Revision as of 21:53, 31 January 2023 editJoel Brennan (talk | contribs)Extended confirmed users3,724 editsm added wikilinks← Previous edit | Revision as of 01:48, 1 February 2023 edit undoJacobolus (talk | contribs)Extended confirmed users35,697 edits this 'alternative' of replacing tan(x) with sec(x)sin(x) is not worth the space it takes; removing it. also split some math markup onto multiple lines for legibilityNext edit → | ||
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:<math display=inline>\begin{align} | :<math display=inline>\begin{align} | ||
\int \sec^3 x \, dx | \int \sec^3 x \, dx | ||
&= \tfrac12\sec x \tan x + \tfrac12 \int \sec x\, dx + C \\ | &= \tfrac12\sec x \tan x + \tfrac12 \int \sec x\, dx + C \\ | ||
&= \tfrac12(\sec x \tan x + \ln \left|\sec x + \tan x\right|) + C \\ | &= \tfrac12(\sec x \tan x + \ln \left|\sec x + \tan x\right|) + C \\ | ||
&= \tfrac12(\sec x \tan x + \operatorname{gd}^{-1} x) + C, \qquad |x| < \tfrac12\pi | &= \tfrac12(\sec x \tan x + \operatorname{gd}^{-1} x) + C, \qquad |x| < \tfrac12\pi | ||
\end{align}</math> | \end{align}</math> | ||
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where | where | ||
⚫ | :<math> | ||
u = \sec x,\quad dv = \sec^2 x\,dx,\quad v | |||
⚫ | = \tan x,\quad du = \sec x \tan x\,dx. | ||
</math> | |||
Then | Then | ||
:<math>\begin{align} | :<math>\begin{align} | ||
\int \sec^3 x \, dx & |
\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{align}</math> | \end{align}</math> | ||
Next add <math>\int\sec^3 x \,dx</math> to both sides |
Next add <math display=inline>\int\sec^3 x \,dx</math> to both sides:{{efn|The ] are absorbed in the remaining integral term.}} | ||
:<math>\begin{align} | :<math>\begin{align} | ||
2 \int \sec^3 x \, dx |
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{align}</math> | \end{align}</math> | ||
using the ], <math display=inline>\int \sec x \,dx = \ln \left|\sec x + \tan x\right| + C.</math><ref name=":1" /> | |||
Finally, divide both sides by 2: | Finally, divide both sides by 2: | ||
:<math> | |||
⚫ | |||
\int \sec^3 x \, dx | |||
⚫ | = \tfrac12(\sec x \tan x + \ln \left|\sec x + \tan x\right|) + C, | ||
</math> | |||
which was to be derived.<ref name=":1" /> | which was to be derived.<ref name=":1" /> | ||
=== Reduction to an integral of a rational function === | === Reduction to an integral of a rational function === | ||
:<math> | |||
: <math>\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}</math> | |||
\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} | |||
</math> | |||
where <math>u = \sin x</math>, so that <math>du = \cos x\,dx</math>. This admits a decomposition by ]: | where <math>u = \sin x</math>, so that <math>du = \cos x\,dx</math>. This admits a decomposition by ]: | ||
:<math> | |||
⚫ | |||
\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}. | ||
</math> | |||
Antidifferentiating term-by-term, one gets | Antidifferentiating term-by-term, one gets | ||
:<math>\begin{align} | :<math>\begin{align} | ||
\int \sec^3 x \, dx &= \ |
\int \sec^3 x \, dx | ||
&= \tfrac14 \ln |1+u| - \frac{1}{4(1+u)} - \tfrac14 \ln|1-u| + \frac{1}{4(1-u)} + C \\ | |||
&= \ |
&= \tfrac14 \ln \Biggl| \frac{1+u}{1-u} \Biggl| + \frac{u}{2(1-u^2)} + C \\ | ||
&= \ |
&= \tfrac14 \ln \Biggl|\frac{1+\sin x}{1-\sin x} \Biggl| + \frac{\sin x}{2\cos^2 x} + C\\ | ||
&= \ |
&= \tfrac14 \ln \left|\frac{1+\sin x}{1-\sin x}\right| + \tfrac12 \sec x \tan x + C \\ | ||
&= \ |
&= \tfrac14 \ln \left|\frac{(1+\sin x)^2}{1-\sin^2 x}\right| + \tfrac12 \sec x \tan x + C \\ | ||
&= \ |
&= \tfrac14 \ln \left|\frac{(1+\sin x)^2}{\cos^2 x}\right| + \tfrac12 \sec x \tan x + C \\ | ||
&= \ |
&= \tfrac12 \ln \left|\frac{1+\sin x}{\cos x}\right| + \tfrac12 \sec x \tan x + C \\ | ||
&= \ |
&= \tfrac12 (\ln|\sec x + \tan x| + \sec x \tan x) + C. | ||
⚫ | |||
\end{align}</math> | \end{align}</math> | ||
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:<math>\begin{align} | :<math>\begin{align} | ||
\sec x & |
\sec x &= \cosh u \\ | ||
\tan x & |
\tan x &= \sinh u \\ | ||
\sec^2 x \, dx & |
\sec^2 x \, dx &= \cosh u \, du \text{ or } \sec x \tan x\, dx = \sinh u \, du \\ | ||
\sec x \, dx & |
\sec x \, dx &= \, du \text{ or } dx = \operatorname{sech} u \, du \\ | ||
u & |
u &= \operatorname{arcosh} (\sec x ) = \operatorname{arsinh} ( \tan x ) = \ln|\sec x + \tan x| | ||
\end{align}</math> | \end{align}</math> | ||
Note that <math>\int \sec x \, dx = \ln|\sec x + \tan x|</math> follows directly from this substitution. | Note that <math>\int \sec x \, dx = \ln|\sec x + \tan x|</math> follows directly from this substitution. | ||
:<math> | :<math>\begin{align} | ||
\int \sec^3 x \, dx | |||
\begin{align} | |||
&= \int \cosh^2 u\,du \\ | |||
& |
&= \tfrac12 \int ( \cosh 2u +1) \,du \\ | ||
& |
&= \tfrac12 \left( \tfrac12 \sinh2u + u\right) + C\\ | ||
& |
&= \tfrac12 ( \sinh u \cosh u + u ) + C \\ | ||
& |
&= \tfrac12 (\sec x \tan x + \ln \left|\sec x + \tan x\right|) + C | ||
\end{align} | \end{align}</math> | ||
⚫ | < |
||
== Higher odd powers of secant == | == Higher odd powers of secant == | ||
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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: | 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: | ||
:<math> | |||
⚫ | |||
\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 \ne 1\text{)}\,\! | ||
Alternatively: | |||
</math> | |||
: <math>\int \sec^n x \, dx = \frac{\sec^{n-1} x \sin x}{n-1} \,+\, \frac{n-2}{n-1}\int \sec^{n-2} x \, dx \qquad \text{ (for }n \ne 1\text{)}\,\!</math> | |||
Even powers of tangents can be accommodated by using ] to form an odd ] of secant and using these formulae on the largest term and combining like terms. | Even powers of tangents can be accommodated by using ] to form an odd ] of secant and using these formulae on the largest term and combining like terms. |
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The integral of secant cubed is a frequent and challenging indefinite integral of elementary calculus:
where 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
- where 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:
where
Then
Next add to both sides:
using the integral of the secant function,
Finally, divide both sides by 2:
which was to be derived.
Reduction to an integral of a rational function
where , so that . This admits a decomposition by partial fractions:
Antidifferentiating term-by-term, one gets
Hyperbolic functions
Integrals of the form: can be reduced using the Pythagorean identity if is even or and are both odd. If is odd and is even, hyperbolic substitutions can be used to replace the nested integration by parts with hyperbolic power-reducing formulas.
Note that follows directly from this substitution.
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:
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
Notes
- The constants of integration are absorbed in the remaining integral term.
References
- Spivak, Michael (2008). "Integration in Elementary Terms". Calculus. p. 382.
This is a tricky and important integral that often comes up.
- ^ Stewart, James (2012). "Section 7.2: Trigonometric Integrals". Calculus - Early Transcendentals. United States: Cengage Learning. pp. 475–6. ISBN 978-0-538-49790-9.
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