We're given the expression:
e − π / 4 + ∫ 0 π / 4 e − x tan 50 x d x ∫ 0 π / 4 e − x ( tan x ) 49 d x + ∫ 0 π / 4 e − x ( tan x ) 51 d x \frac{e^{-\pi/4} + \int_0^{\pi / 4} e^{-x} \tan ^{50} x dx}{\int_0^{\pi / 4} e^{-x}(\tan x)^{49} dx + \int_0^{\pi / 4} e^{-x}(\tan x)^{51} dx} ∫ 0 π /4 e − x ( t a n x ) 49 d x + ∫ 0 π /4 e − x ( t a n x ) 51 d x e − π /4 + ∫ 0 π /4 e − x t a n 50 x d x
Notice that the integrals in the numerator and denominator have the same form. They both involve an integral of e − x tan n x e^{-x} \tan^n x e − x tan n x from 0 to π / 4 \pi / 4 π /4 , where n n n is an integer. Let's denote this integral as I ( n ) I(n) I ( n ) :
I ( n ) = ∫ 0 π / 4 e − x tan n x d x I(n) = \int_0^{\pi / 4} e^{-x} \tan^n x dx I ( n ) = ∫ 0 π /4 e − x tan n x d x
We can then rewrite the original expression in terms of I ( n ) I(n) I ( n ) :
e − π / 4 + I ( 50 ) I ( 49 ) + I ( 51 ) \frac{e^{-\pi/4} + I(50)}{I(49) + I(51)} I ( 49 ) + I ( 51 ) e − π /4 + I ( 50 )
Now, we'll apply the method of integration by parts, which states that for two functions u ( x ) u(x) u ( x ) and v ( x ) v(x) v ( x ) :
∫ u d v = u v − ∫ v d u \int u dv = uv - \int v du ∫ u d v = uv − ∫ v d u
We'll choose:
u = tan n x , d v = e − x d x u = \tan^n x, \quad dv = e^{-x} dx u = tan n x , d v = e − x d x
Then we get:
d u = n tan n − 1 x sec 2 x d x , v = − e − x du = n \tan^{n-1} x \sec^2 x dx, \quad v = -e^{-x} d u = n tan n − 1 x sec 2 x d x , v = − e − x
Applying integration by parts, we have:
I ( n ) = − e − x tan n x ∣ 0 π / 4 + n ∫ 0 π / 4 e − x tan n − 1 x sec 2 x d x I(n) = -e^{-x} \tan^n x \Bigg|_0^{\pi / 4} + n \int_0^{\pi / 4} e^{-x} \tan^{n-1} x \sec^2 x dx I ( n ) = − e − x tan n x 0 π /4 + n ∫ 0 π /4 e − x tan n − 1 x sec 2 x d x
Since tan ( π / 4 ) = 1 \tan(\pi / 4) = 1 tan ( π /4 ) = 1 , the first term evaluates to:
− e − π / 4 -e^{-\pi / 4} − e − π /4
The second term becomes:
n ∫ 0 π / 4 e − x tan n − 1 x ( 1 + tan 2 x ) d x = n ∫ 0 π / 4 e − x tan n − 1 x d x + n ∫ 0 π / 4 e − x tan n + 1 x d x n \int_0^{\pi / 4} e^{-x} \tan^{n-1} x (1 + \tan^2 x) dx = n \int_0^{\pi / 4} e^{-x} \tan^{n-1} x dx + n \int_0^{\pi / 4} e^{-x} \tan^{n+1} x dx n ∫ 0 π /4 e − x tan n − 1 x ( 1 + tan 2 x ) d x = n ∫ 0 π /4 e − x tan n − 1 x d x + n ∫ 0 π /4 e − x tan n + 1 x d x
This is equal to:
n ( I ( n − 1 ) + I ( n + 1 ) ) n(I(n-1) + I(n+1)) n ( I ( n − 1 ) + I ( n + 1 ))
So we have:
I ( n ) = − e − π / 4 + n ( I ( n − 1 ) + I ( n + 1 ) ) I(n) = -e^{-\pi / 4} + n(I(n-1) + I(n+1)) I ( n ) = − e − π /4 + n ( I ( n − 1 ) + I ( n + 1 ))
Now we can substitute n = 50 n = 50 n = 50 into this equation:
I ( 50 ) = − e − π / 4 + 50 ( I ( 49 ) + I ( 51 ) ) I(50) = -e^{-\pi / 4} + 50(I(49) + I(51)) I ( 50 ) = − e − π /4 + 50 ( I ( 49 ) + I ( 51 ))
So the original expression becomes:
e − π / 4 + I ( 50 ) I ( 49 ) + I ( 51 ) = e − π / 4 − e − π / 4 + 50 ( I ( 49 ) + I ( 51 ) ) I ( 49 ) + I ( 51 ) = 50 \frac{e^{-\pi/4} + I(50)}{I(49) + I(51)} = \frac{e^{-\pi/4} - e^{-\pi / 4} + 50(I(49) + I(51))}{I(49) + I(51)} = 50 I ( 49 ) + I ( 51 ) e − π /4 + I ( 50 ) = I ( 49 ) + I ( 51 ) e − π /4 − e − π /4 + 50 ( I ( 49 ) + I ( 51 )) = 50