The waves described by the functions
and![]()
can be added algebraically to produce the resultant wave
![]()
We can define new variables
and
through the equations
![]()
![]()
we can write![]()
The resultant wave above is a sinusoidal wave of the same frequency,
with
![]()
and![]()
For a standing wave
and
since the reflected wave required for a standing wave to be formed undergoes a phase change of
on reflection.
which is not defined. Consideration of the sign of the numerator implies we may take![]()