Concept:
The solution involves trigonometric simplification and the property of periodic functions in definite integrals:
• Half-angle formula: \( 1 - \cos \theta = 2\sin^2(\frac{\theta}{2}) \).
• Identity: \( \sqrt{x^2} = |x| \).
• Periodic Property: If \( f(x) \) is periodic with period \( T \), then \( \int_{0}^{nT} f(x) \, dx = n \int_{0}^{T} f(x) \, dx \).
Step 1: Simplifying the integrand using trigonometric identities.
We know that \( 1 - \cos 4x = 2\sin^2(2x) \).
Substituting this into the integral:
\[
I = \int_{0}^{32\pi} \sqrt{2\sin^2(2x)} \, dx = \sqrt{2} \int_{0}^{32\pi} |\sin 2x| \, dx
\]
Step 2: Applying the periodicity property.
The function \( f(x) = |\sin 2x| \) is periodic. The period of \( \sin x \) is \( 2\pi \), so the period of \( \sin 2x \) is \( \frac{2\pi}{2} = \pi \).
However, the period of the absolute value function \( |\sin 2x| \) is \( \frac{\pi}{2} \).
We can express the upper limit \( 32\pi \) in terms of the period \( \frac{\pi}{2} \):
\[
32\pi = 64 \times \left( \frac{\pi}{2} \right)
\]
Using the property \( \int_{0}^{nT} f(x) \, dx = n \int_{0}^{T} f(x) \, dx \):
\[
I = \sqrt{2} \times 64 \int_{0}^{\pi/2} |\sin 2x| \, dx
\]
Step 3: Evaluating the definite integral.
In the interval \( [0, \pi/2] \), \( 2x \) ranges from \( 0 \) to \( \pi \). In this range, \( \sin 2x \) is non-negative, so we can remove the modulus:
\[
I = 64\sqrt{2} \int_{0}^{\pi/2} \sin 2x \, dx
\]
\[
I = 64\sqrt{2} \left[ \frac{-\cos 2x}{2} \right]_{0}^{\pi/2} = \frac{64\sqrt{2}}{2} [ -\cos(\pi) - (-\cos 0) ]
\]
\[
I = 32\sqrt{2} [ -(-1) + 1 ] = 32\sqrt{2} [ 1 + 1 ] = 64\sqrt{2} \times 2 = 128\sqrt{2}
\]