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 45 on this concept.
- CBSE 2025Set 65/2/11 markMCQQ.If f(2a−x)=f(x), then ∫02af(x)dx is: (A) ∫02af(2x)dx (B) ∫0af(x)dx (C) 2∫a0f(x)dx (D) 2∫0af(x)dx
›Reveal solutionSolution
The condition f(2a−x)=f(x) implies that the function f(x) is symmetric about the line x=a, which simplifies the definite integral ∫02af(x)dx to 2∫0af(x)dx.
This problem tests your understanding of a fundamental property of definite integrals related to symmetry. The condition f(2a−x)=f(x) is key here. It tells us something profound about the function's behaviour over the interval [0,2a].
Concept and Intuition: Symmetry in Definite Integrals
Imagine the interval [0,2a] on the x-axis. The midpoint of this interval is x=a.
The condition f(2a−x)=f(x) means that the value of the function at any point x is the same as its value at the point 2a−x.
Let's pick a point x1 in the interval [0,a]. Its symmetric counterpart with respect to x=a is x2=2a−x1.
For example, if a=5 and x1=2, then 2a−x1=10−2=8. The condition f(2)=f(8) means the function has the same height at x=2 and x=8. Both points are 3 units away from x=5.
This implies that the graph of f(x) is symmetric about the vertical line x=a.
When a function is symmetric about x=a over the interval [0,2a], the area under the curve from 0 to a must be exactly equal to the area under the curve from a to 2a.
Therefore, the total area from 0 to 2a is simply twice the area from 0 to a. This is the intuition behind the property we are about to derive.
If f(2a−x)=f(x), then ∫02af(x)dx=2∫0af(x)dx.
If f(2a−x)=−f(x), then ∫02af(x)dx=0.
Let's prove this property step-by-step.
- Split the integral: We can split the given integral into two parts at the midpoint a:
∫02af(x)dx=∫0af(x)dx+∫a2af(x)dx
Let's call the second integral $I_2 = \int_{a}^{2a} f(x)\,dx$.2. Apply substitution to the second integral:
To make use of the given condition f(2a−x)=f(x), we perform a substitution in I2.
Let t=2a−x.
Then, differentiating with respect to x, we get dt=−dx.
We also need to change the limits of integration:
* When x=a, t=2a−a=a.
* When x=2a, t=2a−2a=0.
Substituting these into $I_2$:I2=∫a0f(2a−t)(−dt)
- Simplify the substituted integral: Using the property ∫bag(t)dt=−∫abg(t)dt, we can reverse the limits and remove the negative sign:
I2=−∫a0f(2a−t)dt=∫0af(2a−t)dt
- Apply the given condition: We are given that f(2a−x)=f(x). Since t is just a dummy variable, this also means f(2a−t)=f(t). Substituting this into our expression for I2:
I2=∫0af(t)dt
Since the variable of integration is a dummy variable, we can replace $t$ with $x$:I2=∫0af(x)dx
This confirms our intuition that the area from $a$ to $2a$ is the same as the area from $0$ to $a$.5. Combine the results:
Now, substitute this back into our original split integral from Step 1:
∫02af(x)dx=∫0af(x)dx+I2
∫02af(x)dx=∫0af(x)dx+∫0af(x)dx
∫02af(x)dx=2∫0af(x)dx
This matches option (D).
TipThis property is often used in competitive exams. Recognizing the form f(2a−x)=f(x) or f(a−x)=f(x) (for an integral from 0 to a) can save significant time. Always look for symmetry in the integrand and limits.
Watch outDo not confuse f(2a−x)=f(x) with f(−x)=f(x) (an even function) or f(x+T)=f(x) (a periodic function). Each property has specific implications for definite integrals over different intervals.
✓Final answerGiven f(2a−x)=f(x), the value of ∫02af(x)dx is 2∫0af(x)dx.
- CBSE 2026Set 65/3/11 markMCQQ.∫−11(1−∣x∣)dx is equal to: (A) 2∫01(1+x)dx (B) 2∫−10(1+x)dx (C) 0 (D) 2∫−10(1−x)dx
›Reveal solutionSolution
The integral ∫−11(1−∣x∣)dx evaluates to 1. Using symmetry, the integrand is even, so the integral equals 2∫01(1−x)dx, which matches option (B) after a variable substitution.
The key here is the absolute value function ∣x∣. It makes the integrand 1−∣x∣ an even function — symmetric about the y-axis. For any even function f(x), we have the property:
∫−aaf(x)dx=2∫0af(x)dx
This is because the area from −a to 0 is a mirror image of the area from 0 to a. So instead of dealing with the absolute value directly, we can exploit this symmetry to simplify the integral.
Let’s work through it step by step.
- Identify the symmetry. The function f(x)=1−∣x∣ is even because ∣x∣ is even, and subtracting an even function from a constant keeps it even. So:
∫−11(1−∣x∣)dx=2∫01(1−∣x∣)dx
But for x≥0, ∣x∣=x. Therefore:
∫−11(1−∣x∣)dx=2∫01(1−x)dx
- Evaluate the integral directly (to know the target value). Compute:
2∫01(1−x)dx=2[x−2x2]01=2(1−21)=2⋅21=1
So the integral equals 1. Now we check which option also gives 1.
- Examine each option.
- (A) 2∫01(1+x)dx=2[x+2x2]01=2(1+21)=3 — not equal to 1.
- (B) 2∫−10(1+x)dx — let’s evaluate this carefully. For x from −1 to 0, 1+x is positive? Actually at x=−1, 1+(−1)=0; at x=0, 1+0=1. So:
2∫−10(1+x)dx=2[x+2x2]−10=2(0−(−1+21))=2(0−(−21))=2⋅21=1
This matches!- (C) 0 — clearly not 1.
- (D) 2∫−10(1−x)dx — for x from −1 to 0, 1−x ranges from 2 to 1, so:
2∫−10(1−x)dx=2[x−2x2]−10=2(0−(−1−21))=2(0−(−23))=3
Not equal to $1$.Watch outA common mistake is to forget that ∣x∣ changes definition at 0. If you try to integrate 1−∣x∣ from −1 to 1 without splitting, you’ll get the wrong sign. Always split at the point where the absolute value expression changes — here at x=0.
TipNotice that option (B) is actually the same as 2∫01(1−x)dx after substituting u=−x in the integral. Because if x runs from −1 to 0, then u=−x runs from 1 to 0, and 1+x=1−u. So:
2∫−10(1+x)dx=2∫10(1−u)(−du)=2∫01(1−u)du
which is exactly our symmetric form. So (B) is just a disguised version of the correct expression.
✓Final answerThe correct option is (B).
- CBSE 2024Set 65/1/11 markMCQQ.∫abf(x)dx is equal to: (A) ∫abf(a−x)dx (B) ∫abf(a+b−x)dx (C) ∫abf(x−(a+b))dx (D) ∫abf((a−x)+(b−x))dx
›Reveal solutionSolution
The definite integral ∫abf(x)dx remains unchanged if we replace x with a+b−x. This is a fundamental property of definite integrals, making option (B) the correct choice.
The question asks us to identify an equivalent expression for the definite integral ∫abf(x)dx. This involves understanding a key property of definite integrals related to symmetry.
Concept and Intuition: The King Property of Definite Integrals
One of the most useful properties of definite integrals is that the value of the integral remains the same if we replace the variable of integration, x, with a+b−x within the limits [a,b]. This is often called the "King Property" or Property 4 in many textbooks.
Why does this work?
Imagine the interval of integration is [a,b]. The transformation x→a+b−x effectively reflects the variable x about the midpoint of the interval, which is 2a+b.
- If x=a (the lower limit), then a+b−x=a+b−a=b (the upper limit).
- If x=b (the upper limit), then a+b−x=a+b−b=a (the lower limit).
- If x=2a+b (the midpoint), then a+b−x=a+b−2a+b=2a+b (the midpoint itself).
This reflection means that the "shape" of the function being integrated over the interval, when viewed from x or from a+b−x, is essentially the same, just traversed in the opposite direction, which is accounted for by the change in the differential dx.
Let's prove this property using a substitution.
-
Define the integral:
Let I=∫abf(x)dx.
-
Introduce a substitution:
We will use the substitution t=a+b−x. This is the core idea behind this property.
-
Change the limits of integration:
When x=a (the lower limit), t=a+b−a=b.
When x=b (the upper limit), t=a+b−b=a.
-
Change the differential:
Differentiate the substitution t=a+b−x with respect to x:
dxdt=dxd(a+b−x)=0+0−1=−1.
So, dt=−dx, which means dx=−dt.
-
Substitute into the integral:
Now, replace x with a+b−t, dx with −dt, and change the limits from a to b to b to a:
I=∫baf(a+b−t)(−dt).
-
Simplify using properties of definite integrals:
We know that ∫pq−g(t)dt=−∫pqg(t)dt.
So, I=−∫baf(a+b−t)dt.
Also, we know that ∫pqg(t)dt=−∫qpg(t)dt.
Applying this, ∫baf(a+b−t)dt=−∫abf(a+b−t)dt.
Substituting this back into the expression for I:
I=−(−∫abf(a+b−t)dt)=∫abf(a+b−t)dt.
-
Replace the dummy variable:
The value of a definite integral does not depend on the variable of integration. We can replace t with x without changing the value:
I=∫abf(a+b−x)dx.
The fundamental property used here is:
∫abf(x)dx=∫abf(a+b−x)dx
Comparing this result with the given options:
(A) ∫abf(a−x)dx
(B) ∫abf(a+b−x)dx
(C) ∫abf(x−(a+b))dx
(D) ∫abf((a−x)+(b−x))dx
Our derived expression matches option (B).
✓Final answerThe integral ∫abf(x)dx is equal to ∫abf(a+b−x)dx.
- CBSE 2026Set 65/1/11 markMCQQ.The value of ∫−11x2+2∣x∣+1x3dx is (A) 0 (B) log2 (C) 2log2 (D) 21log2
›Reveal solutionSolution
The integrand is an odd function (satisfies f(−x)=−f(x)), so its integral over the symmetric interval [−1,1] vanishes. The value is 0.
When you see an integral over a symmetric interval like [−1,1], the first instinct should be to check whether the integrand has any special symmetry. Two types matter:
- Even function: f(−x)=f(x) for all x. Then ∫−aaf(x)dx=2∫0af(x)dx.
- Odd function: f(−x)=−f(x) for all x. Then ∫−aaf(x)dx=0.
The second property is powerful: if you can show the integrand is odd, the integral is zero immediately, no computation needed. The geometric reason is that the area under the curve from −a to 0 exactly cancels the area from 0 to a.
Let's check our integrand f(x)=x2+2∣x∣+1x3.
Step-by-step verification
-
Compute f(−x).
Substitute −x for x:
f(−x)=(−x)2+2∣−x∣+1(−x)3=x2+2∣x∣+1−x3
Notice that (−x)3=−x3, (−x)2=x2, and crucially ∣−x∣=∣x∣ (the absolute value kills the sign).
-
Compare with f(x).
We have
f(−x)=x2+2∣x∣+1−x3=−x2+2∣x∣+1x3=−f(x)
This is exactly the definition of an odd function.
-
Apply the symmetry property.
Since f(x) is odd and the interval [−1,1] is symmetric about the origin,
∫−11x2+2∣x∣+1x3dx=0
TipWhenever you see x3 (or any odd power of x) in the numerator and even powers or absolute values in the denominator over a symmetric interval, check for odd symmetry first. It saves enormous effort.
Watch outDon't be distracted by the absolute value ∣x∣ in the denominator. The key is that ∣x∣ is an even function, so the entire denominator x2+2∣x∣+1 is even. An odd function (numerator) divided by an even function (denominator) is odd.
✓Final answerThe value is 0, so the correct option is (A).
- CBSE 2024Set 65/3/11 markMCQQ.∫−aaf(x)dx=0, if: (A) f(−x)=f(x) (B) f(−x)=−f(x) (C) f(a−x)=f(x) (D) f(a−x)=−f(x)
›Reveal solutionSolution
The integral of a function over a symmetric interval [−a,a] vanishes if and only if the function is odd, i.e., f(−x)=−f(x). The answer is (B).
Understanding Definite Integral Symmetry
When we integrate a function over an interval symmetric about the origin, [−a,a], the geometry of the function determines whether contributions from the left and right halves reinforce or cancel each other.
The key insight is to split the integral at the center of symmetry and examine what happens when we change variables. For any function f(x), we can write:
∫−aaf(x)dx=∫−a0f(x)dx+∫0af(x)dx
Now let's see what each option implies.
Step-by-step analysis
- Split and substitute in the left integral In the first integral ∫−a0f(x)dx, substitute x=−u. Then dx=−du, and when x=−a, u=a; when x=0, u=0:
∫−a0f(x)dx=∫a0f(−u)(−du)=∫0af(−u)du
Renaming the dummy variable u→x:
∫−a0f(x)dx=∫0af(−x)dx
- Combine the two halves Our original integral becomes:
∫−aaf(x)dx=∫0af(−x)dx+∫0af(x)dx=∫0a[f(−x)+f(x)]dx
- When does this equal zero? The integral vanishes if and only if the integrand is identically zero:
f(−x)+f(x)=0⟺f(−x)=−f(x)
This is precisely the definition of an odd function.
TipGeometrically, an odd function has rotational symmetry about the origin: if you rotate the graph 180° about (0,0), it looks identical. The area under the curve from −a to 0 is the negative of the area from 0 to a, so they cancel.
- Check the other options
- (A) f(−x)=f(x) (even function): The integral becomes ∫0a2f(x)dx, which is generally not zero.
- (C) and (D) involve f(a−x), which relates values within the interval but doesn't create the necessary cancellation across the origin. These conditions don't guarantee symmetry about x=0.
Watch outDon't confuse even/odd symmetry (about the origin) with symmetry about other points like x=a/2. Only odd symmetry about the center of the integration interval guarantees cancellation.
✓Final answerThe correct option is (B): ∫−aaf(x)dx=0 when f(−x)=−f(x).
- CBSE 2026Set V11 markMCQQ.The value of ∫−2π2πsin7xdx(a) 1(b) 0(c) −1(d) 7
›Reveal solutionSolution
An odd function integrated over symmetric limits gives 0; answer (b).
Let g(x)=sin7x. Then
g(−x)=sin7(−x)=(−sinx)7=−sin7x=−g(x),
so g is odd. For any odd function,
∫−aag(x)dx=0.
Hence ∫−π/2π/2sin7xdx=0.
✓Final answer(b) 0
- CBSE 2026Set A1 markMCQQ.∫−ππsin5xdx=(a) 43π(b) 2π(c) 65π(d) 0
›Reveal solutionSolution
Odd function over a symmetric interval integrates to 0.
Since sin(−x)=−sinx, we have sin5(−x)=(−sinx)5=−sin5x, so sin5x is odd. For any odd function f, ∫−aaf(x)dx=0. Therefore
∫−ππsin5xdx=0.
✓Final answer(D) 0.
- CBSE 2026Set ANNUAL1 markMCQQ.Write the value of ∫−aa{f(x)−f(−x)}dx.(a) 0(b) 2f(a)(c) 2f(−a)(d) 2f(0)
›Reveal solutionSolution
g(x)=f(x)−f(−x) is an odd function, so ∫−aag(x)dx=0.
Let g(x)=f(x)−f(−x). Check whether g is odd or even by evaluating g(−x):
g(−x)=f(−x)−f(−(−x))=f(−x)−f(x)=−[f(x)−f(−x)]=−g(x)
Since g(−x)=−g(x), g is an odd function.
A key property of definite integrals states that for any odd function g,
∫−aag(x)dx=0
(intuitively, the contributions from x and −x cancel exactly).
✓Final answerThe correct option is (a) 0.
- CBSE 2026Set ANNUAL1 markQ.Evaluate ∫−11sin5xcos4xdx.
›Reveal solutionSolution
Recognise that the integrand is an odd function; the integral of any odd function over a symmetric interval [−a,a] is always zero.
Let f(x)=sin5xcos4x.
Test for odd/even symmetry:
f(−x)=sin5(−x)cos4(−x)=(−sinx)5(cosx)4=−sin5xcos4x=−f(x)
(using sin(−x)=−sinx so sin5(−x)=−sin5x, and cos(−x)=cosx so cos4(−x)=cos4x.)
So f(x) is an odd function.
Apply the property ∫−aaf(x)dx=0 whenever f is odd:
∫−11sin5xcos4xdx=0
✓Final answer0
- CBSE 2025Set E1 markMCQQ.∫−11sin7xcos13xdx=(a) 0(b) 1(c) 20(d) 6
›Reveal solutionSolution
An odd function integrated over a symmetric interval gives 0.
Let f(x)=sin7xcos13x. Since sin7(−x)=−sin7x (odd power of an odd function) and cos13(−x)=cos13x (even function),
f(−x)=−sin7xcos13x=−f(x),
so f is odd. By the property ∫−aaf(x)dx=0 for an odd f,
∫−11sin7xcos13xdx=0.
✓Final answer(A) 0.
- CBSE 2025Set E1 markMCQQ.∫αβϕ(x)dx+∫βαϕ(x)dx=(a) 2(b) 1(c) 0(d) 2∫αβϕ(x)dx
›Reveal solutionSolution
By the property ∫baϕ=−∫abϕ, the two integrals cancel to 0.
A basic property of definite integrals is ∫βαϕ(x)dx=−∫αβϕ(x)dx. Therefore
∫αβϕ(x)dx+∫βαϕ(x)dx=∫αβϕ(x)dx−∫αβϕ(x)dx=0.
✓Final answer(C) 0.
- CBSE 2025Set E1 markMCQQ.∫−11sin13xcos12xdx=(a) 0(b) 1(c) 21(d) 2
›Reveal solutionSolution
sin13xcos12x is odd, so its integral over [−1,1] is 0.
Let f(x)=sin13xcos12x. Since sin(−x)=−sinx and cos(−x)=cosx:
f(−x)=(−sinx)13(cosx)12=−sin13xcos12x=−f(x),
so f is odd. The integral of an odd function over a symmetric interval [−a,a] is 0:
∫−11sin13xcos12xdx=0.
✓Final answer(A) 0.
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