Q.Evaluate ∫0π/2logsinxdx
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Definite Integral Symmetry: The Shortcut That Saves You Work
Asked to find the area under f(x)=x3 from x=−2 to x=2? You could integrate directly — but there's a much faster way if you notice the symmetry of the graph.
The Intuition: What Does "Symmetry" Mean Here?
A function can be symmetric about the y-axis (like x2 or cosx) or about the origin (like x3 or sinx). When you integrate over a symmetric interval — from −a to a — these symmetries create a predictable cancellation or doubling.
Even functions (symmetric about the y-axis): f(−x)=f(x) — think x2, x4, cosx, ∣x∣. The left side mirrors the right, so the area from −a to 0 equals the area from 0 to a. The total is double the area on one side.
Odd functions (symmetric about the origin): f(−x)=−f(x) — think x3, x5, sinx, tanx. The left side is the negative mirror of the right, so every positive area on the right is cancelled by an equal negative area on the left. The total is zero.
This only works when the limits are symmetric about zero — from −a to a. For [0,a] or [1,3], symmetry doesn't help directly.
The Precise Statement
Let f be continuous on [−a,a].
- If f is even (f(−x)=f(x)), then ∫−aaf(x)dx=2∫0af(x)dx
- If f is odd (f(−x)=−f(x)), then ∫−aaf(x)dx=0
∫−aaf(x)dx={2∫0af(x)dx0if f is evenif f is odd
Why Does This Work? (A Quick Proof)
Split at zero:
∫−aaf(x)dx=∫−a0f(x)dx+∫0af(x)dx
For the first term substitute u=−x (dx=−du; x=−a→u=a, x=0→u=0):
∫−a0f(x)dx=∫0af(−u)du
Now use symmetry:
- If f is even, f(−u)=f(u), so this becomes ∫0af(u)du; adding the second term gives 2∫0af(x)dx.
- If f is odd, f(−u)=−f(u), so this becomes −∫0af(u)du; adding the second term gives 0.
Common Mistakes to Avoid
Don't assume symmetry without checking. A "balanced"-looking function need not be even or odd — e.g. f(x)=x2+x is neither, so these formulas don't apply. Always verify f(−x)=f(x) or f(−x)=−f(x) for all x.
The interval must be [−a,a]. If the limits are [−2,3], symmetry doesn't apply directly — split the integral or shift variables.
Examples to Cement the Idea
Example 1: ∫−33x4dx — x4 is even, so
∫−33x4dx=2∫03x4dx=2[5x5]03=2⋅5243=5486 …
The key idea is to use the symmetry of the definite integral, often called the King's property: ∫0af(x)dx=∫0af(a−x)dx.
Let I=∫0π/2logsinxdx.
Using the substitution x→2π−x, we get
I=∫0π/2logsin(2π−x)dx=∫0π/2logcosxdx.
Add the two expressions for I:
2I=∫0π/2(logsinx+logcosx)dx=∫0π/2log(sinxcosx)dx.
Use sinxcosx=21sin2x, so
2I=∫0π/2log(21sin2x)dx=∫0π/2log21dx+∫0π/2logsin2xdx.
The first term is −2πlog2. For the second, let t=2x, then dx=dt/2, limits 0 to π: …
This classic integral is solved using the symmetry property of definite integrals. By substituting x→2π−x and adding the two forms, we transform the product sinxcosx into 21sin2x, leading to a simple equation whose solution is ∫0π/2logsinxdx=−2πlog2.
The integral I=∫0π/2logsinxdx is a famous one — it appears in many contexts, from probability to number theory. The trick is not to integrate directly (the antiderivative involves the dilogarithm), but to exploit symmetry.
Why symmetry works: The interval [0,π/2] is symmetric about π/4. The function logsinx is not symmetric itself, but if we replace x by 2π−x, we get logcosx. Adding the two forms gives log(sinxcosx)=log(21sin2x), which splits into a constant term and a scaled version of the original integral. This creates an equation we can solve for I.
Let’s walk through it step by step.
- Define the integral and apply the substitution x→2π−x. Let I=∫0π/2logsinxdx. Substitute x=2π−t. Then dx=−dt, and when x=0, t=π/2; when x=π/2, t=0. So:
I=∫π/20logsin(2π−t)(−dt)=∫0π/2logcostdt.
Renaming the dummy variable back to x, we have:
I=∫0π/2logcosxdx.
So the integral of logsinx equals the integral of logcosx over the same interval.
- Add the two expressions for I.
2I=∫0π/2logsinxdx+∫0π/2logcosxdx=∫0π/2log(sinxcosx)dx.
Using the identity sinxcosx=21sin2x, we get:
2I=∫0π/2log(21sin2x)dx=∫0π/2(log21+logsin2x)dx.
The constant log(1/2)=−log2 factors out:
2I=−log2∫0π/21dx+∫0π/2logsin2xdx=−2πlog2+∫0π/2logsin2xdx.
- Handle the integral ∫0π/2logsin2xdx with another substitution. Let u=2x. Then dx=du/2, and when x=0, u=0; when x=π/2, u=π. So:
∫0π/2logsin2xdx=21∫0πlogsinudu.
Now, the integral from 0 to π of logsinu can be split at π/2:
∫0πlogsinudu=∫0π/2logsinudu+∫π/2πlogsinudu. …
Method: Reflection plus double-angle self-similarity for log-trig integrals
Use this for integrals like ∫0π/2logsinxdx where direct antidifferentiation fails (the antiderivative is non-elementary) but the interval [0,2π] has sin↔cos symmetry.
Steps
Step 1: Reflect with x→2π−x.
By ∫0af(x)dx=∫0af(a−x)dx, the integral of logsinx equals the integral of logcosx over the same interval. So I can be written two ways.
Step 2: Add the two forms and use a product identity.
2I=∫0π/2log(sinxcosx)dx=∫0π/2log(21sin2x)dx.
Splitting the log separates a constant term ∫0π/2log21dx from a new logsin2x term.
Step 3: Rescale the double angle back to the original integral. …
Common Mistakes
Mistake 1: Dropping the 21 factor when substituting t=2x.
Why it's wrong: t=2x gives dx=2dt, so ∫0π/2logsin2xdx=21∫0πlogsintdt; omitting the 21 doubles that term and gives a wrong final value. Correct approach: carry the Jacobian dx=2dt through carefully.
Mistake 2: Splitting log(21sin2x) incorrectly. …
Showing the 12 most recent of 48 on this concept.
- AP EAPCET 2025Set eng-2025-05-21-AN1 markMCQQ.∫0π/2log∣tanx+cotx∣dx= (A) πlog2 (B) −πlog2 (C) 2πlog2 (D) 2πlog2
›Reveal solutionSolution
Simplify tanx+cotx=2/sin2x, split the log, and use the classical result ∫0πlogsinudu=−πlog2. Answer: πlog2.
Concept and Intuition
tanx+cotx always simplifies to sin2x2 via the Pythagorean identity — a very common simplification in definite-integral problems. This converts the problem into the well-known integral of logsin, whose value over a full "half-period" (0 to π) is a standard memorized result, −πlog2.
Step-by-Step Solution
- tanx+cotx=cosxsinx+sinxcosx=sinxcosxsin2x+cos2x=sinxcosx1=sin2x2.
- So log∣tanx+cotx∣=log2−log(sin2x) (since sin2x>0 on (0,π/2)).
- ∫0π/2log∣tanx+cotx∣dx=2πlog2−∫0π/2log(sin2x)dx.
- Let I=∫0π/2log(sin2x)dx. Substitute u=2x,du=2dx: I=21∫0πlog(sinu)du. …
- AP EAPCET 2024Set eng-2024-05-22-FN1 markMCQQ.∫0π/4log(1+tanx)dx= (A) πlog2+1 (B) 2πlog2+1 (C) 4πlog2 (D) 8πlog2
›Reveal solutionSolution
A textbook symmetry trick (x→π/4−x) doubles the integral into something trivial to evaluate. Answer: 8πlog2.
Concept and Intuition
Whenever the limits are 0 to a and the integrand involves tanx, trying the substitution x→a−x is a classic move — here it converts log(1+tanx) into log(1+tanx2), and adding the original and transformed integrals collapses most of the complexity.
Step-by-Step Solution
- Let I=∫0π/4log(1+tanx)dx.
- Substitute x→4π−x: tan(4π−x)=1+tanx1−tanx, so 1+tan(4π−x)=1+tanx2.
- So I=∫0π/4log(1+tanx2)dx=∫0π/4log2dx−∫0π/4log(1+tanx)dx=4πlog2−I. …
- AP EAPCET 2024Set eng-2024-05-20-AN1 markMCQQ.∫−1/241/24secxlog(1+x1−x)dx= (A) 2π (B) π (C) 1 (D) 0
›Reveal solutionSolution
The integrand is odd (even × odd), and it's integrated over a symmetric interval [−1/24,1/24], so the integral is 0 — (D).
Concept and Intuition
Rather than actually evaluating a messy integral, check the parity of the integrand first: if f(−x)=−f(x) (odd) and the limits are symmetric about 0, the positive and negative halves cancel exactly, giving 0 — no computation needed.
Step-by-Step Solution
- Let g(x)=log(1+x1−x). Then g(−x)=log(1+(−x)1−(−x))=log(1−x1+x)=log[(1+x1−x)−1]=−log(1+x1−x)=−g(x). So g is odd.
- secx is an even function (sec(−x)=secx).
- The product secx⋅g(x) is even × odd = odd.
- The limits of integration, −241 to 241, are symmetric about 0. …
- AP EAPCET 2025Set eng-2025-05-21-FN1 markMCQQ.∫0π1+cos2xxsinxdx= (A) 4π2 (B) 2π (C) 2π2 (D) 4π
›Reveal solutionSolution
This is the classic ∫0πxf(sinx,cosx)dx trick using the substitution x→π−x; the answer is (A).
Concept and Intuition
For integrals of the form ∫0πxg(cosx)sinxdx, substituting x→π−x (using sin(π−x)=sinx and cos(π−x)=−cosx, but here cos2 is unaffected) converts the x factor into π−x, letting you solve for the integral algebraically in terms of a simpler integral without the x weight.
Step-by-Step Solution
- Let I=∫0π1+cos2xxsinxdx.
- Substitute x→π−x: sin(π−x)=sinx, cos2(π−x)=cos2x, so
I=∫0π1+cos2x(π−x)sinxdx=π∫0π1+cos2xsinxdx−I.
- So 2I=π∫0π1+cos2xsinxdx. …
- AP EAPCET 2024Set eng-2024-05-20-AN1 markMCQQ.∫0π1+cos2xxsinxdx= (A) 0 (B) 2π (C) 2π2 (D) 4π2
›Reveal solutionSolution
This is the classic "xf(sinx)" King's-rule setup; it reduces to π/2 times a standard arctan integral, giving 4π2 — (D).
Concept and Intuition
Whenever the integrand has the shape x⋅g(sinx,cos2x) over [0,π] and g is invariant under x→π−x (true here since sin(π−x)=sinx and cos2(π−x)=cos2x), the King's-rule substitution x→π−x lets us replace the "x" prefactor with "π−x", and adding the two forms eliminates the awkward x entirely.
Step-by-Step Solution
- Let I=∫0π1+cos2xxsinxdx and f(x)=1+cos2xsinx.
- Check f(π−x)=1+cos2(π−x)sin(π−x)=1+cos2xsinx=f(x) — confirmed invariant.
- By King's rule: I=∫0π(π−x)f(x)dx=π∫0πf(x)dx−I.
- So 2I=π∫0πf(x)dx=πJ, where J=∫0π1+cos2xsinxdx. …
- AP EAPCET 2024Set eng-2024-05-20-FN1 markMCQQ.∫−ππ4−cos2xxsin3xdx= (A) 2π(1−log3) (B) 2π(1−43log3) (C) π(1−43log3) (D) 4π(1−log3)
›Reveal solutionSolution
Use symmetry (odd integrand times x, plus f(π−x)=f(x)) to strip the x out of the integral, then finish with a u=cosx substitution and partial fractions.
Concept and Intuition
Integrals of the form ∫−aaxg(x)dx where g is odd become 2∫0axg(x)dx (since xg(x) is even). If additionally g(π−x)=g(x) on [0,π], the classic "King's Rule" trick ∫0πxg(x)dx=2π∫0πg(x)dx removes the x factor entirely.
Step-by-Step Solution
- Let g(x)=4−cos2xsin3x. Since sin3(−x)=−sin3x and cos2(−x)=cos2x, g is odd, so xg(x) is even: ∫−ππxg(x)dx=2∫0πxg(x)dx.
- Also g(π−x)=4−cos2(π−x)sin3(π−x)=4−cos2xsin3x=g(x) (since sin(π−x)=sinx, cos(π−x)=−cosx), so King's Rule gives ∫0πxg(x)dx=2π∫0πg(x)dx.
- Combining: original integral =2⋅2π∫0πg(x)dx=π∫0πg(x)dx=πJ.
- Compute J=∫0π4−cos2xsin3xdx via u=cosx: J=∫−114−u21−u2du=2∫01[1−4−u23]du (using 1−u2=(4−u2)−3). …
- AP EAPCET 2024Set eng-2024-05-22-FN1 markMCQQ.∫−ππ1+cos2xxsinxdx= (A) 43π2 (B) 2π+1 (C) 4π2 (D) 2π2
›Reveal solutionSolution
Combine the even-function property over [−π,π] with the classic x→π−x symmetry trick for integrals of xg(sinx,cosx). Answer: π2/2.
Concept and Intuition
First check parity: since sin(−x)=−sinx and cos2(−x)=cos2x, the integrand f(x)=1+cos2xxsinx satisfies f(−x)=f(x) — it's even, so the integral over [−π,π] is twice the integral over [0,π]. Then, for integrals of x times a function of sinx,cosx over [0,π], the substitution x→π−x is the standard tool to eliminate the explicit x.
Step-by-Step Solution
- Since f(−x)=f(x): ∫−ππfdx=2∫0πfdx=2J, where J=∫0π1+cos2xxsinxdx.
- Substitute x→π−x in J: sin(π−x)=sinx, cos(π−x)=−cosx (so cos2 unchanged): J=∫0π1+cos2x(π−x)sinxdx=π∫0π1+cos2xsinxdx−J.
- So 2J=πK where K=∫0π1+cos2xsinxdx. …
- AP EAPCET 2025Set eng-2025-05-22-FN1 markMCQQ.∫0πsin2x+2cos2xxsinxdx= (A) 2π (B) 2π2 (C) 4π2 (D) 4π
›Reveal solutionSolution
Rewriting sin2x+2cos2x=1+cos2x and applying the classical ∫0πxf(sinx,cos2x)dx=2π∫0πfdx symmetry reduces the problem to a standard arctangent integral, giving π2/4.
Concept and Intuition
Whenever an integrand over [0,π] depends on x only through sinx and cos2x (both invariant, or simply transformed, under x↦π−x), the King's-rule substitution I=∫0πxf(x)dx=2π∫0πf(x)dx eliminates the explicit x factor.
Step-by-Step Solution
- Simplify the denominator: sin2x+2cos2x=(sin2x+cos2x)+cos2x=1+cos2x.
- Let I=∫0π1+cos2xxsinxdx.
- Apply x→π−x: sin(π−x)=sinx, cos(π−x)=−cosx⇒cos2(π−x)=cos2x. So I=∫0π1+cos2x(π−x)sinxdx=π∫0π1+cos2xsinxdx−I.
- So 2I=πJ where J=∫0π1+cos2xsinxdx. …
- AP EAPCET 2026Set eng-2026-05-12-AN1 markMCQQ.∫0π/2sinx+cosxsin3xdx= (A) 4π+1 (B) 2π−2 (C) 4π−2 (D) 4π−1
›Reveal solutionSolution
By symmetry I=J (the cos3 analogue) and I+J=π/2−1/2 via a sum-of-cubes factorisation, giving I=(π−1)/4.
Concept and Intuition
Define J as the same integral with sin3x replaced by cos3x. The substitution x→π/2−x shows I=J exactly (not just numerically), because it swaps sine and cosine while leaving sinx+cosx and the interval unchanged. Then the sum-of-cubes identity sin3x+cos3x=(sinx+cosx)(1−sinxcosx) lets I+J collapse to an elementary integral, and since I=J, each equals half of that sum.
Step-by-Step Solution
- Let I=∫0π/2sinx+cosxsin3xdx and J=∫0π/2sinx+cosxcos3xdx.
- Substituting u=π/2−x in I: sinx→cosu, cosx→sinu, limits unchanged, giving I=∫0π/2cosu+sinucos3udu=J. So I=J.
- I+J=∫0π/2sinx+cosxsin3x+cos3xdx. Using sin3x+cos3x=(sinx+cosx)(sin2x−sinxcosx+cos2x)=(sinx+cosx)(1−sinxcosx), this simplifies to ∫0π/2(1−sinxcosx)dx. …
- AP EAPCET 2022Set eng-2022-07-04-FN1 markMCQQ.∫0πx(sin2(sinx)+cos2(cosx))dx= (A) π2 (B) π2/2 (C) 2π (D) π/4
›Reveal solutionSolution
Uses the ∫0axf(x)dx=2a∫0af(x)dx trick (valid when f(a−x)=f(x)) plus a π/2-symmetry identity to collapse the integrand to a constant; the answer is π2/2.
Concept and Intuition
Whenever ∫0axf(x)dx appears with f(a−x)=f(x), King's Property gives ∫0axf(x)dx=2a∫0af(x)dx — the x weight averages out. Separately, sin2(sinx)+cos2(cosx) has a beautiful complementary-angle identity that makes its integral over a quarter period trivial.
Step-by-Step Solution
- Let h(x)=sin2(sinx)+cos2(cosx). Check h(π−x): sin(π−x)=sinx and cos(π−x)=−cosx, and since cos(−cosx)=cos(cosx) (cosine is even), we get h(π−x)=h(x).
- By King's property, I=∫0πxh(x)dx=2π∫0πh(x)dx.
- Since h(π−x)=h(x), h is symmetric about x=π/2, so ∫0πhdx=2∫0π/2hdx.
- On [0,π/2], substitute x→π/2−x in just the cosine part: ∫0π/2cos2(cosx)dx=∫0π/2cos2(sinx)dx (since cos(π/2−x)=sinx). …
- AP EAPCET 2023Set eng-2023-05-17-AN1 markMCQQ.∫π/6π/31+cotx1dx= (A) π/4 (B) π/2 (C) π/6 (D) π/12
›Reveal solutionSolution
Using the reflection property ∫abf(x)dx=∫abf(a+b−x)dx with a+b=π/2 makes the two forms of the integrand add up to exactly 1, giving I=π/12.
Concept and Intuition
Integrals of the shape ∫1+h(x)dx over symmetric limits around x=π/4-type reflections often pair up with their "co-function" version to sum to a constant — a classic trick that avoids ever actually antidifferentiating cot or tan raised to a half power.
Step-by-Step Solution
- Let I=∫π/6π/31+cotxdx.
- Since π/6+π/3=π/2, substitute x→π/2−x: cot(π/2−x)=tanx, so I=∫π/6π/31+tanxdx as well.
- Add the two expressions for I: 2I=∫π/6π/3[1+cotx1+1+tanx1]dx. …
- AP EAPCET 2021Set eng-2021-08-24-FN1 markMCQQ.∫0πsecx+tanxxtanxdx= (A) 2π(π−2) (B) 2π+2 (C) 2π(π+2) (D) 2π−2
›Reveal solutionSolution
The integrand times x over [0,π] is handled with the symmetry trick ∫0axf(x)dx=2a∫0af(x)dx when f(a−x)=f(x).
Concept and Intuition
tanx/(secx+tanx) simplifies to sinx/(1+sinx), a function symmetric under x→π−x. This symmetry lets us replace the troublesome factor of x with a constant π/2, reducing the problem to a standard definite integral.
Step-by-Step Solution
- Simplify: secx+tanxtanx=(1+sinx)/cosxsinx/cosx=1+sinxsinx=f(x).
- Check symmetry: f(π−x)=1+sin(π−x)sin(π−x)=1+sinxsinx=f(x). ✓
- By the King's rule, I=∫0πxf(x)dx=2π∫0πf(x)dx.
- Compute J=∫0π1+sinxsinxdx=∫0π[1−1+sinx1]dx=π−∫0π1+sinxdx. …
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