Given integral
We need to evaluate
I ( x ) = ∫ sec 2 x − 2022 sin 2022 x d x I(x)=\int \frac{\sec^2 x-2022}{\sin^{2022}x}\,dx I ( x ) = ∫ sin 2022 x sec 2 x − 2022 d x
with the condition
I ( π 4 ) = 2 1011 . I\left(\frac\pi4\right)=2^{1011}. I ( 4 π ) = 2 1011 .
We must then compare I ( π 3 ) I\left(\frac\pi3\right) I ( 3 π ) and I ( π 6 ) I\left(\frac\pi6\right) I ( 6 π ) .
Rewrite the integrand
Notice that
d d x ( cot x ) = − csc 2 x . \frac{d}{dx}(\cot x)=-\csc^2 x. d x d ( cot x ) = − csc 2 x .
Let
t = cot x . t=\cot x. t = cot x .
Then
d t = − csc 2 x d x = − 1 sin 2 x d x ⇒ d x = − sin 2 x d t . dt=-\csc^2 x\,dx=-\frac{1}{\sin^2 x}dx
\quad\Rightarrow\quad
dx=-\sin^2 x\,dt. d t = − csc 2 x d x = − sin 2 x 1 d x ⇒ d x = − sin 2 x d t .
Also,
sin 2 x = 1 1 + cot 2 x = 1 1 + t 2 , \sin^2 x=\frac{1}{1+\cot^2 x}=\frac{1}{1+t^2}, sin 2 x = 1 + cot 2 x 1 = 1 + t 2 1 ,
so
sin 2022 x = ( 1 1 + t 2 ) 1011 . \sin^{2022}x=\left(\frac{1}{1+t^2}\right)^{1011}. sin 2022 x = ( 1 + t 2 1 ) 1011 .
Now simplify the numerator:
sec 2 x − 2022 = ( 1 + tan 2 x ) − 2022. \sec^2 x-2022=(1+\tan^2 x)-2022. sec 2 x − 2022 = ( 1 + tan 2 x ) − 2022.
But a better route is to express using sin x , cos x \sin x,\cos x sin x , cos x :
sec 2 x − 2022 sin 2022 x = 1 cos 2 x sin 2022 x − 2022 sin 2022 x . \frac{\sec^2 x-2022}{\sin^{2022}x}
=\frac{1}{\cos^2 x\sin^{2022}x}-\frac{2022}{\sin^{2022}x}. sin 2022 x sec 2 x − 2022 = cos 2 x sin 2022 x 1 − sin 2022 x 2022 .
This looks messy directly, so instead observe a pattern with differentiation.
Recognize the derivative form
Consider
d d x ( cot x sin 2020 x ) . \frac{d}{dx}\left(\frac{\cot x}{\sin^{2020}x}\right). d x d ( sin 2020 x cot x ) .
Since
cot x sin 2020 x = cos x sin − 2021 x , \frac{\cot x}{\sin^{2020}x}=\cos x\,\sin^{-2021}x, sin 2020 x cot x = cos x sin − 2021 x ,
we differentiate:
d d x ( cos x sin − 2021 x ) = − sin x sin − 2021 x + cos x ( − 2021 ) sin − 2022 x cos x . \frac{d}{dx}(\cos x\sin^{-2021}x)
=-\sin x\sin^{-2021}x+\cos x(-2021)\sin^{-2022}x\cos x. d x d ( cos x sin − 2021 x ) = − sin x sin − 2021 x + cos x ( − 2021 ) sin − 2022 x cos x .
So
= − sin − 2020 x − 2021 cos 2 x sin 2022 x . = -\sin^{-2020}x-2021\frac{\cos^2 x}{\sin^{2022}x}. = − sin − 2020 x − 2021 sin 2022 x cos 2 x .
Now use cos 2 x = 1 − sin 2 x \cos^2 x=1-\sin^2 x cos 2 x = 1 − sin 2 x :
− sin − 2020 x − 2021 1 − sin 2 x sin 2022 x = − sin − 2020 x − 2021 sin − 2022 x + 2021 sin − 2020 x . -\sin^{-2020}x-2021\frac{1-\sin^2 x}{\sin^{2022}x}
= -\sin^{-2020}x-2021\sin^{-2022}x+2021\sin^{-2020}x. − sin − 2020 x − 2021 sin 2022 x 1 − sin 2 x = − sin − 2020 x − 2021 sin − 2022 x + 2021 sin − 2020 x .
Hence
d d x ( cot x sin 2020 x ) = 2020 sin − 2020 x − 2021 sin − 2022 x . \frac{d}{dx}\left(\frac{\cot x}{\sin^{2020}x}\right)
=2020\sin^{-2020}x-2021\sin^{-2022}x. d x d ( sin 2020 x cot x ) = 2020 sin − 2020 x − 2021 sin − 2022 x .
This is still not exactly the integrand.
Let us instead try differentiating
tan x sin − 2021 x . \tan x\,\sin^{-2021}x. tan x sin − 2021 x .
That is cumbersome too.
So let us do a clean substitution.
Use substitution u = cot x u=\cot x u = cot x properly
Let
u = cot x . u=\cot x. u = cot x .
Then
d u = − csc 2 x d x = − d x sin 2 x ⇒ d x = − sin 2 x d u . du=-\csc^2 x\,dx=-\frac{dx}{\sin^2 x}
\quad\Rightarrow\quad dx=-\sin^2 x\,du. d u = − csc 2 x d x = − sin 2 x d x ⇒ d x = − sin 2 x d u .
Also,
sec 2 x = 1 + tan 2 x = 1 + 1 u 2 = u 2 + 1 u 2 . \sec^2 x = 1+\tan^2 x = 1+\frac{1}{u^2} = \frac{u^2+1}{u^2}. sec 2 x = 1 + tan 2 x = 1 + u 2 1 = u 2 u 2 + 1 .
And since
1 + u 2 = csc 2 x = 1 sin 2 x , 1+u^2=\csc^2 x=\frac1{\sin^2 x}, 1 + u 2 = csc 2 x = sin 2 x 1 ,
we get
sin 2022 x = ( 1 + u 2 ) − 1011 . \sin^{2022}x=(1+u^2)^{-1011}. sin 2022 x = ( 1 + u 2 ) − 1011 .
Therefore,
sec 2 x − 2022 sin 2022 x d x = ( u 2 + 1 u 2 − 2022 ) ( 1 + u 2 ) 1011 ( − sin 2 x ) d u . \frac{\sec^2 x-2022}{\sin^{2022}x}dx
=\left(\frac{u^2+1}{u^2}-2022\right)(1+u^2)^{1011}(-\sin^2 x)du. sin 2022 x sec 2 x − 2022 d x = ( u 2 u 2 + 1 − 2022 ) ( 1 + u 2 ) 1011 ( − sin 2 x ) d u .
But
sin 2 x = 1 1 + u 2 , \sin^2 x=\frac1{1+u^2}, sin 2 x = 1 + u 2 1 ,
so this becomes
− ( u 2 + 1 u 2 − 2022 ) ( 1 + u 2 ) 1010 d u . -\left(\frac{u^2+1}{u^2}-2022\right)(1+u^2)^{1010}du. − ( u 2 u 2 + 1 − 2022 ) ( 1 + u 2 ) 1010 d u .
Now simplify the bracket:
u 2 + 1 u 2 − 2022 = 1 + 1 u 2 − 2022 = 1 u 2 − 2021. \frac{u^2+1}{u^2}-2022=1+\frac1{u^2}-2022=\frac1{u^2}-2021. u 2 u 2 + 1 − 2022 = 1 + u 2 1 − 2022 = u 2 1 − 2021.
Thus
I = ∫ − ( 1 u 2 − 2021 ) ( 1 + u 2 ) 1010 d u . I=\int -\left(\frac1{u^2}-2021\right)(1+u^2)^{1010}du. I = ∫ − ( u 2 1 − 2021 ) ( 1 + u 2 ) 1010 d u .
This still looks complicated, so let us search for a derivative of a simpler expression.
Key observation
Consider
F ( x ) = cot x csc 2020 x = cot x sin 2020 x . F(x)=\cot x\,\csc^{2020}x=\frac{\cot x}{\sin^{2020}x}. F ( x ) = cot x csc 2020 x = sin 2020 x cot x .
Differentiate using product rule in standard trig form:
d d x ( cot x csc 2020 x ) = ( − csc 2 x ) csc 2020 x + cot x ⋅ 2020 csc 2019 x ( − csc x cot x ) . \frac{d}{dx}(\cot x\,\csc^{2020}x)
=( -\csc^2 x)\csc^{2020}x+\cot x\cdot 2020\csc^{2019}x(-\csc x\cot x). d x d ( cot x csc 2020 x ) = ( − csc 2 x ) csc 2020 x + cot x ⋅ 2020 csc 2019 x ( − csc x cot x ) .
So
= − csc 2022 x − 2020 cot 2 x csc 2020 x . = -\csc^{2022}x-2020\cot^2 x\csc^{2020}x. = − csc 2022 x − 2020 cot 2 x csc 2020 x .
Factor csc 2020 x \csc^{2020}x csc 2020 x :
= − csc 2020 x ( csc 2 x + 2020 cot 2 x ) . = -\csc^{2020}x(\csc^2 x+2020\cot^2 x). = − csc 2020 x ( csc 2 x + 2020 cot 2 x ) .
Using
csc 2 x = 1 + cot 2 x , \csc^2 x=1+\cot^2 x, csc 2 x = 1 + cot 2 x ,
we get
csc 2 x + 2020 cot 2 x = 1 + 2021 cot 2 x . \csc^2 x+2020\cot^2 x = 1+2021\cot^2 x. csc 2 x + 2020 cot 2 x = 1 + 2021 cot 2 x .
Hence
d d x ( cot x csc 2020 x ) = − csc 2020 x ( 1 + 2021 cot 2 x ) . \frac{d}{dx}(\cot x\,\csc^{2020}x)= -\csc^{2020}x(1+2021\cot^2 x). d x d ( cot x csc 2020 x ) = − csc 2020 x ( 1 + 2021 cot 2 x ) .
Now write in terms of sin x , cos x \sin x,\cos x sin x , cos x :
− 1 sin 2020 x ( 1 + 2021 cos 2 x sin 2 x ) = − sin 2 x + 2021 cos 2 x sin 2022 x . -\frac{1}{\sin^{2020}x}\left(1+2021\frac{\cos^2 x}{\sin^2 x}\right)
= -\frac{\sin^2 x+2021\cos^2 x}{\sin^{2022}x}. − sin 2020 x 1 ( 1 + 2021 sin 2 x cos 2 x ) = − sin 2022 x sin 2 x + 2021 cos 2 x .
Since
sin 2 x + 2021 cos 2 x = 1 + 2020 cos 2 x , \sin^2 x+2021\cos^2 x = 1+2020\cos^2 x, sin 2 x + 2021 cos 2 x = 1 + 2020 cos 2 x ,
this becomes
− 1 + 2020 cos 2 x sin 2022 x . -\frac{1+2020\cos^2 x}{\sin^{2022}x}. − sin 2022 x 1 + 2020 cos 2 x .
Now compare with the integrand:
sec 2 x − 2022 sin 2022 x . \frac{\sec^2 x-2022}{\sin^{2022}x}. sin 2022 x sec 2 x − 2022 .
Multiply numerator of our derivative expression by sec 2 x \sec^2 x sec 2 x relation:
sec 2 x − 2022 = 1 − 2022 cos 2 x cos 2 x . \sec^2 x-2022=\frac{1-2022\cos^2 x}{\cos^2 x}. sec 2 x − 2022 = cos 2 x 1 − 2022 cos 2 x .
This does not match directly. So we try another candidate.
Try differentiating tan x csc 2021 x \tan x\,\csc^{2021}x tan x csc 2021 x
Let
F ( x ) = tan x csc 2021 x . F(x)=\tan x\,\csc^{2021}x. F ( x ) = tan x csc 2021 x .
Then
F ′ ( x ) = sec 2 x csc 2021 x + tan x ⋅ 2021 csc 2020 x ( − csc x cot x ) . F'(x)=\sec^2 x\,\csc^{2021}x+\tan x\cdot 2021\csc^{2020}x(-\csc x\cot x). F ′ ( x ) = sec 2 x csc 2021 x + tan x ⋅ 2021 csc 2020 x ( − csc x cot x ) .
Since tan x cot x = 1 \tan x\cot x=1 tan x cot x = 1 ,
F ′ ( x ) = sec 2 x csc 2021 x − 2021 csc 2022 x . F'(x)=\sec^2 x\,\csc^{2021}x-2021\csc^{2022}x. F ′ ( x ) = sec 2 x csc 2021 x − 2021 csc 2022 x .
Factor csc 2021 x \csc^{2021}x csc 2021 x :
F ′ ( x ) = csc 2021 x ( sec 2 x − 2021 csc x ) . F'(x)=\csc^{2021}x(\sec^2 x-2021\csc x). F ′ ( x ) = csc 2021 x ( sec 2 x − 2021 csc x ) .
Not the same.
Instead, consider
F ( x ) = tan x sin 2021 x = sec x csc 2020 x ? F(x)=\frac{\tan x}{\sin^{2021}x}=\sec x\csc^{2020}x? F ( x ) = sin 2021 x tan x = sec x csc 2020 x ?
Still awkward.
A simpler direct rewrite
Observe that
sec 2 x = 1 cos 2 x = 1 + tan 2 x = 1 + sin 2 x cos 2 x . \sec^2 x=\frac{1}{\cos^2 x}=1+\tan^2 x=1+\frac{\sin^2 x}{\cos^2 x}. sec 2 x = cos 2 x 1 = 1 + tan 2 x = 1 + cos 2 x sin 2 x .
A much better trick is to split:
sec 2 x − 2022 sin 2022 x = 1 cos 2 x sin 2022 x − 2022 sin 2022 x . \frac{\sec^2 x-2022}{\sin^{2022}x}
=\frac{1}{\cos^2 x\sin^{2022}x}-\frac{2022}{\sin^{2022}x}. sin 2022 x sec 2 x − 2022 = cos 2 x sin 2022 x 1 − sin 2022 x 2022 .
Now let
u = cot x = cos x sin x . u=\cot x=\frac{\cos x}{\sin x}. u = cot x = sin x cos x .
Then
1 + u 2 = csc 2 x , 1+u^2=\csc^2 x, 1 + u 2 = csc 2 x ,
so
sin − 2022 x = ( 1 + u 2 ) 1011 , \sin^{-2022}x=(1+u^2)^{1011}, sin − 2022 x = ( 1 + u 2 ) 1011 ,
and
cos 2 x = u 2 sin 2 x = u 2 1 + u 2 . \cos^2 x=u^2\sin^2 x=\frac{u^2}{1+u^2}. cos 2 x = u 2 sin 2 x = 1 + u 2 u 2 .
Hence
1 cos 2 x sin 2022 x = 1 + u 2 u 2 ( 1 + u 2 ) 1011 = ( 1 + u 2 ) 1012 u 2 . \frac{1}{\cos^2 x\sin^{2022}x}
=\frac{1+u^2}{u^2}(1+u^2)^{1011}
=\frac{(1+u^2)^{1012}}{u^2}. cos 2 x sin 2022 x 1 = u 2 1 + u 2 ( 1 + u 2 ) 1011 = u 2 ( 1 + u 2 ) 1012 .
Also,
d x = − d u 1 + u 2 . dx=-\frac{du}{1+u^2}. d x = − 1 + u 2 d u .
Therefore
I = ∫ [ ( 1 + u 2 ) 1012 u 2 − 2022 ( 1 + u 2 ) 1011 ] ( − d u 1 + u 2 ) . I=\int \left[\frac{(1+u^2)^{1012}}{u^2}-2022(1+u^2)^{1011}\right]\left(-\frac{du}{1+u^2}\right). I = ∫ [ u 2 ( 1 + u 2 ) 1012 − 2022 ( 1 + u 2 ) 1011 ] ( − 1 + u 2 d u ) .
So
I = − ∫ [ ( 1 + u 2 ) 1011 u 2 − 2022 ( 1 + u 2 ) 1010 ] d u . I=-\int \left[\frac{(1+u^2)^{1011}}{u^2}-2022(1+u^2)^{1010}\right]du. I = − ∫ [ u 2 ( 1 + u 2 ) 1011 − 2022 ( 1 + u 2 ) 1010 ] d u .
Now combine terms:
1 + u 2 u 2 − 2022 = 1 u 2 − 2021 , \frac{1+u^2}{u^2}-2022=\frac1{u^2}-2021, u 2 1 + u 2 − 2022 = u 2 1 − 2021 ,
thus
I = − ∫ ( 1 + u 2 ) 1010 ( 1 u 2 − 2021 ) d u . I=-\int (1+u^2)^{1010}\left(\frac1{u^2}-2021\right)du. I = − ∫ ( 1 + u 2 ) 1010 ( u 2 1 − 2021 ) d u .
But
d d u ( ( 1 + u 2 ) 1011 u ) = 2022 u ( 1 + u 2 ) 1010 ⋅ u − ( 1 + u 2 ) 1011 u 2 \frac{d}{du}\left(\frac{(1+u^2)^{1011}}{u}\right)
=\frac{2022u(1+u^2)^{1010}\cdot u-(1+u^2)^{1011}}{u^2} d u d ( u ( 1 + u 2 ) 1011 ) = u 2 2022 u ( 1 + u 2 ) 1010 ⋅ u − ( 1 + u 2 ) 1011
= ( 1 + u 2 ) 1010 ( 2022 u 2 − ( 1 + u 2 ) ) u 2 =\frac{(1+u^2)^{1010}(2022u^2-(1+u^2))}{u^2} = u 2 ( 1 + u 2 ) 1010 ( 2022 u 2 − ( 1 + u 2 ))
= ( 1 + u 2 ) 1010 2021 u 2 − 1 u 2 = − ( 1 + u 2 ) 1010 ( 1 u 2 − 2021 ) . =(1+u^2)^{1010}\frac{2021u^2-1}{u^2}
=-(1+u^2)^{1010}\left(\frac1{u^2}-2021\right). = ( 1 + u 2 ) 1010 u 2 2021 u 2 − 1 = − ( 1 + u 2 ) 1010 ( u 2 1 − 2021 ) .
This is exactly the integrand in u u u .
Hence,
I = ( 1 + u 2 ) 1011 u + C . I=\frac{(1+u^2)^{1011}}{u}+C. I = u ( 1 + u 2 ) 1011 + C .
Substitute back u = cot x u=\cot x u = cot x :
I ( x ) = ( 1 + cot 2 x ) 1011 cot x + C = csc 2022 x cot x + C . I(x)=\frac{(1+\cot^2 x)^{1011}}{\cot x}+C
=\frac{\csc^{2022}x}{\cot x}+C. I ( x ) = cot x ( 1 + cot 2 x ) 1011 + C = cot x csc 2022 x + C .
Since
csc 2022 x cot x = 1 sin 2022 x ⋅ sin x cos x = 1 sin 2021 x cos x , \frac{\csc^{2022}x}{\cot x}
=\frac{1}{\sin^{2022}x}\cdot\frac{\sin x}{\cos x}
=\frac{1}{\sin^{2021}x\cos x}, cot x csc 2022 x = sin 2022 x 1 ⋅ cos x sin x = sin 2021 x cos x 1 ,
we get
I ( x ) = 1 sin 2021 x cos x + C . I(x)=\frac{1}{\sin^{2021}x\cos x}+C. I ( x ) = sin 2021 x cos x 1 + C .
Use the condition I ( π / 4 ) = 2 1011 I(\pi/4)=2^{1011} I ( π /4 ) = 2 1011
At x = π / 4 x=\pi/4 x = π /4 ,
sin π 4 = cos π 4 = 1 2 . \sin\frac\pi4=\cos\frac\pi4=\frac{1}{\sqrt2}. sin 4 π = cos 4 π = 2 1 .
So
I ( π 4 ) = 1 ( 1 2 ) 2021 ( 1 2 ) + C = 1 ( 1 2 ) 2022 + C = 2 1011 + C . I\left(\frac\pi4\right)=\frac{1}{\left(\frac1{\sqrt2}\right)^{2021}\left(\frac1{\sqrt2}\right)}+C
=\frac{1}{\left(\frac1{\sqrt2}\right)^{2022}}+C
=2^{1011}+C. I ( 4 π ) = ( 2 1 ) 2021 ( 2 1 ) 1 + C = ( 2 1 ) 2022 1 + C = 2 1011 + C .
Given this equals 2 1011 2^{1011} 2 1011 , we get
C = 0. C=0. C = 0.
Therefore,
I ( x ) = 1 sin 2021 x cos x . I(x)=\frac{1}{\sin^{2021}x\cos x}. I ( x ) = sin 2021 x cos x 1 .
Compute I ( π 3 ) I\left(\frac\pi3\right) I ( 3 π ) and I ( π 6 ) I\left(\frac\pi6\right) I ( 6 π )
At x = π 3 x=\frac\pi3 x = 3 π
sin π 3 = 3 2 , cos π 3 = 1 2 . \sin\frac\pi3=\frac{\sqrt3}{2},\qquad \cos\frac\pi3=\frac12. sin 3 π = 2 3 , cos 3 π = 2 1 .
Thus
I ( π 3 ) = 1 ( 3 2 ) 2021 ⋅ 1 2 = 2 ( 3 2 ) 2021 . I\left(\frac\pi3\right)=\frac{1}{\left(\frac{\sqrt3}{2}\right)^{2021}\cdot\frac12}
=\frac{2}{\left(\frac{\sqrt3}{2}\right)^{2021}}. I ( 3 π ) = ( 2 3 ) 2021 ⋅ 2 1 1 = ( 2 3 ) 2021 2 .
Now
( 3 2 ) 2021 = 3 1010 ( 3 ) 2 2021 . \left(\frac{\sqrt3}{2}\right)^{2021}=\frac{3^{1010}(\sqrt3)}{2^{2021}}. ( 2 3 ) 2021 = 2 2021 3 1010 ( 3 ) .
So
I ( π 3 ) = 2 ⋅ 2 2021 3 1010 3 = 2 2022 3 1010 3 . I\left(\frac\pi3\right)=2\cdot \frac{2^{2021}}{3^{1010}\sqrt3}
=\frac{2^{2022}}{3^{1010}\sqrt3}. I ( 3 π ) = 2 ⋅ 3 1010 3 2 2021 = 3 1010 3 2 2022 .
At x = π 6 x=\frac\pi6 x = 6 π
sin π 6 = 1 2 , cos π 6 = 3 2 . \sin\frac\pi6=\frac12,\qquad \cos\frac\pi6=\frac{\sqrt3}{2}. sin 6 π = 2 1 , cos 6 π = 2 3 .
Thus
I ( π 6 ) = 1 ( 1 2 ) 2021 ⋅ 3 2 = 2 2022 3 . I\left(\frac\pi6\right)=\frac{1}{\left(\frac12\right)^{2021}\cdot\frac{\sqrt3}{2}}
=\frac{2^{2022}}{\sqrt3}. I ( 6 π ) = ( 2 1 ) 2021 ⋅ 2 3 1 = 3 2 2022 .
Therefore,
I ( π 6 ) = 3 1010 I ( π 3 ) . I\left(\frac\pi6\right)=3^{1010}I\left(\frac\pi3\right). I ( 6 π ) = 3 1010 I ( 3 π ) .
Equivalently,
3 1010 I ( π 3 ) − I ( π 6 ) = 0. 3^{1010}I\left(\frac\pi3\right)-I\left(\frac\pi6\right)=0. 3 1010 I ( 3 π ) − I ( 6 π ) = 0.
So Option A is correct.
Check all options
A: 3 1010 I ( π 3 ) − I ( π 6 ) = 0 3^{1010}I\left(\frac\pi3\right)-I\left(\frac\pi6\right)=0 3 1010 I ( 3 π ) − I ( 6 π ) = 0 ✅
B: 3 1010 I ( π 6 ) − I ( π 3 ) = 0 3^{1010}I\left(\frac\pi6\right)-I\left(\frac\pi3\right)=0 3 1010 I ( 6 π ) − I ( 3 π ) = 0 ❌
C: 3 1011 I ( π 3 ) − I ( π 6 ) = 0 3^{1011}I\left(\frac\pi3\right)-I\left(\frac\pi6\right)=0 3 1011 I ( 3 π ) − I ( 6 π ) = 0 ❌
D: 3 1011 I ( π 6 ) − I ( π 3 ) = 0 3^{1011}I\left(\frac\pi6\right)-I\left(\frac\pi3\right)=0 3 1011 I ( 6 π ) − I ( 3 π ) = 0 ❌
Hence the single correct answer is A .
Comparison with stored correct answer
Stored correct answer: A
Our derived answer: A
So they agree.