Theorems from Reduction formulae All theorems from Reduction formulae.
[ THEOREM ] For an integer n ≥ 0 n\ge0 n ≥ 0 , choose compatible representatives
I n I_n I n of the antiderivatives of x n e x x^n e^x x n e x . Then
I n = x n e x − n I n − 1 , n ≥ 1. I_n=x^n e^x-n I_{n-1},\qquad n\ge 1. I n = x n e x − n I n − 1 , n ≥ 1. Each application lowers the power of x x x by one. Two antiderivatives can
differ by a constant, so use the recurrence to construct one representative
and add a single arbitrary constant when the reduction stops.
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[ THEOREM ] Let I n = ∫ 0 π / 2 sin n x d x I_n=\int_0^{\pi/2}\sin^n x \, dx I n = ∫ 0 π /2 sin n x d x and J n = ∫ 0 π / 2 cos n x d x J_n=\int_0^{\pi/2}\cos^n x \, dx J n = ∫ 0 π /2 cos n x d x . Then
I n = n − 1 n I n − 2 , J n = n − 1 n J n − 2 , I_n=\frac{n-1}{n} I_{n-2},\qquad J_n=\frac{n-1}{n} J_{n-2}, I n = n n − 1 I n − 2 , J n = n n − 1 J n − 2 , for n ≥ 2 n\ge 2 n ≥ 2 .
The recurrence stops at I 0 = π 2 I_0=\frac{\pi}{2} I 0 = 2 π when n n n is even and at I 1 = 1 I_1=1 I 1 = 1 when n n n is odd and likewise for J n J_n J n . In the proof, collect the reintroduced copy of I n I_n I n before dividing by n n n .
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[ THEOREM ] Let I n = ∫ 0 π / 4 sec n x d x I_n=\int_0^{\pi/4}\sec^n x \, dx I n = ∫ 0 π /4 sec n x d x . Then
I n = 1 n − 1 ( 2 ( n − 2 ) / 2 + ( n − 2 ) I n − 2 ) I_n=\frac{1}{n-1}\bigl(2^{(n-2)/2}+(n-2)I_{n-2}\bigr) I n = n − 1 1 ( 2 ( n − 2 ) /2 + ( n − 2 ) I n − 2 ) for n ≥ 2 n\ge 2 n ≥ 2 .
The base values are
I 0 = ∫ 0 π / 4 1 d x = π 4 I_0=\int_0^{\pi/4}1\,dx=\frac{\pi}{4} I 0 = ∫ 0 π /4 1 d x = 4 π and
I 1 = ∫ 0 π / 4 sec x d x = ln ( 1 + 2 ) I_1=\int_0^{\pi/4}\sec x\,dx=\ln(1+\sqrt{2}) I 1 = ∫ 0 π /4 sec x d x = ln ( 1 + 2 ) .
Without the limits, the same splitting sec n x = sec n − 2 x sec 2 x \sec^n x=\sec^{n-2}x\sec^2 x sec n x = sec n − 2 x sec 2 x produces the antiderivative of sec 3 x \sec^3 x sec 3 x .
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[ THEOREM ] Let J n = ∫ 0 π / 4 tan n x d x J_n=\int_0^{\pi/4}\tan^n x \, dx J n = ∫ 0 π /4 tan n x d x . Then
J n = 1 n − 1 − J n − 2 , n ≥ 2. J_n=\frac{1}{n-1}-J_{n-2},\qquad n\ge 2. J n = n − 1 1 − J n − 2 , n ≥ 2. This recurrence needs no parts: the identity tan 2 x = sec 2 x − 1 \tan^2 x=\sec^2 x-1 tan 2 x = sec 2 x − 1 turns the leftover into an elementary integral in u = tan x u=\tan x u = tan x .
Its base values are J 0 = π 4 J_0=\frac{\pi}{4} J 0 = 4 π and
J 1 = ∫ 0 π / 4 tan x d x = ln 2 J_1=\int_0^{\pi/4}\tan x\,dx=\ln\sqrt{2} J 1 = ∫ 0 π /4 tan x d x = ln 2 .
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[ THEOREM ] Let K n = ∫ 0 π / 4 tan n θ sec θ d θ K_n=\int_0^{\pi/4}\tan^n\theta\sec\theta \, d\theta K n = ∫ 0 π /4 tan n θ sec θ d θ . Then
K n = 1 n ( 2 − ( n − 1 ) K n − 2 ) K_n=\frac{1}{n}\bigl(\sqrt{2}-(n-1)K_{n-2}\bigr) K n = n 1 ( 2 − ( n − 1 ) K n − 2 ) for n ≥ 2 n\ge 2 n ≥ 2 .
Its base values are
K 0 = ∫ 0 π / 4 sec θ d θ = ln ( 1 + 2 ) K_0=\int_0^{\pi/4}\sec\theta\,d\theta=\ln(1+\sqrt{2}) K 0 = ∫ 0 π /4 sec θ d θ = ln ( 1 + 2 ) and
K 1 = ∫ 0 π / 4 tan θ sec θ d θ = 2 − 1 K_1=\int_0^{\pi/4}\tan\theta\sec\theta\,d\theta=\sqrt{2}-1 K 1 = ∫ 0 π /4 tan θ sec θ d θ = 2 − 1 .
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Reduction formulae Leads to Seen questions .