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Trigonometric Representation of the Beta Function 📂Functions

Trigonometric Representation of the Beta Function

Theorem

B(p,q)=20π2(sinθ)2p1(cosθ)2q1dθ B(p,q) = 2 \int_{0}^{{\pi} \over {2}} \left( \sin \theta \right) ^{2p-1} \left( \cos \theta \right) ^{2q-1} d \theta

Description

No matter what kind of mathematics it is, being able to express a function in a different way is a good thing.

Proof

If we substitute from B(p,q)=01tp1(1t)q1dt\displaystyle B(p,q) = \int_{0}^{1} t^{p-1} (1-t)^{q-1} dt to t=sin2θt = \sin^2 \theta, B(p,q)=0π2(sin2θ)p1(1sin2θ)q12sinθcosθdθ B(p,q) = \int_{0}^{{\pi} \over {2}} \left( \sin^2 \theta \right)^{p-1} \left( 1 - \sin^2 \theta \right) ^{q-1} 2 \sin \theta \cos \theta d \theta since 1sin2θ=cos2θ1 - \sin^2 \theta = \cos ^2 \theta, B(p,q)=20π2(sinθ)2p1(cosθ)2q1dθ B(p,q) = 2 \int_{0}^{{\pi} \over {2}} \left( \sin \theta \right)^{2p-1} \left( \cos \theta \right) ^{2q-1} d \theta

Corollary

In particular, if we substitute again with sinθ=t\sin \theta = t, we obtain a lemma to derive Legendre’s duplication formula. B(p,q)=201t2p1(1t2)q1dt B(p,q) = 2 \int_{0}^{1} t^{2p-1} \left( 1 - t^2 \right)^{q-1} dt

See Also