Next: Mixed sine and cosine
Up: Orthogonality of trigonometric functions
Previous: Preliminary results
From (1), we have
Substituting this into (2) gives
Hence, for
, we have
and
Alternatively, we can prove the same results by integrating by parts,
as follows.
(by (1)). Hence,
. This argument also holds only for
, since otherwise
becomes
and so we get
, so
that
is not necessarily zero.
In the case when
, we have
Since (1) is valid for
as well as
, we have
where
is the Kronecker delta.
Next: Mixed sine and cosine
Up: Orthogonality of trigonometric functions
Previous: Preliminary results
Alexander Frolkin
2001-02-17