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Indefinite Integrals question

2022 · 29 Jul · Shift 2 · Q28
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  5. /2022 · 29 Jul · Shift 2 · Q28

Indefinite Integrals question

2022 · 29 Jul · Shift 2 · Q28

JEE MainMathematicsIndefinite IntegralsMCQ+4 / −1
For I(x)=∫sec⁡2x−2022sin⁡2022xdxI(x)=\int \frac{\sec ^{2} x-2022}{\sin ^{2022} x} d xI(x)=∫sin2022xsec2x−2022​dx, if I(π4)=21011I\left(\frac{\pi}{4}\right)=2^{1011}I(4π​)=21011, then
  1. A
    31010I(π3)−I(π6)=03^{1010} I\left(\frac{\pi}{3}\right)-I\left(\frac{\pi}{6}\right)=031010I(3π​)−I(6π​)=0
  2. B
    31010I(π6)−I(π3)=03^{1010} I\left(\frac{\pi}{6}\right)-I\left(\frac{\pi}{3}\right)=031010I(6π​)−I(3π​)=0
  3. C
    31011I(π3)−I(π6)=03^{1011} I\left(\frac{\pi}{3}\right)-I\left(\frac{\pi}{6}\right)=031011I(3π​)−I(6π​)=0
  4. D
    31011I(π6)−I(π3)=03^{1011} I\left(\frac{\pi}{6}\right)-I\left(\frac{\pi}{3}\right)=031011I(6π​)−I(3π​)=0
View written solutionFree

Correct answer: A

  1. Given integral

We need to evaluate

I(x)=∫sec⁡2x−2022sin⁡2022x dxI(x)=\int \frac{\sec^2 x-2022}{\sin^{2022}x}\,dxI(x)=∫sin2022xsec2x−2022​dx

with the condition

I(π4)=21011.I\left(\frac\pi4\right)=2^{1011}.I(4π​)=21011.

We must then compare I(π3)I\left(\frac\pi3\right)I(3π​) and I(π6)I\left(\frac\pi6\right)I(6π​).


  1. Rewrite the integrand

Notice that

ddx(cot⁡x)=−csc⁡2x.\frac{d}{dx}(\cot x)=-\csc^2 x.dxd​(cotx)=−csc2x.

Let

t=cot⁡x.t=\cot x.t=cotx.

Then

dt=−csc⁡2x dx=−1sin⁡2xdx⇒dx=−sin⁡2x dt.dt=-\csc^2 x\,dx=-\frac{1}{\sin^2 x}dx \quad\Rightarrow\quad dx=-\sin^2 x\,dt.dt=−csc2xdx=−sin2x1​dx⇒dx=−sin2xdt.

Also,

sin⁡2x=11+cot⁡2x=11+t2,\sin^2 x=\frac{1}{1+\cot^2 x}=\frac{1}{1+t^2},sin2x=1+cot2x1​=1+t21​,

so

sin⁡2022x=(11+t2)1011.\sin^{2022}x=\left(\frac{1}{1+t^2}\right)^{1011}.sin2022x=(1+t21​)1011.

Now simplify the numerator:

sec⁡2x−2022=(1+tan⁡2x)−2022.\sec^2 x-2022=(1+\tan^2 x)-2022.sec2x−2022=(1+tan2x)−2022.

But a better route is to express using sin⁡x,cos⁡x\sin x,\cos xsinx,cosx:

sec⁡2x−2022sin⁡2022x=1cos⁡2xsin⁡2022x−2022sin⁡2022x.\frac{\sec^2 x-2022}{\sin^{2022}x} =\frac{1}{\cos^2 x\sin^{2022}x}-\frac{2022}{\sin^{2022}x}.sin2022xsec2x−2022​=cos2xsin2022x1​−sin2022x2022​.

This looks messy directly, so instead observe a pattern with differentiation.


  1. Recognize the derivative form

Consider

ddx(cot⁡xsin⁡2020x).\frac{d}{dx}\left(\frac{\cot x}{\sin^{2020}x}\right).dxd​(sin2020xcotx​).

Since

cot⁡xsin⁡2020x=cos⁡x sin⁡−2021x,\frac{\cot x}{\sin^{2020}x}=\cos x\,\sin^{-2021}x,sin2020xcotx​=cosxsin−2021x,

we differentiate:

ddx(cos⁡xsin⁡−2021x)=−sin⁡xsin⁡−2021x+cos⁡x(−2021)sin⁡−2022xcos⁡x.\frac{d}{dx}(\cos x\sin^{-2021}x) =-\sin x\sin^{-2021}x+\cos x(-2021)\sin^{-2022}x\cos x.dxd​(cosxsin−2021x)=−sinxsin−2021x+cosx(−2021)sin−2022xcosx.

So

=−sin⁡−2020x−2021cos⁡2xsin⁡2022x.= -\sin^{-2020}x-2021\frac{\cos^2 x}{\sin^{2022}x}.=−sin−2020x−2021sin2022xcos2x​.

Now use cos⁡2x=1−sin⁡2x\cos^2 x=1-\sin^2 xcos2x=1−sin2x:

−sin⁡−2020x−20211−sin⁡2xsin⁡2022x=−sin⁡−2020x−2021sin⁡−2022x+2021sin⁡−2020x.-\sin^{-2020}x-2021\frac{1-\sin^2 x}{\sin^{2022}x} = -\sin^{-2020}x-2021\sin^{-2022}x+2021\sin^{-2020}x.−sin−2020x−2021sin2022x1−sin2x​=−sin−2020x−2021sin−2022x+2021sin−2020x.

Hence

ddx(cot⁡xsin⁡2020x)=2020sin⁡−2020x−2021sin⁡−2022x.\frac{d}{dx}\left(\frac{\cot x}{\sin^{2020}x}\right) =2020\sin^{-2020}x-2021\sin^{-2022}x.dxd​(sin2020xcotx​)=2020sin−2020x−2021sin−2022x.

This is still not exactly the integrand.

Let us instead try differentiating

tan⁡x sin⁡−2021x.\tan x\,\sin^{-2021}x.tanxsin−2021x.

That is cumbersome too.

So let us do a clean substitution.


  1. Use substitution u=cot⁡xu=\cot xu=cotx properly

Let

u=cot⁡x.u=\cot x.u=cotx.

Then

du=−csc⁡2x dx=−dxsin⁡2x⇒dx=−sin⁡2x du.du=-\csc^2 x\,dx=-\frac{dx}{\sin^2 x} \quad\Rightarrow\quad dx=-\sin^2 x\,du.du=−csc2xdx=−sin2xdx​⇒dx=−sin2xdu.

Also,

sec⁡2x=1+tan⁡2x=1+1u2=u2+1u2.\sec^2 x = 1+\tan^2 x = 1+\frac{1}{u^2} = \frac{u^2+1}{u^2}.sec2x=1+tan2x=1+u21​=u2u2+1​.

And since

1+u2=csc⁡2x=1sin⁡2x,1+u^2=\csc^2 x=\frac1{\sin^2 x},1+u2=csc2x=sin2x1​,

we get

sin⁡2022x=(1+u2)−1011.\sin^{2022}x=(1+u^2)^{-1011}.sin2022x=(1+u2)−1011.

Therefore,

sec⁡2x−2022sin⁡2022xdx=(u2+1u2−2022)(1+u2)1011(−sin⁡2x)du.\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.sin2022xsec2x−2022​dx=(u2u2+1​−2022)(1+u2)1011(−sin2x)du.

But

sin⁡2x=11+u2,\sin^2 x=\frac1{1+u^2},sin2x=1+u21​,

so this becomes

−(u2+1u2−2022)(1+u2)1010du.-\left(\frac{u^2+1}{u^2}-2022\right)(1+u^2)^{1010}du.−(u2u2+1​−2022)(1+u2)1010du.

Now simplify the bracket:

u2+1u2−2022=1+1u2−2022=1u2−2021.\frac{u^2+1}{u^2}-2022=1+\frac1{u^2}-2022=\frac1{u^2}-2021.u2u2+1​−2022=1+u21​−2022=u21​−2021.

Thus

I=∫−(1u2−2021)(1+u2)1010du.I=\int -\left(\frac1{u^2}-2021\right)(1+u^2)^{1010}du.I=∫−(u21​−2021)(1+u2)1010du.

This still looks complicated, so let us search for a derivative of a simpler expression.


  1. Key observation

Consider

F(x)=cot⁡x csc⁡2020x=cot⁡xsin⁡2020x.F(x)=\cot x\,\csc^{2020}x=\frac{\cot x}{\sin^{2020}x}.F(x)=cotxcsc2020x=sin2020xcotx​.

Differentiate using product rule in standard trig form:

ddx(cot⁡x csc⁡2020x)=(−csc⁡2x)csc⁡2020x+cot⁡x⋅2020csc⁡2019x(−csc⁡xcot⁡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).dxd​(cotxcsc2020x)=(−csc2x)csc2020x+cotx⋅2020csc2019x(−cscxcotx).

So

=−csc⁡2022x−2020cot⁡2xcsc⁡2020x.= -\csc^{2022}x-2020\cot^2 x\csc^{2020}x.=−csc2022x−2020cot2xcsc2020x.

Factor csc⁡2020x\csc^{2020}xcsc2020x:

=−csc⁡2020x(csc⁡2x+2020cot⁡2x).= -\csc^{2020}x(\csc^2 x+2020\cot^2 x).=−csc2020x(csc2x+2020cot2x).

Using

csc⁡2x=1+cot⁡2x,\csc^2 x=1+\cot^2 x,csc2x=1+cot2x,

we get

csc⁡2x+2020cot⁡2x=1+2021cot⁡2x.\csc^2 x+2020\cot^2 x = 1+2021\cot^2 x.csc2x+2020cot2x=1+2021cot2x.

Hence

ddx(cot⁡x csc⁡2020x)=−csc⁡2020x(1+2021cot⁡2x).\frac{d}{dx}(\cot x\,\csc^{2020}x)= -\csc^{2020}x(1+2021\cot^2 x).dxd​(cotxcsc2020x)=−csc2020x(1+2021cot2x).

Now write in terms of sin⁡x,cos⁡x\sin x,\cos xsinx,cosx:

−1sin⁡2020x(1+2021cos⁡2xsin⁡2x)=−sin⁡2x+2021cos⁡2xsin⁡2022x.-\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}.−sin2020x1​(1+2021sin2xcos2x​)=−sin2022xsin2x+2021cos2x​.

Since

sin⁡2x+2021cos⁡2x=1+2020cos⁡2x,\sin^2 x+2021\cos^2 x = 1+2020\cos^2 x,sin2x+2021cos2x=1+2020cos2x,

this becomes

−1+2020cos⁡2xsin⁡2022x.-\frac{1+2020\cos^2 x}{\sin^{2022}x}.−sin2022x1+2020cos2x​.

Now compare with the integrand:

sec⁡2x−2022sin⁡2022x.\frac{\sec^2 x-2022}{\sin^{2022}x}.sin2022xsec2x−2022​.

Multiply numerator of our derivative expression by sec⁡2x\sec^2 xsec2x relation:

sec⁡2x−2022=1−2022cos⁡2xcos⁡2x.\sec^2 x-2022=\frac{1-2022\cos^2 x}{\cos^2 x}.sec2x−2022=cos2x1−2022cos2x​.

This does not match directly. So we try another candidate.


  1. Try differentiating tan⁡x csc⁡2021x\tan x\,\csc^{2021}xtanxcsc2021x

Let

F(x)=tan⁡x csc⁡2021x.F(x)=\tan x\,\csc^{2021}x.F(x)=tanxcsc2021x.

Then

F′(x)=sec⁡2x csc⁡2021x+tan⁡x⋅2021csc⁡2020x(−csc⁡xcot⁡x).F'(x)=\sec^2 x\,\csc^{2021}x+\tan x\cdot 2021\csc^{2020}x(-\csc x\cot x).F′(x)=sec2xcsc2021x+tanx⋅2021csc2020x(−cscxcotx).

Since tan⁡xcot⁡x=1\tan x\cot x=1tanxcotx=1,

F′(x)=sec⁡2x csc⁡2021x−2021csc⁡2022x.F'(x)=\sec^2 x\,\csc^{2021}x-2021\csc^{2022}x.F′(x)=sec2xcsc2021x−2021csc2022x.

Factor csc⁡2021x\csc^{2021}xcsc2021x:

F′(x)=csc⁡2021x(sec⁡2x−2021csc⁡x).F'(x)=\csc^{2021}x(\sec^2 x-2021\csc x).F′(x)=csc2021x(sec2x−2021cscx).

Not the same.

Instead, consider

F(x)=tan⁡xsin⁡2021x=sec⁡xcsc⁡2020x?F(x)=\frac{\tan x}{\sin^{2021}x}=\sec x\csc^{2020}x?F(x)=sin2021xtanx​=secxcsc2020x?

Still awkward.


  1. A simpler direct rewrite

Observe that

sec⁡2x=1cos⁡2x=1+tan⁡2x=1+sin⁡2xcos⁡2x.\sec^2 x=\frac{1}{\cos^2 x}=1+\tan^2 x=1+\frac{\sin^2 x}{\cos^2 x}.sec2x=cos2x1​=1+tan2x=1+cos2xsin2x​.

A much better trick is to split:

sec⁡2x−2022sin⁡2022x=1cos⁡2xsin⁡2022x−2022sin⁡2022x.\frac{\sec^2 x-2022}{\sin^{2022}x} =\frac{1}{\cos^2 x\sin^{2022}x}-\frac{2022}{\sin^{2022}x}.sin2022xsec2x−2022​=cos2xsin2022x1​−sin2022x2022​.

Now let

u=cot⁡x=cos⁡xsin⁡x.u=\cot x=\frac{\cos x}{\sin x}.u=cotx=sinxcosx​.

Then

1+u2=csc⁡2x,1+u^2=\csc^2 x,1+u2=csc2x,

so

sin⁡−2022x=(1+u2)1011,\sin^{-2022}x=(1+u^2)^{1011},sin−2022x=(1+u2)1011,

and

cos⁡2x=u2sin⁡2x=u21+u2.\cos^2 x=u^2\sin^2 x=\frac{u^2}{1+u^2}.cos2x=u2sin2x=1+u2u2​.

Hence

1cos⁡2xsin⁡2022x=1+u2u2(1+u2)1011=(1+u2)1012u2.\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}.cos2xsin2022x1​=u21+u2​(1+u2)1011=u2(1+u2)1012​.

Also,

dx=−du1+u2.dx=-\frac{du}{1+u^2}.dx=−1+u2du​.

Therefore

I=∫[(1+u2)1012u2−2022(1+u2)1011](−du1+u2).I=\int \left[\frac{(1+u^2)^{1012}}{u^2}-2022(1+u^2)^{1011}\right]\left(-\frac{du}{1+u^2}\right).I=∫[u2(1+u2)1012​−2022(1+u2)1011](−1+u2du​).

So

I=−∫[(1+u2)1011u2−2022(1+u2)1010]du.I=-\int \left[\frac{(1+u^2)^{1011}}{u^2}-2022(1+u^2)^{1010}\right]du.I=−∫[u2(1+u2)1011​−2022(1+u2)1010]du.

Now combine terms:

1+u2u2−2022=1u2−2021,\frac{1+u^2}{u^2}-2022=\frac1{u^2}-2021,u21+u2​−2022=u21​−2021,

thus

I=−∫(1+u2)1010(1u2−2021)du.I=-\int (1+u^2)^{1010}\left(\frac1{u^2}-2021\right)du.I=−∫(1+u2)1010(u21​−2021)du.

But

ddu((1+u2)1011u)=2022u(1+u2)1010⋅u−(1+u2)1011u2\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}dud​(u(1+u2)1011​)=u22022u(1+u2)1010⋅u−(1+u2)1011​ =(1+u2)1010(2022u2−(1+u2))u2=\frac{(1+u^2)^{1010}(2022u^2-(1+u^2))}{u^2}=u2(1+u2)1010(2022u2−(1+u2))​ =(1+u2)10102021u2−1u2=−(1+u2)1010(1u2−2021).=(1+u^2)^{1010}\frac{2021u^2-1}{u^2} =-(1+u^2)^{1010}\left(\frac1{u^2}-2021\right).=(1+u2)1010u22021u2−1​=−(1+u2)1010(u21​−2021).

This is exactly the integrand in uuu.

Hence,

I=(1+u2)1011u+C.I=\frac{(1+u^2)^{1011}}{u}+C.I=u(1+u2)1011​+C.

Substitute back u=cot⁡xu=\cot xu=cotx:

I(x)=(1+cot⁡2x)1011cot⁡x+C=csc⁡2022xcot⁡x+C.I(x)=\frac{(1+\cot^2 x)^{1011}}{\cot x}+C =\frac{\csc^{2022}x}{\cot x}+C.I(x)=cotx(1+cot2x)1011​+C=cotxcsc2022x​+C.

Since

csc⁡2022xcot⁡x=1sin⁡2022x⋅sin⁡xcos⁡x=1sin⁡2021xcos⁡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},cotxcsc2022x​=sin2022x1​⋅cosxsinx​=sin2021xcosx1​,

we get

I(x)=1sin⁡2021xcos⁡x+C.I(x)=\frac{1}{\sin^{2021}x\cos x}+C.I(x)=sin2021xcosx1​+C.
  1. Use the condition I(π/4)=21011I(\pi/4)=2^{1011}I(π/4)=21011

At x=π/4x=\pi/4x=π/4,

sin⁡π4=cos⁡π4=12.\sin\frac\pi4=\cos\frac\pi4=\frac{1}{\sqrt2}.sin4π​=cos4π​=2​1​.

So

I(π4)=1(12)2021(12)+C=1(12)2022+C=21011+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(4π​)=(2​1​)2021(2​1​)1​+C=(2​1​)20221​+C=21011+C.

Given this equals 210112^{1011}21011, we get

C=0.C=0.C=0.

Therefore,

I(x)=1sin⁡2021xcos⁡x.I(x)=\frac{1}{\sin^{2021}x\cos x}.I(x)=sin2021xcosx1​.
  1. Compute I(π3)I\left(\frac\pi3\right)I(3π​) and I(π6)I\left(\frac\pi6\right)I(6π​)

At x=π3x=\frac\pi3x=3π​

sin⁡π3=32,cos⁡π3=12.\sin\frac\pi3=\frac{\sqrt3}{2},\qquad \cos\frac\pi3=\frac12.sin3π​=23​​,cos3π​=21​.

Thus

I(π3)=1(32)2021⋅12=2(32)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(3π​)=(23​​)2021⋅21​1​=(23​​)20212​.

Now

(32)2021=31010(3)22021.\left(\frac{\sqrt3}{2}\right)^{2021}=\frac{3^{1010}(\sqrt3)}{2^{2021}}.(23​​)2021=2202131010(3​)​.

So

I(π3)=2⋅22021310103=22022310103.I\left(\frac\pi3\right)=2\cdot \frac{2^{2021}}{3^{1010}\sqrt3} =\frac{2^{2022}}{3^{1010}\sqrt3}.I(3π​)=2⋅310103​22021​=310103​22022​.

At x=π6x=\frac\pi6x=6π​

sin⁡π6=12,cos⁡π6=32.\sin\frac\pi6=\frac12,\qquad \cos\frac\pi6=\frac{\sqrt3}{2}.sin6π​=21​,cos6π​=23​​.

Thus

I(π6)=1(12)2021⋅32=220223.I\left(\frac\pi6\right)=\frac{1}{\left(\frac12\right)^{2021}\cdot\frac{\sqrt3}{2}} =\frac{2^{2022}}{\sqrt3}.I(6π​)=(21​)2021⋅23​​1​=3​22022​.

Therefore,

I(π6)=31010I(π3).I\left(\frac\pi6\right)=3^{1010}I\left(\frac\pi3\right).I(6π​)=31010I(3π​).

Equivalently,

31010I(π3)−I(π6)=0.3^{1010}I\left(\frac\pi3\right)-I\left(\frac\pi6\right)=0.31010I(3π​)−I(6π​)=0.

So Option A is correct.


  1. Check all options
  • A: 31010I(π3)−I(π6)=03^{1010}I\left(\frac\pi3\right)-I\left(\frac\pi6\right)=031010I(3π​)−I(6π​)=0 ✅
  • B: 31010I(π6)−I(π3)=03^{1010}I\left(\frac\pi6\right)-I\left(\frac\pi3\right)=031010I(6π​)−I(3π​)=0 ❌
  • C: 31011I(π3)−I(π6)=03^{1011}I\left(\frac\pi3\right)-I\left(\frac\pi6\right)=031011I(3π​)−I(6π​)=0 ❌
  • D: 31011I(π6)−I(π3)=03^{1011}I\left(\frac\pi6\right)-I\left(\frac\pi3\right)=031011I(6π​)−I(3π​)=0 ❌

Hence the single correct answer is A.


  1. Comparison with stored correct answer

Stored correct answer: A

Our derived answer: A

So they agree.

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