If I=∫0π2sin⁡12xsin⁡2x+cos⁡2x dxI = \int_0^{\frac{\pi}{2}} \frac{\sin \frac{1}{2} x}{\sin^2 x + \cos^2 x} \, dx, then ∫02Ixsin⁡xcos⁡xsin⁡2x+cos⁡4x dx\int_0^{2I} \frac{x \sin x \cos x}{\sin^2 x + \cos^4 x} \, dx equals:

Answer: The problem statement is mathematically underdetermined due to an inconsistency in the upper limit of the second integral. If 2I2I is assumed to be π\pi, the integral can be simplified further, but with I=2−2I = 2 - \sqrt{2}, 2I≠π2I \neq \pi. Therefore, a unique numerical answer cannot be provided without further clarification or correction of the problem statement.

Step-by-step solution

Step 1: Simplify the first integral

The denominator of the first integral is sin⁡2x+cos⁡2x\sin^2 x + \cos^2 x. This is a fundamental trigonometric identity, which simplifies to 11. So, the integral II becomes ∫0π2sin⁡12x dx\int_0^{\frac{\pi}{2}} \sin \frac{1}{2} x \, dx.

Step 2: Evaluate the first integral

To evaluate the integral, we find the antiderivative of sin⁡12x\sin \frac{1}{2} x, which is −2cos⁡12x-2 \cos \frac{1}{2} x. Then, we apply the limits of integration from 00 to π2\frac{\pi}{2}.

Step 3: Calculate the value of I

Substitute the values of cos⁡π4=12\cos \frac{\pi}{4} = \frac{1}{\sqrt{2}} and cos⁡0=1\cos 0 = 1 into the expression. Simplify the result to find the value of II.

Step 4: Define the second integral and apply property

Let the second integral be JJ. We substitute the value of II we just calculated into the upper limit of the integral. The integral is of the form ∫0af(x) dx\int_0^a f(x) \, dx.

Step 5: Apply the property ∫0af(x)dx=∫0af(a−x)dx\int_0^a f(x) dx = \int_0^a f(a-x) dx

We use the property of definite integrals that ∫0af(x) dx=∫0af(a−x) dx\int_0^a f(x) \, dx = \int_0^a f(a-x) \, dx. Here, a=2Ia = 2I. This property is often useful when the integrand has symmetry.

Step 6: Observe the symmetry of the integrand

The value of 2I=2(2−2)≈1.1722I = 2(2-\sqrt{2}) \approx 1.172. This is not a standard angle like π\pi or π2\frac{\pi}{2}. For the property sin⁡(a−x)=sin⁡x\sin(a-x) = \sin x and cos⁡(a−x)=−cos⁡x\cos(a-x) = -\cos x to hold, aa must be π\pi. If we assume the problem intended 2I=π2I = \pi, then sin⁡(π−x)=sin⁡x\sin(\pi-x) = \sin x and cos⁡(π−x)=−cos⁡x\cos(\pi-x) = -\cos x. Substituting these into the integral, we get a new expression for JJ.

Step 7: Add the original and modified integrals (assuming 2I=π2I = \pi)

Adding the original integral JJ and the modified integral JJ (after applying the property), we combine the numerators. This step is part of a common technique to solve integrals of this form, but it requires the upper limit to be π\pi for the trigonometric identities to simplify the expression further.

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