Q.Evaluate the definite integral: ∫−11(x+1) dx
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 that the definite integral of a sum can be split, and the integral of an odd function over a symmetric interval is zero.
Step 1: Split the integral:
∫−11(x+1)dx=∫−11xdx+∫−111dx
Step 2: The function x is odd, and the interval [−1,1] is symmetric about zero, so:
∫−11xdx=0
Step 3: The integral of the constant 1 over [−1,1] is the length of the interval:
∫−111dx=1−(−1)=2
Step 4: Adding the results:
0+2=2
The value is 2.
The integral ∫−11(x+1)dx equals 2. This is found by using the symmetry of the odd part (x) and the even part (1) over a symmetric interval, or by direct antiderivative evaluation.
The key insight here is that the interval [−1,1] is symmetric about 0. When you have a sum of functions, you can often break the integral into parts and use symmetry to simplify calculations. The function x+1 is not purely odd or even, but it is the sum of an odd function (x) and an even function (1). Over a symmetric interval [−a,a], the integral of an odd function is zero, while the integral of an even function is twice the integral from 0 to a. This saves you from having to compute the antiderivative directly, though that also works perfectly.
Let’s go through it step by step.
- Separate the integral into two parts
∫−11(x+1)dx=∫−11xdx+∫−111dx
This is valid because the integral of a sum is the sum of the integrals.
- Handle the odd part: ∫−11xdx The function f(x)=x is odd, meaning f(−x)=−f(x). For any odd function integrated over a symmetric interval [−a,a], the result is zero.
∫−11xdx=0
A quick check: the antiderivative of x is 2x2, and evaluating from −1 to 1 gives 212−2(−1)2=21−21=0. Same result.
- Handle the even part: ∫−111dx The constant function g(x)=1 is even, since g(−x)=g(x). For an even function over [−a,a], the integral equals twice the integral from 0 to a:
∫−111dx=2∫011dx
Now ∫011dx is just the length of the interval from 0 to 1, which is 1. So:
2×1=2
- Combine the results
∫−11(x+1)dx=0+2=2
A common mistake is to forget that the constant 1 is even and treat it like an odd function. Another pitfall is incorrectly applying symmetry when the interval is not symmetric — but here it is, so we’re safe.
If you prefer the direct antiderivative method, it’s just as straightforward:
∫(x+1)dx=2x2+x
Evaluating from −1 to 1:
(212+1)−(2(−1)2+(−1))=(21+1)−(21−1)=23−(−21)=23+21=2
Same answer, confirming our symmetry approach.
The value of the definite integral is 2.
Method: Evaluate a definite integral by the Fundamental Theorem of Calculus
For ∫abf(x)dx, find any antiderivative F, then compute F(b)−F(a) — no constant of integration needed.
Steps
Step 1: Integrate term by term to get an antiderivative. For a linear integrand x+1, use the power rule: F(x)=2x2+x.
Step 2: Write the evaluation bracket.
∫ab(x+1)dx=[2x2+x]ab.
Step 3: Substitute the upper limit, then the lower, and subtract.
F(b)−F(a), being careful with signs when the lower limit is negative.
Step 4: Simplify to a number. The definite integral is a value, not a function, and needs no +C.
Common Mistakes
Mistake 1: Adding +C to a definite integral.
Why it's wrong: the constant cancels in F(b)−F(a). Correct approach: drop C for definite integrals.
Mistake 2: Sign slip at a negative lower limit.
Why it's wrong: at x=−1, 2(−1)2+(−1)=21−1=−21; subtracting this adds 21. Correct approach: compute F(−1) fully, then subtract with its sign.
Mistake 3: Assuming "symmetry" makes it zero.
Why it's wrong: x+1 is not an odd function about 0 (the +1 is even), so the integral is not 0. Correct approach: split ∫−11xdx=0 but ∫−111dx=2, giving 2.
Showing the 12 most recent of 48 on this concept.
- 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.
Common Mistakes
- Attempting brute-force integration of each square root term (very messy) instead of noticing the odd symmetry.
- Mis-identifying which term maps to which under x→−x.
✓Final answerThe correct option is (C) — 0.
ANSWER: C
- AP EAPCET 2021Set eng-2021-08-24-AN1 markMCQQ.∫−π/4π/4xtan(1+x2)dx= (A) 0 (B) 4π (C) 4−π (D) 1
›Reveal solutionSolution
This is a symmetric-limits definite integral where checking odd/even parity instantly gives the answer without doing any actual antiderivative work: it is 0.
Concept and Intuition
For ∫−aaf(x)dx: if f is odd (f(−x)=−f(x)) the integral is 0; if f is even it equals 2∫0af(x)dx. Any function built as (odd function of x) × (function of x2) is automatically odd, because a function of x2 never changes sign under x→−x.
Step-by-Step Solution
- Let f(x)=xtan(1+x2).
- Replace x by −x: f(−x)=(−x)tan(1+(−x)2)=−xtan(1+x2)=−f(x).
- So f is odd on the symmetric interval [−4π,4π].
- Therefore ∫−π/4π/4xtan(1+x2)dx=0.
Common Mistakes
- Trying to find the actual antiderivative instead of noticing the much faster parity shortcut.
- Misjudging 1+x2 as odd — it is even, since squaring removes the sign, and adding a constant keeps it even.
✓Final answerThe correct option is (A) — 0.
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 2025Set eng-2025-05-23-AN1 markMCQQ.∫−π/2π/2sin2xcos2x(sinx+cosx)dx= (A) 0 (B) 152 (C) 154 (D) 52
›Reveal solutionSolution
This tests using odd/even symmetry over a symmetric interval to kill half the integral, then a simple u=sinx substitution for the rest. The answer is 154, option (C).
Concept and Intuition
Over a symmetric interval [−a,a], an odd integrand integrates to zero and an even integrand integrates to twice the integral over [0,a]. Expanding (sinx+cosx) splits the problem cleanly into one odd term and one even term, so only the even term survives — turning a seemingly complicated integral into a single elementary substitution.
Step-by-Step Solution
- Expand: sin2xcos2x(sinx+cosx)=sin3xcos2x+sin2xcos3x.
- g(x)=sin3xcos2x: since sin3(−x)=−sin3x and cos2(−x)=cos2x, g(−x)=−g(x) — odd. So ∫−π/2π/2g(x)dx=0.
- h(x)=sin2xcos3x: both factors are even, so h is even, and ∫−π/2π/2hdx=2∫0π/2hdx.
- Write h(x)=sin2xcos2xcosx=sin2x(1−sin2x)cosx. Let u=sinx, du=cosxdx; limits 0→1.
- ∫0π/2hdx=∫01u2(1−u2)du=[3u3−5u5]01=31−51=152.
- So the full integral =2×152=154.
Common Mistakes
- Missing the odd/even split and trying to integrate the whole product directly, which is much more error-prone.
- Forgetting the factor of 2 from doubling the [0,π/2] integral for the even part.
✓Final answerThe correct option is (C) — 154.
ANSWER: C
- 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.
- So ∫1∞1+x41+x2dx=∫t=10−t4+1t2+1dt=∫011+t41+t2dt=B.
- Therefore A=B+B=2B.
Common Mistakes
- Losing track of the sign flips: the substitution flips the limits AND introduces a minus sign, and the two cancel — many students keep only one and get A=0 or similar nonsense.
- Trying to evaluate the improper integral A directly (it can be done, but it's slower and error-prone compared to this symmetry argument).
✓Final answerThe correct option is (C) — 2B=A.
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 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.
The antiderivative's value is 2π−21.
5. Subtract: (24051π−21)−(2π−21)=24051π−π=24050π=2025π.
Common Mistakes
- Attempting to integrate the original rational-trig form directly instead of simplifying with the Pythagorean identity first.
- Miscounting whether 4051 is odd (it is), which determines whether cos(4051π)=−1 or +1 and whether the cosine terms cancel or double.
✓Final answerThe correct option is (D) — 2025π.
ANSWER: D
- 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.
- Common denominator: 21522−22522=522⋅21×2222−21=462522.
Common Mistakes
- Sign error on flipping the limits after substitution (forgetting the extra −1 from dx=−du, which cancels with the limit flip).
- Arithmetic slip combining 211−221 or losing a power of 5.
✓Final answerThe correct option is (D) — 462522.
ANSWER: D
- 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.
- Now use the property ∫0af(x)dx=∫0af(a−x)dx (substitute x→a−x in either integral — the limits swap and flip sign twice, leaving the same value), which is option (D).
Common Mistakes
- Assuming option (C), ∫0a[f(x)+f(a−x)]dx, is the answer — that expression actually equals 2∫0af(x)dx, twice too large.
- Forgetting the sign flip when substituting x=−t in the lower half of the symmetric integral.
✓Final answerThe correct option is (D) — ∫0af(a−x)dx.
ANSWER: D
- AP EAPCET 2024Set eng-2024-05-22-FN1 markMCQQ.∫0π/4log(1+tanx)dx= (A) πlog2+1 (B) 2πlog2+1 (C) 4πlog2 (D) 8πlog2
›Reveal solutionSolution
A textbook symmetry trick (x→π/4−x) doubles the integral into something trivial to evaluate. Answer: 8πlog2.
Concept and Intuition
Whenever the limits are 0 to a and the integrand involves tanx, trying the substitution x→a−x is a classic move — here it converts log(1+tanx) into log(1+tanx2), and adding the original and transformed integrals collapses most of the complexity.
Step-by-Step Solution
- Let I=∫0π/4log(1+tanx)dx.
- Substitute x→4π−x: tan(4π−x)=1+tanx1−tanx, so 1+tan(4π−x)=1+tanx2.
- So I=∫0π/4log(1+tanx2)dx=∫0π/4log2dx−∫0π/4log(1+tanx)dx=4πlog2−I.
- So 2I=4πlog2⇒I=8πlog2.
Common Mistakes
- Forgetting to flip the limits' effect correctly and losing the minus sign on the second integral, which would double I instead of cancelling it.
- Miscomputing tan(π/4−x) from the tangent subtraction formula.
✓Final answerThe correct option is (D) — 8πlog2.
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 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).
- Add the original expression for I to this: 2I=∫ab[1+tanx1+1+tanxtanx]dx=∫ab1dx=b−a.
- b−a=229π−11π=229π−222π=227π.
- I=447π.
Common Mistakes
- Forgetting to check that a+b=π/2 first (the trick only works because of this specific limit sum).
✓Final answerThe correct option is (D) — 447π.
ANSWER: D
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