Q.Evaluate ∫−11sin5xcos4xdx
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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 the Even Function Property: for an odd function f(x) (i.e., f(−x)=−f(x)), the integral over a symmetric interval [−a,a] is zero.
- Let f(x)=sin5xcos4x.
- Check parity: sin(−x)=−sinx, so sin5(−x)=−sin5x. cos(−x)=cosx, so cos4(−x)=cos4x. …
The integrand sin5xcos4x is an odd function over a symmetric interval [−1,1], so the integral is zero. The value is 0.
Why This Problem Is About Symmetry, Not Computation
If you try to compute ∫−11sin5xcos4xdx by expanding or using substitution, you’ll end up with a messy trigonometric integral. But there’s a much cleaner path: look at the function’s symmetry.
The interval [−1,1] is symmetric about 0. For such intervals, the integral of an odd function is always zero — provided the integral converges (which it does here, since the integrand is continuous). So the real question is: is f(x)=sin5xcos4x odd?
Step-by-Step Reasoning
-
Recall the definitions
A function f(x) is odd if f(−x)=−f(x) for all x in its domain.
A function is even if f(−x)=f(x).
-
Check the parity of each factor
- sin(−x)=−sinx, so sinx is odd.
- cos(−x)=cosx, so cosx is even.
Now raise them to powers:
- (sinx)5: odd power of an odd function → still odd.
- (cosx)4: even power of an even function → still even.
-
Combine the two
The product of an odd function and an even function is odd:
f(−x)=sin5(−x)cos4(−x)=(−sinx)5(cosx)4=−sin5xcos4x=−f(x).
- Apply the symmetric interval property …
Method: Odd/Even Symmetry Over a Symmetric Interval
Use this for ∫−aaf(x)dx: check whether the integrand is odd or even before computing, since odd integrands vanish and even ones halve the work.
Steps
Step 1: Test the parity of the integrand.
Compute f(−x). If f(−x)=−f(x) the function is odd; if f(−x)=f(x) it is even. For sin5xcos4x: sin5(−x)=−sin5x (odd power of an odd function) and cos4(−x)=cos4x (even), so the product is odd.
Step 2: Apply the symmetry rule. …
Common Mistakes
Mistake 1: Grinding out the antiderivative instead of using symmetry.
Why it's wrong: it wastes effort and invites algebra errors when the answer is simply 0. Correct approach: test parity first.
Mistake 2: Mis-judging the parity of the product.
Why it's wrong: sin5x is odd and cos4x is even, so their product is odd (odd × even = odd). Correct approach: multiply the parities correctly. …
Showing the 12 most recent of 48 on this concept.
- AP EAPCET 2026Set eng-2026-05-12-FN1 markMCQQ.If ∫02πsinmxcosnxdx=k∫0π/2sinmxcosnxdx, then (A) k divides (mn) (B) k divides (m+n) (C) When (mn) is divided by k, it leaves the reminder 1 (D) When (m+n) is divided by k, it leaves the reminder 3
›Reveal solutionSolution
The constant k relating the full-period and quarter-period integrals is 4 only when m,n are both even (else 0); in that case k=4 always divides mn, proving option (A).
Concept and Intuition
sinmxcosnx has extra symmetry over [0,2π] that lets us relate the integral over the whole period to the integral over just the first quadrant [0,π/2]. The key is checking how the integrand transforms under the reflections x→π−t, π+t, 2π−t.
Step-by-Step Solution
- Split [0,2π] into [0,π/2],[π/2,π],[π,3π/2],[3π/2,2π] and substitute x=π−t, π+t, 2π−t respectively (each t∈[0,π/2]).
- On [π/2,π]: sinx=sint, cosx=−cost⇒ integrand =(−1)nsinmtcosnt.
- On [π,3π/2]: sinx=−sint, cosx=−cost⇒ integrand =(−1)m+nsinmtcosnt.
- On [3π/2,2π]: sinx=−sint, cosx=cost⇒ integrand =(−1)msinmtcosnt.
- Adding all four pieces: ∫02π=[1+(−1)n+(−1)m+n+(−1)m]∫0π/2sinmxcosnxdx, so k=1+(−1)n+(−1)m+n+(−1)m. …
- AP EAPCET 2026Set eng-2026-05-12-AN1 markMCQQ.∫05x(5−x)20dx= (A) 441520 (B) 441521 (C) 462521 (D) 462522
›Reveal solutionSolution
The substitution u=5−x turns the integral into two elementary power integrals, giving 462522.
Concept and Intuition
Whenever an integral has a linear factor times a high power of (a−x), the substitution u=a−x swaps the roles so the high power becomes the simple variable, and the linear factor becomes (a−u) — turning the whole thing into two standard power-rule integrals.
Step-by-Step Solution
- Let u=5−x, so x=5−u and dx=−du. Limits: x=0⇒u=5; x=5⇒u=0.
- ∫05x(5−x)20dx=∫50(5−u)u20(−du)=∫05(5−u)u20du.
- Split: =5∫05u20du−∫05u21du=5[21u21]05−[22u22]05=215⋅521−22522=21522−22522. …
- AP EAPCET 2026Set eng-2026-05-12-AN1 markMCQQ.∫0π/2sinx+cosx200sinx+100cosxdx= (A) 50π (B) 25π (C) 75π (D) 150π
›Reveal solutionSolution
Using the King's rule x→a−x on [0,π/2] and adding the two equal-value forms of the integral gives I=75π.
Concept and Intuition
For ∫0af(x)dx, the substitution x→a−x leaves the integral's value unchanged but can transform the integrand into a different-looking (but equal-valued) expression. Adding the original and transformed integrands often makes the sines and cosines combine into a constant, collapsing the whole problem to ∫ of a constant.
Step-by-Step Solution
- Let I=∫0π/2sinx+cosx200sinx+100cosxdx.
- Substitute x→2π−x: sinx→cosx, cosx→sinx, and the limits/interval are unchanged, so I=∫0π/2cosx+sinx200cosx+100sinxdx as well.
- Add the two expressions for I: 2I=∫0π/2sinx+cosx(200sinx+100cosx)+(200cosx+100sinx)dx=∫0π/2sinx+cosx300sinx+300cosxdx. …
- 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 2026Set eng-2026-05-14-FN1 markMCQQ.∫2π24051π1+sin2xcos22xdx= (A) 2026π (B) 2047π (C) 2027π (D) 2025π
›Reveal solutionSolution
The Pythagorean identity collapses cos22x/(1+sin2x) to 1−sin2x; integrating this over the given huge range gives 2025π after the cosine boundary terms cancel.
Concept and Intuition
A fraction like 1+sinθcos2θ almost always simplifies using cos2θ=1−sin2θ=(1−sinθ)(1+sinθ), cancelling the (1+sinθ) factor. This turns a seemingly hard rational-trig integral into a trivial polynomial-in-trig integral. The huge integration range is a distractor meant to make direct integration look unpleasant — the simplification removes that entirely.
Step-by-Step Solution
- Simplify the integrand:
1+sin2xcos22x=1+sin2x1−sin22x=1+sin2x(1−sin2x)(1+sin2x)=1−sin2x
(this holds wherever 1+sin2x=0, which is almost everywhere, so it doesn't affect the definite integral).
2. Integrate: ∫(1−sin2x)dx=x+21cos2x+C.
3. Evaluate at the upper limit x=24051π: here 2x=4051π. Since 4051 is odd, cos(4051π)=−1.
So the antiderivative's value is 24051π−21.
4. Evaluate at the lower limit x=2π: here 2x=π, so cosπ=−1. …
- 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 2026Set eng-2026-05-14-AN1 markMCQQ.∫−20(x3+3x2+3x+3+(x+1)cos(x+1))dx= (A) 4 (B) 3 (C) 2 (D) 1
›Reveal solutionSolution
Shifting by u=x+1 centers the integral on [−1,1] and reveals that most of the integrand is odd (vanishes by symmetry), leaving just a constant term to integrate — giving 4.
Concept and Intuition
Integrals over symmetric intervals [−a,a] simplify enormously once you spot odd vs even structure: an odd function integrates to zero over such an interval, so isolating the even (symmetric) part of the integrand is often the fastest route, avoiding any need to actually antidifferentiate terms like ucosu.
Step-by-Step Solution
- Substitute u=x+1 (so x=u−1, dx=du); when x=−2, u=−1; when x=0, u=1.
- Rewrite x3+3x2+3x+3 in terms of u: since (x+1)3=x3+3x2+3x+1, we have x3+3x2+3x+3=(x+1)3+2=u3+2.
- The full integrand becomes u3+2+ucosu, so the integral is ∫−11(u3+2+ucosu)du.
- u3 is odd, so ∫−11u3du=0. …
- AP EAPCET 2026Set eng-2026-05-13-AN1 markMCQQ.∫−3π/2−π/2((x+π)3+cos2(x+3π))dx= (A) 8π (B) 2π (C) 4π−1 (D) 32π4
›Reveal solutionSolution
Shifting the variable to u=x+π turns the limits into a symmetric interval about zero; the odd cubic term vanishes and only the even cos2u term survives, giving π/2.
Concept and Intuition
Whenever an integral's limits and integrand both have a shift-symmetry, substituting to center the interval at 0 lets us exploit odd/even function properties: odd functions integrate to zero over [−a,a], and even functions can be doubled over [0,a].
Step-by-Step Solution
- Let u=x+π, so du=dx. When x=−3π/2, u=−π/2; when x=−π/2, u=π/2.
- cos2(x+3π)=cos2((x+π)+2π)=cos2(u+2π)=cos2u (cosine has period 2π).
- The integral becomes ∫−π/2π/2(u3+cos2u)du.
- u3 is an odd function, so ∫−π/2π/2u3du=0.
- cos2u is even, so ∫−π/2π/2cos2udu=2∫0π/2cos2udu. …
- AP EAPCET 2026Set eng-2026-05-15-AN1 markMCQQ.∫−ππ1+axcos2xdx, (a>0) = (A) aπ (B) aπ (C) 2π (D) 2π
›Reveal solutionSolution
This is the classic "King's rule" property ∫−aa1+bxf(x)dx=21∫−aaf(x)dx for even f; here it directly gives I=π/2, independent of a.
Concept and Intuition
Whenever an even function f(x) is divided by 1+bx and integrated over a symmetric interval [−a,a], replacing x→−x swaps 1/(1+bx) with bx/(1+bx) — and since these two fractions add to exactly 1, averaging the original and transformed integral removes the exponential entirely, leaving half of ∫−aaf(x)dx. This makes the ax term a red herring: the answer depends only on cos2x.
Step-by-Step Solution
- Let I=∫−ππ1+axcos2xdx.
- Substitute x→−x (valid since limits are symmetric): I=∫−ππ1+a−xcos2(−x)dx=∫−ππ1+a−xcos2xdx (using cos2(−x)=cos2x).
- Simplify 1+a−x1=ax+1ax, so I=∫−ππ1+axcos2x⋅axdx.
- Add the two expressions for I: 2I=∫−ππcos2x[1+ax1+1+axax]dx=∫−ππcos2xdx. …
- 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-2025-05-21-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 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. …
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