Q.By using the properties of definite integrals, evaluate the integral ∫0π/2(2logsinx−logsin2x)dx
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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 integrand and the standard result ∫0π/2logsinxdx=−2πlog2.
First, simplify the integrand:
2logsinx−logsin2x=2logsinx−log(2sinxcosx)=2logsinx−(log2+logsinx+logcosx)
=logsinx−logcosx−log2.
So the integral becomes:
I=∫0π/2(logsinx−logcosx)dx−log2∫0π/21dx. …
Using symmetry and the property ∫0af(x)dx=∫0af(a−x)dx, the given integral simplifies to −2πlog2.
The key to this problem lies in recognising that the integrand can be rewritten using logarithm properties, and then applying the standard definite integral symmetry trick. When you see an integral from 0 to 2π involving logsinx, your first instinct should be to use the substitution x→2π−x — this often creates a second copy of the same integral, allowing you to solve for it algebraically.
Let’s break it down.
- Simplify the integrand using log rules. The expression inside the integral is 2logsinx−logsin2x. Using logab=bloga and loga−logb=logba, we get:
2logsinx−logsin2x=log(sin2x)−log(sin2x)=log(sin2xsin2x).
Now recall the double-angle identity: sin2x=2sinxcosx. Substituting:
sin2xsin2x=2sinxcosxsin2x=2cosxsinx=21tanx.
So the integrand becomes log(21tanx)=log21+log(tanx)=−log2+log(tanx).
Therefore, the integral I is:
I=∫0π/2(−log2+log(tanx))dx=−log2∫0π/2dx+∫0π/2log(tanx)dx.
The first part is easy: ∫0π/2dx=2π, so that term is −2πlog2.
-
Now handle the tricky part: J=∫0π/2log(tanx)dx.
At first glance, log(tanx) looks like it might be messy. But here’s the beautiful symmetry trick: use the substitution x→2π−x.
Let x=2π−t. Then dx=−dt, and when x=0, t=2π; when x=2π, t=0. So:
J=∫0π/2log(tanx)dx=∫π/20log(tan(2π−t))(−dt)=∫0π/2log(tan(2π−t))dt.
Now, tan(2π−t)=cott=tant1. So: …
Method: Simplify logs first, then use the ∫0π/2log(tanx)=0 symmetry
For integrands built from logsin, logcos, logsin2x, collapse them with log and double-angle rules, then exploit the reflection x→2π−x that sends logtanx→−logtanx.
Steps
Step 1: Compress with log laws.
Use alogm=logma, logm−logn=lognm, and sin2x=2sinxcosx to reduce the integrand to log(tanx) plus a constant.
Step 2: Split off the constant. …
Common Mistakes
Mistake 1: Expanding logsin2x incorrectly.
Why it's wrong: sin2x=2sinxcosx, so logsin2x=log2+logsinx+logcosx; dropping a term leaves the wrong constant. Correct approach: apply the product-to-sum log rule fully.
Mistake 2: Not recognising ∫0π/2logtanxdx=0. …
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 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. …
- AP EAPCET 2022Set eng-2022-07-05-AN1 markMCQQ.∫−ππ1+cos2x2x(1+sinx)dx= (A) 2π (B) π2 (C) π+2 (D) π/2
›Reveal solutionSolution
Splitting the integrand by parity kills the odd piece immediately; the remaining even piece is handled with the classic "∫0πxf(sinx,cosx)dx=2π∫0πf(sinx,cosx)dx"-style symmetry trick, collapsing to a simple arctangent integral.
Concept and Intuition
Whenever a definite integral is over a symmetric interval like [−π,π], always check parity first: odd integrands vanish, and even integrands can be doubled and computed over [0,π] only. For integrals of the form ∫0πxg(sinx,cosx)dx, the substitution x→π−x often converts the "x" factor into "π−x", letting you solve for the integral in terms of a simpler one without the x multiplier.
Step-by-Step Solution
- Write 1+cos2x2x(1+sinx)=1+cos2x2x+1+cos2x2xsinx.
- The first term, 1+cos2x2x, is odd (odd/even = odd), so ∫−ππ of it is 0.
- The second term, 1+cos2x2xsinx, is even (odd×odd = even, divided by even), so
∫−ππ1+cos2x2xsinxdx=2∫0π1+cos2x2xsinxdx=4∫0π1+cos2xxsinxdx.
- Let J=∫0π1+cos2xxsinxdx. Substituting x→π−x (using sin(π−x)=sinx, cos(π−x)=−cosx, and cos2 unchanged): J=∫0π1+cos2x(π−x)sinxdx=π∫0π1+cos2xsinxdx−J. …
- AP EAPCET 2023Set eng-2023-05-15-AN1 markMCQQ.∫0π/2cosx+sinxsin(π/4+x)+sin(3π/4+x)dx= (A) 2π (B) 22π (C) 32π (D) 42π
›Reveal solutionSolution
Simplify the numerator using angle-addition identities, then use the classic x→π/2−x symmetry trick (King's rule) to evaluate the definite integral without direct antidifferentiation.
Concept and Intuition
Symmetric definite integrals over [0,π/2] often simplify beautifully using the substitution x→π/2−x, which swaps sin and cos. Adding the original and transformed integrals frequently collapses to something trivial.
Step-by-Step Solution
- Expand: sin(π/4+x)=22(cosx+sinx) and sin(3π/4+x)=22(cosx−sinx).
- Sum =22[(cosx+sinx)+(cosx−sinx)]=2cosx.
- So I=∫0π/2cosx+sinx2cosxdx.
- Substitute x→π/2−x: I=∫0π/2sinx+cosx2sinxdx=J (same value, by the King's-rule symmetry). …
- 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 2026Set eng-2026-05-18-FN1 markMCQQ.∫0π/21+4cos22xxsin2xdx= (A) 8π(Tan−12) (B) 4π(Tan−12) (C) 2π(Tan−12) (D) 8π(Tan−14)
›Reveal solutionSolution
Use the King's-rule symmetry ∫0af(x)dx=∫0af(a−x)dx to eliminate the explicit x, then substitute; the result is 8πTan−12.
Concept and Intuition
Whenever an integrand is x times a function that is itself symmetric (or anti-symmetric) under x→a−x, replacing x by a−x and adding to the original kills the explicit x-dependence, leaving a much simpler integral to evaluate.
Step-by-Step Solution
- Let I=∫0π/21+4cos22xxsin2xdx.
- Replace x→2π−x: since sin(π−2x)=sin2x and cos(π−2x)=−cos2x (so cos2 is unchanged),
I=∫0π/21+4cos22x(2π−x)sin2xdx=2π∫0π/21+4cos22xsin2xdx−I.
- So 2I=2πJ where J=∫0π/21+4cos22xsin2xdx.
- Let w=cos2x, dw=−2sin2xdx. Limits: x=0⇒w=1; x=π/2⇒w=−1.
J=∫1−11+4w2−dw/2=∫−111+4w2dw/2=∫011+4w2dw
(using the evenness of the integrand over the symmetric interval). …
- 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 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 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 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. …
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