Q.By using the properties of definite integrals, evaluate the integral ∫0π/2cos2xdx
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
Example 2: ∫−ππsinxdx — sinx is odd, so the integral is 0.
Example 3: ∫−22(x3+5x)dx — both terms are odd, so their sum is odd; the integral is 0.
Example 4: ∫−11(x2+1)dx — x2+1 is even, so
2∫01(x2+1)dx=2[3x3+x]01=2(31+1)=38
When to Use This in Exams
This is a time-saver, not a necessity: if unsure whether a function is even or odd, just integrate directly. But when you spot symmetry, you can cut your work in half (or to zero). Look for powers of x, trigonometric functions, and absolute values.
Quick check: replace x with −x. Same expression back → even. Negative of the expression → odd. Neither → symmetry doesn't apply.
Definite Integral Symmetry — the even and odd function shortcuts for integrals over [-a, a] — is a standard time-saving technique taught in the CBSE Class 12 Integrals chapter, and "even odd function integration trick class 12" is a widely searched revision topic. This shortcut is also frequently exploited in JEE Main and JEE Advanced integral calculus problems to avoid lengthy direct integration.
The key idea is to use the symmetry of cos2x over [0,π/2], or equivalently, the identity cos2x=1−sin2x combined with the property ∫0π/2f(sinx)dx=∫0π/2f(cosx)dx.
Let I=∫0π/2cos2xdx. Using the property ∫0π/2f(sinx)dx=∫0π/2f(cosx)dx, we also have I=∫0π/2sin2xdx.
Adding the two expressions:
2I=∫0π/2(cos2x+sin2x)dx=∫0π/21dx=2π.
Thus I=4π.
The value is 4π.
Using the symmetry property ∫0af(x)dx=∫0af(a−x)dx, we rewrite cos2x as sin2x, add the two forms, and get 2I=∫0π/21dx=2π, so I=4π.
The problem asks us to evaluate ∫0π/2cos2xdx using properties of definite integrals. The direct approach — finding an antiderivative — is straightforward, but the instruction to use properties nudges us toward a more elegant method that builds deeper intuition.
The key property here is the symmetry of the definite integral about the midpoint of the interval. For any function f continuous on [0,a], we have:
∫0af(x)dx=∫0af(a−x)dx
Why does this work? Because as x runs from 0 to a, the quantity a−x runs from a down to 0 — it’s just a reversal of direction. The area under the curve doesn’t care about direction, so the integral stays the same.
Now, apply this to our integral. Let:
I=∫0π/2cos2xdx
Here a=2π. Using the property:
I=∫0π/2cos2(2π−x)dx
But cos(2π−x)=sinx, so:
I=∫0π/2sin2xdx
This is the crucial step: the integral of cos2x from 0 to π/2 equals the integral of sin2x over the same interval.
Now add the two expressions for I:
I+I=∫0π/2cos2xdx+∫0π/2sin2xdx
2I=∫0π/2(cos2x+sin2x)dx
And cos2x+sin2x=1, the most fundamental identity in trigonometry. So:
2I=∫0π/21dx
The integral of 1 from 0 to π/2 is just the length of the interval: 2π−0=2π.
Thus:
2I=2π⇒I=4π
A common mistake is to forget that the property ∫0af(x)dx=∫0af(a−x)dx works only when both limits are the same. Don’t try to apply it blindly to integrals like ∫0πcos2xdx — the symmetry changes because the midpoint shifts.
This trick — writing an integral as the average of itself and its symmetric counterpart — is powerful. It works whenever f(x)+f(a−x) simplifies nicely, especially with trigonometric functions on [0,π/2] or [0,π].
The value of the integral is 4π.
Method: The reflection property ∫0af(x)dx=∫0af(a−x)dx
Replacing x by a−x leaves a definite integral over [0,a] unchanged. Adding the original and reflected forms often produces a trivially integrable sum.
Steps
Step 1: Name the integral and reflect.
Let I=∫0af(x)dx. Apply
∫0af(x)dx=∫0af(a−x)dx.
Step 2: Simplify the reflected integrand.
Use the relevant co-function identities (over [0,2π], sin(2π−x)=cosx and vice-versa), which typically swaps the roles of the functions.
Step 3: Add the two expressions for I.
2I=∫0a[f(x)+f(a−x)]dx; choose the reflection so this sum collapses (e.g. to 1).
Step 4: Integrate the simple sum and halve.
Solve 2I=∫0a(simple)dx for I.
Common Mistakes
Mistake 1: Applying ∫0af(x)dx=∫0af(a−x)dx with mismatched limits.
Why it's wrong: the property needs a lower limit of 0 and the same upper limit a inside f(a−x); using it on, say, ∫0πcos2xdx (where the midpoint differs) gives a wrong reflection. Correct approach: confirm the limits are 0 to a before reflecting.
Mistake 2: Forgetting that cos(2π−x)=sinx, so cos2 becomes sin2.
Why it's wrong: the whole trick relies on the reflected integrand becoming sin2x so that cos2x+sin2x=1. Correct approach: use the co-function identity, add, and get 2I=2π.
Showing the 12 most recent of 48 on this concept.
- 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.
- Compute ∫−ππcos2xdx: using cos2x=21+cos2x, this integral =[2x+4sin2x]−ππ=π (the sin2x terms vanish at ±π).
- So 2I=π⇒I=2π.
Common Mistakes
- Trying to directly integrate cos2x/(1+ax) term by term without using the symmetry trick — this leads to a dead end since ax has no elementary antiderivative combined with cos2x.
- Forgetting that the final answer doesn't depend on a at all, and second-guessing a clean a-independent result.
✓Final answerThe correct option is (C) — 2π.
ANSWER: C
- 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.
- Compute J: let u=cosx, du=−sinxdx. Limits: x=0⇒u=1; x=π⇒u=−1. J=∫1−11+u2−du=∫−111+u2du=[tan−1u]−11=4π−(−4π)=2π.
- So 2I=π⋅2π=2π2⇒I=4π2.
Common Mistakes
- Forgetting to check that f(π−x)=f(x) actually holds before applying King's rule (it's essential — the trick only works when this symmetry is present).
- Sign error handling the limits when substituting u=cosx (easy to flip the sign of the final integral).
✓Final answerThe correct option is (D) — 4π2.
ANSWER: D
- 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.
- Let u=cosx, du=−sinxdx. When x=0,u=1; when x=π,u=−1. So ∫0π1+cos2xsinxdx=∫−111+u2du=[tan−1u]−11=4π−(−4π)=2π.
- So 2I=π⋅2π=2π2, giving I=4π2.
Common Mistakes
- Forgetting that cos2(π−x)=cos2x stays unchanged (unlike cos(π−x)=−cosx), which is essential for the trick to work cleanly.
- Sign errors in the substitution u=cosx.
✓Final answerThe correct option is (A) — 4π2.
ANSWER: A
- 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.
- So the integrand of I becomes (−sinx)3+(−cosx)3(−sinx)3=−(sin3x+cos3x)−sin3x=sin3x+cos3xsin3x, which is exactly the integrand of J. Hence I=J.
- Combining with I+J=3π/2: I=J=43π.
Common Mistakes
- Not noticing the interval length is exactly what makes the "complementary" substitution work cleanly (it must map the interval to itself).
- Overlooking the sign cancellation inside the cube when substituting, and concluding incorrectly that I=−J.
✓Final answerThe correct option is (D) — 43π.
ANSWER: D
- 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.
- ∫0π/21dx=2π; ∫0π/2sinxcosxdx=21∫0π/2sin2xdx=21[−2cos2x]0π/2=21⋅21−(−1)=21.
- So I+J=2π−21.
- Since I=J: 2I=2π−21⇒I=4π−41=4π−1.
Common Mistakes
- Assuming I=J only "by symmetry of appearance" without justifying it via the actual x→π/2−x substitution.
- Sign/factor slip evaluating ∫0π/2sinxcosxdx (easy to lose the 21 from the double-angle rewrite).
✓Final answerThe correct option is (D) — 4π−1.
ANSWER: D
- 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).
- I+J=∫0π/2cosx+sinx2(cosx+sinx)dx=∫0π/22dx=2⋅2π.
- Since I=J: 2I=22π⇒I=42π=22π.
Common Mistakes
- Trying to integrate cosx/(cosx+sinx) directly (messy) instead of using the symmetry trick.
- Forgetting that I=J follows from the substitution, which is what makes I+J=2I solvable trivially.
✓Final answerThe correct option is (B) — π/(22).
ANSWER: B
- 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.
- So 2J=π∫0π1+cos2xsinxdx. Substitute u=cosx, du=−sinxdx: this integral becomes ∫−111+u2du=[arctanu]−11=4π−(−4π)=2π.
- So 2J=π⋅2π=2π2⇒J=4π2.
- The even-part integral is 4J=4⋅4π2=π2. Adding the (zero) odd part, the total is π2.
Common Mistakes
- Forgetting to check parity first and instead attempting direct (much harder) integration.
- Sign slips in the x→π−x substitution, especially with cos(π−x)=−cosx but cos2(π−x)=cos2x (unchanged).
✓Final answerThe correct option is (B) — π2.
ANSWER: B
- 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.
- Evaluate: ∫−11u2du=32, ∫−11u4du=52. So the integral is 32−52=1510−6=154.
- Multiply by 2π: 2π⋅154=152π.
Common Mistakes
- Forgetting to verify the symmetry condition g(π−x)=g(x) before applying the King's-rule-style trick — it fails silently if the power of cos were odd instead.
- Arithmetic slip evaluating ∫−11u2du−∫−11u4du.
✓Final answerThe correct option is (A) — 152π.
ANSWER: A
- 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).
5. ∫011+4w2dw=21[Tan−1(2w)]01=21Tan−12.
6. So 2I=2π⋅21Tan−12=4πTan−12, giving I=8πTan−12.
Common Mistakes
- Forgetting that cos(π−2x)=−cos2x still leaves cos2(π−2x)=cos22x unchanged, so the denominator is genuinely symmetric.
- Losing a sign when flipping the limits of integration after the w=cos2x substitution.
✓Final answerThe correct option is (A) — 8π(Tan−12).
ANSWER: A
- 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).
- So ∫0π/2hdx=∫0π/2[sin2(sinx)+cos2(sinx)]dx=∫0π/21dx=2π (using sin2θ+cos2θ=1 with θ=sinx).
- So ∫0πhdx=2⋅2π=π, and I=2π⋅π=2π2.
Common Mistakes
- Trying to integrate sin2(sinx) and cos2(cosx) directly instead of pairing them via the complementary substitution.
- Forgetting to apply King's property first to remove the x weight.
✓Final answerThe correct option is (B) — π2/2.
ANSWER: B
- 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.
- Let u=cosx, du=−sinxdx. When x=0,u=1; when x=π,u=−1. So J=∫1−11+u2−du=∫−111+u2du=[arctanu]−11=4π−(−4π)=2π.
- So 2I=π⋅2π=2π2⇒I=4π2.
Common Mistakes
- Forgetting that cos2(π−x)=cos2x (even though cos(π−x)=−cosx), which is what makes the King's-rule trick applicable here.
- Sign errors in the u=cosx substitution flipping the limits.
✓Final answerThe correct option is (C) — 4π2.
ANSWER: C
- AP EAPCET 2021Set eng-2021-08-24-FN1 markMCQQ.∫0πsecx+tanxxtanxdx= (A) 2π(π−2) (B) 2π+2 (C) 2π(π+2) (D) 2π−2
›Reveal solutionSolution
The integrand times x over [0,π] is handled with the symmetry trick ∫0axf(x)dx=2a∫0af(x)dx when f(a−x)=f(x).
Concept and Intuition
tanx/(secx+tanx) simplifies to sinx/(1+sinx), a function symmetric under x→π−x. This symmetry lets us replace the troublesome factor of x with a constant π/2, reducing the problem to a standard definite integral.
Step-by-Step Solution
- Simplify: secx+tanxtanx=(1+sinx)/cosxsinx/cosx=1+sinxsinx=f(x).
- Check symmetry: f(π−x)=1+sin(π−x)sin(π−x)=1+sinxsinx=f(x). ✓
- By the King's rule, I=∫0πxf(x)dx=2π∫0πf(x)dx.
- Compute J=∫0π1+sinxsinxdx=∫0π[1−1+sinx1]dx=π−∫0π1+sinxdx.
- With t=tan(x/2): 1+sinx=1+t2(1+t)2, dx=1+t22dt, so 1+sinxdx=(1+t)22dt, and ∫0∞(1+t)22dt=2.
- So J=π−2, and I=2π(π−2)=2π(π−2).
Common Mistakes
- Not spotting the f(π−x)=f(x) symmetry and attempting direct (much harder) integration.
- Sign/limit errors in the Weierstrass (t=tan(x/2)) substitution.
✓Final answerThe correct option is (A) — 2π(π−2).
ANSWER: A
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