Q.Integrate the following function: (1−sinx)(2−sinx)cosx [Hint : Put sinx=t]
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🔒 Start your 14-day free trial to unlock the full solution →Concept understanding — U Substitution
U Substitution: The Reverse Chain Rule
The chain rule differentiates composite functions: the derivative of sin(x2) is cos(x2)⋅2x — differentiate the outer function, then multiply by the derivative of the inside. Integration asks the reverse: given cos(x2)⋅2x, find the original function. That's what u substitution does — it reverses the chain rule.
The Core Intuition
When an integral looks like "a function times the derivative of its inside," substitute the inside with u and the derivative of the inside with du. Consider:
∫2xcos(x2)dx
Here 2x is the derivative of x2, and x2 is the inside of cos(x2). Let u=x2, so du=2xdx:
∫cos(u)du=sin(u)+C=sin(x2)+C
Check: the derivative of sin(x2) is cos(x2)⋅2x.
The Precise Statement
∫f(g(x))⋅g′(x)dx=∫f(u)duwhere u=g(x),du=g′(x)dx
Valid provided g is differentiable and the resulting integral in u is simpler.
The Step-by-Step Method
- Identify a function g(x) whose derivative g′(x) also appears (possibly up to a constant factor).
- Set u=g(x), compute du=g′(x)dx.
- Rewrite the entire integral in u and du — every x and dx must be replaced.
- Integrate with respect to u.
- Substitute back u=g(x).
You cannot mix variables. If any x remains after substitution, you chose the wrong u (or must solve for x in terms of u — rare).
A Second Example (with a constant factor)
Evaluate ∫xx2+1dx. Let u=x2+1, so xdx=21du:
∫u⋅21du=21⋅32u3/2+C=31(x2+1)3/2+C
When Does It Work?
When the integrand is something times the derivative of something inside. Common patterns:
- x⋅f(x2) — derivative of x2 is 2x, so u=x2
- eg(x)⋅g′(x) — derivative of g(x) appears
- g(x)g′(x) — leads to log∣g(x)∣ …
Concept: U Substitution — substitute sinx=t to convert the trigonometric integral into a simpler rational one.
Step 1: Let t=sinx, so dt=cosxdx. The integral becomes
∫(1−sinx)(2−sinx)cosxdx=∫(1−t)(2−t)dt.
Step 2: Decompose into partial fractions:
(1−t)(2−t)1=1−t1−2−t1.
Step 3: Integrate term by term: …
Substituting sinx=t turns the integral into ∫(1−t)(2−t)dt; partial fractions give log1−sinx2−sinx+C.
Substitute. Let t=sinx, so dt=cosxdx:
∫(1−sinx)(2−sinx)cosxdx=∫(1−t)(2−t)dt.
Partial fractions. (1−t)(2−t)1=1−tA+2−tB with 1=A(2−t)+B(1−t). Setting t=1 gives A=1; setting t=2 gives B=−1. So
(1−t)(2−t)1=1−t1−2−t1.
Integrate. Since ∫a−tdt=−log∣a−t∣, …
Method: Trig-to-Rational Substitution, then Partial Fractions
Use this when a trigonometric integrand is a rational function of sinx (or cosx) with its derivative present in the numerator — a hint like "put sinx=t" points the way.
Steps
Step 1: Spot the matching derivative.
If the numerator is cosxdx and the rest depends only on sinx, then t=sinx converts everything.
Step 2: Substitute.
Let t=sinx, so dt=cosxdx. The integral becomes a purely rational one in t, e.g.
∫(1−t)(2−t)dt …
Common Mistakes
Mistake 1: Integrating a−t1 as +log∣a−t∣.
Why it's wrong: dtd(a−t)=−1, so ∫a−tdt=−log∣a−t∣; missing this sign flips both terms. Correct approach: ∫1−tdt−∫2−tdt=−log∣1−t∣+log∣2−t∣.
Mistake 2: Forgetting to replace dx with dt. …
Showing the 12 most recent of 51 on this concept.
- AP EAPCET 2025Set eng-2025-05-21-FN1 markMCQQ.If ∫sin3x+cos3xdx=Alog2−t2+t+BTan−1(t)+c, then (AB,t)= (A) (32,sinx−cosx) (B) (22,sinx−cosx) (C) (32,sinx−cosx) (D) (23,sinx+cosx)
›Reveal solutionSolution
The standard sin3x+cos3x integral, solved via the substitution t=sinx−cosx; matching to the given Alog∣⋯∣+Btan−1t form gives B/A=22 with t=sinx−cosx.
Concept and Intuition
sin3x+cos3x factors as a sum of cubes, (sinx+cosx)(sin2x−sinxcosx+cos2x)=(sinx+cosx)(1−sinxcosx). Both remaining factors can be expressed in terms of t=sinx−cosx (since t2=1−2sinxcosx links sinxcosx to t, and dt=(sinx+cosx)dx conveniently cancels the other factor).
Step-by-Step Solution
- Factor: sin3x+cos3x=(sinx+cosx)(1−sinxcosx).
- Let t=sinx−cosx⇒dt=(cosx+sinx)dx, and t2=1−2sinxcosx⇒sinxcosx=21−t2.
- So 1−sinxcosx=1−21−t2=21+t2.
- Also (sinx+cosx)2=1+2sinxcosx=1+(1−t2)=2−t2, so sinx+cosx=2−t2.
- Rewrite the integral:
∫(sinx+cosx)(1−sinxcosx)dx=∫2−t2⋅21+t2dx.
Since dx=sinx+cosxdt=2−t2dt:
=∫2−t2⋅21+t21⋅2−t2dt=∫(2−t2)(1+t2)2dt.
- Split using 1=3(2−t2)+(1+t2):
(2−t2)(1+t2)2=32⋅(2−t2)(1+t2)(2−t2)+(1+t2)=32[1+t21+2−t21].
- Integrate each piece: ∫1+t2dt=tan−1t; ∫2−t2dt=221log2−t2+t (standard form ∫a2−x2dx=2a1loga−xa+x with a=2).
- So the integral is …
- AP EAPCET 2026Set eng-2026-05-14-AN1 markMCQQ.If ∫sin3x+cos3x1dx=Alog2−t2+t+BTan−1(t)+c, then (AB,t)= (A) (22,sinx+cosx) (B) (92,sinx+cosx) (C) (92,sinx−cosx) (D) (22,sinx−cosx)
›Reveal solutionSolution
Factoring the sum of cubes and substituting t=sinx−cosx turns the trigonometric integral into a clean rational-function integral in t, giving B/A=22 with t=sinx−cosx.
Concept and Intuition
sin3x+cos3x factors as a sum of cubes: (sinx+cosx)(1−sinxcosx). Both sinx+cosx and 1−sinxcosx can be written purely in terms of u=sinx−cosx, because (sinx+cosx)2+(sinx−cosx)2=2 and 1−sinxcosx=21+(sinx−cosx)2. Crucially, dxdu=cosx+sinx, which is exactly the factor left over after using the second identity — so the whole integral collapses into a rational function of u alone.
Step-by-Step Solution
- Factor: sin3x+cos3x=(sinx+cosx)(1−sinxcosx).
- Let u=sinx−cosx. Then u2=1−2sinxcosx, so 1−sinxcosx=21+u2.
- Also (sinx+cosx)2=1+2sinxcosx=2−u2, so sinx+cosx=2−u2 (taking the appropriate branch), and dxdu=cosx+sinx=2−u2.
- So sin3x+cos3x=2−u2⋅21+u2, and
I=∫sin3x+cos3xdx=∫2−u2(1+u2)2dx=∫2−u2(1+u2)2⋅2−u2du=∫(2−u2)(1+u2)2du.
- Partial fractions (by symmetry, only even terms survive): (2−u2)(1+u2)2=2−u22/3+1+u22/3. …
- AP EAPCET 2026Set eng-2026-05-15-FN1 markMCQQ.∫10+sin2xcosx−sinxdx= (A) 21log(10+sin2x)+c (B) 31log(10+sin2x)+c (C) 31Tan−1(3sinx+cosx)+c (D) 31Tan−1(10+sin2x)+c
›Reveal solutionSolution
The numerator cosx−sinx is exactly d(sinx+cosx), and the denominator rewrites in terms of u=sinx+cosx via sin2x=u2−1. That collapses the integral to a standard ∫du/(a2+u2) arctangent form. Answer: 31Tan−1(3sinx+cosx)+c.
Concept and Intuition
Whenever an integrand contains both sinx−cosx (or cosx−sinx) and sin2x, it is worth trying u=sinx+cosx (or sinx−cosx) as the substitution, because u2=1±sin2x links the two.
Step-by-Step Solution
- Let u=sinx+cosx. Then du=(cosx−sinx)dx — this is exactly the numerator times dx.
- Also u2=sin2x+cos2x+2sinxcosx=1+sin2x, so sin2x=u2−1.
- Denominator: 10+sin2x=10+u2−1=9+u2.
- The integral becomes ∫9+u2du=31Tan−1(3u)+c. …
- AP EAPCET 2025Set eng-2025-05-27-FN1 markMCQQ.∫(1+x)x−x2dx= (A) −21−x1+x+c (B) −1+x1−x+c (C) −21+x1−x+c (D) 21−x1+x+c
›Reveal solutionSolution
Substituting t=x turns the surd-heavy integrand into ∫(1+t)3/2(1−t)1/22dt, whose antiderivative is exactly −21+t1−t.
Concept and Intuition
When an integrand mixes x and x−x2=x1−x, substituting t=x clears every square root of x at once, converting the whole thing into a rational-power integral in t that matches the derivative of 1+t1−t — a standard "recognise the derivative" pattern worth memorising for CET-style problems.
Step-by-Step Solution
- Write x−x2=x(1−x)=x1−x, so the integral is
I=∫(1+x)x1−xdx.
- Let t=x, so x=t2, dx=2tdt:
I=∫(1+t)⋅t⋅1−t22tdt=∫(1+t)(1−t)(1+t)2dt=∫(1+t)3/2(1−t)1/22dt.
- Let y=1+t1−t. Differentiating y2=1+t1−t: 2yy′=(1+t)2−(1+t)−(1−t)=(1+t)2−2 ⇒ y′=y(1+t)2−1=(1+t)3/2(1−t)1/2−1. …
- AP EAPCET 2024Set eng-2024-05-20-AN1 markMCQQ.∫sin3xcos(x−α)dx= (A) cosα1cotx+tanα+c (B) cosα1cotx−tanα+c (C) sinα−1cotx+tanα+c (D) cosα−2cotx+tanα+c
›Reveal solutionSolution
Expanding cos(x−α) and substituting u=cotx reduces this to a simple square-root integral; final answer is (D).
Concept and Intuition
The key move is expanding cos(x−α) and factoring out sin4x from inside the square root so that a substitution u=cotx (whose differential is −csc2xdx, conveniently matching what's left outside) linearizes the whole thing.
Step-by-Step Solution
- cos(x−α)=cosxcosα+sinxsinα.
- sin3xcos(x−α)=sin3xcosxcosα+sin4xsinα=sin4x(sinxcosxcosα+sinα)=sin4x(cotxcosα+sinα).
- So sin3xcos(x−α)=sin2xcotxcosα+sinα (taking sin2x>0 outside the root).
- The integral is ∫sin2xcosαcotx+sinαdx=∫cosαcotx+sinαcsc2xdx.
- Let u=cotx, du=−csc2xdx. Integral becomes −∫cosαu+sinαdu=−cosα2cosαu+sinα+c. …
- AP EAPCET 2021Set eng-2021-08-25-AN1 markMCQQ.∫cosxdx= (A) 2xsinx+2cosx+c (B) 2xsinx+2sinx+c (C) 2xsinx−2cosx+c (D) xcosx−2sinx+c
›Reveal solutionSolution
Substitute t=x to turn the integral into a standard integration-by-parts problem. Answer: 2xsinx+2cosx+c.
Concept and Intuition
Whenever you see x trapped inside a trig or exponential function, substituting t=x converts it into a polynomial-times-trig integral solvable by parts.
Step-by-Step Solution
- Let t=x⇒x=t2, dx=2tdt.
- ∫cosxdx=∫cost⋅2tdt=2∫tcostdt.
- Integrate by parts: ∫tcostdt=tsint−∫sintdt=tsint+cost. …
- AP EAPCET 2024Set eng-2024-05-21-FN1 markMCQQ.If n≥2 is a natural number and 0<θ<2π, then ∫cosn+1θ(cosnθ−cosθ)1/nsinθdθ= (A) n−1n(cos(1−n)θ−1)2+c (B) (n+1)(1−n)n(cos(1−n)θ−1)1+n1+c (C) n−11(cos(n−1)θ−1)2+c (D) 1−n2n(1−cos(1−n)θ)(n+1)/n
›Reveal solutionSolution
Factor out cosnθ from inside the radical to isolate a clean power of cosθ, then substitute w=cos1−nθ to reduce the whole integral to ∫w1/ndw.
Concept and Intuition
The key move is factoring cosnθ−cosθ=cosnθ(1−cos1−nθ) so the n-th root pulls a clean cosθ outside, cancelling nicely against the cosn+1θ in the denominator and leaving a single power of w=cos1−nθ whose differential exactly matches sinθdθ/cosnθ in the integrand.
Step-by-Step Solution
- Factor: cosnθ−cosθ=cosnθ(1−cos1−nθ), so
(cosnθ−cosθ)1/n=cosθ(1−cos1−nθ)1/n.
- Divide by cosn+1θ:
cosn+1θ(cosnθ−cosθ)1/n=cosnθ(1−cos1−nθ)1/n.
- Let w=cos1−nθ. Then dθdw=(1−n)cos−nθ⋅(−sinθ)=(n−1)sinθcos−nθ, so cosnθsinθdθ=n−1dw.
- The whole integrand times dθ becomes (1−w)1/n⋅n−1dw — wait, more directly w1/n is the factor (1−cos1−nθ)1/n once we track 1−cos1−nθ as the base; carrying the substitution through consistently: …
- AP EAPCET 2022Set eng-2022-07-06-FN1 markMCQQ.∫(sinx+cosx+2sin2x)21dx= (A) (3+tan2x)3−(1+3tanx)+C (B) 3(1+tanx)3−(1+3tanx)+C (C) 3(1+3tanx)2−(1+tanx)+C (D) (1+3tanx)31+C
›Reveal solutionSolution
Recognising the denominator as (sinx+cosx)4 and substituting u=tanx reduces this to a rational integral, giving −3(1+tanx)31+3tanx+C.
Concept and Intuition
The key algebraic identity here is (sinx+cosx)2=sinx+cosx+2sinxcosx=sinx+cosx+2sin2x (since 2sinxcosx=4sinxcosx=2sin2x). That matches the given denominator's base exactly, turning a scary-looking radical expression into a clean fourth power.
Step-by-Step Solution
- Verify (sinx+cosx)2=sinx+cosx+2sinxcosx=sinx+cosx+2sin2x, matching sinx+cosx+2sin2x.
- So the denominator is (sinx+cosx)4.
- Factor out cosx: sinx+cosx=cosx(tanx+1), so the denominator =cos2x(1+tanx)4.
- Integral becomes ∫(1+tanx)4sec2xdx. Let t=tanx, dt=sec2xdx: ∫(1+t)4dt.
- Let u=t, t=u2, dt=2udu: ∫(1+u)42udu.
- Write 2u=2(1+u)−2: ∫[(1+u)32−(1+u)42]du=−(1+u)21+3(1+u)32+C. …
- AP EAPCET 2023Set eng-2023-05-15-AN1 markMCQQ.∫4+5cosxdx= (A) −31log3−tan2x3+tan2x+C (B) 31log3−tan2x3+tan2x+C (C) −91log3+tan2x3−tan2x+C (D) 91log3+tan2x3−tan2x+C
›Reveal solutionSolution
The Weierstrass substitution t=tan(x/2) turns this into a standard ∫dt/(a2−t2) integral, giving option (B).
Concept and Intuition
For ∫a+bcosxdx the substitution t=tan(x/2) (so cosx=1+t21−t2, dx=1+t22dt) always converts the integral into a rational function of t alone.
Step-by-Step Solution
- cosx=1+t21−t2, dx=1+t22dt, with t=tan(x/2).
- 4+5cosx=4+5⋅1+t21−t2=1+t24(1+t2)+5(1−t2)=1+t29−t2.
- Integral becomes ∫(9−t2)/(1+t2)2dt/(1+t2)=∫9−t22dt.
- Using ∫a2−t2dt=2a1loga−ta+t+C with a=3: ∫9−t2dt=61log3−t3+t+C. …
- AP EAPCET 2022Set eng-2022-07-06-AN1 markMCQQ.∫cos4xcos2x1dx=421log(1−f(x)1+f(x))−21logg(x)+C, then g(6π)−2f(6π)= (A) 22π (B) π+3 (C) 2 (D) 1
›Reveal solutionSolution
Solving the integral via t=sin2x identifies f(x)=2sin2x and g(x)=1−sin2x1+sin2x; evaluating at x=π/6 gives g(π/6)−2f(π/6)=2.
Concept and Intuition
The integral ∫cos4xcos2xdx is tackled by substituting t=sin2x, since cos4x=1−2sin22x=1−2t2 turns the whole integrand into a rational function of t, solvable by partial fractions into two logarithmic terms — one built from 1−t2 and one from 1−2t2, matching exactly the two-log structure given in the problem.
Step-by-Step Solution
- Let t=sin2x, so dt=2cos2xdx and cos4x=1−2t2.
- Rewriting the integral in terms of t: ∫cos4xcos2xdx=∫2(1−t2)(1−2t2)dt.
- Partial fractions: (1−t2)(1−2t2)1=1−t2−1+1−2t22.
- Integrating each piece gives standard log forms: one in 1−t1+t (from the 1−t2 term) and one in 1−2t1+2t (from the 1−2t2 term), exactly matching the pattern 421log1−f1+f−21logg with f(x)=2sin2x and g(x)=1−sin2x1+sin2x.
- Evaluate at x=π/6: 2x=π/3, sin(π/3)=23. …
- AP EAPCET 2021Set eng-2021-10-05-FN1 markMCQQ.∫sin3xsinxdx= (A) 231log3−tanx3+tanx+c (B) 231log3+tanx3−tanx+c (C) 431log3−tanx3+tanx+c (D) 431log3+tanx3−tanx+c
›Reveal solutionSolution
Use the triple-angle identity to cancel sinx, rewrite in terms of cos2x, then apply the Weierstrass-type substitution t=tanx to reduce to a standard rational integral. The answer is (A).
Concept and Intuition
sin3x factors as sinx(3−4sin2x), so sinx cancels immediately with the numerator, turning a trigonometric-looking integral into a much simpler one in sin2x (hence in cos2x), which is a textbook target for the t=tanx substitution.
Step-by-Step Solution
- sin3x=3sinx−4sin3x=sinx(3−4sin2x).
- sin3xsinx=3−4sin2x1.
- Using sin2x=21−cos2x: 4sin2x=2−2cos2x, so 3−4sin2x=1+2cos2x.
- Integral becomes ∫1+2cos2xdx.
- Substitute t=tanx, dx=1+t2dt, cos2x=1+t21−t2: 1+2cos2x=1+t2(1+t2)+2(1−t2)=1+t23−t2.
- Integral =∫3−t21+t2⋅1+t2dt=∫3−t2dt. …
- AP EAPCET 2024Set eng-2024-05-23-FN1 markMCQQ.∫(logx)mxndx= (A) ∫tmentdt, t=ex (B) ∫tme(n+1)tdt, t=ex (C) ∫tme(n+1)tdt, x=et (D) ∫tmentdt, x=et
›Reveal solutionSolution
The substitution x=et (equivalently t=logx) converts a (logx)mxn integral into an exponential-times-power integral in t.
Concept and Intuition
When an integrand is built from logx and powers of x, setting x=et makes logx=t directly, and turns xndx into an exponential in t — a very standard substitution for this integral family.
Step-by-Step Solution
- Let x=et, so t=logx and dx=etdt.
- Then (logx)m=tm and xn=(et)n=ent.
- Substitute into the integral: ∫(logx)mxndx=∫tm⋅ent⋅etdt=∫tme(n+1)tdt. …
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