Aller au contenu principal

Trigonometric substitution


Trigonometric substitution


In mathematics, a trigonometric substitution replaces a trigonometric function for another expression. In calculus, trigonometric substitutions are a technique for evaluating integrals. In this case, an expression involving a radical function is replaced with a trigonometric one. Trigonometric identities may help simplify the answer. Like other methods of integration by substitution, when evaluating a definite integral, it may be simpler to completely deduce the antiderivative before applying the boundaries of integration.

Case I: Integrands containing a2x2

Let x = a sin θ , {\displaystyle x=a\sin \theta ,} and use the identity 1 sin 2 θ = cos 2 θ . {\displaystyle 1-\sin ^{2}\theta =\cos ^{2}\theta .}

Examples of Case I

Example 1

In the integral

we may use

Then,

The above step requires that a > 0 {\displaystyle a>0} and cos θ > 0. {\displaystyle \cos \theta >0.} We can choose a {\displaystyle a} to be the principal root of a 2 , {\displaystyle a^{2},} and impose the restriction π / 2 < θ < π / 2 {\displaystyle -\pi /2<\theta <\pi /2} by using the inverse sine function.

For a definite integral, one must figure out how the bounds of integration change. For example, as x {\displaystyle x} goes from 0 {\displaystyle 0} to a / 2 , {\displaystyle a/2,} then sin θ {\displaystyle \sin \theta } goes from 0 {\displaystyle 0} to 1 / 2 , {\displaystyle 1/2,} so θ {\displaystyle \theta } goes from 0 {\displaystyle 0} to π / 6. {\displaystyle \pi /6.} Then,

Some care is needed when picking the bounds. Because integration above requires that π / 2 < θ < π / 2 {\displaystyle -\pi /2<\theta <\pi /2} , θ {\displaystyle \theta } can only go from 0 {\displaystyle 0} to π / 6. {\displaystyle \pi /6.} Neglecting this restriction, one might have picked θ {\displaystyle \theta } to go from π {\displaystyle \pi } to 5 π / 6 , {\displaystyle 5\pi /6,} which would have resulted in the negative of the actual value.

Alternatively, fully evaluate the indefinite integrals before applying the boundary conditions. In that case, the antiderivative gives

as before.

Example 2

The integral

may be evaluated by letting x = a sin θ , d x = a cos θ d θ , θ = arcsin x a , {\textstyle x=a\sin \theta ,\,dx=a\cos \theta \,d\theta ,\,\theta =\arcsin {\dfrac {x}{a}},} where a > 0 {\displaystyle a>0} so that a 2 = a , {\textstyle {\sqrt {a^{2}}}=a,} and π / 2 θ π / 2 {\textstyle -\pi /2\leq \theta \leq \pi /2} by the range of arcsine, so that cos θ 0 {\displaystyle \cos \theta \geq 0} and cos 2 θ = cos θ . {\textstyle {\sqrt {\cos ^{2}\theta }}=\cos \theta .}

Then,

For a definite integral, the bounds change once the substitution is performed and are determined using the equation θ = arcsin x a , {\textstyle \theta =\arcsin {\dfrac {x}{a}},} with values in the range π / 2 θ π / 2. {\textstyle -\pi /2\leq \theta \leq \pi /2.} Alternatively, apply the boundary terms directly to the formula for the antiderivative.

For example, the definite integral

may be evaluated by substituting x = 2 sin θ , d x = 2 cos θ d θ , {\displaystyle x=2\sin \theta ,\,dx=2\cos \theta \,d\theta ,} with the bounds determined using θ = arcsin x 2 . {\textstyle \theta =\arcsin {\dfrac {x}{2}}.}

Because arcsin ( 1 / 2 ) = π / 6 {\displaystyle \arcsin(1/{2})=\pi /6} and arcsin ( 1 / 2 ) = π / 6 , {\displaystyle \arcsin(-1/2)=-\pi /6,}

On the other hand, direct application of the boundary terms to the previously obtained formula for the antiderivative yields

as before.

Case II: Integrands containing a2 + x2

Let x = a tan θ , {\displaystyle x=a\tan \theta ,} and use the identity 1 + tan 2 θ = sec 2 θ . {\displaystyle 1+\tan ^{2}\theta =\sec ^{2}\theta .}

Examples of Case II

Example 1

In the integral

we may write

so that the integral becomes

provided a 0. {\displaystyle a\neq 0.}

For a definite integral, the bounds change once the substitution is performed and are determined using the equation θ = arctan x a , {\displaystyle \theta =\arctan {\frac {x}{a}},} with values in the range π 2 < θ < π 2 . {\displaystyle -{\frac {\pi }{2}}<\theta <{\frac {\pi }{2}}.} Alternatively, apply the boundary terms directly to the formula for the antiderivative.

For example, the definite integral

may be evaluated by substituting x = tan θ , d x = sec 2 θ d θ , {\displaystyle x=\tan \theta ,\,dx=\sec ^{2}\theta \,d\theta ,} with the bounds determined using θ = arctan x . {\displaystyle \theta =\arctan x.}

Since arctan 0 = 0 {\displaystyle \arctan 0=0} and arctan 1 = π / 4 , {\displaystyle \arctan 1=\pi /4,}

Meanwhile, direct application of the boundary terms to the formula for the antiderivative yields

same as before.

Example 2

The integral

may be evaluated by letting x = a tan θ , d x = a sec 2 θ d θ , θ = arctan x a , {\displaystyle x=a\tan \theta ,\,dx=a\sec ^{2}\theta \,d\theta ,\,\theta =\arctan {\frac {x}{a}},}

where a > 0 {\displaystyle a>0} so that a 2 = a , {\displaystyle {\sqrt {a^{2}}}=a,} and π 2 < θ < π 2 {\displaystyle -{\frac {\pi }{2}}<\theta <{\frac {\pi }{2}}} by the range of arctangent, so that sec θ > 0 {\displaystyle \sec \theta >0} and sec 2 θ = sec θ . {\displaystyle {\sqrt {\sec ^{2}\theta }}=\sec \theta .}

Then,

The integral of secant cubed may be evaluated using integration by parts. As a result,

Case III: Integrands containing x2a2

Let x = a sec θ , {\displaystyle x=a\sec \theta ,} and use the identity sec 2 θ 1 = tan 2 θ . {\displaystyle \sec ^{2}\theta -1=\tan ^{2}\theta .}

Examples of Case III

Integrals such as

can also be evaluated by partial fractions rather than trigonometric substitutions. However, the integral

cannot. In this case, an appropriate substitution is:

where a > 0 {\displaystyle a>0} so that a 2 = a , {\displaystyle {\sqrt {a^{2}}}=a,} and 0 θ < π 2 {\displaystyle 0\leq \theta <{\frac {\pi }{2}}} by assuming x > 0 , {\displaystyle x>0,} so that tan θ 0 {\displaystyle \tan \theta \geq 0} and tan 2 θ = tan θ . {\displaystyle {\sqrt {\tan ^{2}\theta }}=\tan \theta .}

Then,

One may evaluate the integral of the secant function by multiplying the numerator and denominator by ( sec θ + tan θ ) {\displaystyle (\sec \theta +\tan \theta )} and the integral of secant cubed by parts. As a result,

When π 2 < θ π , {\displaystyle {\frac {\pi }{2}}<\theta \leq \pi ,} which happens when x < 0 {\displaystyle x<0} given the range of arcsecant, tan θ 0 , {\displaystyle \tan \theta \leq 0,} meaning tan 2 θ = tan θ {\displaystyle {\sqrt {\tan ^{2}\theta }}=-\tan \theta } instead in that case.

Substitutions that eliminate trigonometric functions

Substitution can be used to remove trigonometric functions.

For instance,

The last substitution is known as the Weierstrass substitution, which makes use of tangent half-angle formulas.

For example,

Hyperbolic substitution

Substitutions of hyperbolic functions can also be used to simplify integrals.

For example, to integrate 1 / a 2 + x 2 {\displaystyle 1/{\sqrt {a^{2}+x^{2}}}} , introduce the substitution x = a sinh u {\displaystyle x=a\sinh {u}} (and hence d x = a cosh u d u {\displaystyle dx=a\cosh u\,du} ), then use the identity cosh 2 ( x ) sinh 2 ( x ) = 1 {\displaystyle \cosh ^{2}(x)-\sinh ^{2}(x)=1} to find:

If desired, this result may be further transformed using other identities, such as using the relation sinh 1 z = arsinh z = ln ( z + z 2 + 1 ) {\displaystyle \sinh ^{-1}{z}=\operatorname {arsinh} {z}=\ln(z+{\sqrt {z^{2}+1}})} :

See also

  • Integration by substitution
  • Weierstrass substitution
  • Euler substitution

References



Text submitted to CC-BY-SA license. Source: Trigonometric substitution by Wikipedia (Historical)