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单词 ALectureOnTrigonometricIntegralsAndTrigonometricSubstitution
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A lecture on trigonometric integrals and trigonometric substitution


1 Trigonometric Integrals

First, we must recall a few trigonometric identities:

sin2x+cos2x=1(1)
sec2x=1+tan2x(2)
sin2x=1-cos(2x)2(3)
cos2x=1+cos(2x)2(4)
sin(2x)=2sinxcosx(5)
cos(2x)=cos2x-sin2x.(6)

The most usual integralsDlmfPlanetmath which involve trigonometric functionsDlmfMathworldPlanetmath canbe solved using the identities above.

Example 1.1.

sinxdx=-cosx+C and cosxdx=sinx+C areimmediate integrals.

Example 1.2.

For sin2xdx,cos2xdx we use formulas (3) and(4) respectively, e.g.

sin2xdx=1-cos(2x)2𝑑x=12(1-cos(2x))𝑑x=12(x-sin(2x)2)+C.
Example 1.3.

For integrals of the form cosmxsinxdxor sinmxcosxdx we use substitution with u=cosxor u=sinx respectively, e.g.

cos2xsinxdx=-u2du=-u33+C=-cos3x3+C.[u=cosx,du=-sinxdx]

In the following examples, we use equations (1) in the formssin2x=1-cos2x or cos2x=1-sin2x to transform theintegral into one of the type described in Example 1.3.

Example 1.4.
sin3xdx=sin2xsinxdx=(1-cos2x)sinxdx
=sinxdx-cos2xsinxdx
=-cosx+cos3x3+C.

Similarly one can solve cos3xdx.

Example 1.5.
cos3xsin2xdx=cos2xcosxsin2xdx=(1-sin2x)cosxsin2xdx
=cosxsin2xdx-cosxsin4xdx
=sin3x3-sin5x5+C.
Example 1.6.

In order to solve cos5xsin3xdx we express it firstas cos5xsin2xsinx=cos5x(1-cos2x)sinxdx and then proceed as in the previous example.

One can use similar tricks to solve integrals which involveproducts of powers of secx and tanx, by using Equation(2). Also, recall that the derivative of tanx is sec2xwhile the derivative of secx is secxtanx.

Example 1.7.
tan5xsec4xdx=tan5xsec2xsec2xdx=tan5x(1+tan2x)sec2xdx
=tan5xsec2xdx+tan7xsec2xdx
=tan6x6+tan8x8+C.
Example 1.8.
tan3xsec4xdx=tanxtan2xsec4xdx=tanx(sec2x-1)sec4xdx
=tanxsecxsec5xdx-tanxsecxsec3xdx
=sec6x6-sec4x4+C.

2 Trigonometric Substitutions

One can easily deduce that 011-x2𝑑x has valueπ4. Why? Simply because the graph of the functionMathworldPlanetmathy=1-x2 is half a circumference of radius r=1 (becauseif you square both sides of y=1-x2 you obtainx2+y2=1 which is the equation of a circle or radius r=1).Therefore, the area under the graph is a quarter of the area of acircle.

How does one compute 011-x2𝑑x without using thegeometry of the problem? This is the prototype of integral where atrigonometric substitution will work very nicely. Notice thatneither substitution nor integration by parts will workappropriately.

Example 2.1.

Suppose we want to solve 011-x2𝑑x with analyticmethods. We will use a substitution x=sinθ (so θwill be our new variable of integration), because, as we know fromEquation (1), 1-x2=1-sin2θ=cosθ,thus getting rid of the pesky square root. Notice thatdx=cosθdθ. We also need to find the new limits ofintegration with respect to the new variable of integration,namely θ. When x=0=sinθ we must have θ=0.Similarly, when x=1=sinθ one has θ=π/2. We arenow ready to integrate:

011-x2𝑑x=0π/2(cosθ)cosθdθ=0π/2cos2θdθ
=0π/21+cos(2θ)2𝑑θ=12(θ+sin(2θ)2)0π/2=π/4.

Notice that we made use of Equation (4) in the second line.

Example 2.2.

Similarly, one can solve 0rr2-x2𝑑x by using asubstitution x=rsinθ. Indeed,r2-x2=r2-r2sin2θ=rcosθ anddx=rcosθdθ. The limits of integration with respectto θ are again θ=0 to θ=π/2 (check this!).Thus:

0rr2-x2𝑑x=0π/2r2(cosθ)cosθdθ=r20π/2cos2θdθ
=r20π/21+cos(2θ)2𝑑θ=r22(θ+sin(2θ)2)0π/2=r2π/4.

Thus, we have proved that a quarter of a circle of radius r hasarea r2π/4 which implies that the area of such a circle isπr2, as usual.

The trigonometric substitutions usually work whenexpressions like r2-x2, r2+x2,x2-r2 appear in the integral at hand, for some realnumber r. Here is a table of the suggested change of variablesin each particular case:

Remark 2.3.

The above are “suggested” substitutions, they may not be themost ideal choice! For example, for the integral 2x1-x2𝑑x, the change u=1-x2 will work much better thanx=sinθ.

Example 2.4.

We would like to find the value of

221x3x2-1𝑑x.

Since neither a u-substitution nor integration by parts seemappropriate, we try x=secθ, dx=secθtanθdθ. When x=2=secθ one has θ=π/4while x=2 implies θ=π/3. Hence:

221x3x2-1𝑑x=π/4π/3secθtanθsec3θtanθ𝑑θ=π/4π/31sec2θ𝑑θ=π/4π/3cos2θdθ

and the last integral is easy to compute using Equation (4).

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更新时间:2025/5/4 17:03:22