Solving Integrals by Trigonometric substitution/Introduction

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A Note

The prerequisites for this book are just as one would think, trigonometry, and some Calculus. As for the amount of Calculus, when most classes introduce the general method of substitution would be a good time; but really only the base knowledge of an integral is needed.

Introduction

The main purpose of this text is to explain a certain method of solving a large class of integral calculus problems, affectionally known as trigonometric substitution.

One of the reasons why trigonometry has such a bad reputation is probably because there are a lot of trigonometric identities, and they seem to have no apparent immediate application. While trigonometric substitution may or may not be considered as an answer to the latter, it certainly puts the former in good use.

The idea behind the trigonometric substitution is actually quite simple: to reduce complicated expressions involving square roots to polynomials of standard trigonometric functions. Integrals involving polynomial expressions (albeit in trigonometric functions) are much easier to solve than the ones containing square roots.

Let us demonstrate this idea in practice: consider the expression 1x2. Probably the most basic trigonometric identity is sin2(θ)+cos2(θ)=1 for an arbitrary angle θ. If we replace x in this expression by sin(θ), with the help of this trigonometric identity we see

1x2=1sin2(θ)=cos2(θ)=cos(θ)

Note that therefore θ=arcsin(x) since we replaced x2 with sin2(θ) We would like to mention that technically one should write the absolute value of cos(θ), in other words |cos(θ)| as our final answer since A2=|A| for all possible A. But as long as we are careful about the domain of all possible x and how cos(θ) is used in the final computation, this simplification does not constitute a problem. However, we cannot directly interchange the simple expression cos(θ) with the complicated 1x2 wherever it may appear, remembering that we did not take into consideration the fact that dx=cos(θ)dθ and the dθ is necessary for the integral. Thus, if we see an integral of the form

1x2dx

we can rewrite it as

cos(θ)d(sin(θ))=cos2(θ)dθ

by using the fact that d(sin(θ)=cos(θ)dθ and the fact that dx=cos(θ)dθ. Since cos2(θ)=.5(1+cos(2θ)) our original integral reduces to: .5dθ + .5cos(2θ)

This integral = θ/2 + sin(2θ) or θ/2 + 2sin(θ)cos(θ)

We now know the integral; however, this is in terms of θ and not in terms of x, how it was given. To rewrite it in x, we simply plug in the values we already know.

sin(θ)=x and dx=cos(θ)dθ and θ=arcsin(x)
By using these substitutions we find θ/2 + 2sin(θ)cos(θ) = arcsin(x)/2 + x1x2

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