Q.By using the properties of definite integrals, evaluate the integral ∫02πcos5xdx
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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 …
Use symmetry over the full period. First, since cos5(2π−x)=cos5x,
∫02πcos5xdx=2∫0πcos5xdx.
Next, cos5(π−x)=(−cosx)5=−cos5x, so on [0,π] the function is odd about x=2π and …
Over a full period the positive and negative loops of an odd power of cosine cancel exactly, so ∫02πcos5xdx=0.
The idea
We use two definite-integral properties:
∫02af(x)dx=2∫0af(x)dxif f(2a−x)=f(x),
∫0af(x)dx=0if f(a−x)=−f(x).
1. Fold [0,2π] onto [0,π]
With a=π, check f(2π−x)=cos5(2π−x)=cos5x=f(x). So
∫02πcos5xdx=2∫0πcos5xdx.
2. Show the half-integral is zero …
Method: Fold a full-period integral, then use half-interval sign symmetry
For an odd power of cos (or sin) over a full period, combine two reflection properties: first fold [0,2a] onto [0,a], then show the half-integral vanishes by a sign flip.
Steps
Step 1: Fold using f(2a−x)=f(x).
If cosn(2π−x)=cosnx, then ∫02π=2∫0π.
Step 2: Test the half-interval for anti-symmetry.
Check f(a−x)=−f(x): since cos(π−x)=−cosx, an odd power gives cosn(π−x)=−cosnx. …
Common Mistakes
Mistake 1: Assuming an integral over a full period is automatically zero.
Why it's wrong: ∫02πcos2xdx=π=0 — only odd powers cancel; even powers have positive net area. Correct approach: it is the odd power (and the sign flip cos(π−x)=−cosx) that forces 0 here.
Mistake 2: Mishandling the folding property. …
Showing the 12 most recent of 48 on this concept.
- 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 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 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-2025-05-26-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-2026-05-15-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 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 2022Set eng-2022-07-08-FN1 markMCQQ.∫02πcosmxcosnxdx+∫−ππsinmxcosnxdx= (A) 0, if m=n and m,n∈Z (B) π if m=n, m,n∈Z (C) π if m=n, m,n∈Z (D) 2π ∀ m,n∈R
›Reveal solutionSolution
This tests Fourier orthogonality of cos and the odd/even symmetry trick for integrals over [−π,π]. The answer is π when m=n.
Concept and Intuition
When you integrate a product of trig functions over a full period, the result depends on whether the functions are 'in phase' (same frequency) or not. cosmx and cosnx are orthogonal on a period unless m=n, in which case you're integrating cos2(mx), which has a nonzero average. Separately, integrating an ODD function over a symmetric interval like [−π,π] always gives zero by symmetry — the negative half exactly cancels the positive half — no computation needed.
Step-by-Step Solution
- Second integral first (symmetry shortcut): f(x)=sinmxcosnx. Since sin(−mx)=−sinmx and cos(−nx)=cosnx, we get f(−x)=−f(x): f is odd. Hence ∫−ππf(x)dx=0 for any m,n.
- First integral: Use the product-to-sum identity cosmxcosnx=21[cos((m−n)x)+cos((m+n)x)].
- If m=n (integers), both cos((m−n)x) and cos((m+n)x) complete a whole number of periods over [0,2π] (unless m+n=0, but that case still integrates a nonzero-frequency cosine unless m=n=0), so the integral is 0. …
- 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 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 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 2024Set eng-2024-05-19-AN1 markMCQQ.∫0πxsin4xcos6xdx= (A) 5123π2 (B) 2563π2 (C) 256π2 (D) 512π2
›Reveal solutionSolution
Using the King's-rule symmetry ∫0πxf(x)dx=2π∫0πf(x)dx (valid because cos6 is unaffected by the sign flip under x→π−x) reduces the problem to a standard Wallis-formula integral, giving 5123π2.
Concept and Intuition
Whenever an integral has the form ∫0πxf(x)dx and f(π−x)=f(x) (i.e. f is symmetric about the midpoint x=π/2), substituting x→π−x shows the integral equals 2π∫0πf(x)dx — the "x" essentially averages out to π/2. Here f(x)=sin4xcos6x is such a function because raising cosx to an even power erases the sign flip from cos(π−x)=−cosx.
Step-by-Step Solution
- Let I=∫0πxsin4xcos6xdx and f(x)=sin4xcos6x.
- Substituting x→π−x: sin(π−x)=sinx and cos(π−x)=−cosx, so f(π−x)=sin4x(−cosx)6=sin4xcos6x=f(x) (even power kills the sign).
- So I=∫0π(π−x)f(x)dx=π∫0πf(x)dx−I⇒2I=π∫0πf(x)dx⇒I=2π∫0πf(x)dx.
- By symmetry about x=π/2 (again since f(π−x)=f(x)), ∫0πf(x)dx=2∫0π/2sin4xcos6xdx. …
- 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. …
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