Solving Euler Integrals Homework: Show B(a,b)

In summary, the given conversation discusses the proof of the identity B(a,b) = \int_0^1{x^{a-1}(1-x)^{b-1}\,dx} = \frac{\Gamma(a)\Gamma(b)}{\Gamma(a+b)} for a > 0 and b > 0 using polar coordinates. The solution involves using the substitution x=u^{2} and applying Fubini's theorem to transform the double integral into a single integral. The identity is then obtained by making the substitution \cos^{2}\varphi=z.
  • #1
cepheid
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Homework Statement



For fun: show that

[tex] B(a,b) = \int_0^1{x^{a-1}(1-x)^{b-1}\,dx} = \frac{\Gamma(a)\Gamma(b)}{\Gamma(a+b)} [/tex]

where [itex] a > 0 [/itex], [itex] b > 0 [/itex]. Hint: start from the product [itex]\Gamma(a)\Gamma(b)[/itex] and switch to polar coordinates. The radial integral is proportional to [itex]\Gamma(a+b)[/itex].

Homework Equations



[tex] \Gamma(a) = \int_0^{\infty}{x^{a-1}e^{-x}\,dx} [/tex]

The Attempt at a Solution



[tex] \Gamma(a)\Gamma(b) = \int_0^{\infty}{x^{a-1}e^{-x}\,dx}\int_0^{\infty}{y^{b-1}e^{-y}\,dy} = \int_0^{\infty}\!\!\int_0^{\infty}{x^{a-1}e^{-x}y^{b-1}e^{-y}\,dxdy}
[/tex]

[tex] x = r\cos\theta, \ y = r\sin\theta, \ \ \ \ dxdy = rdrd\theta [/tex]

[tex] \Gamma(a)\Gamma(b) = \int_0^{2\pi}\!\!\int_0^{\infty}{(r\cos\theta)^{a-1}e^{-r\cos\theta}(r\sin\theta)^{b-1}e^{-r\sin\theta}\,rdrd\theta}
[/tex]

[tex] = \int_0^{2\pi}\!\!\int_0^{\infty}{r^{a-1}r^{b-1}(\cos\theta)^{a-1}(\sin\theta)^{b-1}e^{-r(\cos\theta+\sin\theta)}\,rdrd\theta}
[/tex]

I'm stuck here. I don't know how to sort out the exponential term (which depends on both r and [itex]\theta[/itex]) in order to obtain a separate radial integral.
 
Last edited:
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  • #2
There's a trick here:

[tex] \Gamma (a)=\int_{0}^{\infty} x^{a-1} e^{-x} {} dx [/tex]

Make the substitution [itex] x=u^{2} [/itex] and get

[tex] \Gamma (a)=2\int_{0}^{\infty} u^{2a-1} e^{-u^{2}} {} du [/tex]

Do the same for

[tex] \Gamma (b)=2\int_{0}^{\infty} v^{2b-1} e^{-v^{2}} {} dv [/tex]

Consider the product of the 2 integrals+ Fubini's theorem to get

[tex] \Gamma (a)\Gamma (b)=4\int_{0}^{\infty} \int_{0}^{\infty} u^{2a-1} v^{2v-1} e^{-(u^{2}+v^{2})} {} du {} dv [/tex]

Switch to polar coordinates [itex] (r,\varphi) [/itex] and perform the "r" integration to get

[tex] \Gamma (a)\Gamma (b)=2\Gamma (a+b)\int_{0}^{\pi/2} \left(\cos^{2}\varphi\right)^{\frac{2a-1}{2}} \left(\sin^{2}\varphi\right)^{\frac{2b-1}{2}} \ d\varphi [/tex]

and finally make the substitution [itex] \cos^{2}\varphi=z [/itex]

You'll get the identity easily, just watch the "-" signs and reversing the order of integration.
 
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  • #3
The [itex]\theta[/itex] integral is NOT from 0 to [itex]2\pi[/itex], it is from o to [itex]\pi /2[/itex]. I'm not sure why you are doing that however. The problem does not ask you to evaluate the integrals, just show that the two sides are the same.
 

1. What is an Euler integral?

An Euler integral is a type of mathematical integral that was first studied by Leonhard Euler in the 18th century. It is used to solve certain types of differential equations and is an important tool in the field of calculus.

2. How do you solve an Euler integral?

To solve an Euler integral, you can use a variety of techniques such as substitution, integration by parts, and partial fractions. The specific method used will depend on the form of the integral and the techniques you are familiar with.

3. What is the purpose of showing B(a,b) in the integral?

The B(a,b) in the integral represents the beta function, which is a special type of integral that is closely related to Euler integrals. It is often used as a tool for solving more complex integrals and can help simplify the solution process.

4. Are there any common mistakes when solving Euler integrals?

Yes, some common mistakes when solving Euler integrals include forgetting to apply the chain rule, making errors in algebraic simplification, and using incorrect substitution techniques. It is important to double-check your work and be mindful of these potential errors.

5. Can Euler integrals be used in real-world applications?

Yes, Euler integrals have many real-world applications in fields such as physics, engineering, and economics. They can be used to model and solve various problems involving rates of change and accumulation.

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