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

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SUMMARY

The discussion focuses on proving the identity for the Beta function, specifically B(a,b) = ∫₀¹ x^(a-1)(1-x)^(b-1) dx = Γ(a)Γ(b)/Γ(a+b) for a > 0 and b > 0. The solution involves using the properties of the Gamma function and switching to polar coordinates to simplify the integrals. The key steps include substituting x = u² and y = v², applying Fubini's theorem, and performing the radial integral to ultimately demonstrate the equality of both sides of the equation.

PREREQUISITES
  • Understanding of Gamma functions, specifically Γ(a) = ∫₀^∞ x^(a-1)e^(-x) dx
  • Knowledge of polar coordinates and their application in double integrals
  • Familiarity with Fubini's theorem for changing the order of integration
  • Basic calculus skills, particularly integration techniques
NEXT STEPS
  • Study the properties and applications of the Gamma function in depth
  • Learn about polar coordinates and their use in evaluating double integrals
  • Explore Fubini's theorem and its implications in multivariable calculus
  • Practice solving Beta and Gamma function identities through various examples
USEFUL FOR

Students and mathematicians interested in advanced calculus, particularly those studying integral transforms and special functions. This discussion is especially beneficial for those tackling problems related to the Beta and Gamma functions.

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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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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.
 
Last edited:
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.
 

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