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Calculate Value of Expression Involving Definite Integral

Consider the definite integral given by I=2π∫−π/4π/4dx(1+esin⁡x)(2−cos⁡2x)I = \frac{2}{\pi} \int_{-\pi/4}^{\pi/4} \frac{dx}{(1 + e^{\sin x})(2 - \cos 2x)} Find the value of 27I227 I^2.

Official Numerical Answer4

Step-by-Step Solution

To find the value of 27I227 I^2, we begin by analyzing the given integral:

I=2π∫−π/4π/4dx(1+esin⁡x)(2−cos⁡2x)I = \frac{2}{\pi} \int_{-\pi/4}^{\pi/4} \frac{dx}{(1 + e^{\sin x})(2 - \cos 2x)}

Let J=∫−π/4π/4dx(1+esin⁡x)(2−cos⁡2x)J = \int_{-\pi/4}^{\pi/4} \frac{dx}{(1 + e^{\sin x})(2 - \cos 2x)}, so that I=2πJI = \frac{2}{\pi} J.

Using the property of definite integrals ∫abf(x) dx=∫abf(a+b−x) dx\int_{a}^{b} f(x) \, dx = \int_{a}^{b} f(a+b-x) \, dx, with a=−π/4a = -\pi/4 and b=π/4b = \pi/4, we replace xx with −x-x:

J=∫−π/4π/4dx(1+e−sin⁡x)(2−cos⁡(−2x))J = \int_{-\pi/4}^{\pi/4} \frac{dx}{(1 + e^{-\sin x})(2 - \cos(-2x))}

Since cos⁡(−2x)=cos⁡(2x)\cos(-2x) = \cos(2x), we rewrite 1+e−sin⁡x1 + e^{-\sin x} as 1+1esin⁡x=esin⁡x+1esin⁡x1 + \frac{1}{e^{\sin x}} = \frac{e^{\sin x} + 1}{e^{\sin x}}:

J=∫−π/4π/4esin⁡x dx(1+esin⁡x)(2−cos⁡2x)J = \int_{-\pi/4}^{\pi/4} \frac{e^{\sin x} \, dx}{(1 + e^{\sin x})(2 - \cos 2x)}

Adding the two expressions for JJ:

2J=∫−π/4π/41+esin⁡x(1+esin⁡x)(2−cos⁡2x) dx2J = \int_{-\pi/4}^{\pi/4} \frac{1 + e^{\sin x}}{(1 + e^{\sin x})(2 - \cos 2x)} \, dx

2J=∫−π/4π/4dx2−cos⁡2x2J = \int_{-\pi/4}^{\pi/4} \frac{dx}{2 - \cos 2x}

Since the integrand 12−cos⁡2x\frac{1}{2 - \cos 2x} is an even function of xx, we can simplify the integral bounds:

2J=2∫0π/4dx2−cos⁡2x  ⟹  J=∫0π/4dx2−cos⁡2x2J = 2 \int_{0}^{\pi/4} \frac{dx}{2 - \cos 2x} \implies J = \int_{0}^{\pi/4} \frac{dx}{2 - \cos 2x}

Using the trigonometric identity cos⁡2x=1−tan⁡2x1+tan⁡2x\cos 2x = \frac{1 - \tan^2 x}{1 + \tan^2 x}:

2−cos⁡2x=2−1−tan⁡2x1+tan⁡2x=2(1+tan⁡2x)−(1−tan⁡2x)1+tan⁡2x=1+3tan⁡2x1+tan⁡2x2 - \cos 2x = 2 - \frac{1 - \tan^2 x}{1 + \tan^2 x} = \frac{2(1 + \tan^2 x) - (1 - \tan^2 x)}{1 + \tan^2 x} = \frac{1 + 3\tan^2 x}{1 + \tan^2 x}

Since 1+tan⁡2x=sec⁡2x1 + \tan^2 x = \sec^2 x, the integral becomes:

J=∫0π/4sec⁡2x dx1+3tan⁡2xJ = \int_{0}^{\pi/4} \frac{\sec^2 x \, dx}{1 + 3\tan^2 x}

Let t=tan⁡xt = \tan x, so dt=sec⁡2x dxdt = \sec^2 x \, dx.

  • When x=0x = 0, t=0t = 0.
  • When x=π/4x = \pi/4, t=1t = 1.

Substituting tt into the integral:

J=∫01dt1+(3t)2=[13tan⁡−1(3t)]01J = \int_{0}^{1} \frac{dt}{1 + (\sqrt{3}t)^2} = \left[ \frac{1}{\sqrt{3}} \tan^{-1}(\sqrt{3}t) \right]_{0}^{1}

J=13(tan⁡−1(3)−tan⁡−1(0))=13(π3−0)=π33J = \frac{1}{\sqrt{3}} \left( \tan^{-1}(\sqrt{3}) - \tan^{-1}(0) \right) = \frac{1}{\sqrt{3}} \left( \frac{\pi}{3} - 0 \right) = \frac{\pi}{3\sqrt{3}}

Now, substituting JJ back to find II:

I=2πJ=2π⋅π33=233I = \frac{2}{\pi} J = \frac{2}{\pi} \cdot \frac{\pi}{3\sqrt{3}} = \frac{2}{3\sqrt{3}}

Squaring II:

I2=(233)2=427I^2 = \left( \frac{2}{3\sqrt{3}} \right)^2 = \frac{4}{27}

Finally, we calculate the required value:

27I2=27×427=427 I^2 = 27 \times \frac{4}{27} = 4