Q.By using the properties of definite integrals, evaluate the integral ∫0ax+a−xxdx
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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 property of definite integrals: ∫0af(x)dx=∫0af(a−x)dx.
Let I=∫0ax+a−xxdx.
Replace x by a−x. Since dx becomes −dx but the limits swap, we have:
I=∫0aa−x+xa−xdx.
Now add the two expressions for I: …
Using the symmetry property ∫0af(x)dx=∫0af(a−x)dx, we add the original integral to its transformed version, simplify the sum to a, and obtain the value 2a.
The key insight here is that the integrand has a beautiful symmetry when you replace x with a−x. The denominator x+a−x simply swaps its two terms, while the numerator x becomes a−x. This kind of structure is tailor-made for the property:
∫0af(x)dx=∫0af(a−x)dx
This holds for any function f that is integrable on [0,a]. It works because as x runs from 0 to a, the quantity a−x runs from a down to 0 — a perfect reversal. The area under the curve doesn't change.
Let's apply it.
- Define the integral Let
I=∫0ax+a−xxdx.
- Apply the substitution x→a−x Using the property above, replace x by a−x everywhere in the integrand. The limits stay the same (0 and a), and dx remains dx:
I=∫0aa−x+xa−xdx.
Notice the denominator is the same as before — just the two terms swapped — so it's unchanged. The numerator is now a−x.
- Add the two expressions for I We now have two different-looking integrals that are actually equal. Add them:
I+I=∫0ax+a−xxdx+∫0aa−x+xa−xdx.
Since the denominators are identical, we can combine the integrands over a single integral:
2I=∫0ax+a−xx+a−xdx.
- Simplify …
Method: The general f+f(a−x)f complementary trick ⇒2a
For ∫0af(x)+f(a−x)f(x)dx, reflection produces the complementary fraction; the two always add to 1, giving half the interval length regardless of f.
Steps
Step 1: Reflect with x→a−x.
I=∫0af(a−x)+f(x)f(a−x)dx.
Step 2: Add — the denominators are identical. …
Common Mistakes
Mistake 1: Trying to integrate x+a−xx by rationalising directly.
Why it's wrong: direct manipulation is messy and unnecessary — the f+f(a−x)f pattern gives 2a by reflection. Correct approach: reflect x→a−x and add.
Mistake 2: Doubting the answer because it has no x in it. …
Showing the 12 most recent of 48 on this concept.
- AP EAPCET 2022Set eng-2022-07-06-FN1 markMCQQ.∫−aaf(x)dx−∫0af(−x)dx= (A) ∫−aaf(a−x)dx (B) ∫−aaf(x)+f(a−x)dx (C) ∫0af(x)+f(a−x)dx (D) ∫0af(a−x)dx
›Reveal solutionSolution
The expression simplifies to ∫0af(x)dx, which by the standard reflection property equals ∫0af(a−x)dx.
Concept and Intuition
Split the symmetric integral at the origin and use the substitution x→−x on the negative half to relate it to ∫0af(−x)dx — this is exactly the term being subtracted, so it cancels, leaving a plain ∫0af(x)dx. Then apply the classic property ∫0af(x)dx=∫0af(a−x)dx (true for any integrable f, by substituting x→a−x) to match it to the given answer choices.
Step-by-Step Solution
- Split: ∫−aaf(x)dx=∫−a0f(x)dx+∫0af(x)dx.
- In ∫−a0f(x)dx, substitute x=−t, dx=−dt; limits x=−a→t=a, x=0→t=0: ∫−a0f(x)dx=∫a0f(−t)(−dt)=∫0af(−t)dt=∫0af(−x)dx.
- So ∫−aaf(x)dx=∫0af(−x)dx+∫0af(x)dx.
- Subtracting ∫0af(−x)dx from both sides (as required by the question) leaves exactly ∫0af(x)dx. …
- 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-2024-05-23-FN1 markMCQQ.If A=∫0∞1+x41+x2dx, B=∫011+x41+x2dx, then (A) 2A=B (B) A=B (C) 2B=A (D) 2B+A=0
›Reveal solutionSolution
The reciprocal substitution x=1/t maps [1,∞) onto [0,1] and leaves this particular integrand invariant, so the tail ∫1∞ equals B itself, giving A=2B.
Concept and Intuition
For integrands of the form 1+x41+x2, the substitution x→1/x is special: both the numerator/denominator structure and the dx=−dt/t2 factor combine to reproduce the SAME function of the new variable. Recognizing this self-similarity avoids ever computing the (messy) closed form of the integral.
Step-by-Step Solution
- Write A=∫011+x41+x2dx+∫1∞1+x41+x2dx=B+∫1∞1+x41+x2dx.
- In the second integral, substitute x=t1, so dx=−t2dt; as x:1→∞, t:1→0.
- 1+x2=1+t21=t2t2+1, and 1+x4=1+t41=t4t4+1, so 1+x41+x2=t4+1(t2+1)t2.
- Multiplying by dx=−dt/t2: the integrand becomes t4+1(t2+1)t2⋅(−t21)dt=−t4+1t2+1dt. …
- AP EAPCET 2023Set eng-2023-05-17-AN1 markMCQQ.∫π/6π/31+cotx1dx= (A) π/4 (B) π/2 (C) π/6 (D) π/12
›Reveal solutionSolution
Using the reflection property ∫abf(x)dx=∫abf(a+b−x)dx with a+b=π/2 makes the two forms of the integrand add up to exactly 1, giving I=π/12.
Concept and Intuition
Integrals of the shape ∫1+h(x)dx over symmetric limits around x=π/4-type reflections often pair up with their "co-function" version to sum to a constant — a classic trick that avoids ever actually antidifferentiating cot or tan raised to a half power.
Step-by-Step Solution
- Let I=∫π/6π/31+cotxdx.
- Since π/6+π/3=π/2, substitute x→π/2−x: cot(π/2−x)=tanx, so I=∫π/6π/31+tanxdx as well.
- Add the two expressions for I: 2I=∫π/6π/3[1+cotx1+1+tanx1]dx. …
- 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-2024-05-21-AN1 markMCQQ.∫−11(1+x+x2−1−x+x2)dx= (A) 2 (B) 4 (C) 0 (D) 8
›Reveal solutionSolution
The integrand is an odd function of x, so its integral over the symmetric interval [−1,1] vanishes.
Concept and Intuition
∫−aaf(x)dx=0 whenever f is odd, i.e. f(−x)=−f(x). Recognising this symmetry avoids a painful direct integration of the square roots.
Step-by-Step Solution
- Let g(x)=1+x+x2. Then g(−x)=1−x+x2.
- The integrand is f(x)=g(x)−g(−x).
- Check parity: f(−x)=g(−x)−g(x)=−(g(x)−g(−x))=−f(x) — so f is odd.
- Hence ∫−11f(x)dx=0. …
- 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 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-2025-05-23-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-2022-07-08-FN1 markMCQQ.∫π/119π/221+tanxdx= (A) π/4 (B) π/22 (C) π/11 (D) 7π/44
›Reveal solutionSolution
This tests the classic King's-rule substitution x→a+b−x for definite integrals whose limits sum to π/2, applied to a 1/(1+tanx) integrand.
Concept and Intuition
Whenever the limits of integration sum to a value that makes tanx→cotx under the substitution x→a+b−x (here a+b=π/2, so tan(π/2−x)=cotx), adding the original and transformed integrals often produces a simple constant integrand.
Step-by-Step Solution
- Check a+b: 11π+229π=222π+229π=2211π=2π.
- Substitute x→2π−x: tan(2π−x)=cotx=tanx1, so the transformed integrand is 1+1/tanx1=1+tanxtanx.
- So I=∫ab1+tanxtanxdx as well (same value as the original, by the substitution property). …
- 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. …
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