Q.∫02πcosec7xdx=
(A) 0
(B) 1
(C) 4
(D) 2π
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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 Definite Integral Symmetry: for an odd function about the midpoint of a symmetric interval, the integral is zero.
Step 1: The integrand is csc7x=sin7x1.
Step 2: Over [0,2π], sinx is symmetric about x=π: sin(π+t)=−sin(π−t). Hence csc7(π+t)=−csc7(π−t), making the function odd about x=π. …
csc7x is odd about x=π, and [0,2π] is symmetric about π, so the two halves cancel and the integral is 0 — option (A).
Let I=∫02πcsc7xdx.
Key symmetry. Because sin(x+π)=−sinx and the power 7 is odd,
csc7(x+π)=sin7(x+π)1=(−sinx)71=−csc7x,
so the integrand is odd about the line x=π.
Split at the midpoint.
I=∫0πcsc7xdx+∫π2πcsc7xdx.
In the second integral substitute x=π+t (so dx=dt; x=π⇒t=0, x=2π⇒t=π):
∫π2πcsc7xdx=∫0πcsc7(π+t)dt=−∫0πcsc7tdt. …
Method: Odd symmetry about the centre of the interval
Use this when a definite integral over a full or symmetric interval has an integrand that flips sign under reflection about the interval's midpoint — the two halves then cancel to 0 without any antiderivative.
Steps
Step 1: Identify the midpoint c of the interval [a,b].
c=2a+b.
Step 2: Test the integrand's behaviour under x→2c−x (or x→x+half-period).
If f(2c−x)=−f(x), the graph is odd about x=c. For trigonometric powers, use identities like sin(x+π)=−sinx; an odd power of such a term inherits the sign flip.
Step 3: Split at the midpoint and substitute.
I=∫acfdx+∫cbfdx, …
Common Mistakes
Mistake 1: Assuming symmetry gives 0 without checking the sign flip.
Why it's wrong: the cancellation needs f(2c−x)=−f(x); an even power like csc6x would instead double, not vanish. Correct approach: confirm the power is odd and that sin(x+π)=−sinx genuinely flips the sign.
Mistake 2: Using even/odd rules meant for [−a,a] blindly.
Why it's wrong: the textbook rule ∫−aa(odd)=0 is about symmetry around 0; here the symmetry is about x=π, the midpoint of [0,2π]. Correct approach: reflect about the actual midpoint c=π, not about the origin. …
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 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-2022-07-04-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 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 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 2023Set eng-2023-05-18-AN1 markMCQQ.∫−4π4πtan9xsin6xcos3xdx= (A) 16×2π (B) 8×32 (C) 16×1714×1512×…×32 (D) 0
›Reveal solutionSolution
Odd × even × even = odd, and the integral of any odd function over a symmetric interval is zero — no actual antiderivative work is needed.
Concept and Intuition
Before grinding through a nasty trig integral, always check parity. tan(−x)=−tanx (odd), and raising an odd function to an odd power (9) keeps it odd. sin(−x)=−sinx raised to an even power (6) becomes even, and cos(−x)=cosx raised to any power stays even. Odd times even times even is odd, and an odd function's graph is antisymmetric about the origin, so equal positive and negative area cancels exactly over any interval symmetric about 0.
Step-by-Step Solution
- Let g(x)=tan9xsin6xcos3x.
- g(−x)=tan9(−x)sin6(−x)cos3(−x)=(−tanx)9(sinx)6(cosx)3=−tan9xsin6xcos3x=−g(x).
- So g is an odd function. …
- 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 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-2025-05-26-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 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. …
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