The provided voltage function is:
\[ V(t) = 220 \sin(100\pi t). \]
The angular frequency \( \omega \) is derived from the sine function's argument:
\[ \omega = 100\pi. \]
The period \( T \) of this sinusoidal function is calculated as:
\[ T = \frac{2\pi}{\omega} = \frac{2\pi}{100\pi} = \frac{1}{50} \text{ seconds} = 20 \, \text{ms}. \]
To determine the duration for the voltage (and consequently, the current, assuming a purely resistive load) to increase from half its peak value to its maximum value, we examine the time required for a sine wave to transition from \( \frac{1}{2} \) of its maximum to its maximum.
For a sine function, this duration corresponds to a phase shift of \( \frac{\pi}{6} \) radians (from \( \sin(\theta) = \frac{1}{2} \) to \( \sin(\theta) = 1 \)).
The time \( t \) for this phase change is:
\[ t = \frac{\pi/6}{\omega} = \frac{\pi/6}{100\pi} = \frac{1}{600} \text{ seconds}. \]
Converting this time to milliseconds:
\[ t = \frac{1}{600} \times 1000 = 3.33 \, \text{ms}. \]
