Q.Evaluate ∫π/6π/31+tanxdx
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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 (King’s property)
Use the substitution x→a+b−x, where a=π/6, b=π/3.
Let I=∫π/6π/31+tanxdx.
Step 1: Replace x by π/2−x (since a+b=π/2).
Then dx→−dx, and the limits swap, giving:
I=∫π/6π/31+tan(π/2−x)dx=∫π/6π/31+cotxdx.
Step 2: Since cotx=1/tanx, rewrite:
I=∫π/6π/31+tanx1dx=∫π/6π/31+tanxtanxdx. …
Using the property ∫abf(x)dx=∫abf(a+b−x)dx, the given integral simplifies to half the length of the interval, yielding the value 12π.
When you see an integral with a complicated function like tanx, the first instinct might be to try a substitution. But here, the limits π/6 and π/3 are symmetric about π/4, and the integrand has a special structure. The key is to use a symmetry property of definite integrals — often called the "King's property" — which lets you replace x with a+b−x without changing the value of the integral. This trick is especially powerful when the integrand has terms like tanx and cotx that swap under this transformation.
Let’s see how it works.
- State the property. For any continuous function f on [a,b], we have:
∫abf(x)dx=∫abf(a+b−x)dx
Here, a=π/6 and b=π/3, so a+b=π/2. Thus:
I=∫π/6π/31+tanxdx=∫π/6π/31+tan(π/2−x)dx
- Simplify the transformed integrand. Recall that tan(π/2−x)=cotx=tanx1. So:
tan(π/2−x)=cotx=tanx1
Therefore:
I=∫π/6π/31+tanx1dx=∫π/6π/31+tanxtanxdx
- Add the two expressions for I. We now have two forms of the same integral:
I=∫π/6π/31+tanxdxandI=∫π/6π/31+tanxtanxdx
Adding them: …
Method: The reflection (a+b-x) property for a self-complementary integrand
Use this when a definite integral ∫abf(x)dx has an integrand that turns into "1 minus itself" under the substitution x→a+b−x — typically a fraction of the form 1+g(x)1 where g(a+b−x)=g(x)1.
Steps
Step 1: Write down the reflection property.
For any continuous f on [a,b],
∫abf(x)dx=∫abf(a+b−x)dx.
This does not change the value — it only re-expresses the same area, reading the interval from the other end.
Step 2: Compute a+b and substitute.
Add the two endpoints to find the "reflection centre" a+b. Replace x by a+b−x inside f and simplify each trig/algebraic piece (e.g. tan(2π−x)=cotx, so tan becomes cot=1/tan). …
Common Mistakes
Mistake 1: Trying to integrate 1+tanx1 directly.
Why it's wrong: this integrand has no elementary antiderivative you could find in an exam, so a t=tanx substitution just produces an unmanageable rational function. Correct approach: recognise the symmetric limits and apply the x→a+b−x reflection property instead.
Mistake 2: Using the wrong reflection centre. …
Showing the 12 most recent of 48 on this concept.
- 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 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-2024-05-22-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. …
- 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 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 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-2025-05-21-AN1 markMCQQ.∫0π/2log∣tanx+cotx∣dx= (A) πlog2 (B) −πlog2 (C) 2πlog2 (D) 2πlog2
›Reveal solutionSolution
Simplify tanx+cotx=2/sin2x, split the log, and use the classical result ∫0πlogsinudu=−πlog2. Answer: πlog2.
Concept and Intuition
tanx+cotx always simplifies to sin2x2 via the Pythagorean identity — a very common simplification in definite-integral problems. This converts the problem into the well-known integral of logsin, whose value over a full "half-period" (0 to π) is a standard memorized result, −πlog2.
Step-by-Step Solution
- tanx+cotx=cosxsinx+sinxcosx=sinxcosxsin2x+cos2x=sinxcosx1=sin2x2.
- So log∣tanx+cotx∣=log2−log(sin2x) (since sin2x>0 on (0,π/2)).
- ∫0π/2log∣tanx+cotx∣dx=2πlog2−∫0π/2log(sin2x)dx.
- Let I=∫0π/2log(sin2x)dx. Substitute u=2x,du=2dx: I=21∫0πlog(sinu)du. …
- 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 2024Set eng-2024-05-20-FN1 markMCQQ.∫−ππ4−cos2xxsin3xdx= (A) 2π(1−log3) (B) 2π(1−43log3) (C) π(1−43log3) (D) 4π(1−log3)
›Reveal solutionSolution
Use symmetry (odd integrand times x, plus f(π−x)=f(x)) to strip the x out of the integral, then finish with a u=cosx substitution and partial fractions.
Concept and Intuition
Integrals of the form ∫−aaxg(x)dx where g is odd become 2∫0axg(x)dx (since xg(x) is even). If additionally g(π−x)=g(x) on [0,π], the classic "King's Rule" trick ∫0πxg(x)dx=2π∫0πg(x)dx removes the x factor entirely.
Step-by-Step Solution
- Let g(x)=4−cos2xsin3x. Since sin3(−x)=−sin3x and cos2(−x)=cos2x, g is odd, so xg(x) is even: ∫−ππxg(x)dx=2∫0πxg(x)dx.
- Also g(π−x)=4−cos2(π−x)sin3(π−x)=4−cos2xsin3x=g(x) (since sin(π−x)=sinx, cos(π−x)=−cosx), so King's Rule gives ∫0πxg(x)dx=2π∫0πg(x)dx.
- Combining: original integral =2⋅2π∫0πg(x)dx=π∫0πg(x)dx=πJ.
- Compute J=∫0π4−cos2xsin3xdx via u=cosx: J=∫−114−u21−u2du=2∫01[1−4−u23]du (using 1−u2=(4−u2)−3). …
- 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 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]. …
- AP EAPCET 2023Set eng-2023-05-18-AN1 markMCQQ.∫−4π4πtan9xsin6xcos3xdx= (A) 16×2π (B) 8×32 (C) 16×1714×1512×…×32 (D) 0
›Reveal solutionSolution
Odd × even × even = odd, and the integral of any odd function over a symmetric interval is zero — no actual antiderivative work is needed.
Concept and Intuition
Before grinding through a nasty trig integral, always check parity. tan(−x)=−tanx (odd), and raising an odd function to an odd power (9) keeps it odd. sin(−x)=−sinx raised to an even power (6) becomes even, and cos(−x)=cosx raised to any power stays even. Odd times even times even is odd, and an odd function's graph is antisymmetric about the origin, so equal positive and negative area cancels exactly over any interval symmetric about 0.
Step-by-Step Solution
- Let g(x)=tan9xsin6xcos3x.
- g(−x)=tan9(−x)sin6(−x)cos3(−x)=(−tanx)9(sinx)6(cosx)3=−tan9xsin6xcos3x=−g(x).
- So g is an odd function. …
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