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integration by parts formula
∫u dv = uv - ∫v du
exponential(integration by parts)
dv
trigonometric(integration by parts)
dv
algebraic(integration by parts)
u or dv
inverse trig(integration by parts)
u
logarithmic(integration by parts)
u
∫tan(x)dx
−ln∣cos(x)∣+C
∫cot(x)dx
ln∣sin(x)∣+C
∫sec(x)dx
ln∣sec(x)+tan(x)∣+C
∫csc(x)dx
−ln∣csc(x)+cot(x)∣+C
Odd Number of Cosines(∫sinn(x)cosm(x)dx )
save one factor of cos(x) for du=cos(x)dx, convert the remaining even powers of cosine using cos2(x)=1−sin2(x), and substitute u=sin(x).
Odd number of sines(∫sinn(x)cosm(x)dx )
save one factor of sin(x) for du=−sin(x)dx, convert the remaining even powers of sine using sin2(x)=1−cos2(x), and substitute u=cos(x).
Odd number of tangents/cotangents(∫tann(x)secm(x)dx )
save a factor of sec(x)tan(x) for du=sec(x)tan(x)dx, convert remaining tangents using tan2(x)=sec2(x)−1, and substitute u=sec(x).
Even Number of Secants/Cosecants(∫tann(x)secm(x)dx )
save a factor of sec2(x) for du=sec2(x)dx, convert remaining secants using sec2(x)=1+tan2(x), and substitute u=tan(x).
special: Zero Secants and Even Number of Tangents(∫tann(x)dx )
convert using using tan2(x)=sec2(x)−1 , if more than 2, substitute u=tan(x) and du = \sec^2(x)\differentialD x
sin2(θ)
21−cos(2θ)
cos2(θ)
21+cos(2θ)
Even number of Sines and Cosines
The identities sin2(θ)=21−cos(2θ) and cos2(θ)=21+cos(2θ) , used to evaluate trigonometric integrals containing an even number of sines and an even number of cosines.
Even Tangents and Odd Secants(ex. ∫sec3(x)dx )
Use integration by parts
1−x2
x=sin(θ)
1+x2
x=tan(θ)
x2−1
x=sec(θ)
Improper Integral
A definite integral ∫abf(x)dx in which either the interval of integration is infinite or the integrand f(x) is undefined or discontinuous at some value x∈[a,b].
Type 1 Improper Integral
An improper integral with infinite integration limits, evaluated as a limit of the form limT→∞∫aTf(x)dx or limT→−∞∫Tbf(x)dx.
Type 2 Improper Integral
An improper integral where the integrand has a vertical asymptote or discontinuity on the interval [a,b], evaluated by taking a one-sided limit toward the point of discontinuity.