Q.∫−π/4π/4log(sinx+cosx)dx
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🔒 Start your 14-day free trial to unlock the full solution →Concept understanding — Definite Integral Symmetry
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 property of definite integrals with symmetric limits:
∫−aaf(x)dx=∫0a[f(x)+f(−x)]dx.
Step 1: Let I=∫−π/4π/4log(sinx+cosx)dx.
Replace x by −x in the integrand:
f(−x)=log(sin(−x)+cos(−x))=log(−sinx+cosx).
Step 2: Add f(x) and f(−x):
f(x)+f(−x)=log(sinx+cosx)+log(cosx−sinx)
=log[(cosx+sinx)(cosx−sinx)]=log(cos2x−sin2x)=log(cos2x).
Step 3: Using the symmetry property:
I=∫0π/4log(cos2x)dx.
Substitute t=2x, so dx=dt/2, limits: 0 to π/2: …
Using the symmetry property ∫−aaf(x)dx=∫0a[f(x)+f(−x)]dx, the integrand simplifies to log(cos2x) after combining f(x) and f(−x). The integral then becomes ∫0π/4log(cos2x)dx, which evaluates to −4πlog2.
The key insight here is that the limits are symmetric about zero, from −π/4 to π/4. When you see symmetric limits, your first instinct should be to check if the integrand has any symmetry — even, odd, or something that simplifies when you replace x with −x. Here, the integrand is log(sinx+cosx), which is neither even nor odd. But the symmetry trick still works: we can rewrite the integral as half the sum of the function and its reflection.
Let’s walk through it.
- Apply the symmetry property for definite integrals. For any function f(x) integrated over [−a,a], we have:
∫−aaf(x)dx=∫0a[f(x)+f(−x)]dx.
This is because the integral from −a to 0 can be transformed by substituting x→−x, and then adding it to the integral from 0 to a.
Here, a=π/4 and f(x)=log(sinx+cosx). So:
I=∫−π/4π/4log(sinx+cosx)dx=∫0π/4[log(sinx+cosx)+log(sin(−x)+cos(−x))]dx.
- Simplify f(−x). Since sin(−x)=−sinx and cos(−x)=cosx, we get:
f(−x)=log(−sinx+cosx)=log(cosx−sinx).
So the sum inside the integral becomes:
log(sinx+cosx)+log(cosx−sinx)=log[(sinx+cosx)(cosx−sinx)].
- Use the identity (sinx+cosx)(cosx−sinx)=cos2x−sin2x=cos2x. This is a standard double-angle identity. So:
I=∫0π/4log(cos2x)dx.
Notice how the symmetry turned a sum of two logs into a single log of a product, and that product collapsed into a simple trigonometric function. This is the power of the f(x)+f(−x) trick — it often reveals hidden simplifications.
- Substitute to simplify further. Let t=2x. Then dx=dt/2, and when x=0, t=0; when x=π/4, t=π/2. So:
I=∫0π/2log(cost)⋅2dt=21∫0π/2log(cost)dt.
- Recall the standard result for ∫0π/2log(cost)dt. This is a well-known integral. One way to derive it is to use the identity ∫0π/2log(sint)dt=∫0π/2log(cost)dt (by substituting t→π/2−t), and then note that:
∫0π/2log(sin2t)dt=∫0π/2log(2sintcost)dt=log2⋅2π+∫0π/2log(sint)dt+∫0π/2log(cost)dt.
But the left side, with u=2t, becomes 21∫0πlog(sinu)du, and using symmetry, that equals ∫0π/2log(sint)dt. Solving gives:
∫0π/2log(cost)dt=−2πlog2.
›Proof
Derivation of ∫0π/2log(cost)dt=−2πlog2: …
Method: Symmetric limits via f(x)+f(−x)
When the limits are [−a,a] but the integrand is neither plainly even nor odd, use ∫−aaf(x)dx=∫0a[f(x)+f(−x)]dx.
Steps
Step 1: Form f(x)+f(−x).
Replace x by −x using sin(−x)=−sinx, cos(−x)=cosx, and add. For log integrands, logP+logQ=log(PQ) often collapses to a simple product.
Step 2: Simplify the combined integrand. …
Common Mistakes
Mistake 1: Assuming log(sinx+cosx) is even or odd.
Why it's wrong: it is neither, so neither the "double it" nor the "it's zero" shortcut applies. Correct approach: use ∫−aaf=∫0a[f(x)+f(−x)]dx, which turns the sum into logcos2x.
Mistake 2: Dropping the 21 from the substitution t=2x. …
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 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 2021Set eng-2021-08-24-AN1 markMCQQ.∫−π/4π/4xtan(1+x2)dx= (A) 0 (B) 4π (C) 4−π (D) 1
›Reveal solutionSolution
This is a symmetric-limits definite integral where checking odd/even parity instantly gives the answer without doing any actual antiderivative work: it is 0.
Concept and Intuition
For ∫−aaf(x)dx: if f is odd (f(−x)=−f(x)) the integral is 0; if f is even it equals 2∫0af(x)dx. Any function built as (odd function of x) × (function of x2) is automatically odd, because a function of x2 never changes sign under x→−x.
Step-by-Step Solution
- Let f(x)=xtan(1+x2).
- Replace x by −x: f(−x)=(−x)tan(1+(−x)2)=−xtan(1+x2)=−f(x).
- So f is odd on the symmetric interval [−4π,4π]. …
- 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 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-2024-05-22-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 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 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 2026Set eng-2026-05-14-FN1 markMCQQ.∫−2π2π(1+cosx)3(1−cosx)4dx= (A) 0 (B) 5π (C) 25π (D) 45π
›Reveal solutionSolution
Factoring (1+cosx)3(1−cosx)4 into sin6x(1−cosx) and splitting the integral shows the cosxsin6x part vanishes by symmetry, leaving 4∫0πsin6xdx=45π.
Concept and Intuition
Products of (1±cosx) raised to powers usually simplify via (1+cosx)(1−cosx)=1−cos2x=sin2x. Pairing three factors from each gives sin6x, leaving one leftover (1−cosx) factor. Splitting that leftover separates the integral into an even, periodic sin6x piece and an odd-derivative sin6xcosx piece that integrates to zero over a range where sinx returns to the same value at both ends.
Step-by-Step Solution
- Rewrite the product:
(1+cosx)3(1−cosx)4=[(1+cosx)(1−cosx)]3⋅(1−cosx)=(sin2x)3(1−cosx)=sin6x−sin6xcosx
- Split the integral:
∫−2π2πsin6xdx−∫−2π2πsin6xcosxdx
- Second integral: sin6xcosx=dxd(7sin7x), so
∫−2π2πsin6xcosxdx=[7sin7x]−2π2π=70−0=0
since sin(2π)=sin(−2π)=0.
4. First integral: sin6x has period π (because sin(x+π)=−sinx⇒sin6(x+π)=sin6x). The interval [−2π,2π] has length 4π, i.e. exactly 4 periods of length π:
∫−2π2πsin6xdx=4∫0πsin6xdx …
- AP EAPCET 2022Set eng-2022-07-05-AN1 markMCQQ.∫−113−∣x∣sinx−x2dx= (A) 7+18log(3/2) (B) 18log(9/4) (C) 7+9log(9/4) (D) 7−18log(3/2)
›Reveal solutionSolution
The sinx part is an odd function over a symmetric interval and vanishes; only the even x2 part survives, reducing to a straightforward rational-function integral solved via polynomial division.
Concept and Intuition
sinx is odd, x2 is even, and 3−∣x∣ is even, so 3−∣x∣sinx is odd (integrates to 0 over [−1,1]) while 3−∣x∣x2 is even (double the integral over [0,1], where ∣x∣=x).
Step-by-Step Solution
- Split: ∫−113−∣x∣sinx−x2dx=∫−113−∣x∣sinxdx−∫−113−∣x∣x2dx.
- First integral =0 (odd integrand over symmetric limits).
- Second integral: even integrand, so =2∫013−xx2dx (using ∣x∣=x for x∈[0,1]).
- Polynomial division: 3−xx2=−x−3+3−x9 (check: (−x−3)(3−x)=x2−9, so x2=(−x−3)(3−x)+9).
- Integrate: ∫01(−x−3+3−x9)dx=[−2x2−3x−9log(3−x)]01.
- At x=1: −21−3−9log2=−27−9log2. At x=0: −9log3. …
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