Q.By using the properties of definite integrals, evaluate the integral ∫0π/21+sinxcosxsinx−cosxdx
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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 …
Concept: Definite Integral Symmetry — use the substitution x→2π−x to exploit symmetry about the midpoint.
Let I=∫0π/21+sinxcosxsinx−cosxdx.
Substitute x=2π−t. Then sinx=cost, cosx=sint, dx=−dt, and the limits swap: …
The integral evaluates to 0 because the integrand is an odd function about the midpoint x=π/4 of the interval, causing symmetric cancellation.
The key insight here is symmetry — but not the usual symmetry about x=0. The interval is [0,π/2], and the integrand involves both sinx and cosx, which swap roles when x is replaced by π/2−x. That substitution is the classic trick for integrals over [0,π/2] with mixed sine and cosine terms.
Let’s see why this works.
- Set up the substitution. Let I=∫0π/21+sinxcosxsinx−cosxdx. Use the substitution x→π/2−x. Then dx becomes −dx, and the limits swap: when x=0, the new variable is π/2; when x=π/2, it’s 0. So:
I=∫π/201+sin(π/2−x)cos(π/2−x)sin(π/2−x)−cos(π/2−x)(−dx)=∫0π/21+cosxsinxcosx−sinxdx.
- Notice the relationship. The denominator is unchanged because sin(π/2−x)cos(π/2−x)=cosxsinx=sinxcosx. The numerator becomes cosx−sinx=−(sinx−cosx). So we have:
I=∫0π/21+sinxcosx−(sinx−cosx)dx=−I.
- Solve the equation. From I=−I, we get 2I=0, so I=0. …
Method: Reflection giving I=−I — forced-zero integrals
If reflecting the integrand reproduces its negative, then I=−I, which forces I=0 — a fast route for integrands anti-symmetric about the interval's midpoint.
Steps
Step 1: Reflect x→a−x (here 2π−x).
Apply I=∫0af(a−x)dx and use co-function identities (sin↔cos).
Step 2: Check whether the reflected integrand is −f(x). …
Common Mistakes
Mistake 1: Reaching for the t=tan(x/2) Weierstrass substitution.
Why it's wrong: it produces a messy rational integral, when reflection x→2π−x shows the integrand equals its own negative and the answer is 0. Correct approach: reflect and observe I=−I.
Mistake 2: Not noticing the denominator is reflection-symmetric. …
Showing the 12 most recent of 48 on this concept.
- 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-2024-05-20-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-2025-05-23-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 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 2023Set eng-2023-05-15-AN1 markMCQQ.∫0π/2cosx+sinxsin(π/4+x)+sin(3π/4+x)dx= (A) 2π (B) 22π (C) 32π (D) 42π
›Reveal solutionSolution
Simplify the numerator using angle-addition identities, then use the classic x→π/2−x symmetry trick (King's rule) to evaluate the definite integral without direct antidifferentiation.
Concept and Intuition
Symmetric definite integrals over [0,π/2] often simplify beautifully using the substitution x→π/2−x, which swaps sin and cos. Adding the original and transformed integrals frequently collapses to something trivial.
Step-by-Step Solution
- Expand: sin(π/4+x)=22(cosx+sinx) and sin(3π/4+x)=22(cosx−sinx).
- Sum =22[(cosx+sinx)+(cosx−sinx)]=2cosx.
- So I=∫0π/2cosx+sinx2cosxdx.
- Substitute x→π/2−x: I=∫0π/2sinx+cosx2sinxdx=J (same value, by the King's-rule symmetry). …
- 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 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 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 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 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-2025-05-23-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 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]. …
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