fourier series 2
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TRANSCRIPT
Fourier Series 2
N. B. Vyas
Department of Mathematics,Atmiya Institute of Tech. & Science,
Rajkot (Guj.)- INDIA
N. B. Vyas Fourier Series 2
Functions of any Period p = 2L
Let f(x) be a periodic function with an arbitrary period 2Ldefined in the interval c < x < c+ 2L
The Fourier series of f(x) is given by
f(x) =a02
+∞∑n=1
[an cos
(nπxL
)+ bn sin
(nπxL
)]where a0 =
1
L
∫ c+2L
c
f(x) dx
an =1
L
∫ c+2L
c
f(x) cos(nπxL
)dx
bn =1
L
∫ c+2L
c
f(x) sin(nπxL
)dx
N. B. Vyas Fourier Series 2
Functions of any Period p = 2L
Let f(x) be a periodic function with an arbitrary period 2Ldefined in the interval c < x < c+ 2L
The Fourier series of f(x) is given by
f(x) =a02
+∞∑n=1
[an cos
(nπxL
)+ bn sin
(nπxL
)]where a0 =
1
L
∫ c+2L
c
f(x) dx
an =1
L
∫ c+2L
c
f(x) cos(nπxL
)dx
bn =1
L
∫ c+2L
c
f(x) sin(nπxL
)dx
N. B. Vyas Fourier Series 2
Functions of any Period p = 2L
Let f(x) be a periodic function with an arbitrary period 2Ldefined in the interval c < x < c+ 2L
The Fourier series of f(x) is given by
f(x) =a02
+∞∑n=1
[an cos
(nπxL
)+ bn sin
(nπxL
)]
where a0 =1
L
∫ c+2L
c
f(x) dx
an =1
L
∫ c+2L
c
f(x) cos(nπxL
)dx
bn =1
L
∫ c+2L
c
f(x) sin(nπxL
)dx
N. B. Vyas Fourier Series 2
Functions of any Period p = 2L
Let f(x) be a periodic function with an arbitrary period 2Ldefined in the interval c < x < c+ 2L
The Fourier series of f(x) is given by
f(x) =a02
+∞∑n=1
[an cos
(nπxL
)+ bn sin
(nπxL
)]where a0 =
1
L
∫ c+2L
c
f(x) dx
an =1
L
∫ c+2L
c
f(x) cos(nπxL
)dx
bn =1
L
∫ c+2L
c
f(x) sin(nπxL
)dx
N. B. Vyas Fourier Series 2
Functions of any Period p = 2L
Let f(x) be a periodic function with an arbitrary period 2Ldefined in the interval c < x < c+ 2L
The Fourier series of f(x) is given by
f(x) =a02
+∞∑n=1
[an cos
(nπxL
)+ bn sin
(nπxL
)]where a0 =
1
L
∫ c+2L
c
f(x) dx
an =1
L
∫ c+2L
c
f(x) cos(nπxL
)dx
bn =1
L
∫ c+2L
c
f(x) sin(nπxL
)dx
N. B. Vyas Fourier Series 2
Functions of any Period p = 2L
Let f(x) be a periodic function with an arbitrary period 2Ldefined in the interval c < x < c+ 2L
The Fourier series of f(x) is given by
f(x) =a02
+∞∑n=1
[an cos
(nπxL
)+ bn sin
(nπxL
)]where a0 =
1
L
∫ c+2L
c
f(x) dx
an =1
L
∫ c+2L
c
f(x) cos(nπxL
)dx
bn =1
L
∫ c+2L
c
f(x) sin(nπxL
)dx
N. B. Vyas Fourier Series 2
Functions of any Period p = 2L
Corollary 1: If c = 0 the interval becomes 0 < x < 2L
f(x) =a02
+∞∑n=1
[an cos
(nπxL
)+ bn sin
(nπxL
)]where a0 =
1
L
∫ 2L
0
f(x) dx
an =1
L
∫ 2L
0
f(x) cos(nπxL
)dx
bn =1
L
∫ 2L
0
f(x) sin(nπxL
)dx
N. B. Vyas Fourier Series 2
Functions of any Period p = 2L
Corollary 1: If c = 0 the interval becomes 0 < x < 2L
f(x) =a02
+∞∑n=1
[an cos
(nπxL
)+ bn sin
(nπxL
)]
where a0 =1
L
∫ 2L
0
f(x) dx
an =1
L
∫ 2L
0
f(x) cos(nπxL
)dx
bn =1
L
∫ 2L
0
f(x) sin(nπxL
)dx
N. B. Vyas Fourier Series 2
Functions of any Period p = 2L
Corollary 1: If c = 0 the interval becomes 0 < x < 2L
f(x) =a02
+∞∑n=1
[an cos
(nπxL
)+ bn sin
(nπxL
)]where a0 =
1
L
∫ 2L
0
f(x) dx
an =1
L
∫ 2L
0
f(x) cos(nπxL
)dx
bn =1
L
∫ 2L
0
f(x) sin(nπxL
)dx
N. B. Vyas Fourier Series 2
Functions of any Period p = 2L
Corollary 1: If c = 0 the interval becomes 0 < x < 2L
f(x) =a02
+∞∑n=1
[an cos
(nπxL
)+ bn sin
(nπxL
)]where a0 =
1
L
∫ 2L
0
f(x) dx
an =1
L
∫ 2L
0
f(x) cos(nπxL
)dx
bn =1
L
∫ 2L
0
f(x) sin(nπxL
)dx
N. B. Vyas Fourier Series 2
Functions of any Period p = 2L
Corollary 1: If c = 0 the interval becomes 0 < x < 2L
f(x) =a02
+∞∑n=1
[an cos
(nπxL
)+ bn sin
(nπxL
)]where a0 =
1
L
∫ 2L
0
f(x) dx
an =1
L
∫ 2L
0
f(x) cos(nπxL
)dx
bn =1
L
∫ 2L
0
f(x) sin(nπxL
)dx
N. B. Vyas Fourier Series 2
Functions of any Period p = 2L
Corollary 2: If c = −L the interval becomes −L < x < L
f(x) =a02
+∞∑n=1
[an cos
(nπxL
)+ bn sin
(nπxL
)]where a0 =
1
L
∫ L
−Lf(x) dx
an =1
L
∫ L
−Lf(x) cos
(nπxL
)dx
bn =1
L
∫ L
−Lf(x) sin
(nπxL
)dx
N. B. Vyas Fourier Series 2
Functions of any Period p = 2L
Corollary 2: If c = −L the interval becomes −L < x < L
f(x) =a02
+∞∑n=1
[an cos
(nπxL
)+ bn sin
(nπxL
)]
where a0 =1
L
∫ L
−Lf(x) dx
an =1
L
∫ L
−Lf(x) cos
(nπxL
)dx
bn =1
L
∫ L
−Lf(x) sin
(nπxL
)dx
N. B. Vyas Fourier Series 2
Functions of any Period p = 2L
Corollary 2: If c = −L the interval becomes −L < x < L
f(x) =a02
+∞∑n=1
[an cos
(nπxL
)+ bn sin
(nπxL
)]where a0 =
1
L
∫ L
−Lf(x) dx
an =1
L
∫ L
−Lf(x) cos
(nπxL
)dx
bn =1
L
∫ L
−Lf(x) sin
(nπxL
)dx
N. B. Vyas Fourier Series 2
Functions of any Period p = 2L
Corollary 2: If c = −L the interval becomes −L < x < L
f(x) =a02
+∞∑n=1
[an cos
(nπxL
)+ bn sin
(nπxL
)]where a0 =
1
L
∫ L
−Lf(x) dx
an =1
L
∫ L
−Lf(x) cos
(nπxL
)dx
bn =1
L
∫ L
−Lf(x) sin
(nπxL
)dx
N. B. Vyas Fourier Series 2
Functions of any Period p = 2L
Corollary 2: If c = −L the interval becomes −L < x < L
f(x) =a02
+∞∑n=1
[an cos
(nπxL
)+ bn sin
(nπxL
)]where a0 =
1
L
∫ L
−Lf(x) dx
an =1
L
∫ L
−Lf(x) cos
(nπxL
)dx
bn =1
L
∫ L
−Lf(x) sin
(nπxL
)dx
N. B. Vyas Fourier Series 2
Example
Ex. The Fourier series of f(x) = x2, 0 < x < 2 wheref(x+ 2) = f(x).
Hence deduce that 1− 1
22+
1
32− 1
42+ . . . =
π2
12
N. B. Vyas Fourier Series 2
Example
Ex. The Fourier series of f(x) = x2, 0 < x < 2 wheref(x+ 2) = f(x).
Hence deduce that 1− 1
22+
1
32− 1
42+ . . . =
π2
12
N. B. Vyas Fourier Series 2
Example
Sol. Step 1: The Fourier series of f(x) is given by
f(x) =a02
+∞∑n=1
[an cos
(nπxL
)+ bn sin
(nπxL
)]where a0 =
1
L
∫ 2
0
f(x) dx
an =1
L
∫ 2
0
f(x) cos(nπxL
)dx
bn =1
L
∫ 2
0
f(x) sin(nπxL
)dx
Here p = 2L = 2⇒ L = 1
N. B. Vyas Fourier Series 2
Example
Sol. Step 1: The Fourier series of f(x) is given by
f(x) =a02
+∞∑n=1
[an cos
(nπxL
)+ bn sin
(nπxL
)]
where a0 =1
L
∫ 2
0
f(x) dx
an =1
L
∫ 2
0
f(x) cos(nπxL
)dx
bn =1
L
∫ 2
0
f(x) sin(nπxL
)dx
Here p = 2L = 2⇒ L = 1
N. B. Vyas Fourier Series 2
Example
Sol. Step 1: The Fourier series of f(x) is given by
f(x) =a02
+∞∑n=1
[an cos
(nπxL
)+ bn sin
(nπxL
)]where a0 =
1
L
∫ 2
0
f(x) dx
an =1
L
∫ 2
0
f(x) cos(nπxL
)dx
bn =1
L
∫ 2
0
f(x) sin(nπxL
)dx
Here p = 2L = 2⇒ L = 1
N. B. Vyas Fourier Series 2
Example
Sol. Step 1: The Fourier series of f(x) is given by
f(x) =a02
+∞∑n=1
[an cos
(nπxL
)+ bn sin
(nπxL
)]where a0 =
1
L
∫ 2
0
f(x) dx
an =1
L
∫ 2
0
f(x) cos(nπxL
)dx
bn =1
L
∫ 2
0
f(x) sin(nπxL
)dx
Here p = 2L = 2⇒ L = 1
N. B. Vyas Fourier Series 2
Example
Sol. Step 1: The Fourier series of f(x) is given by
f(x) =a02
+∞∑n=1
[an cos
(nπxL
)+ bn sin
(nπxL
)]where a0 =
1
L
∫ 2
0
f(x) dx
an =1
L
∫ 2
0
f(x) cos(nπxL
)dx
bn =1
L
∫ 2
0
f(x) sin(nπxL
)dx
Here p = 2L = 2⇒ L = 1
N. B. Vyas Fourier Series 2
Example
Sol. Step 1: The Fourier series of f(x) is given by
f(x) =a02
+∞∑n=1
[an cos
(nπxL
)+ bn sin
(nπxL
)]where a0 =
1
L
∫ 2
0
f(x) dx
an =1
L
∫ 2
0
f(x) cos(nπxL
)dx
bn =1
L
∫ 2
0
f(x) sin(nπxL
)dx
Here p = 2L = 2⇒ L = 1
N. B. Vyas Fourier Series 2
Example
Step 2. Now a0 =1
1
∫ 2
0
f(x) dx
a0 =
∫ 2
0
(x)2 dx
=
[x3
3
]20
=8
3
N. B. Vyas Fourier Series 2
Example
Step 2. Now a0 =1
1
∫ 2
0
f(x) dx
a0 =
∫ 2
0
(x)2 dx
=
[x3
3
]20
=8
3
N. B. Vyas Fourier Series 2
Example
Step 2. Now a0 =1
1
∫ 2
0
f(x) dx
a0 =
∫ 2
0
(x)2 dx
=
[x3
3
]20
=8
3
N. B. Vyas Fourier Series 2
Example
Step 2. Now a0 =1
1
∫ 2
0
f(x) dx
a0 =
∫ 2
0
(x)2 dx
=
[x3
3
]20
=8
3
N. B. Vyas Fourier Series 2
Example
Step 3. an =1
1
∫ 2
0
f(x) cos(nπx
1
)dx
an =
∫ 2
0
x2 cos(nπx) dx
=
[x2(sin nπx
nπ
)− (2x)
(−cos nπx
n2π2
)+ 2
(−sin nπx
n3π3
)]20
=4
n2π2
N. B. Vyas Fourier Series 2
Example
Step 3. an =1
1
∫ 2
0
f(x) cos(nπx
1
)dx
an =
∫ 2
0
x2 cos(nπx) dx
=
[x2(sin nπx
nπ
)− (2x)
(−cos nπx
n2π2
)+ 2
(−sin nπx
n3π3
)]20
=4
n2π2
N. B. Vyas Fourier Series 2
Example
Step 3. an =1
1
∫ 2
0
f(x) cos(nπx
1
)dx
an =
∫ 2
0
x2 cos(nπx) dx
=
[x2(sin nπx
nπ
)− (2x)
(−cos nπx
n2π2
)+ 2
(−sin nπx
n3π3
)]20
=4
n2π2
N. B. Vyas Fourier Series 2
Example
Step 3. an =1
1
∫ 2
0
f(x) cos(nπx
1
)dx
an =
∫ 2
0
x2 cos(nπx) dx
=
[x2(sin nπx
nπ
)− (2x)
(−cos nπx
n2π2
)+ 2
(−sin nπx
n3π3
)]20
=4
n2π2
N. B. Vyas Fourier Series 2
Example
Step 4. bn =1
1
∫ 2
0
f(x) sin(nπx
1
)dx
bn =
∫ 2
0
x2 sin(nπx) dx
=
[x2(−cos nπx
nπ
)− (2x)
(−sin nπx
n2π2
)+ 2
(cos nπxn3π3
)]20
= − 4
nπ
N. B. Vyas Fourier Series 2
Example
Step 4. bn =1
1
∫ 2
0
f(x) sin(nπx
1
)dx
bn =
∫ 2
0
x2 sin(nπx) dx
=
[x2(−cos nπx
nπ
)− (2x)
(−sin nπx
n2π2
)+ 2
(cos nπxn3π3
)]20
= − 4
nπ
N. B. Vyas Fourier Series 2
Example
Step 4. bn =1
1
∫ 2
0
f(x) sin(nπx
1
)dx
bn =
∫ 2
0
x2 sin(nπx) dx
=
[x2(−cos nπx
nπ
)− (2x)
(−sin nπx
n2π2
)+ 2
(cos nπxn3π3
)]20
= − 4
nπ
N. B. Vyas Fourier Series 2
Example
Step 4. bn =1
1
∫ 2
0
f(x) sin(nπx
1
)dx
bn =
∫ 2
0
x2 sin(nπx) dx
=
[x2(−cos nπx
nπ
)− (2x)
(−sin nπx
n2π2
)+ 2
(cos nπxn3π3
)]20
= − 4
nπ
N. B. Vyas Fourier Series 2
Example
Step 5. Substituting values of a0, an and bn in (1), we get therequired Fourier series of f(x) in the interval (0, 2)
f(x) =8
6+∞∑n=1
(4
n2π2
)cos(nπx
1
)+∞∑n=1
(− 4
nπ
)sin(nπx
1
)=
4
3+
4
π2
∞∑n=1
cos(nπx)
n2− 4
π
∞∑n=1
sin(nπx)
n
Putting x = 1, we get
1 =4
3+
4
π2
[− 1
11+
1
22− 1
32+ . . .
]−1
3=
4
π2
[− 1
11+
1
22− 1
32+ . . .
]π2
12=
1
12− 1
22+
1
32− 1
42+ . . .
N. B. Vyas Fourier Series 2
Example
Step 5. Substituting values of a0, an and bn in (1), we get therequired Fourier series of f(x) in the interval (0, 2)
f(x) =8
6+∞∑n=1
(4
n2π2
)cos(nπx
1
)+∞∑n=1
(− 4
nπ
)sin(nπx
1
)
=4
3+
4
π2
∞∑n=1
cos(nπx)
n2− 4
π
∞∑n=1
sin(nπx)
n
Putting x = 1, we get
1 =4
3+
4
π2
[− 1
11+
1
22− 1
32+ . . .
]−1
3=
4
π2
[− 1
11+
1
22− 1
32+ . . .
]π2
12=
1
12− 1
22+
1
32− 1
42+ . . .
N. B. Vyas Fourier Series 2
Example
Step 5. Substituting values of a0, an and bn in (1), we get therequired Fourier series of f(x) in the interval (0, 2)
f(x) =8
6+∞∑n=1
(4
n2π2
)cos(nπx
1
)+∞∑n=1
(− 4
nπ
)sin(nπx
1
)=
4
3+
4
π2
∞∑n=1
cos(nπx)
n2− 4
π
∞∑n=1
sin(nπx)
n
Putting x = 1, we get
1 =4
3+
4
π2
[− 1
11+
1
22− 1
32+ . . .
]−1
3=
4
π2
[− 1
11+
1
22− 1
32+ . . .
]π2
12=
1
12− 1
22+
1
32− 1
42+ . . .
N. B. Vyas Fourier Series 2
Example
Step 5. Substituting values of a0, an and bn in (1), we get therequired Fourier series of f(x) in the interval (0, 2)
f(x) =8
6+∞∑n=1
(4
n2π2
)cos(nπx
1
)+∞∑n=1
(− 4
nπ
)sin(nπx
1
)=
4
3+
4
π2
∞∑n=1
cos(nπx)
n2− 4
π
∞∑n=1
sin(nπx)
n
Putting x = 1, we get
1 =4
3+
4
π2
[− 1
11+
1
22− 1
32+ . . .
]−1
3=
4
π2
[− 1
11+
1
22− 1
32+ . . .
]π2
12=
1
12− 1
22+
1
32− 1
42+ . . .
N. B. Vyas Fourier Series 2
Example
Step 5. Substituting values of a0, an and bn in (1), we get therequired Fourier series of f(x) in the interval (0, 2)
f(x) =8
6+∞∑n=1
(4
n2π2
)cos(nπx
1
)+∞∑n=1
(− 4
nπ
)sin(nπx
1
)=
4
3+
4
π2
∞∑n=1
cos(nπx)
n2− 4
π
∞∑n=1
sin(nπx)
n
Putting x = 1, we get
1 =4
3+
4
π2
[− 1
11+
1
22− 1
32+ . . .
]
−1
3=
4
π2
[− 1
11+
1
22− 1
32+ . . .
]π2
12=
1
12− 1
22+
1
32− 1
42+ . . .
N. B. Vyas Fourier Series 2
Example
Step 5. Substituting values of a0, an and bn in (1), we get therequired Fourier series of f(x) in the interval (0, 2)
f(x) =8
6+∞∑n=1
(4
n2π2
)cos(nπx
1
)+∞∑n=1
(− 4
nπ
)sin(nπx
1
)=
4
3+
4
π2
∞∑n=1
cos(nπx)
n2− 4
π
∞∑n=1
sin(nπx)
n
Putting x = 1, we get
1 =4
3+
4
π2
[− 1
11+
1
22− 1
32+ . . .
]−1
3=
4
π2
[− 1
11+
1
22− 1
32+ . . .
]
π2
12=
1
12− 1
22+
1
32− 1
42+ . . .
N. B. Vyas Fourier Series 2
Example
Step 5. Substituting values of a0, an and bn in (1), we get therequired Fourier series of f(x) in the interval (0, 2)
f(x) =8
6+∞∑n=1
(4
n2π2
)cos(nπx
1
)+∞∑n=1
(− 4
nπ
)sin(nπx
1
)=
4
3+
4
π2
∞∑n=1
cos(nπx)
n2− 4
π
∞∑n=1
sin(nπx)
n
Putting x = 1, we get
1 =4
3+
4
π2
[− 1
11+
1
22− 1
32+ . . .
]−1
3=
4
π2
[− 1
11+
1
22− 1
32+ . . .
]π2
12=
1
12− 1
22+
1
32− 1
42+ . . .
N. B. Vyas Fourier Series 2
Example
Ex. Find the Fourier series of f(x) = 2x in −1 < x < 1where p = 2L = 2.
N. B. Vyas Fourier Series 2
Example
Sol. Step 1: The Fourier series of f(x) is given by
f(x) =a02
+∞∑n=1
[an cos
(nπxL
)+ bn sin
(nπxL
)]where a0 =
1
L
∫ 1
−1f(x) dx
an =1
L
∫ 1
−1f(x) cos
(nπxL
)dx
bn =1
L
∫ 1
−1f(x) sin
(nπxL
)dx
Here p = 2L = 2⇒ L = 1
N. B. Vyas Fourier Series 2
Example
Sol. Step 1: The Fourier series of f(x) is given by
f(x) =a02
+∞∑n=1
[an cos
(nπxL
)+ bn sin
(nπxL
)]
where a0 =1
L
∫ 1
−1f(x) dx
an =1
L
∫ 1
−1f(x) cos
(nπxL
)dx
bn =1
L
∫ 1
−1f(x) sin
(nπxL
)dx
Here p = 2L = 2⇒ L = 1
N. B. Vyas Fourier Series 2
Example
Sol. Step 1: The Fourier series of f(x) is given by
f(x) =a02
+∞∑n=1
[an cos
(nπxL
)+ bn sin
(nπxL
)]where a0 =
1
L
∫ 1
−1f(x) dx
an =1
L
∫ 1
−1f(x) cos
(nπxL
)dx
bn =1
L
∫ 1
−1f(x) sin
(nπxL
)dx
Here p = 2L = 2⇒ L = 1
N. B. Vyas Fourier Series 2
Example
Sol. Step 1: The Fourier series of f(x) is given by
f(x) =a02
+∞∑n=1
[an cos
(nπxL
)+ bn sin
(nπxL
)]where a0 =
1
L
∫ 1
−1f(x) dx
an =1
L
∫ 1
−1f(x) cos
(nπxL
)dx
bn =1
L
∫ 1
−1f(x) sin
(nπxL
)dx
Here p = 2L = 2⇒ L = 1
N. B. Vyas Fourier Series 2
Example
Sol. Step 1: The Fourier series of f(x) is given by
f(x) =a02
+∞∑n=1
[an cos
(nπxL
)+ bn sin
(nπxL
)]where a0 =
1
L
∫ 1
−1f(x) dx
an =1
L
∫ 1
−1f(x) cos
(nπxL
)dx
bn =1
L
∫ 1
−1f(x) sin
(nπxL
)dx
Here p = 2L = 2⇒ L = 1
N. B. Vyas Fourier Series 2
Example
Sol. Step 1: The Fourier series of f(x) is given by
f(x) =a02
+∞∑n=1
[an cos
(nπxL
)+ bn sin
(nπxL
)]where a0 =
1
L
∫ 1
−1f(x) dx
an =1
L
∫ 1
−1f(x) cos
(nπxL
)dx
bn =1
L
∫ 1
−1f(x) sin
(nπxL
)dx
Here p = 2L = 2⇒ L = 1
N. B. Vyas Fourier Series 2
Example
Step 2. Now a0 =1
1
∫ 1
−1f(x) dx
a0 =
∫ 1
−12x dx
= 0
N. B. Vyas Fourier Series 2
Example
Step 2. Now a0 =1
1
∫ 1
−1f(x) dx
a0 =
∫ 1
−12x dx
= 0
N. B. Vyas Fourier Series 2
Example
Step 2. Now a0 =1
1
∫ 1
−1f(x) dx
a0 =
∫ 1
−12x dx
= 0
N. B. Vyas Fourier Series 2
Example
Step 3. an =1
1
∫ 1
−1f(x) cos
(nπx1
)dx
an =
∫ 1
−12x cos(nπx) dx
=
[2x
(sin nπx
nπ
)− (2)
(−cos nπx
n2π2
)]1−1
=
[0 +
2(−1)n
n2π2− 0− 2(−1)n
n2π2
]= 0
N. B. Vyas Fourier Series 2
Example
Step 3. an =1
1
∫ 1
−1f(x) cos
(nπx1
)dx
an =
∫ 1
−12x cos(nπx) dx
=
[2x
(sin nπx
nπ
)− (2)
(−cos nπx
n2π2
)]1−1
=
[0 +
2(−1)n
n2π2− 0− 2(−1)n
n2π2
]= 0
N. B. Vyas Fourier Series 2
Example
Step 3. an =1
1
∫ 1
−1f(x) cos
(nπx1
)dx
an =
∫ 1
−12x cos(nπx) dx
=
[2x
(sin nπx
nπ
)− (2)
(−cos nπx
n2π2
)]1−1
=
[0 +
2(−1)n
n2π2− 0− 2(−1)n
n2π2
]= 0
N. B. Vyas Fourier Series 2
Example
Step 3. an =1
1
∫ 1
−1f(x) cos
(nπx1
)dx
an =
∫ 1
−12x cos(nπx) dx
=
[2x
(sin nπx
nπ
)− (2)
(−cos nπx
n2π2
)]1−1
=
[0 +
2(−1)n
n2π2
− 0− 2(−1)n
n2π2
]= 0
N. B. Vyas Fourier Series 2
Example
Step 3. an =1
1
∫ 1
−1f(x) cos
(nπx1
)dx
an =
∫ 1
−12x cos(nπx) dx
=
[2x
(sin nπx
nπ
)− (2)
(−cos nπx
n2π2
)]1−1
=
[0 +
2(−1)n
n2π2− 0− 2(−1)n
n2π2
]
= 0
N. B. Vyas Fourier Series 2
Example
Step 3. an =1
1
∫ 1
−1f(x) cos
(nπx1
)dx
an =
∫ 1
−12x cos(nπx) dx
=
[2x
(sin nπx
nπ
)− (2)
(−cos nπx
n2π2
)]1−1
=
[0 +
2(−1)n
n2π2− 0− 2(−1)n
n2π2
]= 0
N. B. Vyas Fourier Series 2
Example
Ex. Find the Fourier series of periodic function
f(x)= −1;−1 < x < 0= 1; 0 < x < 1
p = 2L = 2
N. B. Vyas Fourier Series 2
Example
Ex. Find the Fourier series of periodic function
f(x)= 0;−2 < x < 0= 2; 0 < x < 2
p = 2L = 4
N. B. Vyas Fourier Series 2
Fourier Half Range Series
A function f(x) defined only on the interval of the form0 < x < L.
If f(x) is represented on this interval by a Fourier series ofperiod 2L
Then such Fourier series are known as half range Fourierseries or half range expansions.
Types of Half Range Fourier series
1 Fourier Cosine Series
2 Fourier Sine Series
N. B. Vyas Fourier Series 2
Fourier Half Range Series
A function f(x) defined only on the interval of the form0 < x < L.
If f(x) is represented on this interval by a Fourier series ofperiod 2L
Then such Fourier series are known as half range Fourierseries or half range expansions.
Types of Half Range Fourier series
1 Fourier Cosine Series
2 Fourier Sine Series
N. B. Vyas Fourier Series 2
Fourier Half Range Series
A function f(x) defined only on the interval of the form0 < x < L.
If f(x) is represented on this interval by a Fourier series ofperiod 2L
Then such Fourier series are known as half range Fourierseries or half range expansions.
Types of Half Range Fourier series
1 Fourier Cosine Series
2 Fourier Sine Series
N. B. Vyas Fourier Series 2
Fourier Half Range Series
A function f(x) defined only on the interval of the form0 < x < L.
If f(x) is represented on this interval by a Fourier series ofperiod 2L
Then such Fourier series are known as half range Fourierseries or half range expansions.
Types of Half Range Fourier series
1 Fourier Cosine Series
2 Fourier Sine Series
N. B. Vyas Fourier Series 2
Fourier Half Range Series
A function f(x) defined only on the interval of the form0 < x < L.
If f(x) is represented on this interval by a Fourier series ofperiod 2L
Then such Fourier series are known as half range Fourierseries or half range expansions.
Types of Half Range Fourier series
1 Fourier Cosine Series
2 Fourier Sine Series
N. B. Vyas Fourier Series 2
Fourier Half Range Series
A function f(x) defined only on the interval of the form0 < x < L.
If f(x) is represented on this interval by a Fourier series ofperiod 2L
Then such Fourier series are known as half range Fourierseries or half range expansions.
Types of Half Range Fourier series
1 Fourier Cosine Series
2 Fourier Sine Series
N. B. Vyas Fourier Series 2
Fourier Cosine Series
Let f(x) be piecewise continuous on [o, l].
the Fourier cosine series expansion of f(x) on the half rangeinterval [0, l] is given by
f(x) =ao2
+∞∑n=1
an cos(nπx
l
)where a0 =
2
l
∫ l
0
f(x) dx
an =2
l
∫ l
0
f(x) cos(nπx
l
)dx
N. B. Vyas Fourier Series 2
Fourier Cosine Series
Let f(x) be piecewise continuous on [o, l].
the Fourier cosine series expansion of f(x) on the half rangeinterval [0, l] is given by
f(x) =ao2
+∞∑n=1
an cos(nπx
l
)where a0 =
2
l
∫ l
0
f(x) dx
an =2
l
∫ l
0
f(x) cos(nπx
l
)dx
N. B. Vyas Fourier Series 2
Fourier Cosine Series
Let f(x) be piecewise continuous on [o, l].
the Fourier cosine series expansion of f(x) on the half rangeinterval [0, l] is given by
f(x) =ao2
+∞∑n=1
an cos(nπx
l
)
where a0 =2
l
∫ l
0
f(x) dx
an =2
l
∫ l
0
f(x) cos(nπx
l
)dx
N. B. Vyas Fourier Series 2
Fourier Cosine Series
Let f(x) be piecewise continuous on [o, l].
the Fourier cosine series expansion of f(x) on the half rangeinterval [0, l] is given by
f(x) =ao2
+∞∑n=1
an cos(nπx
l
)where a0 =
2
l
∫ l
0
f(x) dx
an =2
l
∫ l
0
f(x) cos(nπx
l
)dx
N. B. Vyas Fourier Series 2
Fourier Cosine Series
Let f(x) be piecewise continuous on [o, l].
the Fourier cosine series expansion of f(x) on the half rangeinterval [0, l] is given by
f(x) =ao2
+∞∑n=1
an cos(nπx
l
)where a0 =
2
l
∫ l
0
f(x) dx
an =2
l
∫ l
0
f(x) cos(nπx
l
)dx
N. B. Vyas Fourier Series 2
Fourier Sine Series
Let f(x) be piecewise continuous on [o, l].
the Fourier sine series expansion of f(x) on the half rangeinterval [0, l] is given by
f(x) =∞∑n=1
bn sin(nπx
l
)bn =
2
l
∫ l
0
f(x) sin(nπx
l
)dx
N. B. Vyas Fourier Series 2
Fourier Sine Series
Let f(x) be piecewise continuous on [o, l].
the Fourier sine series expansion of f(x) on the half rangeinterval [0, l] is given by
f(x) =∞∑n=1
bn sin(nπx
l
)bn =
2
l
∫ l
0
f(x) sin(nπx
l
)dx
N. B. Vyas Fourier Series 2
Fourier Sine Series
Let f(x) be piecewise continuous on [o, l].
the Fourier sine series expansion of f(x) on the half rangeinterval [0, l] is given by
f(x) =∞∑n=1
bn sin(nπx
l
)
bn =2
l
∫ l
0
f(x) sin(nπx
l
)dx
N. B. Vyas Fourier Series 2
Fourier Sine Series
Let f(x) be piecewise continuous on [o, l].
the Fourier sine series expansion of f(x) on the half rangeinterval [0, l] is given by
f(x) =∞∑n=1
bn sin(nπx
l
)bn =
2
l
∫ l
0
f(x) sin(nπx
l
)dx
N. B. Vyas Fourier Series 2
Example
Ex. Find Fourier cosine and sine series of the functionf(x) = 1 for 0 ≤ x ≤ 2
N. B. Vyas Fourier Series 2
Example
Sol. Here given interval is 0 ≤ x ≤ 2
∴ l = 2
N. B. Vyas Fourier Series 2
Example
Sol. Here given interval is 0 ≤ x ≤ 2
∴ l = 2
N. B. Vyas Fourier Series 2
Example
1 Fourier cosine series
Step 1. f(x) =a02
+∞∑n=1
an cos(nπx
l
)
where a0 =2
l
∫ l
0
f(x)dx
an =2
l
∫ l
0
f(x) cos(nπx
l
)
N. B. Vyas Fourier Series 2
Example
1 Fourier cosine series
Step 1. f(x) =a02
+∞∑n=1
an cos(nπx
l
)where a0 =
2
l
∫ l
0
f(x)dx
an =2
l
∫ l
0
f(x) cos(nπx
l
)
N. B. Vyas Fourier Series 2
Example
1 Fourier cosine series
Step 1. f(x) =a02
+∞∑n=1
an cos(nπx
l
)where a0 =
2
l
∫ l
0
f(x)dx
an =2
l
∫ l
0
f(x) cos(nπx
l
)
N. B. Vyas Fourier Series 2
Example
Step 2. a0 =2
2
∫ 2
0
f(x)dx
=
∫ 2
0
1dx = [x]20 = 2.
N. B. Vyas Fourier Series 2
Example
Step 2. a0 =2
2
∫ 2
0
f(x)dx
=
∫ 2
0
1dx
= [x]20 = 2.
N. B. Vyas Fourier Series 2
Example
Step 2. a0 =2
2
∫ 2
0
f(x)dx
=
∫ 2
0
1dx = [x]20
= 2.
N. B. Vyas Fourier Series 2
Example
Step 2. a0 =2
2
∫ 2
0
f(x)dx
=
∫ 2
0
1dx = [x]20 = 2.
N. B. Vyas Fourier Series 2
Example
Step 3. an =2
2
∫ 2
0
f(x)cos(nπx
2
)dx
=
∫ 2
0
(1) cos(nπx
2
)dx
=
sin(nπx
2
)(nπ
2
)2
0
=
(2
nπ
)(sin (nπ)− sin (0)) = 0
N. B. Vyas Fourier Series 2
Example
Step 3. an =2
2
∫ 2
0
f(x)cos(nπx
2
)dx
=
∫ 2
0
(1) cos(nπx
2
)dx
=
sin(nπx
2
)(nπ
2
)2
0
=
(2
nπ
)(sin (nπ)− sin (0)) = 0
N. B. Vyas Fourier Series 2
Example
Step 3. an =2
2
∫ 2
0
f(x)cos(nπx
2
)dx
=
∫ 2
0
(1) cos(nπx
2
)dx
=
sin(nπx
2
)(nπ
2
)2
0
=
(2
nπ
)(sin (nπ)− sin (0)) = 0
N. B. Vyas Fourier Series 2
Example
Step 3. an =2
2
∫ 2
0
f(x)cos(nπx
2
)dx
=
∫ 2
0
(1) cos(nπx
2
)dx
=
sin(nπx
2
)(nπ
2
)2
0
=
(2
nπ
)(sin (nπ)− sin (0))
= 0
N. B. Vyas Fourier Series 2
Example
Step 3. an =2
2
∫ 2
0
f(x)cos(nπx
2
)dx
=
∫ 2
0
(1) cos(nπx
2
)dx
=
sin(nπx
2
)(nπ
2
)2
0
=
(2
nπ
)(sin (nπ)− sin (0)) = 0
N. B. Vyas Fourier Series 2
Example
∴ Fourier cosine series of f(x) is
f(x) =a02
+∞∑n=1
an cos(nπx
l
)=
2
2+ 0 = 1
N. B. Vyas Fourier Series 2
Example
∴ Fourier cosine series of f(x) is
f(x) =a02
+∞∑n=1
an cos(nπx
l
)
=2
2+ 0 = 1
N. B. Vyas Fourier Series 2
Example
∴ Fourier cosine series of f(x) is
f(x) =a02
+∞∑n=1
an cos(nπx
l
)=
2
2+ 0
= 1
N. B. Vyas Fourier Series 2
Example
∴ Fourier cosine series of f(x) is
f(x) =a02
+∞∑n=1
an cos(nπx
l
)=
2
2+ 0 = 1
N. B. Vyas Fourier Series 2