dr. nirav vyas betagamma functions.pdf
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Beta & Gamma functions
Nirav B. Vyas
Department of MathematicsAtmiya Institute of Technology and Science
Yogidham, Kalavad roadRajkot - 360005 . Gujarat
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Introduction
The Gamma function and Beta functions belong to thecategory of the special transcendental functions and aredened in terms of improper denite integrals.
N. B. Vyas Beta & Gamma functions
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Introduction
The Gamma function and Beta functions belong to thecategory of the special transcendental functions and aredened in terms of improper denite integrals.
These functions are very useful in many areas like asymptoticseries, Riemann-zeta function, number theory, etc. and alsohave many applications in engineering and physics.
N. B. Vyas Beta & Gamma functions
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Introduction
The Gamma function and Beta functions belong to thecategory of the special transcendental functions and aredened in terms of improper denite integrals.
These functions are very useful in many areas like asymptoticseries, Riemann-zeta function, number theory, etc. and alsohave many applications in engineering and physics.The Gamma function was rst introduced by Swiss
mathematician Leonhard Euler
(1707-1783).
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Properties of Gamma function
(1) Γ(n + 1) = nΓn
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Properties of Gamma function
(1) Γ(n + 1) = nΓn(2) Γ(n + 1) = n!, where n is a positive integer
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Properties of Gamma function
(1) Γ(n + 1) = nΓn(2) Γ(n + 1) = n!, where n is a positive integer
(3) Γ(n ) = 2
∞
0e − x
2x 2n − 1dx
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Properties of Gamma function
(1) Γ(n + 1) = nΓn(2) Γ(n + 1) = n!, where n is a positive integer
(3) Γ(n ) = 2
∞
0e − x
2x 2n − 1dx
(4) Γn
t n =
∞
0e − tx x n − 1dx
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Properties of Gamma function
(1) Γ(n + 1) = nΓn(2) Γ(n + 1) = n!, where n is a positive integer
(3) Γ(n ) = 2
∞
0e − x
2x 2n − 1dx
(4) Γn
t n =
∞
0e − tx x n − 1dx
(5) Γ12
= √ π
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Exercise
(1) ∞
−∞
e − k2 x 2 dx
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i
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Exercise
(1) ∞
−∞
e − k2 x 2 dx
(2) ∞
0 e− x 3
dx
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E i
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Exercise
(1) ∞
−∞
e − k2 x 2 dx
(2) ∞
0 e− x 3
dx
(3) 1
0x m log
1x
n
dx
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E i
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Exercise
(1) ∞
−∞
e − k2 x 2 dx
(2) ∞
0 e− x 3
dx
(3) 1
0x m log
1x
n
dx
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B t F ti
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Beta Function
Denition:The Beta function denoted by β (m, n ) or B (m, n ) is dened as
B (m, n ) = 1
0x m − 1(1 − x )
n − 1dx, (m > 0, n > 0)
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Properties of Beta F nction
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Properties of Beta Function
(1) B (m, n ) = B (n, m )
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Properties of Beta Function
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Properties of Beta Function
(1) B (m, n ) = B (n, m )
(2) B (m, n ) = 2 π
2
0sin 2m − 1θ cos 2n − 1θ dθ
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Properties of Beta Function
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Properties of Beta Function
(1) B (m, n ) = B (n, m )
(2) B (m, n ) = 2 π
2
0sin 2m − 1θ cos 2n − 1θ dθ
(3) B (m, n ) = ∞
0
x m − 1
(1 + x)m + ndx
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Exercise
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Exercise
Ex. Prove that
π
2
0sin pθ cos qθ dθ =
1
2β
p + 1
2 ,
q + 1
2
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Exercise
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Exercise
Ex. Prove that
∞
0
x m − 1
(a + bx)m + ndx =
β (m, n )
a n bm
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Relation between Beta and Gamma functions
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Relation between Beta and Gamma functions
β (m, n
) =
Γ(m )Γ( n )
Γ(m + n )
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Exercise
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Exercise
Ex. Prove that
π
2
0
sin pθ cos q θ dθ = 1
2
Γ( p+12 )Γ(q +1
2 )
Γ( p+ q +2
2 )
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Exercise
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Exercise
Ex. Prove that
π
2
0
sin pθ cos q θ dθ = 1
2
Γ( p+12 )Γ(q +1
2 )
Γ( p+ q +2
2 )Ex. Prove that: B (m, n ) = B (m, n + 1) + B (m + 1 , n )
N. B. Vyas Beta & Gamma functions