A beam of silver atoms, for which M=+HB, passes through an inhomogeneous magnetic field, as in the Stern-Gerlach apparatus shown schematically in Fig. 1.15. The field gradient is 0B/0z 103 T m-, the length of the pole piece is L=0.1 m, the distance to the screen is I=1 m and the temperature of the oven is T = 600 K. Assuming that the velocity of the silver atoms is equal to the root-mean-square velocity of (3kT/M)2 (where k is the Boltzmann constant and M is the mass of a silver atom) calculate the maximum separation (P,P, in Fig. on the screen. ) of the two beams
A beam of silver atoms, for which M=+HB, passes through an inhomogeneous magnetic field, as in the Stern-Gerlach apparatus shown schematically in Fig. 1.15. The field gradient is 0B/0z 103 T m-, the length of the pole piece is L=0.1 m, the distance to the screen is I=1 m and the temperature of the oven is T = 600 K. Assuming that the velocity of the silver atoms is equal to the root-mean-square velocity of (3kT/M)2 (where k is the Boltzmann constant and M is the mass of a silver atom) calculate the maximum separation (P,P, in Fig. on the screen. ) of the two beams
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