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@Parth Lohomi you are super intelligent, you know so much of calculus just at the age of 14.
Very smart approach!
Mine involved the use of Raabe's Formula .
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POST POST POST POST!!
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@Pi Han Goh even parth used Raabe's Formula.
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@Aditya Kumar – yes parth have proved it
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@Hasan Kassim – @Hasan Kassim can u help me by telling me some books from where I can learn such concepts. I'm new to these concepts.
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@Aditya Kumar – Actually, I don't have a book . I learn such topics and ideas from exploring different calculus problems and sites... Such as wolfram alpha and wikipedia...
For example, I didn't know the Raabe's formula until I solved this problem in a very long method :)
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@Hasan Kassim – That's what I'm currently doing! I hope I reach upto your level 1 day.
@Aditya Kumar – Sorry I don't understand all these alien symbols. So I don't know what you guys are talking about.
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@Pi Han Goh – Even I'm not so good at questions of this level. It took me 3 days to solve it. I'm thinking of posting few important basic problems which can be used to solve these amazing problems. Should I post them??
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@Aditya Kumar – Yes please!!! It's great that the community can solve more problems. Plus, I haven't seen much calculus problem that doesn't give me headache!
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@Pi Han Goh – Haha sure. Today I'll post at least 2 problems.
∗ ∗ ⟹ We are using the result π 1 ∫ 0 π lo g sin θ d θ = − lo g 2
A+B+C+D=26 not 25
Woah! generaliztion is a key to tough problems of calculus!
By Raabe's Formula, we get: ∫ 0 1 ln Γ ( x + α ) d x = 2 1 ln 2 π + α lo g α − α ; α ≥ 0 ,
This is a well known identity: ∫ 0 1 x α ln n x d x = ( α + 1 ) n + 1 ( − 1 ) n n ! , for n = 0 , 1 , 2 , …
The inner integral comes out to be: ∫ 0 1 ln Γ ( x + y 3 ) d x = 2 1 ln 2 π + 3 y 3 ln y − y 3
Therefore on evaluating the outer integral, we get: ∫ 0 1 ∫ 0 1 ln Γ ( x + y 3 ) d x d y = ∫ 0 1 ( 2 1 ln 2 π + 3 y 3 ln y − y 3 ) d y = 2 1 ln 2 π − 4 2 3 − 4 1 = 2 1 ln 2 π − 1 6 7 .
@Pi Han Goh this is another way by Raabe's formula.
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Hahaha. Where do u get such cool gifs from?
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If you have another approach then do post it .
Let f ( u ) = ∫ 0 1 lo g Γ ( z + u ) d z
f ′ ( u ) = ∫ 0 1 Γ ( z + u ) Γ ′ ( z + u ) d z = [ lo g Γ ( z + u ) ] 0 1 = lo g Γ ( u ) Γ ( u + 1 ) = lo g u
Integrating this gives us f ( u ) = f ( 0 ) + u lo g u − u .So
f ( 0 ) = ∫ 0 1 lo g Γ ( z ) d z = 2 1 ∫ 0 1 lo g ( Γ ( z ) Γ ( 1 − z ) ) d z = 2 1 ∫ 0 1 lo g sin π z π d z = 2 1 ( lo g π − π 1 ∫ 0 π lo g sin θ d θ ) = 2 1 lo g ( 2 π ) ∗ ∗
This gives us
f ( u ) = 2 1 lo g ( 2 π ) + u lo g u − u
so,
I = ∫ 0 1 f ( y 3 ) d y = = = ∫ 0 1 ( 2 1 lo g ( 2 π ) + y 3 lo g ( y 3 ) − y 3 ) d y 2 1 lo g ( 2 π ) + [ 1 6 3 y 4 ( lo g ( y 4 ) − 1 ) − 4 1 y 4 ] 0 1 2 1 lo g ( 2 π ) − 1 6 7