Q.Evaluate ∫−11sin5xcos4xdx
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🔒 Start your 14-day free trial to unlock the full solution →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 …
The key idea is the Even Function Property: for an odd function f(x) (i.e., f(−x)=−f(x)), the integral over a symmetric interval [−a,a] is zero.
- Let f(x)=sin5xcos4x.
- Check parity: sin(−x)=−sinx, so sin5(−x)=−sin5x. cos(−x)=cosx, so cos4(−x)=cos4x. …
The integrand sin5xcos4x is an odd function over a symmetric interval [−1,1], so the integral is zero. The value is 0.
Why This Problem Is About Symmetry, Not Computation
If you try to compute ∫−11sin5xcos4xdx by expanding or using substitution, you’ll end up with a messy trigonometric integral. But there’s a much cleaner path: look at the function’s symmetry.
The interval [−1,1] is symmetric about 0. For such intervals, the integral of an odd function is always zero — provided the integral converges (which it does here, since the integrand is continuous). So the real question is: is f(x)=sin5xcos4x odd?
Step-by-Step Reasoning
-
Recall the definitions
A function f(x) is odd if f(−x)=−f(x) for all x in its domain.
A function is even if f(−x)=f(x).
-
Check the parity of each factor
- sin(−x)=−sinx, so sinx is odd.
- cos(−x)=cosx, so cosx is even.
Now raise them to powers:
- (sinx)5: odd power of an odd function → still odd.
- (cosx)4: even power of an even function → still even.
-
Combine the two
The product of an odd function and an even function is odd:
f(−x)=sin5(−x)cos4(−x)=(−sinx)5(cosx)4=−sin5xcos4x=−f(x).
- Apply the symmetric interval property …
Method: Odd/Even Symmetry Over a Symmetric Interval
Use this for ∫−aaf(x)dx: check whether the integrand is odd or even before computing, since odd integrands vanish and even ones halve the work.
Steps
Step 1: Test the parity of the integrand.
Compute f(−x). If f(−x)=−f(x) the function is odd; if f(−x)=f(x) it is even. For sin5xcos4x: sin5(−x)=−sin5x (odd power of an odd function) and cos4(−x)=cos4x (even), so the product is odd.
Step 2: Apply the symmetry rule. …
Common Mistakes
Mistake 1: Grinding out the antiderivative instead of using symmetry.
Why it's wrong: it wastes effort and invites algebra errors when the answer is simply 0. Correct approach: test parity first.
Mistake 2: Mis-judging the parity of the product.
Why it's wrong: sin5x is odd and cos4x is even, so their product is odd (odd × even = odd). Correct approach: multiply the parities correctly. …
Showing the 12 most recent of 22 on this concept.
- 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 2026Set eng-2026-05-11-AN1 markMCQQ.If ∫ecosxe−cosxecosx+e−cosxsinxdx=−21[f(x)+log(ecosx+e−cosx)]+c and f(3π)=21, then the number of points at which f(x) attains the maximum value in [−2π,2π] is (A) 4 (B) 5 (C) 3 (D) 6
›Reveal solutionSolution
Solving the integral gives f(x)=cosx; it attains its maximum (=1) at x=−2π,0,2π — 3 points.
The integrand simplifies as (writing t=cosx, so sinxdx=−dt):
ecosx+e−cosxecosxsinx=2sinx+21⋅ecosx+e−cosxsinx(ecosx−e−cosx).
The second term integrates to −21log(ecosx+e−cosx) (its derivative is exactly that fraction, up to sign). Matching with the given form
−21[f(x)+log(ecosx+e−cosx)]+c,
the first term forces −21f′(x)=2sinx, i.e. f′(x)=−sinx, so
f(x)=cosx+C. …
- TG EAPCET 2026Set eng-2026-05-11-AN1 markMCQQ.Let f:R→R be an odd function and ∫−11x3f′′(x)dx=58. If g(x)=xf(x), g′(1)=38 and ∫01g(x)dx=152, then f(1)= (A) 21 (B) 32 (C) 43 (D) 54
›Reveal solutionSolution
Using integration by parts and the given oddness of f, we reduce the integral condition to an equation involving f(1) and g′(1), then solve to find f(1)=32.
We are told f is odd: f(−x)=−f(x). This implies f(0)=0 and f′ is even, f′′ is odd. The function g(x)=xf(x) is even (product of odd and odd), so g is even. That symmetry will simplify integrals.
We have three pieces of data:
- ∫−11x3f′′(x)dx=58
- g′(1)=38
- ∫01g(x)dx=152
We want f(1).
- Use integration by parts on the first integral. Since f′′ is odd and x3 is odd, their product is even, so
∫−11x3f′′(x)dx=2∫01x3f′′(x)dx=58.
Hence
∫01x3f′′(x)dx=54.
Now integrate by parts: let u=x3, dv=f′′(x)dx, so du=3x2dx, v=f′(x). Then
∫01x3f′′(x)dx=[x3f′(x)]01−∫013x2f′(x)dx.
At x=0, the term vanishes; at x=1, we get 13f′(1)=f′(1). So
54=f′(1)−3∫01x2f′(x)dx.(1)
- Relate g′(1) to f and f′. Since g(x)=xf(x), differentiate:
g′(x)=f(x)+xf′(x).
At x=1,
g′(1)=f(1)+f′(1)=38.(2)
- Use the integral of g.
∫01g(x)dx=∫01xf(x)dx=152.(3)
- Connect the integral in (1) to the known integral (3). Integrate ∫x2f′(x)dx by parts: let u=x2, dv=f′(x)dx, so du=2xdx, v=f(x). Then
∫01x2f′(x)dx=[x2f(x)]01−∫012xf(x)dx.
At x=0, term is 0; at x=1, we get 12f(1)=f(1). So
∫01x2f′(x)dx=f(1)−2∫01xf(x)dx.
Using (3), ∫01xf(x)dx=152, so
∫01x2f′(x)dx=f(1)−2⋅152=f(1)−154.(4)
- Substitute (4) into (1). From (1):
- 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 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. …
- TG EAPCET 2025Set eng-2025-05-04-FN1 markMCQQ.limn→∞n(2n(2n−1)…(n+2)(n+1))1/n= (A) ∫01logxdx (B) ∫01(x+1)log(x+1)dx (C) ∫01log(1+x)dx (D) ∫01xlogxdx
›Reveal solutionSolution
The product is ∏k=1n(n+k); taking n1-th power and dividing by n turns the log into a Riemann sum for ∫01log(1+x)dx. Answer (C).
Rewrite the product
2n(2n−1)⋯(n+2)(n+1)=∏k=1n(n+k).
So the limit is
L=limn→∞n1(∏k=1n(n+k))1/n=limn→∞(∏k=1nnn+k)1/n=limn→∞(∏k=1n(1+nk))1/n.
Take logarithms …
- TG EAPCET 2024Set eng-2024-05-09-FN1 markMCQQ.∫−22x4(4−x2)7dx= (A) 4π (B) 16π (C) 28π (D) 1283π
›Reveal solutionSolution
With the even integrand and the substitution x=2sinθ, the integral reduces to a Beta function. For the value to be a multiple of π the intended power is (4−x2)7/2; evaluating gives 28π. Answer: (C).
Concept
An integral of the form ∫−22x4(4−x2)mdx with m a half-integer becomes a Beta/Gamma expression under x=2sinθ, producing a rational multiple of π. The choices here (4π, π/16, 28π, 3π/128) are all multiples of π, which is only possible when the exponent is 27 (a half-integer), so the integrand is read as x4(4−x2)7/2.
NoteA strict polynomial power (4−x2)7 would integrate to a rational number with no π, inconsistent with every option. The exponent is therefore taken as 27, which the printed options require; the solution below uses that reading and lands on the exam key.
Solution
1. Use symmetry. The integrand is even, so
I=∫−22x4(4−x2)7/2dx=2∫02x4(4−x2)7/2dx.
2. Substitute x=2sinθ, dx=2cosθdθ, with 4−x2=4cos2θ:
x4=16sin4θ,(4−x2)7/2=(4cos2θ)7/2=128cos7θ.
Therefore
I=2∫0π/216sin4θ⋅128cos7θ⋅2cosθdθ=8192∫0π/2sin4θcos8θdθ.
3. Beta function. Using ∫0π/2sin2p−1θcos2q−1θdθ=21B(p,q) with p=25, q=29: …
- 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 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 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 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 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. …
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