Q.Evaluate ∫0π1+cos2xxsinxdx
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 property of definite integrals: ∫0af(x)dx=∫0af(a−x)dx.
Let I=∫0π1+cos2xxsinxdx.
Replace x by π−x:
I=∫0π1+cos2(π−x)(π−x)sin(π−x)dx=∫0π1+cos2x(π−x)sinxdx.
Add the two expressions for I:
2I=∫0π1+cos2xπsinxdx.
Now evaluate the simpler integral. Let u=cosx, so du=−sinxdx. When x=0, u=1; when x=π, u=−1.
2I=π∫1−11+u2−du=π∫−111+u2du=π[tan−1u]−11=π(4π−(−4π))=π⋅2π=2π2.
Thus I=4π2.
The value is 4π2.
Using the property ∫0af(x)dx=∫0af(a−x)dx simplifies the integral to a form where the x factor is replaced by π−x, allowing us to isolate the x-dependent part and evaluate the remaining trigonometric integral via a standard substitution. The value is 4π2.
When you see an integral from 0 to π (or 0 to a) with a product of x and a trigonometric function, the first instinct should be to check if symmetry can help. The standard trick is to use the property:
∫0af(x)dx=∫0af(a−x)dx
This works because replacing x by a−x just reverses the order of integration, but the limits stay the same. Here a=π, so we replace x by π−x in the integrand.
Let’s see what happens.
- Apply the symmetry property
Let
I=∫0π1+cos2xxsinxdx
Using x→π−x, we get:
I=∫0π1+cos2(π−x)(π−x)sin(π−x)dx
Now recall: sin(π−x)=sinx and cos(π−x)=−cosx, so cos2(π−x)=cos2x. Therefore:
I=∫0π1+cos2x(π−x)sinxdx
- Add the two expressions for I
We now have two expressions for the same I:
I=∫0π1+cos2xxsinxdx
I=∫0π1+cos2x(π−x)sinxdx
Add them:
2I=∫0π1+cos2xxsinx+(π−x)sinxdx=∫0π1+cos2xπsinxdx
So:
2I=π∫0π1+cos2xsinxdx
The x has vanished — that’s the whole point. Now we just need to evaluate the remaining trigonometric integral.
- Evaluate the trigonometric integral
Let J=∫0π1+cos2xsinxdx.
Substitute u=cosx, so du=−sinxdx. When x=0, u=1; when x=π, u=−1. Thus:
J=∫1−11+u2−du=∫−111+u2du
This is a standard integral:
∫1+u2du=arctanu
So:
J=[arctanu]−11=arctan(1)−arctan(−1)=4π−(−4π)=2π
Notice that ∫−111+u2du is an even function integrated over a symmetric interval, so you could also compute 2∫011+u2du=2⋅4π=2π.
- Finish solving for I
We have 2I=π⋅J=π⋅2π=2π2.
Therefore:
I=4π2
A common mistake is to forget that cos2(π−x)=(−cosx)2=cos2x, which is correct — but some students mistakenly think cos(π−x)=cosx (wrong sign) and then square incorrectly. The square saves you here, but be careful with signs before squaring.
The value of the integral is 4π2.
Method: The Symmetry Property ∫0af(x)dx=∫0af(a−x)dx
Use this for a definite integral over [0,a] whose integrand simplifies when x is replaced by a−x, especially when an isolated x factor multiplies a symmetric function.
Steps
Step 1: Write I and form the reflected copy.
Let I=∫0af(x)dx and also I=∫0af(a−x)dx. Replacing x→a−x leaves sin,cos2 etc. unchanged but turns the isolated x into a−x.
Step 2: Add the two forms.
Adding gives 2I=∫0a[f(x)+f(a−x)]dx, in which the x-factor combines into the constant a, cancelling the troublesome x.
Step 3: Evaluate the simpler integral, then divide by 2.
For ∫0π1+cos2xxsinxdx, this reduces to 2π∫0π1+cos2xsinxdx; a substitution u=cosx then gives 4π2.
Common Mistakes
Mistake 1: Assuming f(a−x)=f(x) for every term.
Why it's wrong: only sinx and cos2x are unchanged under x→π−x; the isolated x becomes π−x. Correct approach: substitute carefully into each factor.
Mistake 2: Forgetting to divide by 2 at the end.
Why it's wrong: adding the two forms gives 2I, so the final answer needs the factor 21. Correct approach: solve 2I=⋯ for I.
Mistake 3: Mishandling the leftover substitution.
Why it's wrong: ∫0π1+cos2xsinxdx needs u=cosx with limits 1→−1; a sign slip mis-evaluates the arctan. Correct approach: change limits and track the minus from du=−sinxdx.
Showing the 12 most recent of 48 on this concept.
- 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 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.
- Compute K via c=cosx, dc=−sinxdx: K=∫−111+c2dc=[tan−1c]−11=4π−(−4π)=2π.
- So 2J=π⋅2π=2π2⇒J=4π2.
- Final answer: ∫−ππfdx=2J=2π2.
Common Mistakes
- Skipping the even-function step and only computing J over [0,π], then forgetting to double it for the full [−π,π] range.
- Sign slip when substituting cos(π−x)=−cosx into 1+cos2x (squaring removes the sign, which is easy to mishandle).
✓Final answerThe correct option is (D) — 2π2.
ANSWER: D
- 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 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
- 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 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 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 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-2023-05-18-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 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
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