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JEE Main 2019
Definite Integration
Definite Integration
Hard

Question

The value of the integral π4π4x+π42cos2xdx\int\limits_{ - {\pi \over 4}}^{{\pi \over 4}} {{{x + {\pi \over 4}} \over {2 - \cos 2x}}dx} is :

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Solution

Key Concepts and Formulas

  • King's Property of Definite Integrals: For an integral with limits [a,b][a, b], the following property holds: abf(x)dx=abf(a+bx)dx\int_a^b f(x) dx = \int_a^b f(a+b-x) dx This property is particularly useful for integrals with symmetric limits or when the integrand simplifies upon the substitution xa+bxx \to a+b-x.
  • Algebraic Manipulation of Integrals: If we have two forms of the same integral, say I=abf(x)dxI = \int_a^b f(x) dx and I=abg(x)dxI = \int_a^b g(x) dx, we can add or subtract them: 2I=ab(f(x)+g(x))dx2I = \int_a^b (f(x) + g(x)) dx or 0=ab(f(x)g(x))dx0 = \int_a^b (f(x) - g(x)) dx.
  • Trigonometric Identity: The double angle formula for cosine in terms of tangent: cos(2x)=1tan2x1+tan2x\cos(2x) = \frac{1 - \tan^2 x}{1 + \tan^2 x}
  • Standard Integral Formula: 1a2+x2dx=1atan1(xa)+C\int \frac{1}{a^2 + x^2} dx = \frac{1}{a} \tan^{-1}\left(\frac{x}{a}\right) + C More generally, for a2+u2a^2+u^2: 1a2+u2du=1atan1(ua)+C\int \frac{1}{a^2 + u^2} du = \frac{1}{a} \tan^{-1}\left(\frac{u}{a}\right) + C

Step-by-Step Solution

Let the given integral be II. I=π4π4x+π42cos2xdx(1)I = \int\limits_{ - {\pi \over 4}}^{{\pi \over 4}} {{{x + {\pi \over 4}} \over {2 - \cos 2x}}dx} \quad \cdots (1)

Step 1: Apply King's Property We use the property abf(x)dx=abf(a+bx)dx\int_a^b f(x) dx = \int_a^b f(a+b-x) dx. Here, a=π4a = -\frac{\pi}{4} and b=π4b = \frac{\pi}{4}. So, a+b=π4+π4=0a+b = -\frac{\pi}{4} + \frac{\pi}{4} = 0. Thus, we replace xx with a+bx=0x=xa+b-x = 0-x = -x in the integrand. The denominator involves cos(2x)\cos(2x), and since cos(2(x))=cos(2x)=cos(2x)\cos(2(-x)) = \cos(-2x) = \cos(2x), the denominator remains unchanged. The numerator changes from x+π4x + \frac{\pi}{4} to (x)+π4(-x) + \frac{\pi}{4}. I=π4π4(x)+π42cos(2(x))dxI = \int\limits_{ - {\pi \over 4}}^{{\pi \over 4}} {{{(-x) + {\pi \over 4}} \over {2 - \cos (2(-x))}}dx} I=π4π4x+π42cos2xdx(2)I = \int\limits_{ - {\pi \over 4}}^{{\pi \over 4}} {{{-x + {\pi \over 4}} \over {2 - \cos 2x}}dx} \quad \cdots (2) Reasoning: This step is crucial for simplifying the numerator. By creating a second form of the integral, we can combine it with the original integral to eliminate the xx term in the numerator.

Step 2: Combine the two forms of the integral Add equation (1) and equation (2): I+I=π4π4x+π42cos2xdx+π4π4x+π42cos2xdxI + I = \int\limits_{ - {\pi \over 4}}^{{\pi \over 4}} {{{x + {\pi \over 4}} \over {2 - \cos 2x}}dx} + \int\limits_{ - {\pi \over 4}}^{{\pi \over 4}} {{{-x + {\pi \over 4}} \over {2 - \cos 2x}}dx} 2I=π4π4(x+π4)+(x+π4)2cos2xdx2I = \int\limits_{ - {\pi \over 4}}^{{\pi \over 4}} {{{(x + {\pi \over 4}) + (-x + {\pi \over 4})} \over {2 - \cos 2x}}dx} 2I=π4π42π42cos2xdx2I = \int\limits_{ - {\pi \over 4}}^{{\pi \over 4}} {{{2 {\pi \over 4}} \over {2 - \cos 2x}}dx} 2I=π4π4π22cos2xdx2I = \int\limits_{ - {\pi \over 4}}^{{\pi \over 4}} {{{\pi \over 2}} \over {2 - \cos 2x}}dx I=12π4π4π22cos2xdxI = {1 \over 2} \int\limits_{ - {\pi \over 4}}^{{\pi \over 4}} {{{\pi \over 2}} \over {2 - \cos 2x}}dx I=π4π4π412cos2xdxI = {\pi \over 4} \int\limits_{ - {\pi \over 4}}^{{\pi \over 4}} {{1} \over {2 - \cos 2x}}dx Reasoning: Adding the two integral forms allows us to combine the numerators, which simplifies the expression significantly by canceling out the xx terms.

Step 3: Simplify the integrand using trigonometric identities We use the identity cos(2x)=1tan2x1+tan2x\cos(2x) = \frac{1 - \tan^2 x}{1 + \tan^2 x}. Substitute this into the integrand: 12cos2x=121tan2x1+tan2x\frac{1}{2 - \cos 2x} = \frac{1}{2 - \frac{1 - \tan^2 x}{1 + \tan^2 x}} =1+tan2x2(1+tan2x)(1tan2x)= \frac{1 + \tan^2 x}{2(1 + \tan^2 x) - (1 - \tan^2 x)} =1+tan2x2+2tan2x1+tan2x= \frac{1 + \tan^2 x}{2 + 2\tan^2 x - 1 + \tan^2 x} =1+tan2x1+3tan2x= \frac{1 + \tan^2 x}{1 + 3\tan^2 x} Recall that 1+tan2x=sec2x1 + \tan^2 x = \sec^2 x. So the integrand becomes: sec2x1+3tan2x\frac{\sec^2 x}{1 + 3\tan^2 x} Now, the integral is: I=π4π4π4sec2x1+3tan2xdxI = {\pi \over 4} \int\limits_{ - {\pi \over 4}}^{{\pi \over 4}} {\sec^2 x \over {1 + 3\tan^2 x}}dx Reasoning: Expressing cos(2x)\cos(2x) in terms of tan2x\tan^2 x is a common strategy when the integral involves sec2x\sec^2 x in the numerator, as it allows for a substitution involving tanx\tan x.

Step 4: Perform a substitution Let u=tanxu = \tan x. Then, du=sec2xdxdu = \sec^2 x \, dx. We also need to change the limits of integration. When x=π4x = -\frac{\pi}{4}, u=tan(π4)=1u = \tan(-\frac{\pi}{4}) = -1. When x=π4x = \frac{\pi}{4}, u=tan(π4)=1u = \tan(\frac{\pi}{4}) = 1. The integral becomes: I=π41111+3u2duI = {\pi \over 4} \int\limits_{-1}^{1} {1 \over {1 + 3u^2}}du Reasoning: This substitution simplifies the integrand to a standard form that can be easily integrated.

Step 5: Evaluate the integral with respect to uu We can rewrite the denominator as 12+(3u)21^2 + (\sqrt{3}u)^2. I=π411112+(3u)2duI = {\pi \over 4} \int\limits_{-1}^{1} {1 \over {1^2 + (\sqrt{3}u)^2}}du To match the standard form 1a2+x2dx=1atan1(xa)\int \frac{1}{a^2 + x^2} dx = \frac{1}{a} \tan^{-1}\left(\frac{x}{a}\right), we need to adjust for the coefficient of uu. Let v=3uv = \sqrt{3}u. Then dv=3dudv = \sqrt{3} du, so du=13dvdu = \frac{1}{\sqrt{3}} dv. The limits of integration also change: When u=1u = -1, v=3(1)=3v = \sqrt{3}(-1) = -\sqrt{3}. When u=1u = 1, v=3(1)=3v = \sqrt{3}(1) = \sqrt{3}. I=π433112+v2(13dv)I = {\pi \over 4} \int\limits_{-\sqrt{3}}^{\sqrt{3}} {1 \over {1^2 + v^2}} \left(\frac{1}{\sqrt{3}} dv\right) I=π4333112+v2dvI = {\pi \over 4\sqrt{3}} \int\limits_{-\sqrt{3}}^{\sqrt{3}} {1 \over {1^2 + v^2}} dv Now, apply the standard integral formula 1a2+x2dx=1atan1(xa)\int \frac{1}{a^2 + x^2} dx = \frac{1}{a} \tan^{-1}\left(\frac{x}{a}\right) with a=1a=1 and variable vv. I=π43[11tan1(v1)]33I = {\pi \over 4\sqrt{3}} \left[ {1 \over 1} \tan^{-1}\left(\frac{v}{1}\right) \right]_{-\sqrt{3}}^{\sqrt{3}} I=π43[tan1(v)]33I = {\pi \over 4\sqrt{3}} \left[ \tan^{-1}(v) \right]_{-\sqrt{3}}^{\sqrt{3}} Reasoning: This step involves applying a standard integration formula after a suitable substitution and adjustment for the coefficient.

Step 6: Evaluate the definite integral I=π43(tan1(3)tan1(3))I = {\pi \over 4\sqrt{3}} \left( \tan^{-1}(\sqrt{3}) - \tan^{-1}(-\sqrt{3}) \right) We know that tan1(3)=π3\tan^{-1}(\sqrt{3}) = \frac{\pi}{3} and tan1(3)=π3\tan^{-1}(-\sqrt{3}) = -\frac{\pi}{3} (since tan1\tan^{-1} is an odd function). I=π43(π3(π3))I = {\pi \over 4\sqrt{3}} \left( \frac{\pi}{3} - \left(-\frac{\pi}{3}\right) \right) I=π43(π3+π3)I = {\pi \over 4\sqrt{3}} \left( \frac{\pi}{3} + \frac{\pi}{3} \right) I=π43(2π3)I = {\pi \over 4\sqrt{3}} \left( \frac{2\pi}{3} \right) I=π23(π3)I = {\pi \over {2\sqrt{3}}} \left( \frac{\pi}{3} \right) I=π263I = {{\pi^2} \over {6\sqrt 3 }} Reasoning: Evaluating the tan1\tan^{-1} function at the limits and simplifying the expression yields the final value of the integral.

Common Mistakes & Tips

  • Incorrect application of King's Property: Ensure that a+bxa+b-x is correctly substituted into the entire integrand, especially in the numerator.
  • Trigonometric identity errors: Double-check the conversion of cos(2x)\cos(2x) to tan2x\tan^2 x and the subsequent algebraic simplification.
  • Substitution errors: Be careful with changing the limits of integration and adjusting for any coefficients introduced during substitution (e.g., the 3\sqrt{3} in v=3uv = \sqrt{3}u).

Summary

The integral was solved by first applying King's Property to generate a second form of the integral. Combining the original and transformed integrals simplified the integrand significantly. Subsequently, the trigonometric identity for cos(2x)\cos(2x) in terms of tan2x\tan^2 x was used, followed by a substitution u=tanxu = \tan x. This transformed the integral into a standard form involving tan1\tan^{-1}, which was then evaluated using the fundamental theorem of calculus. The final result obtained is π263\frac{\pi^2}{6\sqrt 3}.

The final answer is π263\boxed{{\frac{\pi^2}{6\sqrt 3}}}.

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