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5

                                                    Angular momentum
















                             Angular momentum plays an important role in both classical and quantum
                             mechanics. In isolated classical systems the total angular momentum is a
                             constant of motion. In quantum systems the angular momentum is important in
                             studies of atomic, molecular, and nuclear structure and spectra and in studies
                             of spin in elementary particles and in magnetism.


                                                 5.1 Orbital angular momentum

                             We ®rst consider a particle of mass m moving according to the laws of classical
                             mechanics. The angular momentum L of the particle with respect to the origin
                             of the coordinate system is de®ned by the relation
                                                            L   r 3 p                           (5:1)
                             where r is the position vector given by equation (2.60) and p is the linear
                             momentum given by equation (2.61). When expressed as a determinant, the
                             angular momentum L is

                                                               i   j   k

                                                        L ˆ     x  y   z


                                                              p x  p y  p z
                             The components L x , L y , L z of the vector L are
                                                          L x ˆ yp z ÿ zp y

                                                          L y ˆ zp x ÿ xp z                     (5:2)
                                                          L z ˆ xp y ÿ yp x
                             The square of the magnitude of the vector L is given in terms of these
                             components by
                                                                  2
                                                                       2
                                                      2
                                                           :
                                                    L ˆ L L ˆ L ‡ L ‡ L     2 z                 (5:3)
                                                                        y
                                                                  x
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