Applied Quantum Mechanics, Second Edition

Chapter 11: Angular Momentum and the Hydrogenic Atom

11.1 Angular Momentum

In classical mechanics the constants of motion of an isolated system are energy, linear momentum, and angular momentum. So far in this book we have not considered angular momentum. In this chapter we start by considering classical angular momentum and then proceed to find the corresponding quantum operators. Following this we consider a hydrogenic atom as a prototype application.

11.1.1 Classical angular momentum

Suppose, as illustrated in Fig. 11.1, we have a point-particle of mass m, linear velocity v at instant t = 0, and momentum p = m v. Angular momentum L about a point r = 0 is defined as [1.]



Fig. 11.1: The angular momentum of a point particle mass m at position r moving with momentum p is defined as L = r p.

where r is the position of particle. Angular momentum is measured in units of J s.

This equation can be written in terms of angular velocity vector ?, normal to the plane of rotation, to give


Making use of the vector relationship a ( b c) = ( a c) b ? ( a b) c, the expression for L may be rewritten as


where the inertia tensor is


In Eq. (11.4) 1 is the unit matrix. If ? = ? n where n is the unit vector in the direction of ? then the...

UNLIMITED FREE
ACCESS
TO THE WORLD'S BEST IDEAS

SUBMIT
Already a GlobalSpec user? Log in.

This is embarrasing...

An error occurred while processing the form. Please try again in a few minutes.

Customize Your GlobalSpec Experience

Category: Gyroscopes
Finish!
Privacy Policy

This is embarrasing...

An error occurred while processing the form. Please try again in a few minutes.