Trigonometric substitution

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Template:Short description Template:Trigonometry Script error: No such module "sidebar". In mathematics, a trigonometric substitution replaces a trigonometric function with another expression. In calculus, trigonometric substitutions are a technique for evaluating integrals. In this case, a radical expression is replaced with a trigonometric one. Trigonometric identities may help simplify the answer.[1][2]

In the case of a definite integral, this substitution changes the interval of integration. Alternatively, the antiderivative of the integrand may be applied to the original interval.

Case I: Integrands containing a2 − x2

Let x=asin⁡θ, and use the identity 1−sin2θ=cos2θ.

Examples of Case I

Geometric construction for Case I

Example 1

In the integral

∫dxa2−x2,

we may use

x=asin⁡θ,dx=acos⁡θdθ,θ=arcsin⁡xa.

Then, ∫dxa2−x2=∫acos⁡θdθa2−a2sin2θ=∫acos⁡θdθa2(1−sin2θ)=∫acos⁡θdθa2cos2θ=∫dθ=θ+C=arcsin⁡xa+C.

The above step requires that a>0 and cos⁡θ>0. We can choose a to be the principal root of a2, and impose the restriction −π/2<θ<π/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 goes from 0 to a/2, then sin⁡θ goes from 0 to 1/2, so θ goes from 0 to π/6. Then,

∫0a/2dxa2−x2=∫0π/6dθ=π6.

Some care is needed when picking the bounds. Because integration above requires that −π/2<θ<π/2 , θ can only go from 0 to π/6. Neglecting this restriction, one might have picked θ to go from π to 5π/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

∫0a/2dxa2−x2=arcsin⁡(xa)|0a/2=arcsin⁡(12)−arcsin⁡(0)=π6 as before.

Example 2

The integral

∫a2−x2dx,

may be evaluated by letting x=asin⁡θ,dx=acos⁡θdθ,θ=arcsin⁡xa, where a>0 so that a2=a, and −π/2≤θ≤π/2 by the range of arcsine, so that cos⁡θ≥0 and cos2θ=cos⁡θ.

Then, ∫a2−x2dx=∫a2−a2sin2θ(acos⁡θ)dθ=∫a2(1−sin2θ)(acos⁡θ)dθ=∫a2(cos2θ)(acos⁡θ)dθ=∫(acos⁡θ)(acos⁡θ)dθ=a2∫cos2θdθ=a2∫(1+cos⁡2θ2)dθ=a22(θ+12sin⁡2θ)+C=a22(θ+sin⁡θcos⁡θ)+C=a22(arcsin⁡xa+xa1−x2a2)+C=a22arcsin⁡xa+x2a2−x2+C.

For a definite integral, the bounds change once the substitution is performed and are determined using the equation θ=arcsin⁡xa, with values in the range −π/2≤θ≤π/2. Alternatively, apply the boundary terms directly to the formula for the antiderivative.

For example, the definite integral

∫−114−x2dx,

may be evaluated by substituting x=2sin⁡θ,dx=2cos⁡θdθ, with the bounds determined using θ=arcsin⁡x2.

Because arcsin⁡(1/2)=π/6 and arcsin⁡(−1/2)=−π/6, ∫−114−x2dx=∫−π/6π/64−4sin2θ(2cos⁡θ)dθ=∫−π/6π/64(1−sin2θ)(2cos⁡θ)dθ=∫−π/6π/64(cos2θ)(2cos⁡θ)dθ=∫−π/6π/6(2cos⁡θ)(2cos⁡θ)dθ=4∫−π/6π/6cos2θdθ=4∫−π/6π/6(1+cos⁡2θ2)dθ=2[θ+12sin⁡2θ]−π/6π/6=[2θ+sin⁡2θ]|−π/6π/6=(π3+sin⁡π3)−(−π3+sin⁡(−π3))=2π3+3.

On the other hand, direct application of the boundary terms to the previously obtained formula for the antiderivative yields ∫−114−x2dx=[222arcsin⁡x2+x222−x2]−11=(2arcsin⁡12+124−1)−(2arcsin⁡(−12)+−124−1)=(2⋅π6+32)−(2⋅(−π6)−32)=2π3+3 as before.

Case II: Integrands containing a2 + x2

Let x=atan⁡θ, and use the identity 1+tan2θ=sec2θ.

Examples of Case II

Geometric construction for Case II

Example 1

In the integral

∫dxa2+x2

we may write

x=atan⁡θ,dx=asec2θdθ,θ=arctan⁡xa,

so that the integral becomes

∫dxa2+x2=∫asec2θdθa2+a2tan2θ=∫asec2θdθa2(1+tan2θ)=∫asec2θdθa2sec2θ=∫dθa=θa+C=1aarctan⁡xa+C,

provided a≠0.

For a definite integral, the bounds change once the substitution is performed and are determined using the equation θ=arctan⁡xa, with values in the range −π2<θ<π2. Alternatively, apply the boundary terms directly to the formula for the antiderivative.

For example, the definite integral

∫014dx1+x2

may be evaluated by substituting x=tan⁡θ,dx=sec2θdθ, with the bounds determined using θ=arctan⁡x.

Since arctan⁡0=0 and arctan⁡1=π/4, ∫014dx1+x2=4∫01dx1+x2=4∫0π/4sec2θdθ1+tan2θ=4∫0π/4sec2θdθsec2θ=4∫0π/4dθ=(4θ)|0π/4=4(π4−0)=π.

Meanwhile, direct application of the boundary terms to the formula for the antiderivative yields ∫014dx1+x2=4∫01dx1+x2=4[11arctan⁡x1]01=4(arctan⁡x)|01=4(arctan⁡1−arctan⁡0)=4(π4−0)=π, same as before.

Example 2

The integral

∫a2+x2dx

may be evaluated by letting x=atan⁡θ,dx=asec2θdθ,θ=arctan⁡xa,

where a>0 so that a2=a, and −π2<θ<π2 by the range of arctangent, so that sec⁡θ>0 and sec2θ=sec⁡θ.

Then, ∫a2+x2dx=∫a2+a2tan2θ(asec2θ)dθ=∫a2(1+tan2θ)(asec2θ)dθ=∫a2sec2θ(asec2θ)dθ=∫(asec⁡θ)(asec2θ)dθ=a2∫sec3θdθ. The integral of secant cubed may be evaluated using integration by parts. As a result, ∫a2+x2dx=a22(sec⁡θtan⁡θ+ln⁡|sec⁡θ+tan⁡θ|)+C=a22(1+x2a2⋅xa+ln⁡|1+x2a2+xa|)+C=12(xa2+x2+a2ln⁡|x+a2+x2a|)+C.

To illustrate an application of this formula, suppose we wish to calculate the arc length of the parabola y=x2 from x=0 and x=2. Denoting the arc length as s, we get

s=∫021+(y′)2dx=∫021+4x2dx=2∫0214+x2dx.

In this instance, we have a=12, which gives

s=(x14+x2+14ln⁡|x+14+x212|)x=0x=2=2174+14ln⁡(4+2174)=17+14ln⁡(4+17)≈4.64678

Case III: Integrands containing x2 − a2

Let x=asec⁡θ, and use the identity sec2θ−1=tan2θ.

Examples of Case III

Geometric construction for Case III

Integrals such as

∫dxx2−a2

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

∫x2−a2dx

cannot. In this case, an appropriate substitution is: x=asec⁡θ,dx=asec⁡θtan⁡θdθ,θ=arcsec⁡xa,

where a>0 so that a2=a, and 0≤θ<π2 by assuming x>0, so that tan⁡θ≥0 and tan2θ=tan⁡θ.

Then, ∫x2−a2dx=∫a2sec2θ−a2⋅asec⁡θtan⁡θdθ=∫a2(sec2θ−1)⋅asec⁡θtan⁡θdθ=∫a2tan2θ⋅asec⁡θtan⁡θdθ=∫a2sec⁡θtan2θdθ=a2∫(sec⁡θ)(sec2θ−1)dθ=a2∫(sec3θ−sec⁡θ)dθ.

One may evaluate the integral of the secant function by multiplying the numerator and denominator by (sec⁡θ+tan⁡θ) and the integral of secant cubed by parts.[3] As a result, ∫x2−a2dx=a22(sec⁡θtan⁡θ+ln⁡|sec⁡θ+tan⁡θ|)−a2ln⁡|sec⁡θ+tan⁡θ|+C=a22(sec⁡θtan⁡θ−ln⁡|sec⁡θ+tan⁡θ|)+C=a22(xa⋅x2a2−1−ln⁡|xa+x2a2−1|)+C=12(xx2−a2−a2ln⁡|x+x2−a2a|)+C.

When π2<θ≤π, which happens when x<0 given the range of arcsecant, tan⁡θ≤0, meaning tan2θ=−tan⁡θ instead in that case.

Substitutions that eliminate trigonometric functions

Substitution can be used to remove trigonometric functions.

For instance,

∫f(sin⁡(x),cos⁡(x))dx=∫1±1−u2f(u,±1−u2)duu=sin⁡(x)∫f(sin⁡(x),cos⁡(x))dx=∫1∓1−u2f(±1−u2,u)duu=cos⁡(x)∫f(sin⁡(x),cos⁡(x))dx=∫21+u2f(2u1+u2,1−u21+u2)duu=tan⁡(x2)

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

For example,

∫4cos⁡x(1+cos⁡x)3dx=∫21+u24(1−u21+u2)(1+1−u21+u2)3du=∫(1−u2)(1+u2)du=∫(1−u4)du=u−u55+C=tan⁡x2−15tan5x2+C.

Hyperbolic substitution

Substitutions of hyperbolic functions can also be used to simplify integrals.[4]

For example, to integrate 1/a2+x2, introduce the substitution x=asinh⁡u (and hence dx=acosh⁡udu), then use the identity cosh2(x)−sinh2(x)=1 to find:

∫dxa2+x2=∫acosh⁡udua2+a2sinh2u=∫cosh⁡udu1+sinh2u=∫cosh⁡ucosh⁡udu=u+C=sinh−1xa+C.

If desired, this result may be further transformed using other identities, such as using the relation sinh−1z=arsinh⁡z=ln⁡(z+z2+1): sinh−1xa+C=ln⁡(xa+x2a2+1)+C=ln⁡(x+x2+a2a)+C.

See also

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References

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