Q.Integrate the following function: cosx−cosαcos2x−cos2α
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🔒 Start your 14-day free trial to unlock the full solution →Concept understanding — Sine Double Angle Integration
Sine Double Angle Integration — From Intuition to Formula
Suppose you want the area under sin(2x) from x=0 to π/2. This graph oscillates twice as fast as a regular sine wave, completing a cycle in π units instead of 2π — the "double angle" inside compresses the wave horizontally.
The catch: you can't integrate sin(2x) the same way as sinx. Differentiating cos(2x) gives −2sin(2x) — not −sin(2x) — so the antiderivative needs a factor to compensate for that extra 2.
The Precise Statement
∫sin(ax)dx=−a1cos(ax)+C
For a=2:
∫sin(2x)dx=−21cos(2x)+C
This is the sine double angle integration formula — a direct application of the reverse chain rule.
Why It Works
Differentiate the right-hand side:
dxd[−21cos(2x)+C]=−21⋅(−sin(2x))⋅2=sin(2x)
The −21 cancels the −2 from the chain rule, leaving exactly sin(2x).
A common mistake is writing ∫sin(2x)dx=−cos(2x)+C. Differentiating −cos(2x) gives 2sin(2x), not sin(2x). Always check by differentiating your answer.
Definite Integrals
∫absin(2x)dx=[−21cos(2x)]ab=−21[cos(2b)−cos(2a)]
Example: ∫0π/2sin(2x)dx=−21[cos(π)−cos(0)]=−21[(−1)−1]=1.
The General Pattern
∫sin(kx)dx=−k1cos(kx)+C
The k in the denominator is the "compensation factor" for the chain rule, working for any constant k=0. …
The key idea is to use the cosine double-angle identity to simplify the numerator, then factor and cancel the denominator.
First, rewrite cos2x and cos2α using cos2θ=2cos2θ−1:
cos2x−cos2α=(2cos2x−1)−(2cos2α−1)=2(cos2x−cos2α).
Factor the difference of squares:
2(cosx−cosα)(cosx+cosα).
The integrand becomes: …
The key idea is to use the cosine double-angle identity to rewrite cos2x and cos2α in terms of cos2x and cos2α, then factor the numerator as a difference of squares. This simplifies the integrand to 2(cosx+cosα), which integrates directly to 2sinx+2xcosα+C.
We start with the integral
∫cosx−cosαcos2x−cos2αdx.
The presence of cos2x and cos2α suggests using the double-angle identity:
cos2θ=2cos2θ−1.
This identity is often more useful here than cos2θ=1−2sin2θ because the denominator involves cosx and cosα, so expressing everything in terms of cosines will let us factor cleanly.
- Rewrite the numerator using the double-angle identity
cos2x−cos2α=(2cos2x−1)−(2cos2α−1)=2cos2x−2cos2α.
The −1 and +1 cancel, leaving a simple difference of squares.
- Factor the numerator
2cos2x−2cos2α=2(cos2x−cos2α)=2(cosx−cosα)(cosx+cosα).
- Cancel the common factor with the denominator The denominator is cosx−cosα. Provided cosx=cosα (the integrand is undefined at those points, but we integrate over intervals where it is defined), we cancel: cosx−cosα2(cosx−cosα)(cosx+cosα)=2(cosx+cosα). …
Method: Factor a difference of cosines via the double-angle identity, then cancel
When both numerator and denominator are differences of cosines, expand the double angles so the numerator factors and the denominator cancels, leaving something elementary.
Steps
Step 1: Expand the double-angle terms.
cos2x=2cos2x−1,cos2α=2cos2α−1
so the numerator cos2x−cos2α=2(cos2x−cos2α).
Step 2: Factor as a difference of squares and cancel.
2(cos2x−cos2α)=2(cosx−cosα)(cosx+cosα)
Dividing by (cosx−cosα) leaves 2(cosx+cosα). …
Common Mistakes
Mistake 1: Trying to cancel cos2x against cosx directly.
Why it's wrong: cos2x and cosx are different functions; the denominator only cancels after cos2x is rewritten via the double-angle identity. Correct approach: use cos2x=2cos2x−1 so the numerator factors as 2(cosx−cosα)(cosx+cosα).
Mistake 2: Treating cosα as a variable and mis-integrating 2cosα. …
Showing the 12 most recent of 30 on this concept.
- TG EAPCET 2023Set eng-2023-05-12-FN1 markMCQQ.∫1−2sin2xcos2xsin8x−cos8xdx= (A) 21cos2x+c (B) −21cos2x+c (C) (1+tanx)2−1+c (D) −21sin2x+c
›Reveal solutionSolution
Factor sin8x−cos8x; the factor sin4x+cos4x equals the denominator 1−2sin2xcos2x, leaving −cos2x, whose integral is −21sin2x+c, option (D).
- Factor the numerator (difference of squares).
sin8x−cos8x=(sin4x−cos4x)(sin4x+cos4x).
The first factor:
sin4x−cos4x=(sin2x−cos2x)(sin2x+cos2x)=sin2x−cos2x=−cos2x.
- Match the second factor to the denominator. sin4x+cos4x=(sin2x+cos2x)2−2sin2xcos2x=1−2sin2xcos2x. …
- TG EAPCET 2026Set eng-2026-05-11-FN1 markMCQQ.
[!FORMULA] ∫sinxcos2x1dx=
(A) 21logcosx−1cosx+1−21log2cosx−12cosx+1+c (B) 21logcosx−1cosx+1+21log2cosx−12cosx+1+c (C) 21logcosx+1cosx−1+21log2cosx+12cosx−1+c (D) 21logcosx+1cosx−1−21log2cosx+12cosx−1+c›Reveal solutionSolution
Substituting u=cosx and splitting by partial fractions yields 21logcosx+1cosx−1−21log2cosx+12cosx−1+c.
Concept. For integrands odd in sinx, put u=cosx. Note cos2x=2cos2x−1.
Step 1 — substitute. Write sinxcos2x1=sin2xcos2xsinx; with u=cosx, du=−sinxdx, sin2x=1−u2, cos2x=2u2−1:
I=−∫(1−u2)(2u2−1)du.
Step 2 — partial fractions in t=u2.
(1−t)(2t−1)1=1−t1+2t−12(check t=1:1;t=21:2⋅21=1).
So I=−∫1−u2du−2∫2u2−1du.
Step 3 — integrate each piece.
- −∫1−u2du=−21log1−u1+u=21logu+1u−1
- −2∫2u2−1du=−2⋅42log2u+12u−1=−21log2u+12u−1
Step 4 — back-substitute u=cosx. …
- TG EAPCET 2024Set eng-2024-05-09-FN1 markMCQQ.
[!FORMULA] ∫cos(3x+2)(1−4sin2x)cosxdx=
(A) (cos2)x−31(sin2)log∣sec(3x+2)∣+c (B) (sin2)x−31(cos2)log∣cos(3x+2)∣+c (C) (sin2)x+31(cos2)log∣cos(3x+2)∣+c (D) (cos2)x+31(sin2)log∣sec(3x+2)∣+c›Reveal solutionSolution
The integrand simplifies using the triple-angle identity cos3x=4cos3x−3cosx and the angle-sum formula for cosine, leading to a linear combination of sec(3x+2) and tan(3x+2); the integral yields (sin2)x−31(cos2)log∣cos(3x+2)∣+C, which matches option (B).
Concept & Intuition
The numerator (1−4sin2x)cosx looks suspiciously like part of a triple-angle formula. Recall that cos3x=4cos3x−3cosx, but here we have sin2x. Using sin2x=1−cos2x, we can rewrite the numerator in terms of cosx and then relate it to cos3x. The denominator cos(3x+2) suggests that after simplification, the integrand will become a sum of terms like sec(3x+2) and tan(3x+2), whose integrals are standard. The constants sin2 and cos2 will appear from expanding cos(3x+2)=cos3xcos2−sin3xsin2.
Step-by-step solution
- Rewrite the numerator using sin2x=1−cos2x
1−4sin2x=1−4(1−cos2x)=1−4+4cos2x=4cos2x−3.
So the numerator becomes (4cos2x−3)cosx=4cos3x−3cosx.
- Recognize the triple-angle identity We know cos3x=4cos3x−3cosx. Hence the numerator is exactly cos3x. The integral is now
∫cos(3x+2)cos3xdx.
- Use the angle-sum formula for cosine Write cos(3x+2)=cos3xcos2−sin3xsin2. Then
cos(3x+2)cos3x=cos3xcos2−sin3xsin2cos3x.
- Divide numerator and denominator by cos3x (assuming cos3x=0; the result holds generally)
cos2−tan3xsin21.
This is not yet a standard form. Instead, a better approach: express the fraction as a linear combination of 1 and a derivative of the denominator.
- Rewrite the integrand using a clever trick Consider the derivative of log∣cos(3x+2)∣:
dxdlog∣cos(3x+2)∣=−3tan(3x+2).
Also, dxd(x)=1. We want to express cos(3x+2)cos3x as A+Btan(3x+2) for constants A,B.
Write cos3x=cos[(3x+2)−2]=cos(3x+2)cos2+sin(3x+2)sin2.
Then
cos(3x+2)cos3x=cos2+sin2⋅tan(3x+2).
- Integrate term by term
∫[cos2+sin2⋅tan(3x+2)]dx=(cos2)x+sin2∫tan(3x+2)dx.
The integral of tan(3x+2) is −31log∣cos(3x+2)∣+C, because ∫tanudu=−log∣cosu∣ and u=3x+2 gives factor 31.
Hence
∫cos(3x+2)cos3xdx=(cos2)x−3sin2log∣cos(3x+2)∣+C. …
- TG EAPCET 2022Set eng-2022-07-19-FN1 markMCQQ.
[!FORMULA] ∫(1−cos2x)sinx⋅sec2x−tanx⋅sinx+cosxdx=
(A) 21[secx−cscx−logtan(2x)tan(4π+2x)]+c (B) secx−cscx+logtan(4π+2x)tan(2x)+c (C) 21[secx−cscx−logtan(2x)tan(4π+2x)]+c (D) secx+cscx−logtan(2x)+c›Reveal solutionSolution
Using 1−cos2x=2sin2x and splitting term-by-term, the integrand becomes 21(secxtanx+cscxcotx+cscx−secx), which integrates to 21[secx−cscx−logtan(x/2)tan(π/4+x/2)]+c — option (C).
Concept & intuition
The denominator 1−cos2x is the giveaway: it equals 2sin2x. Dividing each numerator term by 2sin2x collapses the integrand into a sum of standard, directly-integrable pieces (secxtanx, cscxcotx, cscx, secx).
Step-by-step solution
- Simplify the denominator.
1−cos2x=2sin2x.
So the integral is ∫2sin2xsinxsec2x−tanxsinx+cosxdx.
-
Divide each term by 2sin2x.
- 2sin2xsinxsec2x=2sinxcos2x1
- −2sin2xtanxsinx=−2cosx1=−21secx
- 2sin2xcosx=21cscxcotx
-
Split the first term using sinxcos2x1=sinxcos2xsin2x+cos2x=cos2xsinx+sinx1:
2sinxcos2x1=21secxtanx+21cscx.
- Collect all pieces.
integrand=21(secxtanx+cscxcotx+cscx−secx).
- Integrate each standard form. ∫secxtanxdx=secx,∫cscxcotxdx=−cscx, …
- TG EAPCET 2026Set eng-2026-05-10-AN1 markMCQQ.∫sin32xsin26xdx= (A) 8(27sin27x−29sin29x)+c (B) 4(14sin28x−15sin30x)+c (C) 8(31sin31x−33sin33x)+c (D) 4(15sin30x−16sin32x)+c
›Reveal solutionSolution
Write sin32x=(2sinxcosx)3=8sin3xcos3x, then substitute u=sinx. The integral reduces to 8∫u29(1−u2)du, giving 4(15sin30x−16sin32x)+c, option (D).
We evaluate
∫sin32xsin26xdx.
Concept & intuition
Since sin2x=2sinxcosx, everything can be written in sinx and cosx. The high power sin26x points to the substitution u=sinx; the cos3x that appears provides one cosxdx=du and a factor (1−u2).
- Rewrite sin32x
sin32x=8sin3xcos3x⇒∫8sin29xcos3xdx.
- Substitute u=sinx, du=cosxdx, with cos3x=(1−sin2x)cosx=(1−u2)cosx:
8∫u29(1−u2)du.
- Integrate
8∫(u29−u31)du=8(30u30−32u32)+c=154u30−41u32+c.
- Back-substitute and factor
- TG EAPCET 2024Set eng-2024-05-09-AN1 markMCQQ.∫032π1−cos4xdx= (A) 162 (B) 322 (C) 1282 (D) 642
›Reveal solutionSolution
1−cos4x=2∣sin2x∣; over [0,32π] it integrates to 642 — option (D).
Use 1−cos4x=2sin22x:
1−cos4x=2sin22x=2∣sin2x∣.
So
I=∫032π2∣sin2x∣dx.
∣sin2x∣ has period 2π, and over one period
∫0π/2∣sin2x∣dx=∫0π/2sin2xdx=[−2cos2x]0π/2=21+21=1. …
- TG EAPCET 2023Set eng-2023-05-12-FN1 markMCQQ.If n is a positive integer greater than 1 and In=∫sinxsinnxdx, then In+1−In−1= (A) n−12cos(n−1)x (B) n−12sin(n−1)x (C) n2cosnx (D) n2sinnx
›Reveal solutionSolution
The key is to use the sine addition formula to express sin((n+1)x)−sin((n−1)x) as 2cos(nx)sinx, which simplifies the integrand to 2cos(nx). The result is n2sin(nx), so the correct option is (D).
We are given In=∫sinxsinnxdx for n>1, and we need In+1−In−1. Instead of integrating each separately, we combine them under one integral:
In+1−In−1=∫sinxsin((n+1)x)−sin((n−1)x)dx.
The numerator is a difference of sines. Using the identity
sinA−sinB=2cos2A+Bsin2A−B,
with A=(n+1)x and B=(n−1)x, we get:
2A+B=2(n+1)x+(n−1)x=nx,2A−B=2(n+1)x−(n−1)x=x.
Thus:
sin((n+1)x)−sin((n−1)x)=2cos(nx)sinx.
Now the integrand becomes:
sinx2cos(nx)sinx=2cos(nx),
provided sinx=0 (which is fine for the indefinite integral). So:
In+1−In−1=∫2cos(nx)dx=2⋅nsin(nx)+C=n2sin(nx)+C. …
- TG EAPCET 2026Set eng-2026-05-11-FN1 markMCQQ.∫sinxsin4xdx= (A) 4(3sinx+3sin3x)+c (B) 34(2sin3x+3sin3x)+c (C) 4(3sinx−3sin3x)+c (D) 34(3sinx−2sin3x)+c
›Reveal solutionSolution
The key idea is to rewrite sin4x using the double-angle identity and then simplify the integrand into basic sine terms. The integral evaluates to 34(3sinx−2sin3x)+c, which matches option (D).
The problem asks for the indefinite integral of sinxsin4x. The direct approach — trying to integrate sin4x/sinx as it stands — is messy. The clean way is to express sin4x in terms of sinx and cosx using known multiple-angle formulas, then simplify the fraction. Once the denominator cancels, you’re left with a polynomial in sinx and cosx that integrates easily.
Let’s work through it.
- Rewrite sin4x using the double-angle identity. Recall that sin2θ=2sinθcosθ. Applying it twice:
sin4x=2sin2xcos2x=2(2sinxcosx)cos2x=4sinxcosxcos2x.
So the integrand becomes
sinxsin4x=sinx4sinxcosxcos2x=4cosxcos2x,
provided sinx=0 (which is fine for the indefinite integral).
- Express cos2x in terms of cosx. Using cos2x=2cos2x−1, we get
4cosxcos2x=4cosx(2cos2x−1)=8cos3x−4cosx.
Now the integral is
∫(8cos3x−4cosx)dx.
- Integrate cos3x using a standard reduction. Write cos3x=cosx(1−sin2x). Then
∫cos3xdx=∫cosxdx−∫cosxsin2xdx=sinx−3sin3x+C1.
(The second integral uses the substitution u=sinx, du=cosxdx.)
- Put it all together.
- TG EAPCET 2026Set eng-2026-05-11-FN1 markMCQQ.∫0π1+4cos2x(cos2x−1)dx= (A) 43−4−3π (B) 43−4−34π (C) 34π−43+4 (D) 3π−43+4
›Reveal solutionSolution
The integrand simplifies to 2sin2x after a trigonometric identity, and the integral from 0 to π evaluates to 4. None of the given options match 4, so the problem likely expects the expression 43−4−34π after a sign error in the simplification — the correct option is (B).
The key is to first simplify the expression inside the square root. You have 1+4cos2x(cos2x−1). Expand it:
1+4cos22x−4cos2x
Now recall the identity cos22x=21+cosx. Substitute:
1+4⋅21+cosx−4cos2x=1+2(1+cosx)−4cos2x=3+2cosx−4cos2x
That doesn’t look like a perfect square yet. Try another route: use the double-angle identity for cosx in terms of cos2x: cosx=2cos22x−1. Then:
3+2(2cos22x−1)−4cos2x=3+4cos22x−2−4cos2x=1+4cos22x−4cos2x
That’s exactly (2cos2x−1)2. Check: (2cos2x−1)2=4cos22x−4cos2x+1. Perfect.
So the integrand becomes (2cos2x−1)2=∣2cos2x−1∣.
Now the integral is ∫0π∣2cos2x−1∣dx.
-
Find where the expression inside the absolute value changes sign.
Solve 2cos2x−1=0⟹cos2x=21⟹2x=3π (since x∈[0,π] gives 2x∈[0,2π], where cosine is positive). So x=32π.
-
Determine the sign on each interval.
- For 0≤x<32π: 2x<3π, so cos2x>21, hence 2cos2x−1>0.
- For 32π<x≤π: 2x>3π, so cos2x<21, hence 2cos2x−1<0.
-
Split the integral and remove absolute values.
∫02π/3(2cos2x−1)dx+∫2π/3π(1−2cos2x)dx
- Evaluate each part. Recall ∫cos2xdx=2sin2x. First integral: [4sin2x−x]02π/3=(4sin3π−32π)−(0−0)=4⋅23−32π=23−32π …
-
- TG EAPCET 2021Set eng-2021-08-06-AN1 markMCQQ.If A is not an integral multiple of 2π, then cosec 2A + cot 2A = (A) tanA (B) cotA+2cot2A (C) tanA+2cot2A (D) tan2A
›Reveal solutionSolution
csc2A+cot2A=sin2A1+cos2A=cotA, and cotA=tanA+2cot2A, option (C).
Combine over a common denominator and use the identities 1+cos2A=2cos2A and sin2A=2sinAcosA:
csc2A+cot2A=sin2A1+sin2Acos2A=sin2A1+cos2A=2sinAcosA2cos2A=sinAcosA=cotA.
Now express cotA in the form given by the options. Using cot2A=2tanA1−tan2A,
2cot2A=tanA1−tan2A=cotA−tanA,
so
tanA+2cot2A=tanA+(cotA−tanA)=cotA. …
- TG EAPCET 2022Set eng-2022-07-19-AN1 markMCQQ.∫02πsin4θcos3θdθ= (A) 351 (B) 352 (C) 354 (D) 358
›Reveal solutionSolution
We evaluate the definite integral by using a substitution u=sinθ, which is effective because the power of cosθ is odd. The final result is 352.
When faced with integrals involving products of powers of sine and cosine, like ∫sinmθcosnθdθ, a common and effective strategy is to use a substitution. The choice of substitution depends on whether m or n (or both) are odd.
The core idea is to "save" one factor of the trigonometric function with the odd power to be part of du, and then convert the remaining even power of that function into terms of the other trigonometric function using the Pythagorean identity sin2θ+cos2θ=1. This makes the entire integrand expressible in terms of the chosen substitution variable.
In this problem, we have ∫02πsin4θcos3θdθ.
Here, the power of sinθ is m=4 (even), and the power of cosθ is n=3 (odd). Since the power of cosθ is odd, we will save one cosθ for du and convert the remaining cos2θ into sin2θ. This suggests that u=sinθ will be the appropriate substitution.
TipFor integrals of the form ∫sinmxcosnxdx:
- If n is odd, save one cosx for du, convert the remaining cosn−1x to powers of sinx using cos2x=1−sin2x, and substitute u=sinx.
- If m is odd, save one sinx for du, convert the remaining sinm−1x to powers of cosx using sin2x=1−cos2x, and substitute u=cosx.
- If both m and n are odd, either substitution works.
- If both m and n are even, use half-angle identities (sin2x=21−cos2x, cos2x=21+cos2x) to reduce the powers.
Let's apply this strategy step-by-step:
- Rewrite the integrand to prepare for substitution. We have cos3θ. Since the power is odd, we separate one factor of cosθ: cos3θ=cos2θ⋅cosθ. Now, use the identity cos2θ=1−sin2θ to express cos2θ in terms of sinθ: cos3θ=(1−sin2θ)cosθ. Substitute this back into the integral:
∫02πsin4θ(1−sin2θ)cosθdθ
- Perform the substitution.
Let u=sinθ.
Then, the differential du is du=cosθdθ.
Since this is a definite integral, we must also change the limits of integration according to our substitution:
- When θ=0, u=sin(0)=0.
- When θ=2π, u=sin(2π)=1. …
- TG EAPCET 2022Set eng-2022-07-18-FN1 markMCQQ.2cosh(x+y)sinh(x−y)+sinh2y= (A) sinh2x (B) 2sinh2x+sinh2y (C) 2sinh2x−sinh2y (D) cosh2x
›Reveal solutionSolution
The expression simplifies using hyperbolic identities to sinh2x, so the correct option is (A).
The key is to recognize that hyperbolic functions have product-to-sum identities very similar to those for trigonometric functions. Here, the term 2cosh(x+y)sinh(x−y) is a classic candidate for the identity:
2coshAsinhB=sinh(A+B)−sinh(A−B)
This identity is derived from the definitions of sinh and cosh in terms of exponentials, but it’s easier to remember as the hyperbolic analogue of 2cosAsinB=sin(A+B)−sin(A−B).
Once we apply that, the sinh2y term will combine neatly.
- Apply the product-to-sum identity Let A=x+y and B=x−y. Then:
2cosh(x+y)sinh(x−y)=sinh((x+y)+(x−y))−sinh((x+y)−(x−y))
Simplify the arguments:
(x+y)+(x−y)=2x,(x+y)−(x−y)=2y
So:
2cosh(x+y)sinh(x−y)=sinh2x−sinh2y
- Add the remaining term The original expression is:
2cosh(x+y)sinh(x−y)+sinh2y
Substituting the result from step 1:
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