Q.By using the properties of definite integrals, evaluate the integral ∫0π/2sin5x+cos5xcos5xdx
🔒You're viewing a preview — the full solution, concept, methods & PYQ mapping are locked.
🔒 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 …
Concept: Definite Integral Symmetry — when the integrand has the form f(x)+f(a−x)f(x), the integral over [0,a] equals 2a.
Let I=∫0π/2sin5x+cos5xcos5xdx.
Step 1: Use the property ∫0af(x)dx=∫0af(a−x)dx.
Replace x by 2π−x:
I=∫0π/2sin5(2π−x)+cos5(2π−x)cos5(2π−x)dx=∫0π/2cos5x+sin5xsin5xdx. …
Using the symmetry property ∫0af(x)dx=∫0af(a−x)dx, the given integral equals its own complement, so the sum of the two is π/2, giving the value π/4.
The key insight here is that the integrand has a special structure when you replace x by 2π−x. This is a classic trick for integrals over [0,π/2] where the numerator and denominator are symmetric powers of sine and cosine.
Why this works:
For any function f(x) that is continuous on [0,a], we have the property
∫0af(x)dx=∫0af(a−x)dx.
Here a=π/2, and the integrand is sin5x+cos5xcos5x. When we replace x by 2π−x, cosx becomes sinx and sinx becomes cosx, so the integrand flips to cos5x+sin5xsin5x. That is exactly the "complement" of the original fraction — their sum is simply 1. This lets us add the two forms and solve for the integral.
Let’s work through it step by step.
- Define the integral Let
I=∫0π/2sin5x+cos5xcos5xdx.
- Apply the substitution x→2π−x Using the property ∫0af(x)dx=∫0af(a−x)dx, set t=2π−x. Then dx=−dt, and when x=0, t=π/2; when x=π/2, t=0. The integral becomes
I=∫π/20sin5(2π−t)+cos5(2π−t)cos5(2π−t)(−dt).
Reversing the limits removes the minus sign:
I=∫0π/2sin5(2π−t)+cos5(2π−t)cos5(2π−t)dt.
- Simplify the trigonometric expressions Recall: cos(2π−t)=sint and sin(2π−t)=cost. So the integrand becomes
cos5t+sin5tsin5t.
Since t is a dummy variable, we can rename it back to x:
I=∫0π/2sin5x+cos5xsin5xdx.
- Add the two expressions for I We now have two forms of I:
I=∫0π/2sin5x+cos5xcos5xdxandI=∫0π/2sin5x+cos5xsin5xdx.
Adding them: …
Method: The f+gf complementary-integral trick
For ∫0af(x)+f(a−x)f(x)dx (with f,g swapping under x→a−x), reflection produces the complementary fraction; the two add to 1.
Steps
Step 1: Set I and reflect with x→a−x.
I=∫0af(x)+g(x)f(x)dx⇒I=∫0ag(x)+f(x)g(x)dx,
where the reflection swaps f↔g (e.g. sin↔cos).
Step 2: Add the two forms. …
Common Mistakes
Mistake 1: Attempting a t=tanx or half-angle substitution to integrate directly.
Why it's wrong: sin5x+cos5xcos5x leads to an intractable rational function; the reflection property is the intended, far shorter route. Correct approach: use ∫0af(x)=∫0af(a−x).
Mistake 2: Not simplifying the added fractions to 1. …
Showing the 12 most recent of 48 on this concept.
- AP EAPCET 2025Set eng-2025-05-23-AN1 markMCQQ.∫−π/2π/2sin2xcos2x(sinx+cosx)dx= (A) 0 (B) 152 (C) 154 (D) 52
›Reveal solutionSolution
This tests using odd/even symmetry over a symmetric interval to kill half the integral, then a simple u=sinx substitution for the rest. The answer is 154, option (C).
Concept and Intuition
Over a symmetric interval [−a,a], an odd integrand integrates to zero and an even integrand integrates to twice the integral over [0,a]. Expanding (sinx+cosx) splits the problem cleanly into one odd term and one even term, so only the even term survives — turning a seemingly complicated integral into a single elementary substitution.
Step-by-Step Solution
- Expand: sin2xcos2x(sinx+cosx)=sin3xcos2x+sin2xcos3x.
- g(x)=sin3xcos2x: since sin3(−x)=−sin3x and cos2(−x)=cos2x, g(−x)=−g(x) — odd. So ∫−π/2π/2g(x)dx=0.
- h(x)=sin2xcos3x: both factors are even, so h is even, and ∫−π/2π/2hdx=2∫0π/2hdx.
- Write h(x)=sin2xcos2xcosx=sin2x(1−sin2x)cosx. Let u=sinx, du=cosxdx; limits 0→1. …
- AP EAPCET 2025Set eng-2025-05-23-FN1 markMCQQ.∫03π/2cos3x+sin3xcos3xdx= (A) 0 (B) 1 (C) 4π (D) 43π
›Reveal solutionSolution
Using the substitution x→23π−x swaps the roles of cos3x and sin3x in the integrand, showing the given integral equals its "sine" counterpart; since the two together give the full interval length, each equals 43π.
Concept and Intuition
This is a King's-rule-style symmetry trick: ∫0af(x)dx=∫0af(a−x)dx. Applying it with a=3π/2 swaps cosx↔−sinx and sinx↔−cosx, which exactly interchanges the roles of cos3x and sin3x in the fraction (the minus signs cancel through the cube and the overall ratio), letting us equate the two "complementary" integrals.
Step-by-Step Solution
- Define I=∫03π/2cos3x+sin3xcos3xdx and J=∫03π/2cos3x+sin3xsin3xdx.
- Adding: I+J=∫03π/21dx=23π.
- Substitute x→23π−x in I: cos(23π−x)=−sinx and sin(23π−x)=−cosx. …
- AP EAPCET 2025Set eng-2025-05-26-AN1 markMCQQ.∫0π(sin5xcos3x+sin4xcos4x+sin3xcos4x)dx= (A) 2240873 (B) 1283π+3512 (C) 44801641 (D) 1283π+354
›Reveal solutionSolution
Use the x→π−x symmetry to kill the odd-cos-power term and double the even-cos-power terms' half-range integrals; a Wallis-formula and direct-substitution computation gives 1283π+354.
Concept and Intuition
For f(x)=sinaxcosbx, substituting x→π−x gives sin(π−x)=sinx but cos(π−x)=−cosx, so f(π−x)=(−1)bf(x). Splitting ∫0π=∫0π/2+∫π/2π and substituting in the second piece shows ∫0πfdx=[1+(−1)b]∫0π/2fdx — zero if b is odd, doubled if b is even.
Step-by-Step Solution
- Term 1: sin5xcos3x has b=3 (odd) ⇒∫0π=0.
- Term 2: sin4xcos4x has b=4 (even) ⇒∫0π=2∫0π/2sin4xcos4xdx. Using sinxcosx=21sin2x: sin4xcos4x=161sin4(2x). ∫0π/2sin4(2x)dx=21∫0πsin4tdt=21⋅2∫0π/2sin4tdt=∫0π/2sin4tdt=4!!3!!⋅2π=83⋅2π=163π. So ∫0π/2sin4xcos4xdx=161⋅163π=2563π, doubled gives 1283π. …
- 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 2023Set eng-2023-05-18-FN1 markMCQQ.∫0πxsin3xcos2xdx= (A) 152π (B) 154π (C) 30π (D) 52π
›Reveal solutionSolution
Using the symmetry property ∫0πxg(x)dx=2π∫0πg(x)dx (valid since g(π−x)=g(x) here) reduces the problem to a simple substitution integral, giving 152π.
Concept and Intuition
Whenever the integrand has the form x⋅g(x) over [0,π] and g(π−x)=g(x) (i.e., g is symmetric about x=π/2), we can use the standard trick: let I=∫0πxg(x)dx, substitute x→π−x to get I=∫0π(π−x)g(x)dx=π∫0πg(x)dx−I, so 2I=π∫0πg(x)dx, i.e. I=2π∫0πg(x)dx. This avoids ever integrating xsin3xcos2x directly by parts.
Step-by-Step Solution
- Let g(x)=sin3xcos2x. Check symmetry: g(π−x)=sin3(π−x)cos2(π−x)=(sinx)3(−cosx)2=sin3xcos2x=g(x). ✓
- So ∫0πxsin3xcos2xdx=2π∫0πsin3xcos2xdx.
- Compute ∫0πsin3xcos2xdx=∫0πsinx(1−cos2x)cos2xdx. Substitute u=cosx, du=−sinxdx; limits x:0→π give u:1→−1.
- This becomes ∫1−1(1−u2)u2(−du)=∫−11(u2−u4)du. …
- 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 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-2026-05-15-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 2022Set eng-2022-07-07-AN1 markMCQQ.∫−π/4π/4cos−8xdx= (A) 1514 (B) 35174 (C) 35192 (D) 35198
›Reveal solutionSolution
An even-power secant integral, reduced via sec2x=1+tan2x and the substitution u=tanx. Answer: 35192.
Concept and Intuition
cos−8x=sec8x is an even function, so integrating it over the symmetric interval [−π/4,π/4] is twice the integral over [0,π/4]. For even powers of secant, peel off one factor of sec2x to pair with the dx (since d(tanx)=sec2xdx), and rewrite the remaining even power of secx using sec2x=1+tan2x — this turns the whole integral into a simple polynomial in u=tanx.
Step-by-Step Solution
- ∫−π/4π/4sec8xdx=2∫0π/4sec8xdx (even integrand, symmetric limits).
- Write sec8x=sec6x⋅sec2x=(1+tan2x)3sec2x.
- Substitute u=tanx, du=sec2xdx; limits x=0→u=0, x=π/4→u=1: ∫0π/4sec8xdx=∫01(1+u2)3du.
- Expand: (1+u2)3=1+3u2+3u4+u6.
- Integrate: ∫01(1+3u2+3u4+u6)du=[u+u3+53u5+71u7]01=1+1+53+71. …
- AP EAPCET 2025Set eng-2025-05-24-FN1 markMCQQ.∫−2π2πsin4(2x)cos6(2x)dx= (A) 643π (B) 649π (C) 359π (D) 2809π
›Reveal solutionSolution
Substitute u=2x, use periodicity (period π) to reduce to 8 copies of a Wallis-formula integral over [0,π/2], giving 643π.
Concept and Intuition
sin4(2x)cos6(2x) is a periodic function. Rather than grinding through a power-reduction expansion over the full range [−2π,2π], it's far more efficient to (a) substitute to a clean variable, (b) exploit periodicity to shrink the domain to one period, and (c) use the standard Wallis reduction formula for ∫0π/2sinmcosn.
Step-by-Step Solution
- Let u=2x⇒du=2dx. As x runs from −2π to 2π, u runs from −4π to 4π.
I=∫−2π2πsin4(2x)cos6(2x)dx=21∫−4π4πsin4ucos6udu.
- sin4ucos6u is unchanged under u→u+π (since sin(u+π)=−sinu, cos(u+π)=−cosu, and both powers are even), so it has period π.
- The interval [−4π,4π] has length 8π=8×π, i.e. exactly 8 full periods, so
∫−4π4πsin4ucos6udu=8∫0πsin4ucos6udu.
- On [0,π], the function is symmetric about u=π/2 (since sin(π−u)=sinu and cos(π−u)=−cosu, and cos6 is even in sign), so ∫0π=2∫0π/2.
- By the Wallis formula (both exponents even): …
- 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-2026-05-14-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 …
🎓Unlock everything free for 14 days
- ✓Full step-by-step solutions
- ✓Concept-first explanations
- ✓Methods, shortcuts & mistakes
- ✓PYQ mapping + timed mock tests
Full access for 14 days. No credit card required.