Q.By using the properties of definite integrals, evaluate the integral ∫0π/2sin5x+cos5xcos5xdx
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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 — when the integrand has the form f(x)+f(a−x)f(x), the integral over [0,a] equals 2a.
Let I=∫0π/2sin5x+cos5xcos5xdx.
Step 1: Use the property ∫0af(x)dx=∫0af(a−x)dx.
Replace x by 2π−x:
I=∫0π/2sin5(2π−x)+cos5(2π−x)cos5(2π−x)dx=∫0π/2cos5x+sin5xsin5xdx. …
Using the symmetry property ∫0af(x)dx=∫0af(a−x)dx, the given integral equals its own complement, so the sum of the two is π/2, giving the value π/4.
The key insight here is that the integrand has a special structure when you replace x by 2π−x. This is a classic trick for integrals over [0,π/2] where the numerator and denominator are symmetric powers of sine and cosine.
Why this works:
For any function f(x) that is continuous on [0,a], we have the property
∫0af(x)dx=∫0af(a−x)dx.
Here a=π/2, and the integrand is sin5x+cos5xcos5x. When we replace x by 2π−x, cosx becomes sinx and sinx becomes cosx, so the integrand flips to cos5x+sin5xsin5x. That is exactly the "complement" of the original fraction — their sum is simply 1. This lets us add the two forms and solve for the integral.
Let’s work through it step by step.
- Define the integral Let
I=∫0π/2sin5x+cos5xcos5xdx.
- Apply the substitution x→2π−x Using the property ∫0af(x)dx=∫0af(a−x)dx, set t=2π−x. Then dx=−dt, and when x=0, t=π/2; when x=π/2, t=0. The integral becomes
I=∫π/20sin5(2π−t)+cos5(2π−t)cos5(2π−t)(−dt).
Reversing the limits removes the minus sign:
I=∫0π/2sin5(2π−t)+cos5(2π−t)cos5(2π−t)dt.
- Simplify the trigonometric expressions Recall: cos(2π−t)=sint and sin(2π−t)=cost. So the integrand becomes
cos5t+sin5tsin5t.
Since t is a dummy variable, we can rename it back to x:
I=∫0π/2sin5x+cos5xsin5xdx.
- Add the two expressions for I We now have two forms of I:
I=∫0π/2sin5x+cos5xcos5xdxandI=∫0π/2sin5x+cos5xsin5xdx.
Adding them: …
Method: The f+gf complementary-integral trick
For ∫0af(x)+f(a−x)f(x)dx (with f,g swapping under x→a−x), reflection produces the complementary fraction; the two add to 1.
Steps
Step 1: Set I and reflect with x→a−x.
I=∫0af(x)+g(x)f(x)dx⇒I=∫0ag(x)+f(x)g(x)dx,
where the reflection swaps f↔g (e.g. sin↔cos).
Step 2: Add the two forms. …
Common Mistakes
Mistake 1: Attempting a t=tanx or half-angle substitution to integrate directly.
Why it's wrong: sin5x+cos5xcos5x leads to an intractable rational function; the reflection property is the intended, far shorter route. Correct approach: use ∫0af(x)=∫0af(a−x).
Mistake 2: Not simplifying the added fractions to 1. …
Showing the 12 most recent of 22 on this concept.
- TG EAPCET 2024Set eng-2024-05-11-FN1 markMCQQ.∫−π/15π/151+e5xcos5xdx= (A) 51 (B) 103 (C) 151 (D) 101
›Reveal solutionSolution
The symmetry trick ∫−aa1+ecxf(x)dx=∫0af(x)dx (for even f) reduces this to ∫0π/15cos5xdx=103.
Use the king-property symmetry. Let
I=∫−π/15π/151+e5xcos5xdx.
Replacing x→−x (limits symmetric) and using cos(−5x)=cos5x:
I=∫−π/15π/151+e5xcos5xe5xdx.
Adding the two forms, since 1+e5x1+1+e5xe5x=1:
2I=∫−π/15π/15cos5xdx=2∫0π/15cos5xdx.
Evaluate. …
- TG EAPCET 2021Set eng-2021-08-06-FN1 markMCQQ.
[!FORMULA] ∫0πxf(sinx)dx=
(A) 2π∫0π/4f(sinx)dx (B) π∫0π/4f(sinx)dx (C) 2π∫0π/2f(sinx)dx (D) π∫0π/2f(sinx)dx›Reveal solutionSolution
Use the property ∫0af(x)dx=∫0af(a−x)dx with a=π to rewrite the integral, then add the two forms. The result is π∫0πf(sinx)dx, which simplifies to π∫0π/2f(sinx)dx because f(sinx) is symmetric about π/2. The correct option is (D).
The key idea here is a classic trick for integrals of the form ∫0axg(x)dx: replace x by a−x and add the two expressions. This often cancels the x factor and leaves a simpler integral.
Let I=∫0πxf(sinx)dx. The function f(sinx) depends on x only through sinx, which has the property sin(π−x)=sinx. That symmetry is what we will exploit.
- Apply the substitution x→π−x. Let t=π−x. Then dx=−dt, and when x=0, t=π; when x=π, t=0. So
I=∫0πxf(sinx)dx=∫π0(π−t)f(sin(π−t))(−dt)=∫0π(π−t)f(sint)dt.
Since the dummy variable doesn’t matter, rename t back to x:
I=∫0π(π−x)f(sinx)dx.
- Add the two expressions for I. We now have two forms:
I=∫0πxf(sinx)dxandI=∫0π(π−x)f(sinx)dx.
Adding them:
2I=∫0π[x+(π−x)]f(sinx)dx=∫0ππf(sinx)dx.
Hence
I=2π∫0πf(sinx)dx.
- Simplify the limits using symmetry. …
- TG EAPCET 2023Set eng-2023-05-14-FN1 markMCQQ.∫−2π2πsin2xcos2x(sinx+cosx)dx= (A) 32 (B) 103 (C) 154 (D) 185
›Reveal solutionSolution
The integrand is an odd function over a symmetric interval, so the integral evaluates to zero; none of the given positive options match, but the correct answer is 0, which is not listed — the intended answer is (C) only if the problem had a misprint, but strictly the integral is zero.
The key insight is symmetry. When integrating over [−π/2,π/2], check if the function is odd or even. An odd function integrated over a symmetric interval always gives zero. Here, sin2xcos2x is even, but (sinx+cosx) is a sum of an odd and an even part. The product of an even function with an odd function is odd, and that part integrates to zero. The even part (from cosx) also integrates to zero because of the specific powers? Let’s check carefully.
- Separate the integrand:
sin2xcos2x(sinx+cosx)=sin2xcos2xsinx+sin2xcos2xcosx.
-
Analyze parity:
- sin2xcos2x is even because sin2x and cos2x are both even.
- sinx is odd, so sin2xcos2x⋅sinx is odd.
- cosx is even, so sin2xcos2x⋅cosx is even.
-
Integrate the odd part:
For any odd function f(x), ∫−aaf(x)dx=0.
Thus,
∫−π/2π/2sin2xcos2xsinxdx=0.
- Integrate the even part: The even part is sin2xcos3x. Over a symmetric interval, we can double the integral from 0 to π/2: ∫−π/2π/2sin2xcos3xdx=2∫0π/2sin2xcos3xdx. …
- TG EAPCET 2026Set eng-2026-05-09-FN1 markMCQQ.Let f:[0,1]→R be a function defined as f(x)+f(1−x)=1. Then ∫01f(x)dx= (A) 0 (B) 1 (C) 21 (D) 41
›Reveal solutionSolution
The functional equation f(x)+f(1−x)=1 forces the average value of f over [0,1] to be 21, so the integral is 21. The correct option is (C).
Concept & Intuition
The given condition f(x)+f(1−x)=1 is a symmetry relation: the value at x and the value at its mirror point 1−x always sum to 1. This means the graph of f is symmetric about the point (21,21). If you average f over the whole interval, the contributions from x and 1−x together always give 1, so the overall average must be 21. The integral is just the average value times the length of the interval.
- Set up the integral and use the substitution x→1−x. Let I=∫01f(x)dx. Substitute u=1−x, so du=−dx and when x=0, u=1; when x=1, u=0. Then
I=∫01f(x)dx=∫10f(1−u)(−du)=∫01f(1−u)du.
Renaming the dummy variable back to x, we have
I=∫01f(1−x)dx.
- Add the two expressions for I. We now have two representations:
I=∫01f(x)dxandI=∫01f(1−x)dx.
Adding them gives
2I=∫01[f(x)+f(1−x)]dx.
- Use the given functional equation. The condition f(x)+f(1−x)=1 holds for every x∈[0,1]. Therefore 2I=∫011dx=[x]01=1.…
- TG EAPCET 2024Set eng-2024-05-10-FN1 markMCQQ.0∫π(sin3x+cos2x)2dx= (A) 1615π+158 (B) 1611π+158 (C) 1615π+154 (D) 1611π+154
›Reveal solutionSolution
The integral simplifies by expanding the square, using symmetry and reduction formulas; the final value is 1611π+158, which corresponds to option (B).
We start with
I=∫0π(sin3x+cos2x)2dx.
The key idea: expand the square, then use symmetry and standard trigonometric integrals. The presence of both odd and even powers suggests splitting the interval or using reduction formulas.
- Expand the square
(sin3x+cos2x)2=sin6x+2sin3xcos2x+cos4x.
So
I=∫0πsin6xdx+2∫0πsin3xcos2xdx+∫0πcos4xdx.
- Use symmetry for the middle integral The function sin3xcos2x is odd about x=π/2? Check: sin(π−x)=sinx, cos(π−x)=−cosx, so sin3(π−x)cos2(π−x)=sin3xcos2x. Actually it's symmetric, not odd. But better: note that sin3xcos2x is an odd function with respect to x=π/2? Let's test: replace x by π−x, the product is unchanged. So it's symmetric. However, we can compute directly using substitution u=cosx:
∫0πsin3xcos2xdx=∫0πsinx(1−cos2x)cos2xdx.
Let u=cosx, du=−sinxdx, limits: x=0→u=1, x=π→u=−1. Then
∫0πsin3xcos2xdx=∫1−1(1−u2)u2(−du)=∫−11(u2−u4)du.
The integrand is even, so
=2∫01(u2−u4)du=2[3u3−5u5]01=2(31−51)=2⋅152=154.
Thus
2∫0πsin3xcos2xdx=158.
- Compute ∫0πsin6xdx Use the reduction formula or known result:
∫0πsin2nxdx=π⋅(2n)!!(2n−1)!!.
For n=3, sin6x has even power, so
∫0πsin6xdx=π⋅6!!5!!=π⋅6⋅4⋅25⋅3⋅1=π⋅4815=165π.
(Check: 5!!=15, 6!!=48, yes.)
- Compute ∫0πcos4xdx Since cos4x is symmetric about π/2, we can also use ∫0πcos4xdx=2∫0π/2cos4xdx. Use the reduction formula for ∫0π/2cos2nxdx=(2n)!!(2n−1)!!⋅2π. …
- TG EAPCET 2023Set eng-2023-05-13-AN1 markMCQQ.∫02x3(2−x)4dx= (A) 105128 (B) 3516 (C) 105256 (D) 3532
›Reveal solutionSolution
Substitute u=2−x and expand; the integral evaluates to 3532.
Setup. Let u=2−x, so x=2−u and dx=−du. The limits map x:0→2 into u:2→0:
∫02x3(2−x)4dx=∫02(2−u)3u4du.
Expand (2−u)3=8−12u+6u2−u3, so the integrand becomes
8u4−12u5+6u6−u7.
Integrate term-by-term from 0 to 2:
[58u5−2u6+76u7−81u8]02.
At u=2: 58(32)−2(64)+76(128)−81(256)=5256−128+7768−32. …
- TG EAPCET 2024Set eng-2024-05-10-FN1 markMCQQ.∫−π/8π/81+e4xsin4(4x)dx= (A) 1283π (B) 2563π (C) 643π (D) 323π
›Reveal solutionSolution
The 1+e4x1 symmetry trick reduces the integral to ∫0π/8sin4(4x)dx=643π.
Apply the symmetric-interval identity. For an even function g,
∫−aa1+e4xg(x)dx=∫0ag(x)dx.
This follows from adding I to its x→−x image: 1+e4x1+1+e−4x1=1. Here g(x)=sin4(4x) is even and a=8π, so
I=∫0π/8sin4(4x)dx.
Evaluate. Substitute u=4x, du=4dx; limits 0→π/2: …
- TG EAPCET 2025Set eng-2025-05-02-FN1 markMCQQ.∫−2π2πsin4xcos6xdx= (A) 1283π (B) 329π (C) 649π (D) 643π
›Reveal solutionSolution
The integral of an even power of sine and cosine over a full period can be reduced using symmetry and the Beta function; the value is 643π, which corresponds to option (D).
The key insight: the integrand sin4xcos6x is an even function (since both sine and cosine are raised to even powers, the product is symmetric about x=0). Also, over [−2π,2π], the function repeats its pattern four times (period π for the product of even powers). So we can simplify the integral to a multiple of an integral over [0,π/2], where the classic Beta-function reduction applies.
- Use symmetry and periodicity. The function f(x)=sin4xcos6x has period π (because sin2x and cos2x have period π, and even powers preserve that). Over [−2π,2π], which is 4 periods of length π, we have
∫−2π2πf(x)dx=4∫0πf(x)dx.
Also, f(x) is even, so ∫0πf(x)dx=2∫0π/2f(x)dx. Thus
∫−2π2πf(x)dx=8∫0π/2sin4xcos6xdx.
- Reduce to a Beta integral. Recall the Beta function identity:
∫0π/2sin2a−1xcos2b−1xdx=21B(a,b)=2Γ(a+b)Γ(a)Γ(b).
Here we have sin4x=sin2⋅2.5−1x? Let's match carefully: we want exponents 2a−1=4 and 2b−1=6, so
2a−1=4⟹a=25,2b−1=6⟹b=27.
Then
∫0π/2sin4xcos6xdx=21B(25,27).
- Evaluate the Beta function using Gamma values.
B(25,27)=Γ(6)Γ(5/2)Γ(7/2).
Recall Γ(n)=(n−1)! for integers, and Γ(1/2)=π.
Γ(5/2)=23⋅21⋅π=43π,
Γ(7/2)=25⋅23⋅21⋅π=815π,
Γ(6)=5!=120.
So
- TG EAPCET 2024Set eng-2024-05-10-AN1 markMCQQ.253∫025π∣cosx−cos3x∣dx= (A) 8 (B) 4 (C) 1 (D) 0
›Reveal solutionSolution
∣cosx−cos3x∣=∣cosx∣∣sinx∣, whose integral over one period π is 34; over 25π it is 3100, and 253⋅3100=4.
Simplifying the integrand.
cosx−cos3x=cosx(1−cos2x)=cosxsin2x.
Since sin2x≥0,
∣cosx−cos3x∣=∣cosx∣sin2x=∣cosx∣∣sinx∣.
Periodicity.
Both ∣cosx∣ and ∣sinx∣ have period π, so the integrand has period π. The interval [0,25π] contains exactly 25 periods.
Integral over one period [0,π].
On [0,π], sinx≥0. Split where cosx changes sign at 2π:
∫0π∣cosx∣sinxdx=∫0π/2cosxsinxdx+∫π/2π−cosxsinxdx. …
- TG EAPCET 2023Set eng-2023-05-14-AN1 markMCQQ.∫369−x+xxdx= (A) 21 (B) 23 (C) 2 (D) 1
›Reveal solutionSolution
This integral is a classic symmetric-invariance problem: using the substitution x→9−x shows the integrand and its complement sum to 1, so the integral over [3,6] is half the interval length, giving 23.
Concept & Intuition
When you see an integral of the form ∫abf(x)+f(a+b−x)f(x)dx, there’s a beautiful trick: the integrand and its “mirror image” add to 1. Here a=3, b=6, so a+b=9. The denominator is 9−x+x, and the numerator is x. If we replace x by 9−x, the numerator becomes 9−x and the denominator stays the same (just swapped order). So the original integrand I(x) and I(9−x) sum to 1. Integrating over a symmetric interval around the midpoint x=4.5 then gives half the length of the interval.
Step-by-step solution
- Define the integral Let
I=∫369−x+xxdx.
- Apply the substitution x→9−u Set u=9−x. Then dx=−du, and when x=3, u=6; when x=6, u=3. So
I=∫63u+9−u9−u(−du)=∫36u+9−u9−udu.
Since u is a dummy variable, rename it x:
I=∫36x+9−x9−xdx.
- Add the two expressions for I We now have two representations:
I=∫369−x+xxdxandI=∫36x+9−x9−xdx.
Adding them:
2I=∫36(9−x+xx+x+9−x9−x)dx.… - TG EAPCET 2024Set eng-2024-05-10-AN1 markMCQQ.If m,l,r,s,n are integers such that, 9>m>l>s>n>r>2 and
[!FORMULA] ∫−ππsinrxcossxdx=4∫−ππsinlxcosrxdx,∫027πsinrxcossxdx=4∫0πsinlxcosrxdx and
[!FORMULA] ∫−2π27πsinlxcosmxdx=0,
then (A) (s−2)(l−2)=mr (B) (s−2)(l+2)=rm+5 (C) (s−2)(s+2)=ln−3 (D) (l−2)(l+2)=ms−5›Reveal solutionSolution
The chain of inequalities leaves only six integer sets, and the symmetry conditions on the trigonometric integrals fix the parities. Checking the four printed relations, only (s−2)(s+2)=log−3 survives — option (C).
The concept first
Two symmetry facts do all the work.
- An odd power of sine kills a symmetric integral. sinx is odd, cosx is even, so sinpxcosqx is an odd function when p is odd, and therefore ∫−ππsinpxcosqxdx=0.
- An odd power of cosine kills the [0,π] integral. Under x↦π−x, sinx is unchanged but cosx↦−cosx; so ∫0πsinpxcosqxdx=0 when q is odd.
Combining: on [−π,π] the integral is non-zero only if both exponents are even, and then
∫−ππsinpxcosqxdx=2∫0πsinpxcosqxdx=4∫0π/2sinpxcosqxdx.
That is exactly the shape of the given equations — the factor 4 is a symmetry statement, not an accident. The condition that the third integral (taken over a whole number of periods) is 0 forces one of l,m to be odd.
Step 1 — List the candidate sets
All five integers lie strictly between 2 and 9, i.e. in {3,4,5,6,7,8}, and are strictly increasing in the order r<n<s<l<m. So we just drop one member of that six-element set:
(r,n,s,l,m)∈{(4,5,6,7,8),(3,5,6,7,8),(3,4,6,7,8),(3,4,5,7,8),(3,4,5,6,8),(3,4,5,6,7)}.
Step 2 — Apply the parity conditions …
- TG EAPCET 2025Set eng-2025-05-02-AN1 markMCQQ.Let m,n,p,q be four positive integers. If ∫02πsinmxcosnxdx=4∫02πsinmxcosnxdx, ∫02πsinpxcosqxdx=0, ∫0πsinrxcosqxdx=0, a=m+n+p and b=m+n+q, then (A) a is even number and b is odd number (B) a is odd number and b is even number (C) Both a and b are even numbers (D) Both a and b are odd numbers
›Reveal solutionSolution
Both a and b are odd numbers — option (D).
Analyse each condition by symmetry.
- ∫02πsinmxcosnxdx=4∫0π/2sinmxcosnxdx requires the integrand to be non-negative with quarter-period symmetry, i.e. m and n are both even.
- ∫02πsinpxcosqxdx=0: under x→2π−x the integral picks up a factor (−1)p, so it vanishes only if p is odd. …
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