Q.Evaluate: ∫01(1+x2)1−x2dx (Hint: let x=sinθ)
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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 (trigonometric substitution). The hint x=sinθ simplifies the square root and the limits.
Let x=sinθ, so dx=cosθdθ. When x=0, θ=0; when x=1, θ=2π.
The integral becomes:
∫0π/2(1+sin2θ)1−sin2θcosθdθ=∫0π/2(1+sin2θ)cosθcosθdθ=∫0π/21+sin2θdθ.
Divide numerator and denominator by cos2θ:
∫0π/2sec2θ+tan2θsec2θdθ=∫0π/21+2tan2θsec2θdθ. …
The key idea is to use the substitution x=sinθ, which simplifies the square root 1−x2 to cosθ and transforms the integral into a standard form. The final value is 22π.
Why this substitution works
When you see a 1−x2 in the denominator, your first instinct should be a trigonometric substitution. The hint suggests x=sinθ, which is perfect because:
- 1−x2=1−sin2θ=cosθ (for θ in [0,π/2], where cosine is non-negative)
- dx=cosθdθ
- The limits x=0 and x=1 become θ=0 and θ=π/2
The 1+x2 in the denominator becomes 1+sin2θ, which is a clean expression. This turns a messy-looking integral into something we can handle with standard techniques.
Step-by-step solution
1. Apply the substitution
Let x=sinθ, so dx=cosθdθ. When x=0, θ=0; when x=1, θ=π/2.
The integral becomes:
∫01(1+x2)1−x2dx=∫0π/2(1+sin2θ)cosθcosθdθ
2. Simplify the integrand
The cosθ cancels (provided cosθ=0, which is true except at the endpoint θ=π/2 — a removable issue):
∫0π/21+sin2θdθ
A common mistake is forgetting to change the limits of integration when substituting. Always transform x-limits to θ-limits before proceeding.
3. Transform sin2θ into a form we can integrate
We know sin2θ=1−cos2θ, but that doesn't help directly. Instead, use the identity sin2θ=21−cos2θ:
1+sin2θ=1+21−cos2θ=23−cos2θ
So the integral is:
∫0π/223−cos2θdθ=2∫0π/23−cos2θdθ
4. Substitute again to handle the cos2θ term
Let t=2θ, so dθ=dt/2. When θ=0, t=0; when θ=π/2, t=π.
2∫0π/23−cos2θdθ=2∫0π3−costdt/2=∫0π3−costdt
5. Use the tangent half-angle substitution
This is the classic method for integrals of the form ∫a+bcostdt. Let u=tan(t/2). Then:
- cost=1+u21−u2
- dt=1+u22du
- When t=0, u=0; when t=π, u→∞
The tangent half-angle substitution u=tan(t/2) is your go-to tool for any rational function of sint and cost. It converts trigonometric integrals into rational function integrals. …
Method: Trigonometric substitution x=sinθ
Use this for definite integrals containing 1−x2, especially with an extra 1+x2 factor. Setting x=sinθ clears the root and turns the integral into a manageable trig one.
Steps
Step 1: Substitute x=sinθ.
dx=cosθdθ,1−x2=cosθ.
Step 2: Rewrite the integrand.
∫(1+x2)1−x2dx=∫(1+sin2θ)cosθcosθdθ=∫1+sin2θdθ.
Step 3: Reduce 1+sin2θ using a further substitution.
Divide by cos2θ and let t=tanθ: ∫sec2θ+tan2θsec2θdθ=∫1+2t2dt. …
Common Mistakes
Mistake 1: Not choosing x=sinθ.
Why it's wrong: 1−x2 blocks algebraic substitution; x=sinθ turns it into cosθ and cancels cleanly. Correct approach: use the trig substitution first.
Mistake 2: Getting stuck at ∫1+sin2θdθ.
Why it's wrong: this needs a second step — divide by cos2θ and set t=tanθ to reach ∫1+2t2dt. Correct approach: convert to tanθ form.
Mistake 3: Forgetting the 21 factor / limits. …
Showing the 12 most recent of 51 on this concept.
- 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 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 2025Set eng-2025-05-22-FN1 markMCQQ.∫x2x4+x2+1x4−1dx= (A) x2x4+x2+1+c (B) xx4+x2+1+c (C) 2xx4+x2+1+c (D) x4x4+x2+1+c
›Reveal solutionSolution
Differentiating the candidate xx4+x2+1 reproduces the given integrand exactly, confirming it as the antiderivative.
Concept and Intuition
When an integrand looks like it could come from a quotient rule (a square root over a power of x), it is often faster to differentiate a plausible candidate of that shape and check, rather than search for a substitution from scratch.
Step-by-Step Solution
- Try g(x)=xx4+x2+1=xN where N=x4+x2+1.
- N′=2x4+x2+14x3+2x=Nx(2x2+1).
- Quotient rule: g′(x)=x2N′x−N=x2Nx2(2x2+1)−N=Nx2x2(2x2+1)−N2.
- N2=x4+x2+1, so the numerator is x2(2x2+1)−(x4+x2+1)=2x4+x2−x4−x2−1=x4−1.
- So g′(x)=x2x4+x2+1x4−1 — exactly the given integrand. …
- AP EAPCET 2026Set eng-2026-05-13-AN1 markMCQQ.∫x2(x4+1)3/4dx= (A) (1+x41)3/4+c (B) (1+x61)1/2+c (C) −(1+x41)−1/4+c (D) −(1+x41)1/4+c
›Reveal solutionSolution
Pulling x4 out from under the radical and substituting t=1+x−4 reduces the integral to a simple power rule, giving −(1+1/x4)1/4+c.
Concept and Intuition
When the integrand has (xn+1)p, it often helps to factor out the highest power of x from inside the bracket so that a substitution like t=1+x−n produces a clean differential matching the rest of the integrand.
Step-by-Step Solution
- Write (x4+1)3/4=(x4(1+x41))3/4=x3(1+x41)3/4.
- So x2(x4+1)3/41=x2⋅x3(1+x41)3/41=x5(1+x41)3/41=x−5(1+x−4)−3/4.
- Let t=1+x−4. Then dt=−4x−5dx, so x−5dx=−4dt. …
- AP EAPCET 2026Set eng-2026-05-14-FN1 markMCQQ.∫cos6x+sin6xsin2xcos2xdx= (A) 21Tan−1(tan2x)+c (B) 31Tan−1(tan2x)+c (C) 31Tan−1(tan3x)+c (D) Tan−1(tan3x)+c
›Reveal solutionSolution
Dividing through by cos6x to introduce tanx, then a double substitution (t=tanx, then u=t3), reduces the integral to a standard arctangent form, giving 31Tan−1(tan3x)+c.
Concept and Intuition
When an integrand has sin and cos appearing only in even powers that can be grouped, dividing everything by the highest power of cosx converts the whole expression into a rational function purely of tanx — a very common trick that opens the door to the substitution t=tanx. Here, since the denominator naturally forms 1+tan6x, a further substitution u=t3 turns it into the standard ∫1+u2du arctangent integral.
Step-by-Step Solution
- Divide numerator and denominator of cos6x+sin6xsin2xcos2x by cos6x: numerator becomes cos6xsin2xcos2x=cos4xsin2x=tan2xsec2x; denominator becomes 1+tan6x.
- The integral is now ∫1+tan6xtan2xsec2xdx.
- Substitute t=tanx, so dt=sec2xdx. The integral becomes ∫1+t6t2dt.
- Substitute u=t3, so du=3t2dt, i.e. t2dt=3du. The integral becomes 31∫1+u2du. …
- AP EAPCET 2026Set eng-2026-05-12-AN1 markMCQQ.If ∫(1+sinθ)(3−cos2θ)sin2θdθ=21tan−1(sinθ)+41log(f(θ))+c then f(2π)−f(0)= (A) 21 (B) −21 (C) 0 (D) −43
›Reveal solutionSolution
Reducing the integral via t=sinθ and partial fractions identifies f(θ)=(1+sinθ)21+sin2θ, giving f(π/2)−f(0)=−1/2.
Concept and Intuition
Double-angle identities collapse sin2θ and 3−cos2θ into expressions purely in sinθ and cosθ; then t=sinθ (since cosθdθ=dt appears naturally) turns the whole thing into a rational-function integral solvable by partial fractions — a very standard pattern for trig integrals with even powers/mixed degree-2 denominators.
Step-by-Step Solution
- sin2θ=2sinθcosθ; cos2θ=1−2sin2θ⇒3−cos2θ=2+2sin2θ=2(1+sin2θ).
- Integrand becomes (1+sinθ)⋅2(1+sin2θ)2sinθcosθ=(1+sinθ)(1+sin2θ)sinθcosθ.
- Substitute t=sinθ, dt=cosθdθ: integral =∫(1+t)(1+t2)tdt.
- Partial fractions: (1+t)(1+t2)t=1+t−1/2+1+t2(1/2)t+1/2 (solve t=A(1+t2)+(Bt+C)(1+t), giving A=−1/2, B=1/2, C=1/2).
- Integrate: −21log(1+t)+41log(1+t2)+21tan−1t+c. …
- 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 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 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 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. …
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