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Mathematics · Ch 11 — Integral Calculus

Basic Rules of Integration

11.3

Basic Rules of Integration

Because integration is defined as the reverse of differentiation, every standard derivative formula immediately hands us a matching standard antiderivative — simply read the differentiation rule backwards. Collecting them gives the working toolkit for this whole chapter.

Note

The standard integrals. For a constant cc (constant of integration) and, where relevant, a constant kk:

FunctionStandard integral
00∫0 dx=c\displaystyle\int 0\,dx = c
constant kk∫k dx=kx+c\displaystyle\int k\,dx = kx+c
power xnx^n (n≠−1n\ne-1)∫xn dx=xn+1n+1+c\displaystyle\int x^n\,dx = \frac{x^{n+1}}{n+1}+c (Power rule)
1x\dfrac1x$\displaystyle\int \frac1x,dx = \log
sin⁡x\sin x∫sin⁡x dx=−cos⁡x+c\displaystyle\int \sin x\,dx = -\cos x+c
cos⁡x\cos x∫cos⁡x dx=sin⁡x+c\displaystyle\int \cos x\,dx = \sin x+c
sec⁡2x\sec^2 x∫sec⁡2x dx=tan⁡x+c\displaystyle\int \sec^2 x\,dx = \tan x+c
cosec2x\text{cosec}^2 x∫cosec2x dx=−cot⁡x+c\displaystyle\int \text{cosec}^2 x\,dx = -\cot x+c
sec⁡xtan⁡x\sec x\tan x∫sec⁡xtan⁡x dx=sec⁡x+c\displaystyle\int \sec x\tan x\,dx = \sec x+c
cosec xcot⁡x\text{cosec}\,x\cot x∫cosec xcot⁡x dx=−cosec x+c\displaystyle\int \text{cosec}\,x\cot x\,dx = -\text{cosec}\,x+c
exe^x∫ex dx=ex+c\displaystyle\int e^x\,dx = e^x+c
axa^x (a>0, a≠1a>0,\ a\ne1)∫ax dx=axlog⁡a+c\displaystyle\int a^x\,dx = \frac{a^x}{\log a}+c
11−x2\dfrac{1}{\sqrt{1-x^2}}∫11−x2 dx=sin⁡−1x+c\displaystyle\int \frac{1}{\sqrt{1-x^2}}\,dx = \sin^{-1}x+c
11+x2\dfrac{1}{1+x^2}∫11+x2 dx=tan⁡−1x+c\displaystyle\int \frac{1}{1+x^2}\,dx = \tan^{-1}x+c

Each row is literally the mirror image of an earlier derivative fact: since ddx(c)=0\dfrac{d}{dx}(c)=0, we get ∫0 dx=c\int 0\,dx=c; since ddx(kx)=k\dfrac{d}{dx}(kx)=k, we get ∫k dx=kx+c\int k\,dx=kx+c; since ddx ⁣(xn+1n+1)=xn\dfrac{d}{dx}\!\left(\dfrac{x^{n+1}}{n+1}\right)=x^n, we get the Power rule (the restriction n≠−1n\ne-1 is forced because n+1=0n+1=0 would divide by zero — the n=−1n=-1 case is instead covered separately by the log⁡∣x∣\log|x| row, coming from ddx(log⁡x)=1x\dfrac{d}{dx}(\log x)=\dfrac1x); and so on down every trigonometric, exponential and inverse-trigonometric row.

Applying the power rule directly. Any integrand that can be rewritten as a single power of xx (including negative and fractional powers, via 1xn=x−n\dfrac{1}{x^n}=x^{-n} and xnk=xn/k\sqrt[k]{x^n}=x^{n/k}) integrates by the power rule after that rewriting. For instance ∫x10 dx=x1111+c\displaystyle\int x^{10}\,dx = \frac{x^{11}}{11}+c; and reciprocal powers integrate the same way after converting to a negative exponent, e.g. ∫1x10 dx=∫x−10 dx=x−9−9+c=−19x9+c\displaystyle\int \frac{1}{x^{10}}\,dx=\int x^{-10}\,dx=\frac{x^{-9}}{-9}+c=-\frac{1}{9x^9}+c. Roots integrate identically once written as fractional powers: ∫x dx=∫x1/2 dx=x3/23/2+c=23x3/2+c\displaystyle\int \sqrt{x}\,dx=\int x^{1/2}\,dx=\frac{x^{3/2}}{3/2}+c=\tfrac23 x^{3/2}+c, and ∫1x dx=∫x−1/2 dx=x1/21/2+c=2x+c\displaystyle\int \frac{1}{\sqrt x}\,dx=\int x^{-1/2}\,dx=\frac{x^{1/2}}{1/2}+c=2\sqrt x+c.

Reducing a trig quotient to a standard form. Many integrands that don't look like they are on the table above are simply a standard trig antiderivative in disguise. Recognising a familiar identity is the whole trick:

  • 1cos⁡2x=sec⁡2x\dfrac{1}{\cos^2 x}=\sec^2 x, so ∫dxcos⁡2x=∫sec⁡2x dx=tan⁡x+c\displaystyle\int \frac{dx}{\cos^2 x}=\int\sec^2x\,dx=\tan x+c.
  • cot⁡xsin⁡x=cos⁡xsin⁡2x=cosec xcot⁡x\dfrac{\cot x}{\sin x}=\dfrac{\cos x}{\sin^2 x}=\text{cosec}\,x\cot x, so ∫cot⁡xsin⁡x dx=−cosec x+c\displaystyle\int \frac{\cot x}{\sin x}\,dx=-\text{cosec}\,x+c.
  • sin⁡xcos⁡2x=sin⁡xcos⁡x⋅1cos⁡x=tan⁡xsec⁡x\dfrac{\sin x}{\cos^2 x}=\dfrac{\sin x}{\cos x}\cdot\dfrac{1}{\cos x}=\tan x\sec x, so ∫sin⁡xcos⁡2x dx=∫tan⁡xsec⁡x dx=sec⁡x+c\displaystyle\int \frac{\sin x}{\cos^2 x}\,dx=\int\tan x\sec x\,dx=\sec x+c.
  • 11−x2\dfrac{1}{\sqrt{1-x^2}} and 11+x2\dfrac{1}{1+x^2} integrate directly to sin⁡−1x\sin^{-1}x and tan⁡−1x\tan^{-1}x respectively, straight off the table. …