The problem involves determining the time period of a motion described by the position function of a particle moving along the \(x\)-axis. The position as a function of time is given by:
\(x(t) = \sin^2(\omega t) \cos^3(\omega t)\)
- The first step is to observe any periodic functions involved in the expression. Here, we have trigonometric functions \(\sin(\omega t)\) and \(\cos(\omega t)\), both of which have a fundamental period of \(\frac{2\pi}{\omega}\).
- The given expression can be rewritten using a trigonometric identity:
\(\sin^2(\omega t) = \frac{1 - \cos(2\omega t)}{2}\) and \(\cos^3(\omega t) = \cos(\omega t) \cdot \cos^2(\omega t) = \cos(\omega t) \cdot \frac{1 + \cos(2\omega t)}{2}\).
- Since the fundamental period of both \(\sin(\omega t)\) and \(\cos(\omega t)\) is \(\frac{2\pi}{\omega}\), the function \(x(t)\) will repeat its value after a change in \(t\) by an entire period of \(\frac{2\pi}{\omega}\). This is due to the fact that all terms in the product \(x(t)\) include integer multiples of \(\omega t\).
- Therefore, the time period of \(x(t) = \sin^2(\omega t) \cos^3(\omega t)\) remains \(\frac{2\pi}{\omega}\).
Hence, the correct answer is \(\frac{2\pi}{\omega}\).