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Mathematics · Ch 11 — Integral Calculus

Summary

11.8

Summary

This chapter's toolkit reduces to a short list of building blocks, best remembered in groups.

Power, log, and exponential forms. ∫xn dx=xn+1n+1+c\int x^n\,dx=\dfrac{x^{n+1}}{n+1}+c (n≠−1n\ne-1, the power rule) and its edge case ∫1x dx=log⁡∣x∣+c\int\dfrac1x\,dx=\log|x|+c; ∫ex dx=ex+c\int e^x\,dx=e^x+c and ∫ax dx=axlog⁡a+c\int a^x\,dx=\dfrac{a^x}{\log a}+c; plus the two "do-nothing/scale" rules ∫k dx=kx+c\int k\,dx=kx+c and ∫0 dx=c\int0\,dx=c.

Trigonometric forms. The six basic derivative pairs run in reverse to give ∫sin⁡x dx=−cos⁡x+c\int\sin x\,dx=-\cos x+c, ∫cos⁡x dx=sin⁡x+c\int\cos x\,dx=\sin x+c, ∫sec⁡2x dx=tan⁡x+c\int\sec^2x\,dx=\tan x+c, ∫csc⁡2x dx=−cot⁡x+c\int\csc^2x\,dx=-\cot x+c, ∫sec⁡xtan⁡x dx=sec⁡x+c\int\sec x\tan x\,dx=\sec x+c, and ∫csc⁡xcot⁡x dx=−csc⁡x+c\int\csc x\cot x\,dx=-\csc x+c. Alongside these sit four "integrated-by-manipulation" log-form results: ∫tan⁡x dx=log⁡∣sec⁡x∣+c\int\tan x\,dx=\log|\sec x|+c, ∫cot⁡x dx=log⁡∣sin⁡x∣+c\int\cot x\,dx=\log|\sin x|+c, ∫sec⁡x dx=log⁡∣sec⁡x+tan⁡x∣+c\int\sec x\,dx=\log|\sec x+\tan x|+c, and ∫csc⁡x dx=log⁡∣csc⁡x−cot⁡x∣+c\int\csc x\,dx=\log|\csc x-\cot x|+c.

Inverse-trigonometric forms. ∫dx1−x2=sin⁡−1x+c\int\dfrac{dx}{\sqrt{1-x^2}}=\sin^{-1}x+c and ∫dx1+x2=tan⁡−1x+c\int\dfrac{dx}{1+x^2}=\tan^{-1}x+c are the two seeds from which every Type-I inverse-trig/log result of \S11.7.9 is built, simply by rescaling x→x/ax\to x/a.

The linearity and shift rules that make everything else work. ∫kf(x) dx=k∫f(x) dx\int kf(x)\,dx=k\int f(x)\,dx and ∫(f1(x)±f2(x)) dx=∫f1(x) dx±∫f2(x) dx\int(f_1(x)\pm f_2(x))\,dx=\int f_1(x)\,dx\pm\int f_2(x)\,dx let a complicated integrand be split into pieces and handled one at a time; and if ∫f(x) dx=g(x)+c\int f(x)\,dx=g(x)+c, then ∫f(ax+b) dx=1ag(ax+b)+c\int f(ax+b)\,dx=\dfrac1a g(ax+b)+c, so any already-known antiderivative can be reused whenever the variable is replaced by a linear expression ax+bax+b.

The three general integration methods. Substitution replaces xx by a new variable to turn an unfamiliar integrand into a recognisable one (or, in the ∫f′(x)[f(x)]n dx\int f'(x)[f(x)]^n\,dx / ∫f′(x)f(x) dx\int\frac{f'(x)}{f(x)}\,dx shapes, is spotted directly without writing out a formal substitution). Decomposition rewrites an integrand -- most often a rational function -- as a sum of simpler pieces, via partial fractions or an algebraic/trigonometric identity, before integrating term by term. Integration by parts, ∫u dv=uv−∫v du\int u\,dv=uv-\int v\,du, handles a product of two dissimilar functions (polynomial-times-trig, polynomial-times-exponential, or a lone log/inverse-trig factor); repeated application is systematised by Bernoulli's rule ∫u dv=uv−u′v1+u′′v2−⋯\int u\,dv=uv-u'v_1+u''v_2-\cdots, whose two signature results are the self-referencing pair

∫eaxsin⁡bx dx=eaxa2+b2[asin⁡bx−bcos⁡bx]+c,∫eaxcos⁡bx dx=eaxa2+b2[acos⁡bx+bsin⁡bx]+c.\int e^{ax}\sin bx\,dx=\frac{e^{ax}}{a^2+b^2}[a\sin bx-b\cos bx]+c,\qquad \int e^{ax}\cos bx\,dx=\frac{e^{ax}}{a^2+b^2}[a\cos bx+b\sin bx]+c. …