Q.By using the properties of definite integrals, evaluate the integral ∫02x2−xdx
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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 t=2−x to transform the integral into a standard form.
Step 1: Let t=2−x. Then x=2−t, dx=−dt, and when x=0, t=2; when x=2, t=0.
Step 2: Substitute and reverse the limits:
∫02x2−xdx=∫20(2−t)t(−dt)=∫02(2−t)tdt.
Step 3: Split and integrate:
∫02(2t1/2−t3/2)dt=[2⋅32t3/2−52t5/2]02=[34t3/2−52t5/2]02.
Step 4: Evaluate at t=2: …
Using the substitution t=2−x transforms the integral into a standard power form, yielding the value 15162.
The key insight here is that the integrand x2−x is not symmetric in any obvious way over [0,2], but the factor 2−x suggests a natural substitution: let t=2−x. This flips the limits and often simplifies the square root into a power of t, while the x becomes 2−t. The result is a sum of two simple power integrals — no tricks, just clean algebra.
Let’s work through it step by step.
- Set up the substitution. Let t=2−x. Then x=2−t, and dx=−dt. When x=0, t=2; when x=2, t=0. The integral becomes:
I=∫02x2−xdx=∫20(2−t)t(−dt).
- Simplify the limits. The negative sign in dx and the reversed limits cancel:
I=∫02(2−t)tdt.
Notice the limits are now 0 to 2 again, but the integrand is in terms of t.
- Expand the integrand. Write t=t1/2, so:
I=∫02(2t1/2−t3/2)dt.
- Integrate term by term. Using ∫tndt=n+1tn+1:
∫2t1/2dt=2⋅3/2t3/2=34t3/2,
∫t3/2dt=5/2t5/2=52t5/2.
So:
I=[34t3/2−52t5/2]02.
- Evaluate at the limits. At t=2:
34(2)3/2−52(2)5/2=34⋅22−52⋅42=382−582.
At t=0, both terms are 0. …
Method: The substitution t=a−x to rationalise xa−x
For ∫0axa−xdx, put t=a−x: the square root becomes t and x becomes a−t, leaving a sum of simple fractional-power terms.
Steps
Step 1: Substitute t=a−x.
Then x=a−t, a−x=t, dx=−dt; swapping the limits cancels the minus sign.
Step 2: Expand the integrand in t.
(a−t)t=at1/2−t3/2.
Step 3: Integrate with the power rule. …
Common Mistakes
Mistake 1: Reaching for integration by parts on x2−x.
Why it's wrong: by-parts works but is longer and more error-prone than the substitution t=2−x, which rationalises the root immediately. Correct approach: put t=2−x so the integrand becomes 2t1/2−t3/2.
Mistake 2: Not converting the x outside the root to 2−t. …
Showing the 12 most recent of 48 on this concept.
- 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 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 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 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 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 2024Set eng-2024-05-22-AN1 markMCQQ.∫−22(4−x2)5/2dx= (A) 40π (B) 20π (C) 10π (D) 325π
›Reveal solutionSolution
A trig substitution x=2sinθ reduces this to a standard cos6θ Wallis integral, giving 20π, option (B).
Concept and Intuition
Whenever the integrand contains (a2−x2)n/2 over symmetric limits [−a,a], the substitution x=asinθ removes the square root entirely and turns it into a pure power of cosine, which is evaluated by the Wallis reduction formula.
Step-by-Step Solution
- Let x=2sinθ, so dx=2cosθdθ and 4−x2=4cos2θ. Limits x=−2→2 correspond to θ=−π/2→π/2.
- (4−x2)5/2=(4cos2θ)5/2=45/2cos5θ=32cos5θ.
- Integral becomes ∫−π/2π/232cos5θ⋅2cosθdθ=64∫−π/2π/2cos6θdθ.
- By symmetry, =64⋅2∫0π/2cos6θdθ=128⋅6!!5!!⋅2π=128⋅4815⋅2π. …
- 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 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 2023Set eng-2023-05-15-FN1 markMCQQ.If I=∫−aa(x4−2x2)dx, then I is minimum at a= (A) 2 (B) −2 (C) 2 (D) −2
›Reveal solutionSolution
Treating I(a)=∫−aa(x4−2x2)dx as a function of a and minimizing it via calculus gives the minimum at a=2.
Concept and Intuition
Here a is not the integration variable but a parameter — the problem wants the value of a that minimizes the resulting function I(a). Since x4−2x2 is even, the integral simplifies nicely, and then it's a standard single-variable optimization (first derivative zero, second derivative test).
Step-by-Step Solution
- x4−2x2 is an even function, so I(a)=∫−aa(x4−2x2)dx=2∫0a(x4−2x2)dx.
- ∫0a(x4−2x2)dx=5a5−32a3, so I(a)=52a5−34a3.
- I′(a)=2a4−4a2=2a2(a2−2).
- Set I′(a)=0: a=0 or a2=2⇒a=±2.
- I′′(a)=8a3−8a=8a(a2−1).
- At a=2: I′′(2)=82(2−1)=82>0 → local minimum. …
- AP EAPCET 2026Set eng-2026-05-12-AN1 markMCQQ.∫05x(5−x)20dx= (A) 441520 (B) 441521 (C) 462521 (D) 462522
›Reveal solutionSolution
The substitution u=5−x turns the integral into two elementary power integrals, giving 462522.
Concept and Intuition
Whenever an integral has a linear factor times a high power of (a−x), the substitution u=a−x swaps the roles so the high power becomes the simple variable, and the linear factor becomes (a−u) — turning the whole thing into two standard power-rule integrals.
Step-by-Step Solution
- Let u=5−x, so x=5−u and dx=−du. Limits: x=0⇒u=5; x=5⇒u=0.
- ∫05x(5−x)20dx=∫50(5−u)u20(−du)=∫05(5−u)u20du.
- Split: =5∫05u20du−∫05u21du=5[21u21]05−[22u22]05=215⋅521−22522=21522−22522. …
- 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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