1. Preliminary Knowledge
Definition 1 [1] -[3] Let
be an integrable function on
. Then the coefficients
and
are calculated by

and are called the Fourier coefficients of
.
Definition 2 [1] -[5] Let
with the period
be an integrable function on
, trigonometric series with the Fourier coefficient are called Fourier series of
, denoted by

Lemma 1 [6] Let
be an integrable function on
with period of
, the Fourier coefficients are calculated according to period of
. The calculation indicates there are same results between Fourier
series with period of
and
.
2. Calculating Fourier Series According to the Nature of the Function
Theorem 1 Let
be an integrable function on
and satisfy the condition
, then we have
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where
,
,
.
Proof It was clear that the period of
is
and we have
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Let
, then
. Therefore
.
So we get
.
.
Let
, then
. Therefore
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Therefore, we obtain
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In the same way, we have
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In a word, while
is an even number,
, and
![]()
Thus in this case, the expansion reduces to
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Theorem 2 Let
be an integrable function on
and satisfy the conditions
, then we have
![]()
where
,
.
Proof The period of
is
, so we can calculate Fouries series of
with period of
by Lemma 1. We have
![]()
Let
, then
. Therefore
![]()
So we get
![]()
Let
, then
. Therefore
![]()
We obtain
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In the same way, we have
![]()
Thus in this case, the expansion reduces to
![]()
where
,
.
Theorem 3 Let
be an integrable function on
. When
, it satisfies the condition
. Then we have
(1) While
is an even function in
, then we get
![]()
where
.
(2) While
is an odd function in
,then we get
![]()
where
.
Proof (1) We use the method of periodic extension to
with period of
.
Because
is an even function, we have
,
.
![]()
Let
,
, then we have
![]()
Let
, therefore
![]()
We obtain
![]()
Thus in this case, the expansion reduces to
![]()
where
.
(2) In the same way, we can prove Theorem 3 (2).
Similarly, we can prove the following Theorem 4.
Theorem 4 Let
be an integrable function on
. When
, it satisfies the condition
. Then we have
(1) While
is an even function in
, then we get
![]()
where
.
(2) While
is an odd function in
, then we get
![]()
where
.
3. Conclusion
Suppose the function is defined on
, if we use symmetry extension about the point
and then
use odd and periodic extension, we can get two forms of Fourier series as Theorem 3. If we use symmetry ex-
tension about the line
and then use odd and periodic extension, we can get two forms of Fourier series as Theorem 4. Suppose the function is defined on
, we have a similar conclusion.
Acknowledgements
I would like to thank the referees and the editor for their valuable suggestions.