Detailed Summary
In this section on Displacement, we explore the broader implications of displacement within oscillatory motion. Displacement is not merely a positional change; it encompasses variances in other physical properties such as voltage and pressure, particularly in oscillatory systems.
Examples of displacement include:
- Rectilinear Motion: For a steel ball rolling on a surface, the distance from its starting point represents its displacement as a function of time.
- Oscillatory Systems: Consider a mass on a spring oscillating around its equilibrium position, where its position varies from that midpoint.
- Physical Properties: Displacement can manifest in the voltage across capacitors in AC circuits or variations in pressure due to sound waves.
Mathematically, displacement is expressed as a periodic function of time, such as:
$$ f(t) = A \cos(\omega t) $$
where
- $$ A $$ represents the amplitude,
- $$ \omega $$ is the angular frequency,
- The argument $$ \omega t $$ indicates periodicity as it cycles through values, reinforcing the relationship between displacement and time in periodic motion.
The period is deduced from the function, emphasizing the repetitive nature of oscillations.