Gaussian function goes strongly to zero as displacement increases. i.e., ψ → 0 at large x. The exponent y2 ∝ x2 (mk)1/2 so ψ → 0 more rapidly with high masses and stiff springs. 3) Wavefunctions spread more a v increases.

11 Fig 9.25 Normalized Ψ’s for the v=0 – v=4 states
of a harmonic oscillator

12 Oscillator may be in classically forbidden regions at low v
Fig Probability distributions for the v = 0 – v = 4 states of a harmonic oscillator classical turning points at high v Oscillator may be in classically forbidden regions at low v i.e. tunnelling!

13 Correspondence Principle:
Classical mechanics emerges from quantum mechanics as high quantum numbers are reached i.e., particle may be found anywhere as v → ∞ As v → ∞ the oscillator becomes macroscopic (e.g. a pendulum)


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