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Mathematics · Ch 11 — Integral Calculus

Important Results

11.7.4

Important Results

Two substitution patterns come up so often that it pays to know them as ready-made formulas rather than re-deriving them every time.

Result (1). ∫f′(x)f(x) dx=log⁡∣f(x)∣+c\displaystyle\int\dfrac{f'(x)}{f(x)}\,dx=\log|f(x)|+c — whenever the numerator is (a constant multiple of) the exact derivative of the denominator, the integral is the log of the denominator's absolute value.

Proof (own words). Put u=f(x)u=f(x), so du=f′(x) dxdu=f'(x)\,dx; the integral becomes ∫duu=log⁡∣u∣+c\displaystyle\int\dfrac{du}{u}=\log|u|+c, and re-substituting u=f(x)u=f(x) gives the stated result.

Result (2). ∫f′(x) [f(x)]n dx=[f(x)]n+1n+1+c,n≠−1\displaystyle\int f'(x)\,[f(x)]^n\,dx=\dfrac{[f(x)]^{n+1}}{n+1}+c,\quad n\ne-1 — a "chunk raised to a power" times the exact derivative of that chunk integrates by the ordinary power rule applied to the chunk.

Proof (own words). Again put u=f(x)u=f(x), du=f′(x) dxdu=f'(x)\,dx; the integral becomes ∫un du=un+1n+1+c\displaystyle\int u^n\,du=\dfrac{u^{n+1}}{n+1}+c, and re-substituting gives the result. (Result (1) is really the n=−1n=-1 case of this same pattern, which is exactly why that case has to be stated separately — the power rule itself is undefined at n=−1n=-1.)

The four standard log-form results, each a direct application of Result (1):

Writing tan⁡x=sin⁡xcos⁡x\tan x=\dfrac{\sin x}{\cos x} and setting u=cos⁡xu=\cos x (so du=−sin⁡x dxdu=-\sin x\,dx) gives ∫tan⁡x dx=−log⁡∣cos⁡x∣+c=log⁡∣sec⁡x∣+c\displaystyle\int\tan x\,dx=-\log|\cos x|+c=\log|\sec x|+c. Writing cot⁡x=cos⁡xsin⁡x\cot x=\dfrac{\cos x}{\sin x} and setting u=sin⁡xu=\sin x gives ∫cot⁡x dx=log⁡∣sin⁡x∣+c\displaystyle\int\cot x\,dx=\log|\sin x|+c. For csc⁡x\csc x, multiply and divide by (csc⁡x−cot⁡x)(\csc x-\cot x): csc⁡x=csc⁡x(csc⁡x−cot⁡x)csc⁡x−cot⁡x=csc⁡2x−csc⁡xcot⁡xcsc⁡x−cot⁡x\csc x=\dfrac{\csc x(\csc x-\cot x)}{\csc x-\cot x}=\dfrac{\csc^2x-\csc x\cot x}{\csc x-\cot x}, whose numerator is exactly the derivative of the denominator, so by Result (1), ∫csc⁡x dx=log⁡∣csc⁡x−cot⁡x∣+c\displaystyle\int\csc x\,dx=\log|\csc x-\cot x|+c. Symmetrically, multiplying and dividing sec⁡x\sec x by (sec⁡x+tan⁡x)(\sec x+\tan x) gives numerator sec⁡2x+sec⁡xtan⁡x\sec^2x+\sec x\tan x, the derivative of sec⁡x+tan⁡x\sec x+\tan x, so ∫sec⁡x dx=log⁡∣sec⁡x+tan⁡x∣+c\displaystyle\int\sec x\,dx=\log|\sec x+\tan x|+c.

∫tan⁡x dx=log⁡∣sec⁡x∣+c,∫cot⁡x dx=log⁡∣sin⁡x∣+c,\int\tan x\,dx=\log|\sec x|+c,\qquad \int\cot x\,dx=\log|\sin x|+c,

∫csc⁡x dx=log⁡∣csc⁡x−cot⁡x∣+c,∫sec⁡x dx=log⁡∣sec⁡x+tan⁡x∣+c.\int\csc x\,dx=\log|\csc x-\cot x|+c,\qquad \int\sec x\,dx=\log|\sec x+\tan x|+c. …