Integration by Parts: \int{\sin{(\theta)}*\cos{(\theta)}*d\theta}

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The Integral:
\int{\sin{(\theta)}*\cos{(\theta)}*d\theta}
Attempt to solve by Integration by Parts:
\int{u*dv} = u*v - \int{v*du}
u = \sin{(\theta)}
du = \cos{(\theta)}*d\theta
v = \sin{(\theta)}
dv = \cos{(\theta)}*d\theta
Bringing back to the beginning.
 
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Have you considered using the ##sin(2\theta) = 2 sin(\theta) cos(\theta)## identity or do you need to use parts?

Also what if you add ##udv + vdu## integrals together to be = ## u . v ##?
 
In fact, I wouldn't use the that identity! Since (sin(\theta)'= cos(\theta), the substitution u= sin(\theta) so du= cos(\theta)d\theta gives \int sin(\theta)cos(\theta) d\theta= \int u du= \frac{1}{2}u^2+ C.

But you can do this "by parts" using u= sin(\theta), dv= cos(\theta)d\theta as you suggest. du= cos(\theta)d\theta and v= sin(\theta)d\theta so the integral becomes \int sin(\theta)cos(\theta)d\theta= sin^2(\theta)- \int sin(\theta) cos(\theta) d\theta.

Now, that is NOT "back to the beginning" because we can add \int sin(\theta)cos(\theta) d\theta to both sides to gbet 2 \int sin(\theta)cos(\theta)d\theta= sin^2(\theta) and dividing both sides by 2 gives the previous result.
 
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HallsofIvy has made a good point. Always write down the LHS and the RHS of the equation while integrating by parts when you're dealing with functions which are related to their first few derivatives with a constant (chiefly exponential and trigonometric functions).
 
What HallsOfIvy and PWiz are talking about is using integration by parts and algebraically solving for an integral. Here's an example.
##\int e^x \cos x dx## -- int. by parts, with ##u = e^x, dv = \cos x dx##, so ##du = e^x, v = \sin x##
##= e^x \sin x - \int e^x \sin x dx## -- int. by parts again, with ##u = e^x, dv = -\sin x dx## and ##du = e^x dx, v = \cos x##
##= e^x \sin x + e^x \cos x - \int e^x \cos x dx##

It looks like we've come full circle here, but actually we haven't. The above shows that
##\int e^x \cos x dx = e^x \sin x + e^x \cos x - \int e^x \cos x dx##
Add ##\int e^x \cos x dx## to both sides of the equation above, and solve algebraically for this integral. Of course, you need to add the arbitrary constant in your final answer.
 
You don't need to use integration by parts. Try a simple u-substitution.
 
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