Evaluate
∫ 0 1 x 1 0 0 4 ( 1 − x 2 0 1 0 ) 1 0 0 4 d x 2 2 0 1 0 ∫ 0 1 x 1 0 0 4 ( 1 − x ) 1 0 0 4 d x .
You may try its simpler version first WOWSOME
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My method might be long... i first converted lower integral into a form where gamma formula could be used.. then i applied gamma formula up and down and cancelled all terms and released the several 2s to cancel the already present 2^(2010) to leave 4.
Is there a shorter way?
The problem asks us to compute ∫ 0 1 x 1 0 0 4 ( 1 − x 2 0 1 0 ) 1 0 0 4 d x 2 2 0 1 0 ∫ 0 1 x 1 0 0 4 ( 1 − x ) 1 0 0 4 d x . More generally, we compute ∫ 0 1 x n − 1 ( 1 − x 2 n ) n − 1 d x 2 2 n ∫ 0 1 x n − 1 ( 1 − x ) n − 1 d x , where n is a positive integer.
By the Beta function , ∫ 0 1 x n − 1 ( 1 − x ) n − 1 d x = ( 2 n − 1 ) ! ( n − 1 ) ! ⋅ ( n − 1 ) ! .
For the denominator, let y = x 2 n . Then x = y 1 / ( 2 n ) , and d x = 2 n 1 y 1 / ( 2 n ) − 1 d y , so ∫ 0 1 x n − 1 ( 1 − x 2 n ) n − 1 d x = ∫ 0 1 y ( n − 1 ) / ( 2 n ) ( 1 − y ) n − 1 ⋅ 2 n 1 y 1 / ( 2 n ) − 1 d y = 2 n 1 ∫ 0 1 y − 1 / 2 ( 1 − y ) n − 1 d y .
Again by the Beta function, this is equal to 2 n 1 ⋅ Γ ( n + 2 1 ) Γ ( 2 1 ) ⋅ ( n − 1 ) ! . From the identity Γ ( t + 1 ) = t Γ ( t ) , Γ ( n + 2 1 ) Γ ( 2 1 ) ⋅ ( n − 1 ) ! = ( n − 1 ) ! ⋅ Γ ( 2 3 ) Γ ( 2 1 ) ⋅ Γ ( 2 5 ) Γ ( 2 3 ) ⋯ Γ ( n + 2 1 ) Γ ( n − 2 1 ) = ( n − 1 ) ! ⋅ 1 2 ⋅ 3 2 ⋯ 2 n − 1 2 = ( n − 1 ) ! ⋅ 1 ⋅ 3 ⋅ 5 ⋯ ( 2 n − 1 ) 2 n = ( n − 1 ) ! ⋅ 1 ⋅ 2 ⋯ ( 2 n ) 2 n ⋅ 2 ⋅ 4 ⋯ ( 2 n ) = ( n − 1 ) ! ⋅ ( 2 n ) ! 2 n ⋅ 2 n ⋅ n ! .
Therefore, ∫ 0 1 x n − 1 ( 1 − x 2 n ) n − 1 d x 2 2 n ∫ 0 1 x n − 1 ( 1 − x ) n − 1 d x = 2 n 1 ⋅ ( 2 n ) ! 2 2 n ⋅ ( n − 1 ) ! ⋅ n ! ( 2 n − 1 ) ! 2 2 n ⋅ ( n − 1 ) ! ⋅ ( n − 1 ) ! = n ! ⋅ ( 2 n − 1 ) ! 2 n ⋅ ( n − 1 ) ! ⋅ ( 2 n ) ! = 4 n .
For n = 1 0 0 5 , this is 4 ⋅ 1 0 0 5 = 4 0 2 0 .
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Thanks. I have updated the answer accordingly.
I don't think so there is any short method for this question. I too have solved this using gamma formula.
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Can you review Jon's comment and let me know if anything is wrong with it?
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S o r r y f o r t h e i n c o n v e n i e n c e , i t s a n s w e r s h o u l d b e 4 0 2 0 . I ′ v e a n a n o t h e r s o l u t i o n f o r t h i s q u e s t i o n . S o l v i n g n u m e r a t o r : L e t x = s i n 2 θ d x = 2 s i n θ . c o s θ . d θ t h e r e f o r e , n u m e r a t o r t u r n s o u t t o b e : 2 2 0 1 1 ∫ 0 2 π s i n 2 0 0 9 θ . c o s 2 0 0 9 θ . d θ 4 ∫ 0 2 π s i n 2 0 0 9 2 θ . d θ . . . . . . . . . . . ( 1 ) N o w s o l v i n g d e n o m i n a t o r : L e t x 1 0 0 5 = s i n θ 1 0 0 5 x 1 0 0 4 . d x = c o s θ . d θ x 1 0 0 4 . d x = 1 0 0 5 c o s θ . d θ t h e r e f o r e , d e n o m i n a t o r t u r n s o u t t o b e 1 0 0 5 1 ∫ 0 2 π c o s 2 0 0 9 θ . d θ . . . . . . . . ( 2 ) N o w s u b s t i t u t i n g v a l u e s : ∫ 0 2 π c o s 2 0 0 9 θ . d θ 4 0 2 0 ∫ 0 2 π s i n 2 0 0 9 2 θ . d θ = 4 0 2 0