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... For the ground state of the
H atom the Bohr model assumes an angular momentem of hbar. In the
Schrodinger solution the angular momentum is given by L square = (l)(l+1)h
bar and the z component of the angular momentum by Lz=m hbar. But m must be
less than or equal to l and l must be less than n. For the ground state of
the hydrogen atom n = 1 , l=m=o. It has no (orbital) angular momentum, so
Bohr's initial postulate by which he calculated the energy of the various
levels in the hydrogen atom was wrong. Why does he get the right answer?
Luck I guess.