and no sharp turns are allowed;
that is, the wavefunction must be
smooth and continuous.
6 The solution to Schrödinger’s
equation will always be a series
of relatedsolutions because the
equation is an eigenfunction. The
solutions to all eigenfunctions
have common properties. Each of
the solutions is orthogonal, mean-
ing that for each of the wave-
functions the solution is unique
and, when the wavefunctions for
the hydrogen atom are found, they
will each represent a different pos-
sible orbital for the electrons.
7 Quantum mechanics does not
replace classical mechanics but
complements it when consider-
ing small energies and particles.
According to the Correspond-
ence Principle, the results from
quantum mechanics always must
agree with classical mechanics.
Thus, the results from quantum
mechanics must agree with the
classical mechanics in the appro-
priate limits. For example, quantum
mechanics must still conserve
energy of the observed states.General approach for solving Schrödinger’s equation
There is a general strategy that will be
used to solve Schrödinger’s equation
for the different applications. The
first step is to determine the depend-
ence of the potential energy upon the
distance. We start with the classical
expression of the potential and then
substitute the appropriate operators,
which for distance are simply the190 PART 2 QUANTUM MECHANICS AND SPECTROSCOPY
Not allowed
DiscontinuousNot allowed
Derivative
Not continuousNot allowed
Multiple valuesNot allowed
Infinitex (^)
ψ Allowed
ψ
ψ
ψ
ψ
Figure 9.8The wavefunction ψ(x) must be a smooth,
continuous, and single-valued function. Solutions are
unacceptable if they have a discontinuity or more than one
value for a given value of x.