Q.Evaluate the definite integral: ∫−11(x+1) dx
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 that the definite integral of a sum can be split, and the integral of an odd function over a symmetric interval is zero.
Step 1: Split the integral:
∫−11(x+1)dx=∫−11xdx+∫−111dx
Step 2: The function x is odd, and the interval [−1,1] is symmetric about zero, so:
∫−11xdx=0
Step 3: The integral of the constant 1 over [−1,1] is the length of the interval:
∫−111dx=1−(−1)=2
Step 4: Adding the results:
0+2=2
The value is 2.
The integral ∫−11(x+1)dx equals 2. This is found by using the symmetry of the odd part (x) and the even part (1) over a symmetric interval, or by direct antiderivative evaluation.
The key insight here is that the interval [−1,1] is symmetric about 0. When you have a sum of functions, you can often break the integral into parts and use symmetry to simplify calculations. The function x+1 is not purely odd or even, but it is the sum of an odd function (x) and an even function (1). Over a symmetric interval [−a,a], the integral of an odd function is zero, while the integral of an even function is twice the integral from 0 to a. This saves you from having to compute the antiderivative directly, though that also works perfectly.
Let’s go through it step by step.
- Separate the integral into two parts
∫−11(x+1)dx=∫−11xdx+∫−111dx
This is valid because the integral of a sum is the sum of the integrals.
- Handle the odd part: ∫−11xdx The function f(x)=x is odd, meaning f(−x)=−f(x). For any odd function integrated over a symmetric interval [−a,a], the result is zero.
∫−11xdx=0
A quick check: the antiderivative of x is 2x2, and evaluating from −1 to 1 gives 212−2(−1)2=21−21=0. Same result.
- Handle the even part: ∫−111dx The constant function g(x)=1 is even, since g(−x)=g(x). For an even function over [−a,a], the integral equals twice the integral from 0 to a:
∫−111dx=2∫011dx
Now ∫011dx is just the length of the interval from 0 to 1, which is 1. So:
2×1=2
- Combine the results
∫−11(x+1)dx=0+2=2
A common mistake is to forget that the constant 1 is even and treat it like an odd function. Another pitfall is incorrectly applying symmetry when the interval is not symmetric — but here it is, so we’re safe.
If you prefer the direct antiderivative method, it’s just as straightforward:
∫(x+1)dx=2x2+x
Evaluating from −1 to 1:
(212+1)−(2(−1)2+(−1))=(21+1)−(21−1)=23−(−21)=23+21=2
Same answer, confirming our symmetry approach.
The value of the definite integral is 2.
Method: Evaluate a definite integral by the Fundamental Theorem of Calculus
For ∫abf(x)dx, find any antiderivative F, then compute F(b)−F(a) — no constant of integration needed.
Steps
Step 1: Integrate term by term to get an antiderivative. For a linear integrand x+1, use the power rule: F(x)=2x2+x.
Step 2: Write the evaluation bracket.
∫ab(x+1)dx=[2x2+x]ab.
Step 3: Substitute the upper limit, then the lower, and subtract.
F(b)−F(a), being careful with signs when the lower limit is negative.
Step 4: Simplify to a number. The definite integral is a value, not a function, and needs no +C.
Common Mistakes
Mistake 1: Adding +C to a definite integral.
Why it's wrong: the constant cancels in F(b)−F(a). Correct approach: drop C for definite integrals.
Mistake 2: Sign slip at a negative lower limit.
Why it's wrong: at x=−1, 2(−1)2+(−1)=21−1=−21; subtracting this adds 21. Correct approach: compute F(−1) fully, then subtract with its sign.
Mistake 3: Assuming "symmetry" makes it zero.
Why it's wrong: x+1 is not an odd function about 0 (the +1 is even), so the integral is not 0. Correct approach: split ∫−11xdx=0 but ∫−111dx=2, giving 2.
Showing the 12 most recent of 22 on this concept.
- TG EAPCET 2023Set eng-2023-05-14-FN1 markMCQQ.∫−11x∣x∣dx= (A) 1 (B) 21 (C) 0 (D) 32
›Reveal solutionSolution
The integral of an odd function over a symmetric interval is zero. Since x∣x∣ is odd, the definite integral from −1 to 1 is 0.
The key idea here is symmetry. When you integrate an odd function over an interval symmetric about zero, the positive and negative contributions cancel perfectly. The function f(x)=x∣x∣ is odd because f(−x)=(−x)∣−x∣=−x∣x∣=−f(x). So instead of doing any messy piecewise integration, we can immediately see the result.
Let’s verify this step by step to be thorough.
-
Understand the function
The absolute value makes the function piecewise:
- For x≥0, ∣x∣=x, so x∣x∣=x⋅x=x2.
- For x<0, ∣x∣=−x, so x∣x∣=x⋅(−x)=−x2. So f(x)={−x2,x2,x<0x≥0. This confirms it’s odd: the graph for negative x is the mirror image (with opposite sign) of the graph for positive x.
-
Split the integral at the symmetry point
Since the function changes definition at x=0, we write:
∫−11x∣x∣dx=∫−10(−x2)dx+∫01x2dx.
-
Evaluate each piece
- For the left part: ∫−10−x2dx=−[3x3]−10=−(0−3(−1)3)=−(0+31)=−31.
- For the right part: ∫01x2dx=[3x3]01=31−0=31.
-
Add the results
−31+31=0.
TipRecognizing odd/even symmetry saves time. For any odd function f (i.e., f(−x)=−f(x)), ∫−aaf(x)dx=0 automatically. This is a classic shortcut for symmetric integrals.
Watch outA common mistake is to forget the sign change for negative x when dealing with absolute values. Always check the piecewise definition before integrating.
✓Final answerThe correct option is (C).
ANSWER: C
-
- 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 2021Set eng-2021-08-04-FN1 markMCQQ.
[!FORMULA] ∫−111+x2log(1+x)dx=∫011+x2log(1+x)dx+∫01f(x)dx then f(x)=
(A) 1+x2log(1+x) (B) −1+x2log(1+x) (C) 1+x2log(1−x) (D) 0›Reveal solutionSolution
The key idea is to split the integral at 0 and then use the substitution x→−x on the negative half to rewrite it as an integral from 0 to 1; the function f(x) turns out to be 1+x2log(1−x), which is option (C).
The problem gives you a split of the original integral from −1 to 1 into two parts: one from −1 to 0 and one from 0 to 1. The second part is already written as ∫011+x2log(1+x)dx. The first part, ∫−101+x2log(1+x)dx, is what needs to be transformed into ∫01f(x)dx. So we need to find f(x) such that
∫−101+x2log(1+x)dx=∫01f(x)dx.
The natural way to convert an integral over a negative interval to one over a positive interval is a change of variable that flips the limits. Let’s work through it.
- Set up the substitution. On the interval [−1,0], let x=−t. Then when x=−1, t=1; when x=0, t=0. Also dx=−dt. The integral becomes
∫−101+x2log(1+x)dx=∫101+t2log(1−t)(−dt)=∫011+t2log(1−t)dt.
The minus sign from dx=−dt flips the limits back to 0 to 1, and x2=t2 so the denominator is unchanged.
- Identify f(x). The variable of integration is a dummy, so rename t back to x. We have
∫−101+x2log(1+x)dx=∫011+x2log(1−x)dx.
Therefore, the function f(x) that makes the original equation hold is
f(x)=1+x2log(1−x).
Watch outA common mistake is to forget the sign from dx=−dt or to mishandle the limits. Always check: substituting x=−t gives dx=−dt, and the limits reverse; the two negatives (one from dt, one from swapping limits) cancel cleanly.
TipThis trick — splitting an integral over a symmetric interval and substituting x→−x on the negative part — is a standard technique for integrals of odd/even functions or functions with logarithmic singularities. Here it reveals that the original integral from −1 to 1 equals ∫011+x2log(1+x)+log(1−x)dx, which simplifies further using log(1−x2).
✓Final answerThe correct option is (C): f(x)=1+x2log(1−x).
- 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
logL=limn→∞n1∑k=1nlog(1+nk)=∫01log(1+x)dx.
This is exactly option (C). (Evaluating, ∫01log(1+x)dx=2log2−1, so L=e4.)
✓Final answerlogL=∫01log(1+x)dx — 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 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 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 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 2022Set eng-2022-07-19-FN1 markMCQQ.∫02af(x)dx= (A) 2∫0af(x)dx (B) ∫0a(f(x)+f(x+a))dx (C) 0 (D) ∫02af(2a+x)dx
›Reveal solutionSolution
The key idea is to split the integral at x=a and use a substitution x=a+t to relate the two halves. The correct answer is ∫02af(x)dx=∫0a(f(x)+f(x+a))dx, which is option (B).
The question asks for a general property of definite integrals over an interval of length 2a. This is a standard result often used in problems involving periodic or symmetric functions, but it holds for any integrable function f. The trick is to break the interval into two equal halves and then shift the second half back to start at 0.
- Split the integral at the midpoint. Write the integral from 0 to 2a as the sum of two integrals:
∫02af(x)dx=∫0af(x)dx+∫a2af(x)dx.
This is always valid because the limits are contiguous.
- Change variable in the second integral. In ∫a2af(x)dx, let x=a+t. Then dx=dt, and when x=a, t=0; when x=2a, t=a. So
∫a2af(x)dx=∫0af(a+t)dt.
Since the variable of integration is dummy, we can rename t back to x:
∫a2af(x)dx=∫0af(x+a)dx.
- Combine the two pieces. Putting it together:
∫02af(x)dx=∫0af(x)dx+∫0af(x+a)dx=∫0a(f(x)+f(x+a))dx.
This matches option (B) exactly.
Watch outA common mistake is to think the answer is 2∫0af(x)dx (option A). That would only be true if f(x)=f(x+a) for all x in [0,a], i.e., if f is periodic with period a. The problem gives no such condition, so (A) is not generally correct.
TipThis property is extremely useful: whenever you see an integral from 0 to 2a, try splitting and shifting. It often simplifies problems where f(x) and f(x+a) have a known relationship, like f(x)+f(x+a)=constant.
Now check the other options briefly:
- Option (C) says the integral is 0, which is false for a general function (e.g., f(x)=1 gives 2a=0).
- Option (D) says ∫02af(2a+x)dx. Let u=2a+x, then dx=du, limits x=0→u=2a, x=2a→u=4a, so this equals ∫2a4af(u)du, which is not generally equal to the original integral.
✓Final answerThe correct option is (B): ∫02af(x)dx=∫0a(f(x)+f(x+a))dx.
- TG EAPCET 2023Set eng-2023-05-12-FN1 markMCQQ.If f is defined on R such that f(x)f(−x)=9, then ∫−23233+f(x)dx= (A) 351 (B) 349 (C) 346 (D) 646
›Reveal solutionSolution
Using the symmetry f(x)f(−x)=9 together with the substitution x→−x, the integrand collapses to a constant. The paired integral gives 2I=346, so I=646.
Setting up the symmetry. Let
I=∫−23233+f(x)dx.
Applying the substitution x→−x (which leaves the limits −23 to 23 unchanged) gives an equal value:
I=∫−23233+f(−x)dx.
Using the given relation. Since f(x)f(−x)=9, we have f(−x)=f(x)9. Substituting,
I=∫−23233+f(x)9dx=∫−23233f(x)+9f(x)dx=∫−23233[3+f(x)]f(x)dx.
Adding the two forms of I.
2I=∫−2323[3+f(x)1+3[3+f(x)]f(x)]dx=∫−23233[3+f(x)]3+f(x)dx=∫−232331dx.
The integrand is now the constant 31 over an interval of length 46:
2I=31×46=346⇒I=646.
✓Final answer∫−23233+f(x)dx=646 — option (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 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):
54=f′(1)−3(f(1)−154).
Simplify:
54=f′(1)−3f(1)+54.
Cancel 54 from both sides, giving
0=f′(1)−3f(1)⇒f′(1)=3f(1).(5)
- Combine with (2) to solve for f(1). From (2): f(1)+f′(1)=38. Substitute f′(1)=3f(1):
f(1)+3f(1)=38⇒4f(1)=38⇒f(1)=32.
TipThe cancellation of 54 is not a coincidence — it’s forced by the consistency of the given data. This is a neat check that the numbers were chosen to work out cleanly.
Watch outA common mistake is forgetting that f is odd, which makes x3f′′(x) even, so the integral from −1 to 1 is twice the integral from 0 to 1. Without this, the factor of 2 is lost and the answer changes.
✓Final answerThe correct option is (B).
ANSWER: B
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