Q.Evaluate the definite integral: ∫011+x2dx
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Definite Integral of 1+x21
The function y=1+x21 is a gentle bump that flattens towards zero on both sides. Finding the area under it is exactly where the arctangent appears — because arctanx is the antiderivative of 1+x21.
The core idea
Differentiation and integration undo each other, and
dxd(tan−1x)=1+x21.
So tan−1x is an antiderivative of 1+x21. By the Fundamental Theorem of Calculus, the definite integral over [a,b] is just the difference of the arctangent values at the two ends:
∫ab1+x2dx=tan−1b−tan−1a
Since 1+x21 is defined for every real x, there are never any domain problems — a and b may be negative.
A worked value
∫011+x2dx=tan−11−tan−10=4π−0=4π.
A few standard arctangent values worth knowing: tan−10=0, tan−11=4π, tan−13=3π.
The moment you see 1+x21 inside an integral, your first thought should be "this integrates to tan−1". The more general form is ∫a2+x2dx=a1tan−1ax+C. …
The key idea is that 1+x21 is the derivative of tan−1x, so we can integrate directly without substitution.
Step 1: Recall the standard integral:
∫1+x2dx=tan−1x+C
Step 2: Apply the limits of integration: …
The integral ∫011+x2dx is a standard form that evaluates to arctanx from 0 to 1, giving 4π.
The key here is recognizing that 1+x21 is the derivative of arctanx. This is one of the most fundamental inverse trigonometric integrals, and it appears often in calculus. The integral is already in its simplest form — no substitution is needed because the antiderivative is direct.
Let’s work through it step by step.
- Identify the antiderivative The integral ∫1+x2dx is a standard result:
∫1+x2dx=arctanx+C
This comes from the fact that dxd(arctanx)=1+x21.
- Apply the limits of integration We evaluate the definite integral from 0 to 1:
∫011+x2dx=[arctanx]01=arctan(1)−arctan(0)
- Evaluate the arctan values
- arctan(1)=4π (since tan(π/4)=1)
- arctan(0)=0 (since tan(0)=0) …
Method: Definite integral giving an inverse tangent
Recognise ∫1+x2dx=tan−1x, then evaluate across the limits.
Steps
Step 1: Match the standard form. 1+x21 integrates to tan−1x.
Step 2: Bracket it.
∫ab1+x2dx=[tan−1x]ab. …
Common Mistakes
Mistake 1: Confusing 1+x21 with 1−x21 (arcsine).
Why it's wrong: no square root here, so the antiderivative is tan−1x, not sin−1x. Correct approach: match 1+x2⇒tan−1x.
Mistake 2: Using tan−11=45 (degrees) in a calculus answer. …
Showing the 12 most recent of 16 on this concept.
- TG EAPCET 2026Set eng-2026-05-09-AN1 markMCQQ.∫π/6π/3sin2x(tan4x−cot4x)dx= (A) 81log54 (B) 2tan−1(54) (C) 0 (D) 1
›Reveal solutionSolution
The integral is simplified by successive substitutions u=tanx and v=u4, transforming it into a standard logarithmic integral whose evaluation at symmetric limits results in 0.
Concept and Intuition
When an integral involves a mix of trigonometric functions like sin2x, tanx, and cotx, a highly effective strategy is to express all terms in a common base, typically tanx. This approach is particularly useful when sin2x appears in the denominator, as it can be rewritten using the identity sin2x=1+tan2x2tanx.
The substitution u=tanx then becomes a natural choice. The differential dx transforms as du=sec2xdx=(1+tan2x)dx. Notice how the (1+tan2x) term from the differential often interacts favorably with other parts of the integrand.
After this initial substitution, the integral usually simplifies to a rational function of u. If the powers of u are still high, a further substitution (e.g., v=un) might be necessary to reduce it to a standard integrable form, such as ∫v2−a21dv. Finally, evaluating definite integrals involves substituting the limits. Sometimes, recognizing symmetries in the limits or properties of logarithms can lead to significant cancellations, often resulting in a simple value like zero.
Step-by-step solution
-
Rewrite the integrand using tanx:
The given integral is I=∫π/6π/3sin2x(tan4x−cot4x)dx.
We use the trigonometric identities:
- sin2x=1+tan2x2tanx
- cotx=tanx1
Substitute these into the denominator:
sin2x(tan4x−cot4x)=1+tan2x2tanx(tan4x−tan4x1)
=1+tan2x2tanx(tan4xtan8x−1)=tan3x(1+tan2x)2(tan8x−1)
So the integrand becomes:sin2x(tan4x−cot4x)dx=2(tan8x−1)tan3x(1+tan2x)dx
-
Apply the substitution u=tanx:
Let u=tanx.
Then, the differential du=sec2xdx=(1+tan2x)dx.
This means (1+tan2x)dx=du.
The term sin2x1dx can be conveniently written as 2tanx1+tan2xdx=2u1du.
The term tan4x−cot4x becomes u4−u41=u4u8−1.
Substituting these into the integral:
I=∫u4u8−12u1du=∫2u(u8−1)u4du=∫2(u8−1)u3du
- Change the limits of integration for u: When x=π/6, u=tan(π/6)=31. When x=π/3, u=tan(π/3)=3. The integral now is:
I=∫1/332(u8−1)u3du
-
Apply a second substitution v=u4:
To simplify the denominator u8−1=(u4)2−1=v2−1, let v=u4.
Differentiating with respect to u, we get dv=4u3du, which implies u3du=41dv.
Change the limits of integration for v:
When u=31, v=(31)4=91.
When u=3, v=(3)4=9.
The integral transforms to:
I=∫1/992(v2−1)1(41dv)=81∫1/99v2−11dv
- Evaluate the integral: …
-
- TG EAPCET 2026Set eng-2026-05-10-FN1 markMCQQ.∫10cos2x+cos2x+5dx= (A) 41tan−1(2tanx)+c (B) 81tan−1(2tanx)+c (C) 41tan−1(5tanx)+c (D) 81tan−1(5tanx)+c
›Reveal solutionSolution
Use the identity cos2x=2cos2x−1 to rewrite the denominator entirely in terms of cos2x, then divide numerator and denominator by cos2x to obtain a standard ∫a2+u2du form. The answer is 41tan−1(2tanx)+c.
The key is to notice that the denominator is a quadratic in cos2x once we replace cos2x using the double-angle identity. That lets us factor out cos2x and substitute u=tanx, turning the integral into a familiar arctan form.
- Rewrite cos2x in terms of cos2x Use cos2x=2cos2x−1. The denominator becomes:
10cos2x+(2cos2x−1)+5=12cos2x+4.
So the integral is
∫12cos2x+4dx.
- Factor out the constant
=∫4(3cos2x+1)dx=41∫3cos2x+1dx.
- Divide numerator and denominator by cos2x This is the classic trick for integrals of the form ∫acos2x+bdx:
41∫3+sec2xsec2xdx.
But sec2x=1+tan2x, so the denominator becomes 3+(1+tan2x)=4+tan2x.
Hence
41∫4+tan2xsec2xdx.
- Substitute u=tanx Then du=sec2xdx, and the integral becomes
41∫4+u2du.
- Recognise the standard form …
- TG EAPCET 2025Set eng-2025-05-02-FN1 markMCQQ.0∫2(x+3)(2−x)dx= (A) 825cos−1(51)−46 (B) 825sin−1(51)−46 (C) 2π (D) π
›Reveal solutionSolution
The integrand is a semicircular arc 425−(x+21)2; evaluating gives 825cos−151−46 — option (A).
Complete the square. (x+3)(2−x)=−x2−x+6=425−(x+21)2, so
I=∫02425−(x+21)2dx.
This is a circular arc of radius R=25 centred at x=−21.
Substitute x+21=25sinθ, dx=25cosθdθ. Limits: x=0⇒sinθ=51⇒θ=α=sin−151; x=2⇒θ=2π. The integrand becomes 25cosθ:
I=425∫απ/2cos2θdθ=825[θ+21sin2θ]απ/2.
Evaluate. At 2π: θ=2π, sin2θ=0. At α: cosα=526, so sin2α=2⋅51⋅526=2546. Thus …
- TG EAPCET 2025Set eng-2025-05-02-AN1 markMCQQ.If ∫(x2+9)x2+16dx=371tan−1(16+x2Kx)+c, then K = (A) 37 (B) 37 (C) 73 (D) 73
›Reveal solutionSolution
K=37 — option (A).
Use the standard result
∫(x2+a2)x2+b2dx=ab2−a21tan−1(ax2+b2xb2−a2)+c. …
- TG EAPCET 2025Set eng-2025-05-03-AN1 markMCQQ.∫−111−x2log2−log(1+x)dx= (A) 8πlog2 (B) −2πlog2 (C) −4πlog2 (D) 2πlog2
›Reveal solutionSolution
The substitution x=sinθ collapses the surd, and a symmetry argument reduces the problem to the standard ∫0π/2logcosθdθ=−2πlog2, giving 2πlog2. Answer: (D).
Substitute x=sinθ (dx=cosθdθ, 1−x2=cosθ≥0 on [−2π,2π]):
I=∫−π/2π/2(log2−log(1+sinθ))dθ=πlog2−J,J=∫−π/2π/2log(1+sinθ)dθ.
Evaluate J by symmetry. Replacing θ→−θ gives J=∫−π/2π/2log(1−sinθ)dθ. Adding,
2J=∫−π/2π/2log(1−sin2θ)dθ=∫−π/2π/2log(cos2θ)dθ=2∫−π/2π/2logcosθdθ,
so …
- TG EAPCET 2025Set eng-2025-05-03-FN1 markMCQQ.∫−111−x2log2−log(1+x)dx= (A) −4πlog2 (B) 8πlog2 (C) 2πlog2 (D) −2πlog2
›Reveal solutionSolution
Splitting the log and using ∫−111−x2log(1+x)dx=−πlog2 gives 2πlog2 — option (C).
Solution.
- Split:
I=∫−111−x2log2−log(1+x)dx=log2∫−111−x2dx−J∫−111−x2log(1+x)dx.
-
First integral: ∫−111−x2dx=[arcsinx]−11=π, so the first term is πlog2.
-
For J, put x=cosθ (dx=−sinθdθ, 1−x2=sinθ, θ:π→0):
J=∫0πlog(1+cosθ)dθ.
- Use 1+cosθ=2cos22θ: …
- TG EAPCET 2025Set eng-2025-05-04-AN1 markMCQQ.If ∫0π/2tan14(2x)dx=2[∑n=17f(n)−4π], then f(n)= (A) n−1(−1)n (B) 2n+1(−1)n (C) 2n−1(−1)n+1 (D) n+1(−1)n+1
›Reveal solutionSolution
The integral is transformed via the substitution t=tan(x/2), turning it into a rational integral that expands into an alternating series; matching the given form shows f(n)=2n−1(−1)n+1, which is option (C).
We start with the integral
I=∫0π/2tan14(2x)dx.
The presence of tan(x/2) strongly suggests the standard tangent half-angle substitution: let
t=tan(2x),so thatx=2arctant,dx=1+t22dt.
When x=0, t=0; when x=π/2, t=tan(π/4)=1.
Thus
I=∫01t14⋅1+t22dt=2∫011+t2t14dt.
Now the integrand is a rational function. Since the denominator is 1+t2, we can perform polynomial division or use the geometric series expansion for ∣t∣<1 (valid on [0,1] except at the endpoint, but the integral converges). Write
1+t2t14=t14⋅1+t21=t14∑k=0∞(−1)kt2k=∑k=0∞(−1)kt14+2k.
Integrating termwise from 0 to 1 gives
∫011+t2t14dt=∑k=0∞(−1)k14+2k+11=∑k=0∞2k+15(−1)k.
So
I=2∑k=0∞2k+15(−1)k.
The problem states that
I=2[∑n=17f(n)−4π].
We need to relate the infinite series to a finite sum minus π/4. Recall the Leibniz series for π/4:
4π=∑m=0∞2m+1(−1)m.
Our series starts at k=0 with denominator 2k+15=2(k+7)+1. Let m=k+7, then k=m−7 and when k=0, m=7. So
∑k=0∞2k+15(−1)k=∑m=7∞2m+1(−1)m−7=(−1)−7∑m=7∞2m+1(−1)m.
Since (−1)−7=−1 (because (−1)7=−1), we have
∑k=0∞2k+15(−1)k=−∑m=7∞2m+1(−1)m.
Now the full Leibniz series is
4π=∑m=0∞2m+1(−1)m=∑m=062m+1(−1)m+∑m=7∞2m+1(−1)m.
Thus
∑m=7∞2m+1(−1)m=4π−∑m=062m+1(−1)m.
Substituting back,
∑k=0∞2k+15(−1)k=−(4π−∑m=062m+1(−1)m)=∑m=062m+1(−1)m−4π.
Therefore
- TG EAPCET 2025Set eng-2025-05-04-FN1 markMCQQ.If ∫02πtan14(2x)dx=2[∑n=17f(n)−4π], then f(n)= (A) n+1(−1)n+1 (B) 2n−1(−1)n+1 (C) n−1(−1)n (D) 2n+1(−1)n
›Reveal solutionSolution
The integral reduces to a sum of alternating reciprocals of odd numbers; comparing forms gives f(n)=2n−1(−1)n+1, which is option (B).
The problem asks you to match a definite integral to a given summation form. The integral has a high power of tan(x/2) — that’s a strong hint to use the substitution t=tan(x/2), which turns trigonometric integrals into rational ones. Once you do that, the integral becomes a standard rational function that expands into an alternating series of odd reciprocals.
Let’s walk through it.
- Substitution Put t=tan2x. Then x=2tan−1t, so dx=1+t22dt. When x=0, t=0; when x=2π, t=tan4π=1. The integral becomes
I=∫0π/2tan14(2x)dx=∫01t14⋅1+t22dt.
- Rational function expansion We now have
I=2∫011+t2t14dt.
Since the degree of the numerator (14) is higher than the denominator’s (2), we divide. But there’s a cleaner trick: write
1+t2t14=t12−t10+t8−t6+t4−t2+1−1+t21.
Check: multiply (1+t2) by the polynomial t12−t10+⋯+1; you get t14+1, so subtracting 1+t21 recovers the original fraction. This alternating pattern comes from the geometric series formula:
1+t21=1−t2+t4−t6+⋯(for ∣t∣<1),
rearranged.
- Integrate term by term
I=2∫01(t12−t10+t8−t6+t4−t2+1−1+t21)dt.
Each power integrates to k+11 from 0 to 1, and ∫011+t2dt=4π. So
I=2[131−111+91−71+51−31+1−4π].
- Match to the given form The problem states
- TG EAPCET 2024Set eng-2024-05-09-AN1 markMCQQ.
[!FORMULA] ∫9cos22x+16sin22xdx
(A) 251tan−1(43sec22x)+c (B) 251tan−1(34sec22x)+c (C) 241tan−1(43tan2x)+c (D) 241tan−1(34tan2x)+c›Reveal solutionSolution
Divide by cos22x, substitute t=tan2x: result 241tan−1(34tan2x)+c — option (D).
Divide numerator and denominator by cos22x:
∫9cos22x+16sin22xdx=∫9+16tan22xsec22xdx.
Let t=tan2x⇒dt=2sec22xdx, so sec22xdx=2dt:
=21∫9+16t2dt=21⋅161∫(43)2+t2dt.
Apply ∫a2+t2dt=a1tan−1at with a=43: …
- TG EAPCET 2024Set eng-2024-05-10-FN1 markMCQQ.∫(tan2x+44tan4x+3tan2x−1)dx= (A) 4tanx−417tan−1(4tanx)+c (B) 4tanx−417tan−1(2tanx)+c (C) 4tanx−217tan−1(2tanx)+c (D) 2tanx−217tan−1(2tanx)+c
›Reveal solutionSolution
The integral simplifies by polynomial division of the numerator by the denominator (in terms of u=tanx), leading to a simple polynomial term plus a standard arctangent integral. The result matches option (B).
We are asked to integrate
∫tan2x+44tan4x+3tan2x−1dx.
Concept and intuition:
The integrand is a rational function of tanx. When the numerator’s degree is higher than the denominator’s, we perform polynomial long division (in the variable u=tanx) to rewrite the fraction as a polynomial plus a proper rational remainder. The polynomial part integrates easily, and the remainder becomes a constant times u2+a21, whose integral is an arctangent.
- Substitute u=tanx. Then du=sec2xdx=(1+tan2x)dx=(1+u2)dx, so dx=1+u2du. The integral becomes
∫u2+44u4+3u2−1⋅1+u2du.
- Perform polynomial division of 4u4+3u2−1 by u2+4.
- Divide 4u4 by u2 gives 4u2. Multiply: 4u2(u2+4)=4u4+16u2. Subtract from numerator: (4u4+3u2−1)−(4u4+16u2)=−13u2−1.
- Now divide −13u2 by u2 gives −13. Multiply: −13(u2+4)=−13u2−52. Subtract: (−13u2−1)−(−13u2−52)=51. So
u2+44u4+3u2−1=4u2−13+u2+451.
- Rewrite the integral using this division:
∫(4u2−13+u2+451)1+u2du.
This splits into three integrals:
∫1+u24u2du−∫1+u213du+∫(u2+4)(1+u2)51du.
- Simplify the first integral:
1+u24u2=4−1+u24.
So
∫1+u24u2du=∫4du−∫1+u24du=4u−4tan−1u.
- Second integral is straightforward:
∫1+u213du=13tan−1u.
- Third integral requires partial fractions. Write
(u2+4)(1+u2)51=u2+4Au+B+1+u2Cu+D.
Multiply through by (u2+4)(1+u2):
51=(Au+B)(1+u2)+(Cu+D)(u2+4).
Expand:
Au+Au3+B+Bu2+Cu3+4Cu+Du2+4D.
Group powers:
- u3: A+C=0
- u2: B+D=0
- u1: A+4C=0
- u0: B+4D=51
From A+C=0 and A+4C=0, subtract: (A+4C)−(A+C)=3C=0⇒C=0, then A=0.
From B+D=0 and B+4D=51, subtract: (B+4D)−(B+D)=3D=51⇒D=17, then B=−17.
So
(u2+4)(1+u2)51=u2+4−17+1+u217.
- Integrate the third part: …
- TG EAPCET 2024Set eng-2024-05-11-FN1 markMCQQ.∫5π103πsec2x+(tan2022x−1)(sec2x−1)dx= (A) 20π (B) 52π (C) 203π (D) 53π
›Reveal solutionSolution
The integrand simplifies dramatically using sec2x−1=tan2x and a clever substitution t=tanx, turning the integral into a standard arctangent form; the value is 20π, so the correct option is (A).
Concept & Intuition
The integral looks messy with tan2022x, but that huge exponent is a red herring. The key is to notice that sec2x−1=tan2x, so the denominator becomes sec2x+(tan2022x−1)tan2x. This simplifies to sec2x+tan2024x−tan2x. But sec2x−tan2x=1, so the whole denominator collapses to 1+tan2024x. That’s a clean, symmetric form. Then the substitution t=tanx turns the integral into ∫1+t2024dt, with limits that are reciprocals of each other. That symmetry lets us use the identity ∫a1/a1+tndt=2nπ for a>0, giving the answer directly.
Step-by-step solution
- Simplify the denominator Recall sec2x−1=tan2x. The denominator is
sec2x+(tan2022x−1)(sec2x−1)=sec2x+(tan2022x−1)tan2x.
Expand:
sec2x+tan2024x−tan2x.
Since sec2x−tan2x=1, this becomes
1+tan2024x.
So the integral is
I=∫π/53π/101+tan2024xdx.
- Substitute t=tanx Then dt=sec2xdx, but we have dx alone. Write dx=sec2xdt=1+t2dt. Limits: when x=π/5, t=tan(π/5); when x=3π/10, t=tan(3π/10). Note that tan(3π/10)=tan(π/2−π/5)=cot(π/5)=tan(π/5)1. Let a=tan(π/5)>0. Then the upper limit is 1/a. So
I=∫a1/a1+t20241⋅1+t2dt.
- Use a symmetry trick Consider the substitution u=1/t. Then dt=−du/u2, and 1+t2024 becomes 1+u−2024=u2024u2024+1. Also 1+t2=1+1/u2=u2u2+1. The integrand transforms:
1+t20241⋅1+t21dt=u2024u2024+11⋅u2u2+11⋅(−u2du)=−u2024+1u2024⋅u2+1u2⋅u21du.
Simplify: u2 cancels, leaving
−u2024+1u2024⋅u2+11du=−1+u20241⋅u2+1u2024du.
That’s not obviously simpler. Instead, a better trick: add the original integral to its u-substituted version.
- Add the integral to its reciprocal transform Let I=∫a1/a(1+t2024)(1+t2)dt. Make the substitution t=1/u in I:
I=∫1/aa(1+u−2024)(1+u−2)1⋅(−u2du)=∫a1/a(1+u2024)(1+u2)u2024du.
So we have two expressions for I:
- TG EAPCET 2023Set eng-2023-05-12-AN1 markMCQQ.∫25x−25−xdx= (A) π (B) 2π (C) 23π (D) 4π
›Reveal solutionSolution
This integral is a classic "King's property" problem: substituting x↦7−x reveals symmetry, turning the sum of two identical integrals into a simple constant, giving the result 23π. The correct option is (C).
The key insight is that the integrand has a built-in symmetry: the numerator's 5−x and denominator's x−2 swap roles when we reflect the interval about its midpoint. This is a perfect setup for the King's property of definite integrals:
∫abf(x)dx=∫abf(a+b−x)dx.
Here a=2, b=5, so a+b=7. The trick is to add the original integral to its transformed version; the sum simplifies dramatically, giving twice the integral equals a simple constant.
- Set up the integral and apply the substitution. Let
I=∫25x−25−xdx.
Use the substitution x↦7−x (since 2+5=7). Then dx↦−dx, and the limits swap: when x=2, 7−x=5; when x=5, 7−x=2. So
I=∫52(7−x)−25−(7−x)(−dx)=∫255−xx−2dx.
Notice the numerator and denominator have swapped places.
- Add the two forms of I. We now have two expressions for the same integral:
I=∫25x−25−xdxandI=∫255−xx−2dx.
Adding them:
2I=∫25(x−25−x+5−xx−2)dx.
- Simplify the sum inside the integral. Combine the two fractions over a common denominator:
x−25−x+5−xx−2=x−25−x(5−x)+(x−2)=(x−2)(5−x)3.
So
2I=∫25(x−2)(5−x)3dx.
- Evaluate the resulting integral. The expression (x−2)(5−x) is a quadratic that opens downward. Complete the square:
(x−2)(5−x)=−x2+7x−10=−(x2−7x+449)+49=(23)2−(x−27)2.
Hence
2I=3∫25(23)2−(x−27)2dx. …
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