Q.Integrate the following function: xsin3x
Concept understanding — Integration by Parts
Integration by Parts
The idea: reverse the product rule
Some integrands are a product of two very different functions — xex, xcosx, logx, xsin−1x — where substitution gets you nowhere. Integration by parts is the tool for these. It comes straight from reversing the product rule for differentiation.
Starting from dxd(uv)=uv′+u′v and integrating both sides gives the working formula:
∫udxdvdx=uv−∫vdxdudx.
In words: integral of (first × derivative-of-second) = first × integral-of-second − integral of (derivative-of-first × integral-of-second).
Choosing u: the ILATE rule
The whole game is picking which factor is u (to differentiate) and which is dv (to integrate). Pick u by ILATE — the first type that appears:
- Inverse trig (sin−1x), Logarithmic (logx), Algebraic (x2), Trigonometric (sinx), Exponential (ex).
Whatever comes first in ILATE becomes u; the rest is dv. This makes the new integral ∫vdu simpler than the one you started with.
Worked idea
For ∫xexdx: algebraic before exponential, so u=x, dv=exdx. Then du=dx, v=ex:
∫xexdx=xex−∫exdx=xex−ex+C=ex(x−1)+C.
A single log or a single inverse-trig function (∫logxdx, ∫sin−1xdx) is still "by parts" — take the other factor as 1. And for the special form ∫ex(f(x)+f′(x))dx, the answer is simply exf(x)+C.
If applying the formula gives you back a multiple of the original integral (as with ∫exsinxdx), don't panic — solve for the integral algebraically.
Integration by Parts is one of the most tested methods in the NCERT Class 12 Mathematics chapter on Integrals, and "integration by parts formula ILATE rule" along with "integration by parts class 12 important questions" are among the top searches for students preparing for CBSE board exams and JEE Main calculus. The same ILATE-based technique extends naturally into JEE Advanced integral calculus problems built on this NCERT Class 12 foundation.
The key idea is Integration by Parts, which reverses the product rule. We choose u and dv so that the new integral is simpler.
Let u=x and dv=sin3xdx. Then du=dx and v=∫sin3xdx=−31cos3x.
Apply the formula ∫udv=uv−∫vdu:
∫xsin3xdx=x(−31cos3x)−∫(−31cos3x)dx
Simplify and integrate the remaining term:
=−3xcos3x+31∫cos3xdx=−3xcos3x+31⋅31sin3x+C
The integral is −3xcos3x+91sin3x+C.
The integral ∫xsin3xdx is solved using integration by parts (the product rule in reverse). Choosing u=x and dv=sin3xdx, we get the result −3xcos3x+91sin3x+C.
Why integration by parts?
When you see a product of two different kinds of functions — here, a polynomial (x) and a trigonometric function (sin3x) — the standard tool is integration by parts. It comes from the product rule for derivatives:
dxd(uv)=udxdv+vdxdu
Rearranging and integrating gives:
∫udv=uv−∫vdu
The trick is to pick u and dv so that the new integral ∫vdu is simpler than the original. For xsin3x, we want u to be something that simplifies when differentiated (like x, which becomes 1), and dv to be something we can integrate easily (like sin3x).
A common mistake is to pick u=sin3x and dv=xdx. Then du=3cos3xdx and v=2x2, giving 2x2sin3x−∫23x2cos3xdx — which is worse, not better. Always let the polynomial be u.
Step-by-step solution
1. Set up the parts.
Let u=x and dv=sin3xdx.
2. Differentiate u and integrate dv.
- du=dx
- v=∫sin3xdx=−31cos3x
For ∫sin(ax)dx, the antiderivative is −a1cos(ax). Here a=3, so it's −31cos3x.
3. Apply the integration by parts formula.
∫xsin3xdx=uv−∫vdu
Substitute:
=x⋅(−31cos3x)−∫(−31cos3x)dx
4. Simplify the expression.
=−3xcos3x+31∫cos3xdx
5. Integrate cos3x.
∫cos3xdx=31sin3x
So:
=−3xcos3x+31⋅31sin3x+C
6. Write the final result.
=−3xcos3x+91sin3x+C
The integral is −3xcos3x+91sin3x+C.
Method: Integration by parts with a scaled angle sin(ax)
Same by-parts idea as xsinx, but now the trig function has a coefficient a inside, which introduces factors of a1 at each integration.
Steps
Step 1: Choose u and dv by ILATE.
Algebraic before trigonometric: u=x (differentiates to 1), dv=sin(ax)dx.
Step 2: Integrate dv using the chain-rule factor.
∫sin(ax)dx=−a1cos(ax),∫cos(ax)dx=a1sin(ax).
Each integration of a scaled-angle function multiplies by a1; forgetting this is the usual error.
Step 3: Apply ∫udv=uv−∫vdu.
∫xsin(ax)dx=−axcos(ax)+a1∫cos(ax)dx.
Step 4: Finish and collect the a1 factors.
=−axcos(ax)+a1⋅a1sin(ax)+C=−axcos(ax)+a21sin(ax)+C.
For a=3 this gives the 91sin3x term — note it is a21, not a1.
Common Mistakes
Mistake 1: Ignoring the a1 factor for sin(3x).
Why it's wrong: ∫sin3xdx=−31cos3x and ∫cos3xdx=31sin3x; treating them as if a=1 gives wrong coefficients. Correct approach: Divide by the inner coefficient a=3 at each integration step.
Mistake 2: Writing 31sin3x instead of 91sin3x.
Why it's wrong: The final sin3x term picks up a1 twice (once from v, once from integrating cos3x), giving a21=91. Correct approach: Expect a21 on the sin term for xsin(ax).
Mistake 3: Swapping u and dv.
Why it's wrong: Taking u=sin3x makes the next integral worse. Correct approach: Let the polynomial x be u (ILATE).
Showing the 12 most recent of 39 on this concept.
- AP EAPCET 2026Set eng-2026-05-12-FN1 markMCQQ.If ∫ex((2+x)3/22−x2−x2)dx=exf(x)+c, then the domain of f(x) is (A) (−∞,−2)∪(2,∞) (B) [−2,2] (C) (−2,2] (D) (−∞,−2]∪[2,∞)
›Reveal solutionSolution
This tests the standard trick ∫ex[f(x)+f′(x)]dx=exf(x)+c; here f(x)=(2−x)/(2+x) and its domain is (−2,2].
Concept and Intuition
Whenever an integral has the shape ex×(something) and the answer is stated as exf(x)+c, the 'something' must secretly be f(x)+f′(x) — this is because dxd[exf(x)]=ex[f(x)+f′(x)]. So the real task is pattern-matching the given rational expression to a function plus its derivative.
Step-by-Step Solution
- Guess a form built from the surds present: f(x)=2+x2−x=(2−x)1/2(2+x)−1/2.
- Differentiate using the product/chain rule: let u=(2−x)/(2+x); u′=(2+x)2−(2+x)−(2−x)=(2+x)2−4. Then f′(x)=21u−1/2u′=212−x2+x⋅(2+x)2−4=(2+x)3/2(2−x)1/2−2.
- Add: over the common denominator (2+x)3/2(2−x)1/2, the numerator of f(x) becomes (2−x)(2+x)=4−x2, and f′(x) contributes −2. Sum of numerators: 4−x2−2=2−x2.
- So f(x)+f′(x)=(2+x)3/2(2−x)1/22−x2, matching the given integrand exactly, confirming f(x)=2+x2−x.
- Domain: need 2+x2−x≥0. This ratio is non-negative when numerator and denominator share sign: either both ≥0 (giving −2<x≤2, excluding x=−2 since denominator can't be 0) or both ≤0 (impossible here since that would need x≥2 and x<−2 simultaneously).
- Hence domain of f(x) is (−2,2].
Common Mistakes
- Including x=−2 (denominator zero — not allowed) or excluding x=2 (numerator zero is fine, gives f=0, allowed).
- Forgetting the original integrand itself also requires (2+x)3/2 real, consistent with x>−2.
✓Final answerThe correct option is (C) — (−2,2].
ANSWER: C
- AP EAPCET 2026Set eng-2026-05-13-FN1 markMCQQ.If f(x) is a twice differentiable function and f′(0)=0, then ∫0π/2(f(x)+f′′(x))cosxdx= (A) f(2π) (B) f′(2π) (C) 1 (D) 0
›Reveal solutionSolution
Two rounds of integration by parts on ∫0π/2f′′(x)cosxdx make the
∫f(x)cosxdx term reappear and cancel against the same term from the
original integral, leaving just f(π/2).
Concept and Intuition
When an integral mixes a function with its own second derivative against a
trigonometric weight, two rounds of integration by parts typically bring back a copy of
the original integral (since differentiating cosx twice returns −cosx,
picking up sign changes along the way) — so the two copies combine or cancel, leaving
only boundary terms.
Step-by-Step Solution
- Write the target as ∫0π/2f(x)cosxdx+∫0π/2f′′(x)cosxdx.
- For the second integral, integrate by parts with u=cosx, dv=f′′(x)dx so du=−sinxdx, v=f′(x): ∫0π/2f′′(x)cosxdx=[f′(x)cosx]0π/2+∫0π/2f′(x)sinxdx.
- Evaluate the boundary term: f′(π/2)cos(π/2)−f′(0)cos(0)=0−f′(0)⋅1=0 (using cos(π/2)=0 and the given f′(0)=0).
- So ∫0π/2f′′(x)cosxdx=∫0π/2f′(x)sinxdx.
- Integrate this by parts again, with u=sinx, dv=f′(x)dx so du=cosxdx, v=f(x): ∫0π/2f′(x)sinxdx=[f(x)sinx]0π/2−∫0π/2f(x)cosxdx=f(π/2)−∫0π/2f(x)cosxdx.
- Substituting back into step 1: total =∫0π/2f(x)cosxdx+[f(π/2)−∫0π/2f(x)cosxdx]=f(π/2).
Common Mistakes
- Forgetting to use the given condition f′(0)=0 to kill the first boundary term.
- Sign errors in the repeated integration by parts (the derivative of cosx is −sinx; of sinx is +cosx).
✓Final answerThe correct option is (A) — f(2π).
ANSWER: A
- AP EAPCET 2026Set eng-2026-05-14-AN1 markMCQQ.If ∫ex(x+1)3x3+3x2+4dx=exf(x)+c, then f(x)= (A) (x+1)2x2+2x−2 (B) (x+1)2x2+x−1 (C) (x+1)2x2−2x+2 (D) (x+1)2x2+2x−1
›Reveal solutionSolution
This is the classic ∫ex[f(x)+f′(x)]dx=exf(x)+c recognition problem; matching the rational integrand to g(x)+g′(x) for a guessed quadratic-over-(x+1)2 form pins down f(x)=(x+1)2x2+2x−2.
Concept and Intuition
Whenever an integral has the shape ∫ex⋅h(x)dx and the answer is claimed to be exf(x)+c, it must be that h(x)=f(x)+f′(x) (product rule run backwards). So instead of doing a hard partial-fraction integration of a rational function times ex, we can guess the shape of f(x) from the options (here, degree-2 over (x+1)2) and solve for its unknown coefficients algebraically.
Step-by-Step Solution
- We need f(x) with f(x)+f′(x)=(x+1)3x3+3x2+4. Try f(x)=(x+1)2x2+ax+b.
- Differentiate: f′(x)=(x+1)4(2x+a)(x+1)2−(x2+ax+b)⋅2(x+1)=(x+1)3(2x+a)(x+1)−2(x2+ax+b).
- Expand the numerator: (2x+a)(x+1)−2(x2+ax+b)=2x2+(2+a)x+a−2x2−2ax−2b=(2−a)x+(a−2b).
- So f′(x)=(x+1)3(2−a)x+(a−2b), while f(x)=(x+1)3(x2+ax+b)(x+1).
- Add: f(x)+f′(x)=(x+1)3(x2+ax+b)(x+1)+(2−a)x+(a−2b).
- Expand (x2+ax+b)(x+1)=x3+(1+a)x2+(a+b)x+b; adding the linear correction gives numerator x3+(1+a)x2+(b+2)x+(a−b).
- Match to x3+3x2+0⋅x+4: 1+a=3⇒a=2; b+2=0⇒b=−2; check constant a−b=2−(−2)=4 ✓ — all three equations agree.
- So f(x)=(x+1)2x2+2x−2. (Verified numerically at x=0 and x=1: both sides of the original identity match.)
Common Mistakes
- Forgetting the extra (x+1) multiplier when converting f(x)'s denominator (x+1)2 to the common denominator (x+1)3 before adding to f′(x).
- Not double-checking with the constant-term equation — two of the three equations can look consistent while the coefficient of a or b was mis-set.
✓Final answerThe correct option is (A) — (x+1)2x2+2x−2.
ANSWER: A
- AP EAPCET 2026Set eng-2026-05-18-FN1 markMCQQ.∫x2(logx)2dx= (A) 61x3[3(logx)2−3logx+4]+c (B) 271x3[9(logx)2−6logx+2]+c (C) 271x3[9(logx)2+6logx+2]+c (D) 91x3[6(logx)2−3logx+1]+c
›Reveal solutionSolution
Apply integration by parts twice (reduction formula style) on x2(logx)2; the result is 271x3[9(logx)2−6logx+2]+c.
Concept and Intuition
Each power of logx present costs one integration by parts with u=(logx)k, dv=xndx, reducing the power of the log by one each time. Two applications are needed here since (logx)2 appears.
Step-by-Step Solution
- First application (parts, u=(logx)2, dv=x2dx):
∫x2(logx)2dx=3x3(logx)2−32∫x2logxdx.
- Second application on ∫x2logxdx (u=logx, dv=x2dx):
∫x2logxdx=3x3logx−∫3x3⋅x1dx=3x3logx−9x3.
- Substitute back:
∫x2(logx)2dx=3x3(logx)2−32[3x3logx−9x3]=3x3(logx)2−92x3logx+272x3.
- Factor out 27x3:
=27x3[9(logx)2−6logx+2]+c.
Common Mistakes
- Stopping after one integration by parts (leaving a logx term unintegrated).
- Arithmetic slip when combining fractions with denominators 3 and 9 into the common denominator 27.
✓Final answerThe correct option is (B) — 271x3[9(logx)2−6logx+2]+c.
ANSWER: B
- AP EAPCET 2026Set eng-2026-05-18-AN1 markMCQQ.If ∫ex(n1+tannx)secnxdx=n1(g(x)+k)=F(x) and F(0)=1, then k= (A) n (B) n+1 (C) n−1 (D) 1
›Reveal solutionSolution
Spot that the integrand is exactly the derivative of exsec(nx)/n (a product-rule construction), then use the initial condition F(0)=1 to pin down k.
Concept and Intuition
Many integrals of the form ex[p(x)+p′(x)] (or similar structured combinations) are designed to be exact derivatives of ex⋅(something), since dxd[exh(x)]=exh(x)+exh′(x). Recognizing h(x)=sec(nx)/n here (whose derivative is sec(nx)tan(nx)) collapses the whole integral instantly.
Step-by-Step Solution
- Try h(x)=nsec(nx). Then h′(x)=n1⋅nsec(nx)tan(nx)=sec(nx)tan(nx).
- So dxd[exh(x)]=exh(x)+exh′(x)=ex(nsec(nx)+sec(nx)tan(nx))=ex(n1+tan(nx))sec(nx) — exactly the given integrand.
- So ∫ex(n1+tannx)secnxdx=exh(x)+C=nexsec(nx)+C=n1(exsec(nx)+nC).
- Comparing to the given form n1(g(x)+k): g(x)=exsec(nx) and k=nC (a constant).
- Use F(0)=1: F(0)=n1(g(0)+k)=n1(e0sec0+k)=n1(1+k)=1⇒1+k=n⇒k=n−1.
Common Mistakes
- Trying to integrate term-by-term (splitting n1secnx and tannxsecnx separately) instead of recognizing the exact-derivative structure, which leads to a much messier (and error-prone) path.
- Forgetting that g(x) must be evaluated at x=0, not treated as already containing the constant.
✓Final answerThe correct option is (C) — n−1.
ANSWER: C
- AP EAPCET 2026Set eng-2026-05-18-AN1 markMCQQ.If F(x)=∫x(logx)2dx and F(e)=4e2, then F(1)= (A) 0 (B) 41 (C) 21 (D) 3log(e2)
›Reveal solutionSolution
Integrating x(logx)2 twice by parts gives a closed form; matching F(e) pins the constant, then F(1)=1/4.
Concept and Intuition
∫x(logx)2dx is a repeated integration-by-parts problem: each application of parts trades one power of logx for a simpler integral, since dxd(logx)2=x2logx pairs nicely with ∫xdx=x2/2.
Step-by-Step Solution
- Let u=(logx)2, dv=xdx⇒du=x2logxdx, v=2x2.
F(x)=2x2(logx)2−∫xlogxdx
- For ∫xlogxdx, let u=logx, dv=xdx:
∫xlogxdx=2x2logx−4x2
- Substitute back:
F(x)=2x2(logx)2−2x2logx+4x2+C
- At x=e: loge=1, so
F(e)=2e2−2e2+4e2+C=4e2+C
Given F(e)=4e2, so C=0.
5. At x=1: log1=0, so every log term vanishes:
F(1)=0−0+41+0=41
Common Mistakes
- Forgetting the second integration by parts and stopping at 2x2(logx)2−∫xlogxdx.
- Losing the constant C and assuming F(e) automatically equals the closed-form value without solving for C.
✓Final answerThe correct option is (B) — 41.
ANSWER: B
- AP EAPCET 2026Set eng-2026-05-18-AN1 markMCQQ.If ∫e5xxndx=F(n,x)+c, then 5F(n,x)+nF(n−1,x)= (A) F′(n,x)+k (B) 51F′(n,x)+k (C) 5xF′(n,x)+k (D) F(n,x)x2F′(n,x)+k
›Reveal solutionSolution
Using the standard reduction formula for ∫eaxxndx and the fact that F′(n,x) is just the original integrand recovers 5F(n,x)+nF(n−1,x)=F′(n,x).
Concept and Intuition
F(n,x) is defined as an antiderivative, so by the Fundamental Theorem of Calculus its derivative is simply the integrand: F′(n,x)=e5xxn. Separately, integration by parts on ∫e5xxndx produces a reduction formula relating F(n,x) to F(n−1,x).
Step-by-Step Solution
- Integrate by parts with u=xn, dv=e5xdx⇒du=nxn−1dx, v=5e5x:
∫e5xxndx=5xne5x−5n∫e5xxn−1dx
- In terms of F: F(n,x)=5xne5x−5nF(n−1,x), so
5F(n,x)+nF(n−1,x)=xne5x
- But since F(n,x)+c=∫e5xxndx, differentiating both sides w.r.t. x gives
F′(n,x)=e5xxn
- Therefore 5F(n,x)+nF(n−1,x)=F′(n,x), matching option (A) up to the integration constant k.
Common Mistakes
- Trying to directly differentiate a "closed form" for F(n,x) instead of recognizing F′(n,x) is just the original integrand.
- Sign errors in the reduction formula (forgetting the −n/5 factor).
✓Final answerThe correct option is (A) — F′(n,x)+k.
ANSWER: A
- AP EAPCET 2025Set eng-2025-05-21-FN1 markMCQQ.∫(logx)3x4dx= (A) x5[51(logx)3−253(logx)2+1256logx−6256]+c (B) x5[51(logx)3−252(logx)2+1256logx−12512]+c (C) x5[51(logx)3−254(logx)2−1259logx−1258]+c (D) x5[51(logx)3+253(logx)2−1256logx−1256]+c
›Reveal solutionSolution
Repeated integration by parts (equivalently, the standard reduction formula) on ∫x4(logx)3dx, reducing the power of logx one step at a time. Answer matches option (A).
Concept and Intuition
For ∫xn(logx)kdx, integrating by parts with u=(logx)k, dv=xndx gives the reduction
∫xn(logx)kdx=n+1xn+1(logx)k−n+1k∫xn(logx)k−1dx,
which is applied repeatedly until the power of logx drops to zero (a plain power integral).
Step-by-Step Solution
Here n=4, so the recursion factor is 5k at each step.
- Base (k=0): ∫x4dx=5x5.
- k=1: ∫x4logxdx=5x5logx−51∫x4dx=5x5logx−25x5.
- k=2:
∫x4(logx)2dx=5x5(logx)2−52∫x4logxdx=5x5(logx)2−52(5x5logx−25x5)
=5x5(logx)2−252x5logx+1252x5.
- k=3:
∫x4(logx)3dx=5x5(logx)3−53∫x4(logx)2dx
=5x5(logx)3−53(5x5(logx)2−252x5logx+1252x5)
=5x5(logx)3−253x5(logx)2+1256x5logx−6256x5.
- Factor out x5:
x5[51(logx)3−253(logx)2+1256logx−6256]+c.
Common Mistakes
- Losing track of the sign alternation across successive reduction steps.
- Arithmetic slip in the repeated multiplication by 5k, especially in the constant term 6256 (a common trap that shows up altered in the wrong-answer distractors).
✓Final answerThe correct option is (A) — x5[51(logx)3−253(logx)2+1256logx−6256]+c.
ANSWER: A
- AP EAPCET 2025Set eng-2025-05-21-AN1 markMCQQ.If ∫x2cos2xdx=61f(x)+g(x)sin2x+h(x)cos2x+c, then f(1)+g(2)+h(21)= (A) 0 (B) 2 (C) 1 (D) −1
›Reveal solutionSolution
Use cos2x=(1+cos2x)/2 to split the integral, then integrate x2cos2x by parts (twice) to get the sin2x and cos2x coefficient functions. Answer: f(1)+g(2)+h(1/2)=2.
Concept and Intuition
Squares of trig functions are best handled via the power-reduction (double-angle) identities, turning x2cos2x into a polynomial term plus a polynomial-times-cos2x term. The latter is a standard repeated integration-by-parts pattern (polynomial degree 2 needs two applications), producing terms in sin2x and cos2x with polynomial coefficients — exactly the structure the question sets up.
Step-by-Step Solution
- cos2x=21+cos2x, so x2cos2x=2x2+2x2cos2x.
- ∫2x2dx=6x3.
- For ∫x2cos2xdx, integrate by parts with u=x2,dv=cos2xdx:
∫x2cos2xdx=2x2sin2x−∫xsin2xdx.
- For ∫xsin2xdx, parts again with u=x,dv=sin2xdx:
∫xsin2xdx=−2xcos2x+∫2cos2xdx=−2xcos2x+4sin2x.
- Combine: ∫x2cos2xdx=2x2sin2x+2xcos2x−4sin2x.
- Halve (from step 1's factor 21): ∫2x2cos2xdx=4x2sin2x+4xcos2x−8sin2x.
- Total integral: 6x3+(4x2−81)sin2x+4xcos2x+c.
- Matching 61f(x)+g(x)sin2x+h(x)cos2x+c: f(x)=x3, g(x)=4x2−81, h(x)=4x.
- f(1)=1; g(2)=44−81=1−81=87; h(21)=41/2=81.
- Sum: 1+87+81=1+1=2.
Common Mistakes
- Forgetting to re-distribute the outer 21 factor from step 1 across the by-parts result in step 5, which shifts all coefficients.
- Sign slip in the double by-parts (a very common source of error is the second application's sign on −xcos2x/2).
✓Final answerThe correct option is (B) — 2.
ANSWER: B
- AP EAPCET 2025Set eng-2025-05-23-FN1 markMCQQ.∫cos−1(1+x21−x2)dx= (A) 2[xtan−1x−log1+x2]+c (B) 2xtan−1x+log1+x2+c (C) xtan−1x+log1−x2+c (D) 2[tan−1x−log1+x2]+c
›Reveal solutionSolution
Recognising the standard identity cos−1(1+x21−x2)=2tan−1x turns this into a routine integration-by-parts problem.
Concept and Intuition
Substituting x=tanϕ turns 1+x21−x2 into cos2ϕ (the standard tangent half-angle relation), so cos−1(1+x21−x2)=2ϕ=2tan−1x (for the principal range where this holds).
Step-by-Step Solution
- cos−1(1+x21−x2)=2tan−1x.
- Integral becomes ∫2tan−1xdx.
- Integrate by parts with u=tan−1x, dv=dx: ∫tan−1xdx=xtan−1x−∫1+x2xdx.
- ∫1+x2xdx=21ln(1+x2)=log1+x2.
- So ∫tan−1xdx=xtan−1x−log1+x2+c′, and doubling: 2[xtan−1x−log1+x2]+c.
Common Mistakes
- Forgetting the factor of 2 from the identity when writing the final antiderivative.
- Writing ln(1+x2) instead of log1+x2=21ln(1+x2), doubling the log term incorrectly.
✓Final answerThe correct option is (A) — 2[xtan−1x−log1+x2]+c.
ANSWER: A
- AP EAPCET 2025Set eng-2025-05-26-AN1 markMCQQ.∫(log2x)3dx= (A) x[(log2x)3−3(log2x)2+6(log2x)−6]+c (B) 4x[4(log2x)3−6(log2x)2+6(log2x)−3]+c (C) 2x[(log2x)3−3(log2x)2+3(log2x)−6]+c (D) x[(log2x)3−6(log2x)2+18(log2x)−54]+c
›Reveal solutionSolution
Because log(2x) differentiates exactly like logx, three rounds of integration by parts reproduce the classical (logx)3 antiderivative pattern.
Concept and Intuition
dxdlog(2x)=x1 — the constant factor 2 inside the log vanishes on differentiation. So treating u=log(2x) behaves exactly as u=logx would under repeated integration by parts with dv=dx.
Step-by-Step Solution
- Let t=log2x. Using ∫t3dx=xt3−3∫t2dx (parts: u=t3,dv=dx, du=3t2⋅x1dx, v=x).
- Similarly ∫t2dx=xt2−2∫tdx, and ∫tdx=xt−x.
- Back-substitute: ∫t2dx=xt2−2(xt−x)=xt2−2xt+2x.
- ∫t3dx=xt3−3(xt2−2xt+2x)=xt3−3xt2+6xt−6x.
- So ∫(log2x)3dx=x[(log2x)3−3(log2x)2+6(log2x)−6]+c.
Common Mistakes
- Assuming the factor 2 inside the log changes the coefficients — it doesn't, since it only shifts the log by a constant and disappears on differentiation.
- Losing a factor during the repeated back-substitution.
✓Final answerThe correct option is (A) — x[(log2x)3−3(log2x)2+6(log2x)−6]+c.
ANSWER: A
- AP EAPCET 2025Set eng-2025-05-26-FN1 markMCQQ.∫01xsin−1xdx= (A) 8π (B) 4π (C) 12π (D) 3π
›Reveal solutionSolution
Integration by parts on ∫01xsin−1xdx, with the resulting ∫x2/1−x2dx handled via a standard reduction, gives 8π.
Concept and Intuition
When the integrand is a product of a polynomial and an inverse trig function, integration by parts with u=sin−1x (so u′ is algebraic) and dv=xdx (easy to integrate) is the standard approach — it trades the inverse-trig factor for a simpler algebraic integral.
Step-by-Step Solution
- Let u=sin−1x, dv=xdx. Then du=1−x2dx, v=2x2.
- By parts: ∫xsin−1xdx=2x2sin−1x−∫21−x2x2dx.
- For ∫1−x2x2dx, write x2=1−(1−x2), so it equals ∫1−x2dx−∫1−x2dx=sin−1x−[2x1−x2+21sin−1x]=21sin−1x−2x1−x2.
- So ∫xsin−1xdx=2x2sin−1x−21[21sin−1x−2x1−x2]=2x2sin−1x−41sin−1x+4x1−x2.
- Evaluate at x=1: 21⋅2π−41⋅2π+0=4π−8π=8π.
- Evaluate at x=0: 0−0+0=0.
- Definite integral =8π−0=8π.
Common Mistakes
- Forgetting the standard reduction formula for ∫1−x2dx and trying to integrate it from scratch, introducing errors.
- Sign slip in the by-parts formula when subtracting the second integral.
✓Final answerThe correct option is (A) — 8π.
ANSWER: A
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