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Calculus Level 5

0 x 2 ln ( 2 x ) e x d x = ln a + b c γ \large \int _{ 0 }^{ \infty }{ \dfrac { { x }^{ 2 }\ln { (2x) } }{ { e }^{ x } } \, dx } =\ln { a } +b-c\gamma

If the above equation holds true for positive integers a , b a,b and c c , where γ \gamma denotes the Euler-Mascheroni constant , find a + b + c a+b+c .


The answer is 9.

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3 solutions

Mark Hennings
Jun 7, 2017

The integral is Γ ( 3 ) ln 2 + Γ ( 3 ) = Γ ( 3 ) [ ln 2 + ψ ( 3 ) ] = 2 ln 2 + 3 2 γ = ln 4 + 3 2 γ \Gamma(3)\ln 2 + \Gamma'(3) \; = \; \Gamma(3)\big[\ln2 + \psi(3)\big] \; = \; 2\ln2 + 3 - 2\gamma \; = \; \ln4 + 3 - 2\gamma making the answer 4 + 3 + 2 = 9 4+3+2=\boxed{9} .

First Last
May 12, 2016

Log rule! ln 2 × 0 x 2 e x d x + 0 x 2 ln ( x ) e x d x \displaystyle\ln 2 \times \int_{0}^{\infty}\frac{x^2}{e^x}dx + \int_{0}^{\infty}\frac{x^2\ln(x)}{e^x}dx

ln 2 × 0 x 2 e x d x = ln ( 4 ) \displaystyle\ln 2 \times \int_{0}^{\infty}\frac{x^2}{e^x}dx = \ln(4)

The second integral is more interesting:

0 x 2 ln ( x ) e x d x = x 2 2 x 2 e x ln x 0 + 0 x + 2 e x d x + 2 x e x d x = \displaystyle\int_{0}^{\infty}\frac{x^2\ln(x)}{e^x}dx = \frac{-x^2-2x-2}{e^x}\ln x |_0^{\infty} + \int_{0}^{\infty}\frac{x+2}{e^x}dx + \frac{2}{x e^x}dx = , by integration by parts.

2 lim x 0 ( ln x E i ( x ) ) + 3 = 2 γ + 3 \displaystyle 2 \lim_{x\to 0}( \ln x - Ei(x)) + 3 = -2\gamma + 3

0 x 2 ln ( 2 x ) e x d x = ln 4 + 3 2 γ \displaystyle\int_{0}^{\infty}\frac{x^2\ln(2x)}{e^x}dx = \boxed{\ln{4} + 3 - 2\gamma}

Help me out!!! l e t I = 0 x 2 e x log a x d x d I d a = 0 x 2 e x × a a x d x d I d a = 0 x e x d x d I d a = 1 d I = d a I = a + c I = 2 + c let\quad I=\int _{ 0 }^{ \infty }{ \frac { { x }^{ 2 } }{ { e }^{ x } } } \log { ax } dx\\ \frac { dI }{ da } =\int _{ 0 }^{ \infty }{ \frac { { x }^{ 2 } }{ { e }^{ x } } } \times \frac { a }{ ax } dx\\ \frac { dI }{ da } =\int _{ 0 }^{ \infty }{ \frac { x }{ { e }^{ x } } } dx\\ \frac { dI }{ da } =\quad 1\\ \quad dI\quad =\quad da\\ I\quad =\quad a\quad +\quad c\\ I\quad =\quad 2\quad +\quad c what shall I do after this?? please help!!

@Calvin Lin and others..please see to it

Righved K - 5 years, 1 month ago

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What you've done is define I I as a constant which it is not. When you differentiate I I with respect to a a , then integrate later, I I is still a function of a a .

Your final 2 statements should be: I ( a ) = a + c , I ( 2 ) = 2 + c \displaystyle I(a) = a + c,\quad I(2) = 2 + c

Because there is no easy a a value to plug in originally to get a constant, there is no use for Leibniz rule here. Plugging in anything greater than zero for a would result in the same process to find c c as it would to actually evaluate the integral in the first place. Here is a good video I found explaining Leibniz rule: https://goo.gl/YfwbFP

First Last - 5 years, 1 month ago

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I(the integral) would definitely be a constant value(since it is a definite integral),Moreover the statements that I(me :P) have written are valid..I got through the video(you are right, the constant is difficult to be found) but I as I have approached,there can be a way to solve it, isn't it?..please others and especially @Calvin Lin ..please see to it:)

Righved K - 5 years, 1 month ago

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@Righved K Like I said, you need to find an a a to plug into I ( a ) I(a) originally to get a simple result to later computer c c . This can't be done in this case so finding this a a would be equivalent to solving the specific integral. So there is no use for Leibniz rule.

When I said constant, I meant your "function", I I , which should be I ( a ) I(a) .

First Last - 5 years, 1 month ago

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@First Last Got you. Thank-you so much!:D

Righved K - 5 years, 1 month ago

  1. As pointed out by Jasper, we're looking at the function I ( a ) I(a) . In particular, we are differentiating with respect to a a .
  2. In your second line, what is the value of d log a x d a \frac{ d \log ax} { da} ? Hint: It is not a a x \frac{a}{ax} .
  3. After you fix that step, as pointed out by Jasper, you need to determine the value of c c . This is where most of the work is involved, as seem in the "the second integral is more interesting" comment of the solution. I currently do not see an easy way for Righved's solution to proceed without explicitly performing the integral (but I could be wrong).

Calvin Lin Staff - 5 years, 1 month ago

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Thanks @Calvin Lin, yes I am sorry(I made a school boy error) , it would be 1/a and yes you are right, even I too couldn't find any easy path to proceed in my solution. I could only work out for the ln4 part of the solution :(

Righved K - 5 years, 1 month ago

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@Righved K Right, so we arrived at I ( a ) = 2 ln a + I ( 1 ) I(a) = 2\ln a + I(1) , which could be obtained directly since x 2 e x = 2 \int \frac{ x^2}{e^x} = 2 .

Having said that, don't be discouraged. Differentiating through the integral is a useful approach where we already know the value at a given point and want to extend out along the family​ of curves.

Calvin Lin Staff - 5 years, 1 month ago

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@Calvin Lin @Calvin Lin ..thankyou so much and please edit your reply ( the value of integral would be 2) cheers!!!....thank you so much once again!!!

Righved K - 5 years, 1 month ago
Guilherme Niedu
Jun 1, 2017

I = 0 x 2 ln ( 2 x ) e x d x I = \large \displaystyle \int_0^{\infty} x^2 \ln(2x) e^{-x} dx

Integrating by parts:

I = [ e x x 2 ln ( 2 x ) ] 0 + 0 [ x + 2 x ln ( 2 x ) ] e x d x \large \displaystyle I = - \left [ e^{-x} x^2 \ln(2x) \right ] \Bigg |_0^{\infty} + \int_0^{\infty} \left [ x + 2x \ln(2x) \right ] e^{-x} dx

I = 0 [ x + 2 x ln ( 2 x ) ] e x d x \large \displaystyle I = \int_0^{\infty} \left [ x + 2x \ln(2x) \right ] e^{-x} dx

Integrating by parts again:

I = [ e x ( x + 2 x ln ( 2 x ) ] 0 + 0 [ 1 + 2 ln ( 2 x ) + 2 ] e x d x \large \displaystyle I = - \left [ e^{-x} ( x+ 2x\ln(2x) \right ] \Bigg |_0^{\infty} + \int_0^{\infty} \left [ 1 + 2 \ln(2x) + 2 \right ] e^{-x} dx

I = 0 3 e x d x + 2 0 e x ln ( 2 x ) d x \large \displaystyle I = \int_0^{\infty} 3 e^{-x} dx + 2 \int_0^{\infty} e^{-x} \ln(2x) dx

I = 3 + 2 [ 0 e x ln ( 2 ) + 0 e x ln ( x ) d x ] \large \displaystyle I = 3 + 2 \left[\int_0^{\infty} e^{-x} \ln(2) + \int_0^{\infty} e^{-x} \ln(x)dx \right ]

I = 3 + 2 ln ( 2 ) + 2 0 e x ln ( x ) d x \large \displaystyle I = 3 + 2\ln(2) + 2\int_0^{\infty} e^{-x} \ln(x)dx

Since 0 e x ln ( x ) d x = γ \int_0^{\infty} e^{-x} \ln(x)dx = -\gamma :

I = ln ( 4 ) + 3 2 γ \color{#20A900} \boxed{\large \displaystyle I = \ln(4) + 3 -2\gamma }

Thus:

a = 4 , b = 3 , c = 2 , a + b + c = 9 \color{#3D99F6} \large \displaystyle a=4, b=3, c=2, \boxed{\large \displaystyle a+b+c=9}

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