Integral of secant cubed

Part of a series of articles about
Calculus
${\displaystyle \int _{a}^{b}f'(t)\,dt=f(b)-f(a)}$
Fundamental theorem Limits Continuity Rolle's theorem Mean value theorem Inverse function theorem
Differential Definitions Derivative (generalizations) Differential infinitesimal of a function total Concepts Differentiation notation Second derivative Implicit differentiation Logarithmic differentiation Related rates Taylor's theorem Rules and identities Sum Product Chain Power Quotient L'Hôpital's rule Inverse General Leibniz Faà di Bruno's formula Reynolds
Integral Lists of integrals Integral transform Leibniz integral rule Definitions Antiderivative Integral (improper) Riemann integral Lebesgue integration Contour integration Integral of inverse functions Integration by Parts Discs Cylindrical shells Substitution (trigonometric, tangent half-angle, Euler) Euler's formula Partial fractions Changing order Reduction formulae Differentiating under the integral sign Risch algorithm
Series Geometric (arithmetico-geometric) Harmonic Alternating Power Binomial Taylor Convergence tests Summand limit (term test) Ratio Root Integral Direct comparison Limit comparison Alternating series Cauchy condensation Dirichlet Abel
Vector Gradient Divergence Curl Laplacian Directional derivative Identities Theorems Gradient Green's Stokes' Divergence generalized Stokes Helmholtz decomposition
Multivariable Formalisms Matrix Tensor Exterior Geometric Definitions Partial derivative Multiple integral Line integral Surface integral Volume integral Jacobian Hessian
Advanced Calculus on Euclidean space Generalized functions Limit of distributions
Specialized Fractional Malliavin Stochastic Variations
Miscellaneous Precalculus History Glossary List of topics Integration Bee Mathematical analysis Nonstandard analysis
v t e

The integral of secant cubed is a frequent and challenging^[1] indefinite integral of elementary calculus:

${\textstyle {\begin{aligned}\int \sec ^{3}x\,dx&={\tfrac {1}{2}}\sec x\tan x+{\tfrac {1}{2}}\int \sec x\,dx+C\\[6mu]&={\tfrac {1}{2}}(\sec x\tan x+\ln \left|\sec x+\tan x\right|)+C\\[6mu]&={\tfrac {1}{2}}(\sec x\tan x+\operatorname {gd} ^{-1}x)+C,\qquad |x|<{\tfrac {1}{2}}\pi \end{aligned}}}$

where ${\textstyle \operatorname {gd} ^{-1}}$ is the inverse Gudermannian function, the integral of the secant function.

There are a number of reasons why this particular antiderivative is worthy of special attention:

• The technique used for reducing integrals of higher odd powers of secant to lower ones is fully present in this, the simplest case. The other cases are done in the same way.
• The utility of hyperbolic functions in integration can be demonstrated in cases of odd powers of secant (powers of tangent can also be included).
• This is one of several integrals usually done in a first-year calculus course in which the most natural way to proceed involves integrating by parts and returning to the same integral one started with (another is the integral of the product of an exponential function with a sine or cosine function; yet another the integral of a power of the sine or cosine function).
• This integral is used in evaluating any integral of the form

${\displaystyle \int {\sqrt {a^{2}+x^{2}}}\,dx,}$

where ${\displaystyle a}$ is a constant. In particular, it appears in the problems of:

• rectifying the parabola and the Archimedean spiral
• finding the surface area of the helicoid.

Derivations

Integration by parts

This antiderivative may be found by integration by parts, as follows:^[2]

${\displaystyle \int \sec ^{3}x\,dx=\int u\,dv=uv-\int v\,du}$

where

${\displaystyle u=\sec x,\quad dv=\sec ^{2}x\,dx,\quad v=\tan x,\quad du=\sec x\tan x\,dx.}$

Then

${\displaystyle {\begin{aligned}\int \sec ^{3}x\,dx&=\int (\sec x)(\sec ^{2}x)\,dx\\&=\sec x\tan x-\int \tan x\,(\sec x\tan x)\,dx\\&=\sec x\tan x-\int \sec x\tan ^{2}x\,dx\\&=\sec x\tan x-\int \sec x\,(\sec ^{2}x-1)\,dx\\&=\sec x\tan x-\left(\int \sec ^{3}x\,dx-\int \sec x\,dx\right)\\&=\sec x\tan x-\int \sec ^{3}x\,dx+\int \sec x\,dx.\end{aligned}}}$

Next add ${\textstyle \int \sec ^{3}x\,dx}$ to both sides:^[a]

${\displaystyle {\begin{aligned}2\int \sec ^{3}x\,dx&=\sec x\tan x+\int \sec x\,dx\\&=\sec x\tan x+\ln \left|\sec x+\tan x\right|+C,\end{aligned}}}$

using the integral of the secant function, ${\textstyle \int \sec x\,dx=\ln \left|\sec x+\tan x\right|+C.}$^[2]

Finally, divide both sides by 2:

${\displaystyle \int \sec ^{3}x\,dx={\tfrac {1}{2}}(\sec x\tan x+\ln \left|\sec x+\tan x\right|)+C,}$

which was to be derived.^[2] A possible mnemonic is: "The integral of secant cubed is the average of the derivative and integral of secant".

Reduction to an integral of a rational function

${\displaystyle \int \sec ^{3}x\,dx=\int {\frac {dx}{\cos ^{3}x}}=\int {\frac {\cos x\,dx}{\cos ^{4}x}}=\int {\frac {\cos x\,dx}{(1-\sin ^{2}x)^{2}}}=\int {\frac {du}{(1-u^{2})^{2}}}}$

where ${\displaystyle u=\sin x}$, so that ${\displaystyle du=\cos x\,dx}$. This admits a decomposition by partial fractions:

${\displaystyle {\frac {1}{(1-u^{2})^{2}}}={\frac {1}{(1+u)^{2}(1-u)^{2}}}={\frac {1}{4(1+u)}}+{\frac {1}{4(1+u)^{2}}}+{\frac {1}{4(1-u)}}+{\frac {1}{4(1-u)^{2}}}.}$

Antidifferentiating term-by-term, one gets

${\displaystyle {\begin{aligned}\int \sec ^{3}x\,dx&={\tfrac {1}{4}}\ln |1+u|-{\frac {1}{4(1+u)}}-{\tfrac {1}{4}}\ln |1-u|+{\frac {1}{4(1-u)}}+C\\[6pt]&={\tfrac {1}{4}}\ln {\Biggl |}{\frac {1+u}{1-u}}{\Biggl |}+{\frac {u}{2(1-u^{2})}}+C\\[6pt]&={\tfrac {1}{4}}\ln {\Biggl |}{\frac {1+\sin x}{1-\sin x}}{\Biggl |}+{\frac {\sin x}{2\cos ^{2}x}}+C\\[6pt]&={\tfrac {1}{4}}\ln \left|{\frac {1+\sin x}{1-\sin x}}\right|+{\tfrac {1}{2}}\sec x\tan x+C\\[6pt]&={\tfrac {1}{4}}\ln \left|{\frac {(1+\sin x)^{2}}{1-\sin ^{2}x}}\right|+{\tfrac {1}{2}}\sec x\tan x+C\\[6pt]&={\tfrac {1}{4}}\ln \left|{\frac {(1+\sin x)^{2}}{\cos ^{2}x}}\right|+{\tfrac {1}{2}}\sec x\tan x+C\\[6pt]&={\tfrac {1}{2}}\ln \left|{\frac {1+\sin x}{\cos x}}\right|+{\tfrac {1}{2}}\sec x\tan x+C\\[6pt]&={\tfrac {1}{2}}(\ln |\sec x+\tan x|+\sec x\tan x)+C.\end{aligned}}}$

Hyperbolic functions

Integrals of the form: ${\displaystyle \int \sec ^{n}x\tan ^{m}x\,dx}$ can be reduced using the Pythagorean identity if ${\displaystyle n}$ is even or ${\displaystyle n}$ and ${\displaystyle m}$ are both odd. If ${\displaystyle n}$ is odd and ${\displaystyle m}$ is even, hyperbolic substitutions can be used to replace the nested integration by parts with hyperbolic power-reducing formulas.

${\displaystyle {\begin{aligned}\sec x&=\cosh u\\[6pt]\tan x&=\sinh u\\[6pt]\sec ^{2}x\,dx&=\cosh u\,du{\text{ or }}\sec x\tan x\,dx=\sinh u\,du\\[6pt]\sec x\,dx&=\,du{\text{ or }}dx=\operatorname {sech} u\,du\\[6pt]u&=\operatorname {arcosh} (\sec x)=\operatorname {arsinh} (\tan x)=\ln |\sec x+\tan x|\end{aligned}}}$

Note that ${\displaystyle \int \sec x\,dx=\ln |\sec x+\tan x|}$ follows directly from this substitution.

${\displaystyle {\begin{aligned}\int \sec ^{3}x\,dx&=\int \cosh ^{2}u\,du\\[6pt]&={\tfrac {1}{2}}\int (\cosh 2u+1)\,du\\[6pt]&={\tfrac {1}{2}}\left({\tfrac {1}{2}}\sinh 2u+u\right)+C\\[6pt]&={\tfrac {1}{2}}(\sinh u\cosh u+u)+C\\[6pt]&={\tfrac {1}{2}}(\sec x\tan x+\ln \left|\sec x+\tan x\right|)+C\end{aligned}}}$

Higher odd powers of secant

Just as the integration by parts above reduced the integral of secant cubed to the integral of secant to the first power, so a similar process reduces the integral of higher odd powers of secant to lower ones. This is the secant reduction formula, which follows the syntax:

${\displaystyle \int \sec ^{n}x\,dx={\frac {\sec ^{n-2}x\tan x}{n-1}}\,+\,{\frac {n-2}{n-1}}\int \sec ^{n-2}x\,dx\qquad {\text{ (for }}n\neq 1{\text{)}}\,\!}$

Even powers of tangents can be accommodated by using binomial expansion to form an odd polynomial of secant and using these formulae on the largest term and combining like terms.

See also

• Lists of integrals

Notes

References