Q.Evaluate the definite integral: ∫0πcos2xdx
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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 …
The key idea is to use the symmetry of cos2x about π/2, or equivalently, the identity cos2x=21+cos2x.
Step 1: Use the double-angle identity to rewrite the integrand:
cos2x=21+cos2x.
Step 2: Substitute into the integral and split:
∫0πcos2xdx=21∫0π1dx+21∫0πcos2xdx. …
Using the symmetry of cos2x about π/2, the integral from 0 to π equals twice the integral from 0 to π/2, which evaluates to π/2.
The key to solving ∫0πcos2xdx efficiently is noticing a symmetry — not just any symmetry, but the fact that cos2x is symmetric about the midpoint x=π/2. This is a classic trick for definite integrals of even powers of sine and cosine over a full period or half-period.
Why does this matter? Because instead of integrating over the whole interval [0,π], we can double the integral over [0,π/2], where cos2x has a well-known antiderivative. Let’s walk through it.
- Recognize the symmetry. The function cos2x is periodic with period π, but more importantly, it is symmetric about x=π/2 on [0,π]. That is, cos2(π−x)=cos2x. This means the area under the curve from 0 to π/2 is exactly the same as from π/2 to π. So:
∫0πcos2xdx=2∫0π/2cos2xdx
- Use the double-angle identity. To integrate cos2x, we rewrite it using cos2x=21+cos2x. This is the standard trick — it turns a squared trig function into something linear in cos2x, which is easy to integrate.
∫0π/2cos2xdx=∫0π/221+cos2xdx
- Integrate term by term.
=21∫0π/21dx+21∫0π/2cos2xdx
The first integral is straightforward: ∫0π/21dx=π/2.
For the second, let u=2x, so du=2dx, and when x=0, u=0; when x=π/2, u=π. Then:
∫0π/2cos2xdx=21∫0πcosudu=21[sinu]0π=21(0−0)=0
- Combine the results. …
Method: Definite integral of cos2x via power reduction
An even power of cos (or sin) has no elementary antiderivative as-is; use a double-angle identity to reduce the power first, then evaluate.
Steps
Step 1: Apply the power-reduction identity.
cos2x=21+cos2x.
Step 2: Integrate the reduced form.
∫cos2xdx=2x+4sin2x+C. …
Common Mistakes
Mistake 1: Writing ∫cos2xdx=3cos3x.
Why it's wrong: that is a chain-rule guess with no −sinx present; cos2x is not u2du. Correct approach: use cos2x=21+cos2x.
Mistake 2: Getting the identity sign wrong (cos2x=21−cos2x).
Why it's wrong: that is sin2x; cos2x uses a plus. Correct approach: cos2x=21+cos2x. …
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. …
- 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-2025-05-21-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 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 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 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 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. …
- 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 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 2026Set eng-2026-05-13-AN1 markMCQQ.∫−3π/2−π/2((x+π)3+cos2(x+3π))dx= (A) 8π (B) 2π (C) 4π−1 (D) 32π4
›Reveal solutionSolution
Shifting the variable to u=x+π turns the limits into a symmetric interval about zero; the odd cubic term vanishes and only the even cos2u term survives, giving π/2.
Concept and Intuition
Whenever an integral's limits and integrand both have a shift-symmetry, substituting to center the interval at 0 lets us exploit odd/even function properties: odd functions integrate to zero over [−a,a], and even functions can be doubled over [0,a].
Step-by-Step Solution
- Let u=x+π, so du=dx. When x=−3π/2, u=−π/2; when x=−π/2, u=π/2.
- cos2(x+3π)=cos2((x+π)+2π)=cos2(u+2π)=cos2u (cosine has period 2π).
- The integral becomes ∫−π/2π/2(u3+cos2u)du.
- u3 is an odd function, so ∫−π/2π/2u3du=0.
- cos2u is even, so ∫−π/2π/2cos2udu=2∫0π/2cos2udu. …
- 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 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. …
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