674 Higher Engineering Mathematics
The Laplace transforms of derivatives:
First derivative
L
{
dy
dx
}
=sL{y}−y(0)
wherey( 0 )is the value ofyatx=0.
Second derivative
L
{
dy
dx
}
=s^2 L{y}−sy( 0 )−y′(0)
wherey′( 0 )is the value of
dy
dx
atx=0.
Fourier Series
If f(x)is a periodic function of period 2πthen its
Fourier series is given by:
f(x)=a 0 +
∑∞
n= 1
(ancosnx+bnsinnx)
where, for the range−πto+π:
a 0 =
1
2 π
∫π
−π
f(x)dx
an=
1
π
∫π
−π
f(x)cosnxdx (n= 1 , 2 , 3 ,...)
bn=
1
π
∫π
−π
f(x)sinnxdx (n= 1 , 2 , 3 ,...)
Iff(x)isa periodicfunctionofperiodLthen itsFourier
series is given by:
f(x)=a 0 +
∑∞
n= 1
{
ancos
(
2 πnx
L
)
+bnsin
( 2 πnx
L
)}
where for the range−
L
2
to+
L
2
:
a 0 =
1
L
∫L/ 2
−L/ 2
f(x)dx
an=L^2
∫ L/ 2
−L/ 2
f(x)cos
( 2 πnx
L
)
dx(n= 1 , 2 , 3 ,...)
bn=L^2
∫ L/ 2
−L/ 2
f(x)sin
( 2 πnx
L
)
dx(n= 1 , 2 , 3 ,...)
Complex or exponential Fourier series:
f(x)=
∑∞
n=−∞
cnej
2 πnx
L
where cn=
1
L
∫ L 2
−L 2
f(x)e−j
2 πnx
L dx
For even symmetry,
cn=
2
L
∫ L 2
0
f(x)cos
( 2 πnx
L
)
dx
For odd symmetry,
cn=−j
2
L
∫ L
2
0
f(x)sin
( 2 πnx
L
)
dx