Summary of Integration Techniques

Summary of Integration Techniques

Standard forms

For those with two columns, you can see the right column as an extension of the left column. (The 1p\frac{1}{p} comes from what I call “reverse of Chain Rule”.) After forming a link this way, you only have to remember the left column.

  1. ∫adx=ax+C\int_{}^{}{adx} = ax + C

  1. ∫xndx=xn+1n+1+C, (n≠−1)\int_{}^{}{x^{n}dx} = \frac{x^{n + 1}}{n + 1} + C,\text{ }(n \neq - 1)

∫(px+q)ndx=1p(px+q)n+1n+1+C, (n≠−1)\int_{}^{}{(px + q)^{n}dx} = \frac{1}{p}\frac{(px + q)^{n + 1}}{n + 1} + C,\text{ }(n \neq - 1)

  1. ∫exdx=ex+C\int_{}^{}{e^{x}dx} = e^{x} + C

∫e(px+q)dx=1pepx+q+C\int_{}^{}{e^{(px + q)}dx} = \frac{1}{p}e^{px + q} + C

∫kxdx=kxln⁡k+C\int_{}^{}{k^{x}dx} = \frac{k^{x}}{\ln k} + C

∫k(px+q)dx=kpx+qpln⁡k+C\int_{}^{}{k^{(px + q)}dx} = \frac{k^{px + q}}{p\ln k} + C

  1. ∫1xdx=ln⁡|x|+C\int_{}^{}{\frac{1}{x}dx} = \ln|x| + C

∫1px+qdx=1pln⁡|px+q|+C\int_{}^{}{\frac{1}{px + q}dx} = \frac{1}{p}\ln|px + q| + C

  1. ∫cos⁡xdx=sin⁡x+C\int_{}^{}{\cos xdx = \sin x + C}

∫cos⁡(px+q)dx=1psin⁡(px+q)+C\int_{}^{}{\cos(px + q)dx} = \frac{1}{p}\sin(px + q) + C

∫sin⁡xdx=−cos⁡x+C\int_{}^{}{\sin xdx} = - \cos x + C

∫sin⁡(px+q)dx=−1pcos⁡(px+q)+C\int_{}^{}{\sin(px + q)dx} = - \frac{1}{p}\cos(px + q) + C

∫sec⁡2xdx=tan⁡x+C\int_{}^{}{\sec^{2}xdx} = \tan x + C

∫sec⁡2(px+q)dx=1ptan⁡(px+q)+C\int_{}^{}{\sec^{2}(px + q)dx = \frac{1}{p}\tan(px + q) + C}

∫cosec2xdx=−cot⁡x+C\int_{}^{}{\text{cose}\text{c}^{2}xdx = - \cot x + C}

∫cosec2(px+q)dx=−1pcot⁡(px+q)+C\int_{}^{}{\text{cose}\text{c}^{2}(px + q)dx = - \frac{1}{p}\cot(px + q) + C}

∫sec⁡xtan⁡xdx=sec⁡x+C\int_{}^{}{\sec x\tan x dx} = \sec x + C

∫sec⁡(px+q)tan⁡(px+q)dx=1psec⁡(px+q)+C\int_{}^{}{\sec(px + q)\tan(px + q)dx} = \frac{1}{p}\sec(px + q) + C

∫cosecxcot⁡xdx=−cosecx+C\int_{}^{}{{cosec}x\cot xdx} = - {cosec}x + C

∫cosec(px+q)cot⁡(px+q)dx=−1pcosec(px+q)+C\int_{}^{}{{cosec}(px + q)\cot(px + q)dx} = - \frac{1}{p}{cosec}(px + q) + C

  1. ∫11−x2dx=sin⁡−1x+C\int_{}^{}{\frac{1}{\sqrt{1 - x^{2}}}dx} = \sin^{- 1}x + C

∫1a2−(px+q)2dx=1psin−1px+qa+C\int_{}^{}{\frac{1}{\sqrt{a^{2} - (px + q)^{2}}}dx} = {\frac{1}{p}\sin}^{- 1}\frac{px + q}{a} + C

  1. ∫11+x2dx=tan⁡−1x+C\int_{}^{}{\frac{1}{1 + x^{2}}dx} = \tan^{- 1}x + C

∫1a2+(px+q)2dx=1patan−1px+qa+C\int_{}^{}{\frac{1}{a^{2} + (px + q)^{2}}dx} = {\frac{1}{pa}\tan}^{- 1}\frac{px + q}{a} + C

Expressions containing 𝒇(𝒙)\mathbf{f(x)} and 𝒇'(x) \text{f}\text{ }^{\mathbf{'}}\mathbf{(x)}

  1. ∫ f ′(x)[f(x)]ndx=[f(x)]n+1n+1+C,\int_{}^{}{\text{f}\text{ }'(x)\left\lbrack f(x) \right\rbrack^{n}dx} = \frac{\left\lbrack f(x) \right\rbrack^{n + 1}}{n + 1} + C, n ≠ −1

  1. ∫f′(x)f(x)dx=ln⁡|f(x)|+C\int_{}^{}{\frac{f'(x)}{f(x)}dx} = \ln\left| f(x) \right| + C

Use this for:

∫tan⁡xdx\int_{}^{}{\tan x dx} and ∫cot⁡xdx\int_{}^{}{\cot xdx}

  1. ∫ f '(x)ef(x)dx=ef(x)+C\int_{}^{}{\text{f}\text{ }'(x)e^{f(x)}dx} = e^{f(x)} + C

  1. ∫ f '(x)sin[⁡f(x)]dx=−cos[⁡f(x)]+C\int_{}^{}{\text{f}\text{ }'(x)\sin f(x)dx} = - \cos\ f(x) + C

Techniques of integration

Other trigonometric functions

Integrals

How?

∫sin⁡n(kx) dx or ∫cos⁡n(kx) dx\int_{}^{}{\sin^{n}(kx)\text{ d}x}\text{ or }\int_{}^{}{\cos^{n}(kx)\text{ d}x}, where n is even

sin⁡2x=12[1−cos(2x)]cos⁡2x=12[1+cos(2x)]{\sin^{2}x = \frac{1}{2}\left\lbrack 1 - \cos(2x) \right\rbrack }{\cos^{2}x = \frac{1}{2}\left\lbrack 1 + \cos(2x) \right\rbrack}

∫sin⁡n(kx)dx\int_{}^{}{\sin^{n}(kx)\ }dx

∫cos⁡n(kx)dx\int_{}^{}{\cos^{n}(kx)\ }dx

∫sin⁡m(kx)cos⁡n(kx)dx\int_{}^{}{\sin^{m}(kx)\cos^{n}(kx)\ }dx ∫cos⁡m(kx)sin⁡n(kx)dx\int_{}^{}{\cos^{m}(kx)\sin^{n}(kx)\ }dx

where n is odd and m is integer

Pull out one copy of the one with odd power

E.g.

∫cos⁡2xsin⁡3xdx=∫cos⁡2x(1−cos⁡2x)sin⁡xdx\int_{}^{}{\cos^{2}x\sin^{3}x\ }dx = \int_{}^{}{\cos^{2}x\left( 1 - \cos^{2}x \right)\sin x\ }dx

=∫(cos⁡2x−cos⁡4x)sin⁡xdx= \int_{}^{}{(\cos^{2}x - \cos^{4}x)\sin x\ }dx

Note: If both m and n are even, use cos⁡2x=1−sin⁡2x\cos^{2}x = 1 - \sin^{2}x or sin⁡2x=1−cos⁡2x\sin^{2}x = 1 - \cos^{2}x

E.g.

∫cos⁡2xsin⁡2xdx=∫cos⁡2x(1−cos⁡2x)dx\int_{}^{}{\cos^{2}x\sin^{2}x\ }dx = \int_{}^{}{\cos^{2}x\left( 1 - \cos^{2}x \right)\ }dx

=∫cos⁡2x−cos⁡4xdx= \int_{}^{}{\cos^{2}x - \cos^{4}x\ }dx

∫tan⁡n(kx) dx or ∫cot⁡n(kx) dx\int_{}^{}{\tan^{n}(kx)\text{ d}x}\text{ or }\int_{}^{}{\cot^{n}(kx)\text{ d}x}

n = 1: Use tan (kx) = sin⁡(kx)cos⁡(kx)\frac{\sin(kx)}{\cos(kx)} or cot (kx) = cos⁡(kx)sin⁡(kx)\frac{\cos(kx)}{\sin(kx)},

and then ∫f′(x)f(x)dx=ln⁡|f(x)|+C\int_{}^{}{\frac{f'(x)}{f(x)}dx} = \ln\left| f(x) \right| + C

n ≥ 2: Pull out one copy of: tan⁡2x=sec⁡2x−1\tan^{2}x = \sec^{2}x - 1 cot⁡2x=cosec2x−1\cot^{2}x = \text{cose}\text{c}^{2}x - 1

∫sin⁡(kx)cos⁡(mx) dx\int_{}^{}{\sin(kx)\cos(mx)\text{ d}x}

∫cos⁡(kx)cos⁡(mx) dx\int_{}^{}{\cos(kx)\cos(mx)\text{ d}x}

∫sin⁡(kx)sin⁡(mx) dx\int_{}^{}{\sin(kx)\sin(mx)\text{ d}x}

sin⁡Acos⁡B=12[sin⁡(A+B)+sin⁡(A−B)]\sin A\cos B = \frac{1}{2}\lbrack\sin(A + B) + \sin(A - B)\rbrack

cos⁡Asin⁡B=12[sin⁡(A+B)−sin⁡(A−B)] {\cos A\sin B = \frac{1}{2}\lbrack\sin(A + B) - \sin(A - B)\rbrack}

cos⁡Acos⁡B=12[cos⁡(A−B)+cos⁡(A+B)] {\cos A\cos B = \frac{1}{2}\lbrack\cos(A - B) + \cos(A + B)\rbrack}

sin⁡Asin⁡B=12[cos⁡(A−B)−cos⁡(A+B)] {\sin A\sin B = \frac{1}{2}\lbrack\cos(A - B) - \cos(A + B)\rbrack}

Rational algebraic functions and similar ones

Steps

  1. Improper? If yes, use long division or juggling.

  1. Can each part be integrated by standard forms?

  1. If not, would splitting the numerator help?

  1. If not, would partial fractions do the trick?

Integrals

How?

  1. ∫1ax2+bx+cdx\int_{}^{}{\frac{1}{\sqrt{ax^{2} + bx + c}}dx}

Complete the square for ax2+bx+cax^{2} + bx + c

  1. ∫1ax2+bx+cdx\int_{}^{}{\frac{1}{ax^{2} + bx + c}dx}

If ax2+bx+cax^{2} + bx + c can be factorised, factorise and use partial-fractions method.

If not, complete the square.

  1. ∫px+qax2+bx+cdx\int_{}^{}{\frac{px + q}{\sqrt{ax^{2} + bx + c}}dx}

px+q≡Addx(ax2+bx+c)+Bpx + q \equiv A\frac{d}{dx}(ax^{2} + bx + c) + B

≡A(2ax+b)+B\equiv A(2ax + b) + B

where A and B are constants to be determined

  1. ∫1ax2+bx+cdx\int_{}^{}{\frac{1}{ax^{2} + bx + c}dx}

By substitution

∫g(f(x))dx=∫g(u)dxdudu,whereu=f(x)\int_{}^{}{g\left( f(x) \right)dx} = \int_{}^{}{g(u)\frac{dx}{du}du},\ where\ u = f(x)

(Note: The required substitution would always be given in the question.)

By parts

∫udv = uv−∫v du\int_{}^{}{udv\text{ } = \text{ }uv - \int_{}^{}{v\text{ d}u}}



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