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JEE Main 2021
Definite Integration
Definite Integration
Hard

Question

The integral 0π8xdx4cos2x+sin2x\int_0^\pi \frac{8 x d x}{4 \cos ^2 x+\sin ^2 x} is equal to

Options

Solution

1. Key Concepts and Formulas

  • King Property of Definite Integrals: For an integral abf(x)dx\int_a^b f(x) dx, the property states that abf(x)dx=abf(a+bx)dx\int_a^b f(x) dx = \int_a^b f(a+b-x) dx. This is particularly useful when the integrand has a term involving xx in the numerator and the limits of integration are symmetric or have a convenient sum.
  • Trigonometric Identities:
    • cos2x+sin2x=1\cos^2 x + \sin^2 x = 1
    • sin(2x)=2sinxcosx\sin(2x) = 2 \sin x \cos x
    • cos(2x)=2cos2x1    cos2x=1+cos(2x)2\cos(2x) = 2 \cos^2 x - 1 \implies \cos^2 x = \frac{1 + \cos(2x)}{2}
    • sin2x=1cos(2x)2\sin^2 x = \frac{1 - \cos(2x)}{2}
  • Substitution Rule for Definite Integrals: If u=g(x)u = g(x), then du=g(x)dxdu = g'(x) dx. The limits of integration also change from x=ax=a to u=g(a)u=g(a) and from x=bx=b to u=g(b)u=g(b).
  • Standard Integral: 1a2u2du=12alna+uau+C\int \frac{1}{a^2 - u^2} du = \frac{1}{2a} \ln \left| \frac{a+u}{a-u} \right| + C or 1u2a2du=12alnuau+a+C\int \frac{1}{u^2 - a^2} du = \frac{1}{2a} \ln \left| \frac{u-a}{u+a} \right| + C. Also, sec2xdx=tanx+C\int \sec^2 x dx = \tan x + C.

2. Step-by-Step Solution

Let the given integral be II. I=0π8xdx4cos2x+sin2xI = \int_0^\pi \frac{8 x \, dx}{4 \cos^2 x + \sin^2 x}

Step 1: Apply the King Property We use the King Property, abf(x)dx=abf(a+bx)dx\int_a^b f(x) dx = \int_a^b f(a+b-x) dx. Here, a=0a=0 and b=πb=\pi. So, a+bx=0+πx=πxa+b-x = 0+\pi-x = \pi-x. Applying this to our integral: I=0π8(πx)dx4cos2(πx)+sin2(πx)I = \int_0^\pi \frac{8 (\pi-x) \, dx}{4 \cos^2 (\pi-x) + \sin^2 (\pi-x)} We know that cos(πx)=cosx\cos(\pi-x) = -\cos x and sin(πx)=sinx\sin(\pi-x) = \sin x. Therefore, cos2(πx)=(cosx)2=cos2x\cos^2(\pi-x) = (-\cos x)^2 = \cos^2 x and sin2(πx)=(sinx)2=sin2x\sin^2(\pi-x) = (\sin x)^2 = \sin^2 x. Substituting these back into the integral: I=0π8(πx)dx4cos2x+sin2xI = \int_0^\pi \frac{8 (\pi-x) \, dx}{4 \cos^2 x + \sin^2 x}

Step 2: Add the original and modified integrals Now we have two expressions for II: Equation (1): I=0π8xdx4cos2x+sin2xI = \int_0^\pi \frac{8 x \, dx}{4 \cos^2 x + \sin^2 x} Equation (2): I=0π8(πx)dx4cos2x+sin2xI = \int_0^\pi \frac{8 (\pi-x) \, dx}{4 \cos^2 x + \sin^2 x} Adding Equation (1) and Equation (2): 2I=0π8x4cos2x+sin2xdx+0π8(πx)4cos2x+sin2xdx2I = \int_0^\pi \frac{8 x}{4 \cos^2 x + \sin^2 x} \, dx + \int_0^\pi \frac{8 (\pi-x)}{4 \cos^2 x + \sin^2 x} \, dx Since the denominators are the same, we can combine the numerators: 2I=0π8x+8(πx)4cos2x+sin2xdx2I = \int_0^\pi \frac{8x + 8(\pi-x)}{4 \cos^2 x + \sin^2 x} \, dx 2I=0π8x+8π8x4cos2x+sin2xdx2I = \int_0^\pi \frac{8x + 8\pi - 8x}{4 \cos^2 x + \sin^2 x} \, dx 2I=0π8π4cos2x+sin2xdx2I = \int_0^\pi \frac{8\pi}{4 \cos^2 x + \sin^2 x} \, dx

Step 3: Simplify the denominator and evaluate the integral We can rewrite the denominator using cos2x=1sin2x\cos^2 x = 1 - \sin^2 x: 4cos2x+sin2x=4(1sin2x)+sin2x=44sin2x+sin2x=43sin2x4 \cos^2 x + \sin^2 x = 4(1-\sin^2 x) + \sin^2 x = 4 - 4\sin^2 x + \sin^2 x = 4 - 3\sin^2 x Alternatively, we can write the denominator in terms of tanx\tan x by dividing the numerator and denominator by cos2x\cos^2 x: 2I=0π8π4cos2x+sin2xdx=8π0π14cos2x+sin2xdx2I = \int_0^\pi \frac{8\pi}{4 \cos^2 x + \sin^2 x} \, dx = 8\pi \int_0^\pi \frac{1}{4 \cos^2 x + \sin^2 x} \, dx Divide numerator and denominator by cos2x\cos^2 x: 2I=8π0πsec2x4+tan2xdx2I = 8\pi \int_0^\pi \frac{\sec^2 x}{4 + \tan^2 x} \, dx Now, let's use the substitution u=tanxu = \tan x. Then du=sec2xdxdu = \sec^2 x \, dx. We need to change the limits of integration: When x=0x=0, u=tan(0)=0u = \tan(0) = 0. When x=πx=\pi, u=tan(π)=0u = \tan(\pi) = 0.

This substitution leads to an integral from 0 to 0, which is 0. This indicates that we might have made a simplification too early or there's a subtlety with the interval [0,π][0, \pi]. Let's re-examine the denominator and the interval.

The denominator is 4cos2x+sin2x4 \cos^2 x + \sin^2 x. We can rewrite this as 3cos2x+(cos2x+sin2x)=3cos2x+13 \cos^2 x + (\cos^2 x + \sin^2 x) = 3 \cos^2 x + 1. Or, as 4(1sin2x)+sin2x=43sin2x4(1-\sin^2 x) + \sin^2 x = 4 - 3\sin^2 x.

Let's go back to: 2I=8π0π14cos2x+sin2xdx2I = 8\pi \int_0^\pi \frac{1}{4 \cos^2 x + \sin^2 x} \, dx We can express the denominator in terms of tanx\tan x: 4cos2x+sin2x=cos2x(4+tan2x)4 \cos^2 x + \sin^2 x = \cos^2 x (4 + \tan^2 x) So the integral becomes: 2I=8π0πsec2x4+tan2xdx2I = 8\pi \int_0^\pi \frac{\sec^2 x}{4 + \tan^2 x} \, dx Let u=tanxu = \tan x, so du=sec2xdxdu = \sec^2 x \, dx. The limits are x=0    u=0x=0 \implies u=0 and x=π    u=0x=\pi \implies u=0. This implies the integral evaluates to 0, which is incorrect. The issue is that tanx\tan x has a discontinuity at x=π/2x=\pi/2 within the interval [0,π][0, \pi].

Let's use the property 02af(x)dx=20af(x)dx\int_0^{2a} f(x) dx = 2 \int_0^a f(x) dx if f(2ax)=f(x)f(2a-x) = f(x). And 02af(x)dx=0\int_0^{2a} f(x) dx = 0 if f(2ax)=f(x)f(2a-x) = -f(x). Our integral is from 00 to π\pi. Let's check the integrand for symmetry. Let g(x)=8x4cos2x+sin2xg(x) = \frac{8x}{4 \cos^2 x + \sin^2 x}. g(πx)=8(πx)4cos2(πx)+sin2(πx)=8(πx)4cos2x+sin2xg(\pi-x) = \frac{8(\pi-x)}{4 \cos^2(\pi-x) + \sin^2(\pi-x)} = \frac{8(\pi-x)}{4 \cos^2 x + \sin^2 x}. So I=0πg(x)dx=0πg(πx)dxI = \int_0^\pi g(x) dx = \int_0^\pi g(\pi-x) dx. 2I=0π(g(x)+g(πx))dx=0π8x+8(πx)4cos2x+sin2xdx=0π8π4cos2x+sin2xdx2I = \int_0^\pi (g(x) + g(\pi-x)) dx = \int_0^\pi \frac{8x + 8(\pi-x)}{4 \cos^2 x + \sin^2 x} dx = \int_0^\pi \frac{8\pi}{4 \cos^2 x + \sin^2 x} dx.

Now consider the integral J=0π14cos2x+sin2xdxJ = \int_0^\pi \frac{1}{4 \cos^2 x + \sin^2 x} \, dx. We can use the property 02af(x)dx=20af(x)dx\int_0^{2a} f(x) dx = 2 \int_0^a f(x) dx if f(2ax)=f(x)f(2a-x) = f(x). Here, 2a=π2a = \pi, so a=π/2a = \pi/2. Let f(x)=14cos2x+sin2xf(x) = \frac{1}{4 \cos^2 x + \sin^2 x}. f(πx)=14cos2(πx)+sin2(πx)=14cos2x+sin2x=f(x)f(\pi-x) = \frac{1}{4 \cos^2(\pi-x) + \sin^2(\pi-x)} = \frac{1}{4 \cos^2 x + \sin^2 x} = f(x). So, J=20π/214cos2x+sin2xdxJ = 2 \int_0^{\pi/2} \frac{1}{4 \cos^2 x + \sin^2 x} \, dx.

Divide numerator and denominator by cos2x\cos^2 x: J=20π/2sec2x4+tan2xdxJ = 2 \int_0^{\pi/2} \frac{\sec^2 x}{4 + \tan^2 x} \, dx Let u=tanxu = \tan x. Then du=sec2xdxdu = \sec^2 x \, dx. When x=0x=0, u=tan(0)=0u = \tan(0) = 0. When x=π/2x=\pi/2, u=tan(π/2)u = \tan(\pi/2) \to \infty.

So the integral becomes: J=2014+u2duJ = 2 \int_0^\infty \frac{1}{4 + u^2} \, du This is of the form 1a2+u2du=1aarctan(ua)\int \frac{1}{a^2 + u^2} du = \frac{1}{a} \arctan \left( \frac{u}{a} \right). Here a2=4a^2 = 4, so a=2a=2. J=2[12arctan(u2)]0J = 2 \left[ \frac{1}{2} \arctan \left( \frac{u}{2} \right) \right]_0^\infty J=[arctan(u2)]0J = \left[ \arctan \left( \frac{u}{2} \right) \right]_0^\infty J=arctan()arctan(0)J = \arctan(\infty) - \arctan(0) J=π20=π2J = \frac{\pi}{2} - 0 = \frac{\pi}{2}

Now, recall that 2I=8πJ2I = 8\pi J. 2I=8π(π2)2I = 8\pi \left( \frac{\pi}{2} \right) 2I=4π22I = 4\pi^2 I=4π22I = \frac{4\pi^2}{2} I=2π2I = 2\pi^2

3. Common Mistakes & Tips

  • Division by Zero: Be cautious when dividing by cos2x\cos^2 x if the interval includes π/2\pi/2, where cosx=0\cos x = 0. The King Property and the subsequent splitting of the integral into [0,π/2][0, \pi/2] and [π/2,π][\pi/2, \pi] (or using the property for 2a2a) helps manage this.
  • Incorrect Limit Transformation: Always remember to change the limits of integration when using the substitution rule. For definite integrals, this is crucial.
  • Algebraic Simplification Errors: Double-check algebraic manipulations, especially when dealing with trigonometric functions and their squares.

4. Summary

The integral was evaluated using the King Property of definite integrals, which allowed us to eliminate the xx term in the numerator. By adding the original integral to the modified integral, we obtained a simpler integral involving a constant in the numerator. The denominator was then manipulated to enable a substitution, and the integral was evaluated over the appropriate limits. The property 02af(x)dx=20af(x)dx\int_0^{2a} f(x) dx = 2 \int_0^a f(x) dx for even functions was used to handle the interval [0,π][0, \pi] by splitting it into [0,π/2][0, \pi/2].

The final answer is 2π2\boxed{2 \pi^2}. This corresponds to option (A).

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