Q.By using the properties of definite integrals, evaluate the integral ∫0π/2cos2xdx
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 to use the symmetry of cos2x over [0,π/2], or equivalently, the identity cos2x=1−sin2x combined with the property ∫0π/2f(sinx)dx=∫0π/2f(cosx)dx.
Let I=∫0π/2cos2xdx. Using the property ∫0π/2f(sinx)dx=∫0π/2f(cosx)dx, we also have I=∫0π/2sin2xdx.
Adding the two expressions:
2I=∫0π/2(cos2x+sin2x)dx=∫0π/21dx=2π.
Thus I=4π.
The value is 4π.
Using the symmetry property ∫0af(x)dx=∫0af(a−x)dx, we rewrite cos2x as sin2x, add the two forms, and get 2I=∫0π/21dx=2π, so I=4π.
The problem asks us to evaluate ∫0π/2cos2xdx using properties of definite integrals. The direct approach — finding an antiderivative — is straightforward, but the instruction to use properties nudges us toward a more elegant method that builds deeper intuition.
The key property here is the symmetry of the definite integral about the midpoint of the interval. For any function f continuous on [0,a], we have:
∫0af(x)dx=∫0af(a−x)dx
Why does this work? Because as x runs from 0 to a, the quantity a−x runs from a down to 0 — it’s just a reversal of direction. The area under the curve doesn’t care about direction, so the integral stays the same.
Now, apply this to our integral. Let:
I=∫0π/2cos2xdx
Here a=2π. Using the property:
I=∫0π/2cos2(2π−x)dx
But cos(2π−x)=sinx, so:
I=∫0π/2sin2xdx
This is the crucial step: the integral of cos2x from 0 to π/2 equals the integral of sin2x over the same interval.
Now add the two expressions for I:
I+I=∫0π/2cos2xdx+∫0π/2sin2xdx
2I=∫0π/2(cos2x+sin2x)dx
And cos2x+sin2x=1, the most fundamental identity in trigonometry. So:
2I=∫0π/21dx
The integral of 1 from 0 to π/2 is just the length of the interval: 2π−0=2π.
Thus:
2I=2π⇒I=4π
A common mistake is to forget that the property ∫0af(x)dx=∫0af(a−x)dx works only when both limits are the same. Don’t try to apply it blindly to integrals like ∫0πcos2xdx — the symmetry changes because the midpoint shifts.
This trick — writing an integral as the average of itself and its symmetric counterpart — is powerful. It works whenever f(x)+f(a−x) simplifies nicely, especially with trigonometric functions on [0,π/2] or [0,π].
The value of the integral is 4π.
Method: The reflection property ∫0af(x)dx=∫0af(a−x)dx
Replacing x by a−x leaves a definite integral over [0,a] unchanged. Adding the original and reflected forms often produces a trivially integrable sum.
Steps
Step 1: Name the integral and reflect.
Let I=∫0af(x)dx. Apply
∫0af(x)dx=∫0af(a−x)dx.
Step 2: Simplify the reflected integrand.
Use the relevant co-function identities (over [0,2π], sin(2π−x)=cosx and vice-versa), which typically swaps the roles of the functions.
Step 3: Add the two expressions for I.
2I=∫0a[f(x)+f(a−x)]dx; choose the reflection so this sum collapses (e.g. to 1).
Step 4: Integrate the simple sum and halve.
Solve 2I=∫0a(simple)dx for I.
Common Mistakes
Mistake 1: Applying ∫0af(x)dx=∫0af(a−x)dx with mismatched limits.
Why it's wrong: the property needs a lower limit of 0 and the same upper limit a inside f(a−x); using it on, say, ∫0πcos2xdx (where the midpoint differs) gives a wrong reflection. Correct approach: confirm the limits are 0 to a before reflecting.
Mistake 2: Forgetting that cos(2π−x)=sinx, so cos2 becomes sin2.
Why it's wrong: the whole trick relies on the reflected integrand becoming sin2x so that cos2x+sin2x=1. Correct approach: use the co-function identity, add, and get 2I=2π.
Showing the 12 most recent of 22 on this concept.
- 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.
For n=2: ∫0π/2cos4xdx=4!!3!!⋅2π=4⋅23⋅1⋅2π=163π.
So ∫0πcos4xdx=2⋅163π=83π.
Alternatively, use cos4x=83+21cos2x+81cos4x, integrate from 0 to π:
∫0π83dx=83π, the cosine terms integrate to zero. Same result.
-
Sum the parts
I=165π+158+83π.
Convert 83π to sixteenths: 83π=166π.
So
I=165π+166π+158=1611π+158.
Watch outA common mistake is forgetting the factor of 2 from the middle term or misapplying the symmetry for sin3xcos2x — always check parity or use substitution to be safe.
TipFor integrals of sinmxcosnx over [0,π], if either exponent is odd, a u-substitution often works cleanly. For even powers, reduction formulas or double-angle identities are your friends.
✓Final answerThe correct option is (B).
ANSWER: B
- 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. The function f(sinx) is symmetric about x=π/2 because sin(π−x)=sinx. Therefore the integral from 0 to π is twice the integral from 0 to π/2:
∫0πf(sinx)dx=2∫0π/2f(sinx)dx.
Substituting back:
I=2π⋅2∫0π/2f(sinx)dx=π∫0π/2f(sinx)dx.
Watch outA common mistake is to forget the factor of π/2 from the addition step and jump directly to π∫0πf(sinx)dx without halving. Always add the two forms carefully.
TipThe property ∫0axf(x)dx=2a∫0af(x)dx when f(a−x)=f(x) is a powerful shortcut. Here a=π and f(sinx) satisfies the symmetry, so you can write the answer immediately.
✓Final answerThe correct option is (D): π∫0π/2f(sinx)dx.
- 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.
Use substitution u=sinx, du=cosxdx. Then cos2x=1−u2, so cos3x=(1−u2)cosx. The integral becomes:
2∫01u2(1−u2)du=2∫01(u2−u4)du=2[3u3−5u5]01=2(31−51)=2⋅152=154.
- Combine results: Total integral = 0+154=154.
Watch outA common mistake is to think the whole integrand is odd because sinx+cosx looks “odd-ish,” but cosx is even. Always check each term separately.
TipEven functions can be integrated from 0 to a and doubled; odd functions vanish. This saves half the work.
✓Final answerThe correct option is (C).
ANSWER: C
- 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
B(25,27)=12043π⋅815π=32⋅12045π=384045π=2563π.
- Combine with the factor from step 1.
∫0π/2sin4xcos6xdx=21⋅2563π=5123π.
Then the original integral is
∫−2π2πsin4xcos6xdx=8⋅5123π=51224π=643π.
TipA common shortcut: for ∫02πsin2mxcos2nxdx, the result is 2π⋅(2m+2n)!!(2m−1)!!(2n−1)!!, but careful with double factorials and the range. Here the range is 4π, so it's double that.
Watch outA classic mistake is forgetting that the period is π, not 2π, for even powers. If you mistakenly treat the period as 2π, you'd get half the correct value.
✓Final answerThe correct option is (D).
ANSWER: D
- 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.
I=∫0π/15cos5xdx=[5sin5x]0π/15=51sin(3π)=51⋅23=103.
✓Final answer∫−π/15π/151+e5xcos5xdx=103 — option (B).
- 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:
I=41∫0π/2sin4udu=41⋅163π=643π,
using the Wallis value ∫0π/2sin4udu=4⋅23⋅1⋅2π=163π.
✓Final answer∫−π/8π/81+e4xsin4(4x)dx=643π — option (C).
- 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.
The denominators are identical, so the sum of numerators is x+9−x, which cancels the denominator:
2I=∫361dx.
- Evaluate the simple integral
∫361dx=6−3=3.
Hence 2I=3, so I=23.
TipThis trick works whenever the integrand is of the form f(x)+f(a+b−x)f(x) over [a,b]. The result is always 2b−a, independent of f (as long as f is positive and integrable).
Watch outA common mistake is to try direct substitution or partial fractions — that leads to messy algebra. The symmetry method is far cleaner and avoids any heavy computation.
✓Final answerThe correct option is (B).
ANSWER: B
- 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.
- Solve for I.
I=21.
Watch outA common mistake is to assume f is constant. The condition only forces the sum at symmetric points to be 1, not that f itself is constant. For example, f(x)=x works because x+(1−x)=1, and its integral is indeed 21. The method above works for any function satisfying the condition.
TipThis is a classic “symmetric sum” trick: whenever you see f(x)+f(a−x)=c, the integral over [0,a] is 2ca. Here a=1, c=1, so the answer is 21 immediately.
✓Final answerThe correct option is (C).
ANSWER: C
- TG EAPCET 2022Set eng-2022-07-19-AN1 markMCQQ.∫03[sin(3πx)−cos(3πx)]dx= (A) π−6 (B) 0 (C) π−3 (D) π6
›Reveal solutionSolution
Integrating over one full period-related span [0,3]: the sin term contributes π6 and the cos term contributes 0, so the integral is π6 (option D).
∫03[sin(3πx)−cos(3πx)]dx.
Sine part:
∫03sin(3πx)dx=[−π3cos(3πx)]03=−π3(cosπ−cos0)=−π3(−1−1)=π6.
Cosine part:
∫03cos(3πx)dx=[π3sin(3πx)]03=π3(sinπ−sin0)=0.
Therefore
∫03[sin(3πx)−cos(3πx)]dx=π6−0=π6.
✓Final answerπ6 — Option (D).
- 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.
With u=cosx, each piece gives ∫01udu=[32u3/2]01=32. Total =32+32=34.
Full integral and result.
∫025π∣cosx∣∣sinx∣dx=25⋅34=3100.
253∫025π∣cosx−cos3x∣dx=253⋅3100=4.
✓Final answerThe value is 4 — option (B).
- 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.
Combining over a common denominator 35:
351792−355600+353840−351120=35−1088+354832=3532.
✓Final answer∫02x3(2−x)4dx=3532 — option (D).
- 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:
∫0π/2sin4θcos8θdθ=21Γ(7)Γ(25)Γ(29).
With Γ(25)=43π, Γ(29)=16105π, Γ(7)=720:
Γ(7)Γ(25)Γ(29)=72043π⋅16105π=72064315π=10247π.
So the integral is 21⋅10247π=20487π.
4. Combine.
I=8192⋅20487π=4⋅7π=28π.
✓Final answer∫−22x4(4−x2)7/2dx=28π. Correct option: (C).
ANSWER: C
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