{[ promptMessage ]}

Bookmark it

{[ promptMessage ]}

Lecture18Notes

# Lecture18Notes - Chem 120A Spring 2006 READING The Harmonic...

This preview shows pages 1–3. Sign up to view the full content.

Chem 120A The Harmonic Oscillator, part I 03/01/06 Spring 2006 Lecture 18 READING: Engel (QCS): Chapter 7, 8.3 Introduction to the harmonic oscillator Along with the hydrogen atom, the harmonic oscillator is one of the most important systems in elementary quantum mechanics. Its significance far exceeds the physical chemistry textbook example of a diatomic molecule. Every quantum mechanics textbook treats this system, as does every physical chemistry textbook. Harmonic potential Interatomic potential V(R) R Figure 1: Interatomic potential for a diatomic molecule compared to that of a harmonic oscillator centered at r 0 . 0 R 0 E 0 We begin with a classical discussion in order to point out a few points. Consider a mass m attached to a spring. The potential energy as a function of x is V ( x ) = 1 / 2 kx 2 . The force is F = kx . Another situation is a diatomic molecule, for example HCl. It turns out that the potential energy between the two atoms as a function of relative distance looks like that shown in Figure 1. (This interaction potential is actually a derived result and is one of the great triumphs of quantum mechanics.) Now, V ( R ) can be expanded about its minimum at R 0 : V ( R ) = V 0 + 1 2 d 2 dR 2 V ( R ) R = R 0 ( R R 0 ) 2 + ..., (1) where d 2 dR 2 V ( R ) R = R 0 is the curvature of the potential at the minimum, which we will call k . We will also define R R 0 = x . Thus, near the minimum of the interaction potential, the relative motion undergoes small oscillations. This is what we call a ’harmonic oscillator.’ The deeper the well the more ’harmonic’ the motion is. In other words, to second order within the Taylor expansion of V ( R ) , we can approximate the Chem 120A, Spring 2006, Lecture 18 1

This preview has intentionally blurred sections. Sign up to view the full version.

View Full Document
potential shown in Fig. 1 as a parabola, and the deeper the minimum , the more closely the parabola will match the potential near the minimum. Since V 0 is just a constant, it does not effect the relative motion of the diatomic, so we will ignore it. Now, as we’ve said, the initial positions and momenta determine all future motion. The energy is also determined initially, but it is a conserved quantity and it does not change with time. Suppose that the total energy of the system is E . This bounds the possible position,
This is the end of the preview. Sign up to access the rest of the document.

{[ snackBarMessage ]}

### Page1 / 4

Lecture18Notes - Chem 120A Spring 2006 READING The Harmonic...

This preview shows document pages 1 - 3. Sign up to view the full document.

View Full Document
Ask a homework question - tutors are online