In: Physics
The failure of Rutherford's model of atom led Bohr to propose a
fruitful model on structure of atom. To overcome the difficulty
associated with the classical collapse of the
electron into the nucleus, Bohr proposed that the orbiting electron
could
only exist in certain special states of motion - called stationary
states, in
which no electromagnetic radiation was emitted. In these states,
the angular
momentum of the electron L takes on integer values of Planck’s
constant
divided by 2π, denoted by = h/2π (pronounced h-bar). In these
stationary
states, the electron angular momentum can take on values
h/2pi,2h/2pi,3h/2pi..,
but never non-integer values. This is known as quantization of
angular
momentum, and was one of Bohr’s key hypotheses. Note that
this
differs from Planck’s hypothesis of energy quantization, but as we
will see
it does lead to quantization of energy.
For circular orbits, the position vector of the electron r is
always perpen-
dicular to its linear momentum p. The angular momentum L = r × p
has
magnitude L = rp= mvr in this case. Thus Bohr’s postulate of
quantized
angular momentum is equivalent to
mvr= nh/2pi
where n is a positive integer. v= nh/mr