For a system executing simple harmonic motion, the displacement, velocity, and acceleration are related through their phase differences:
- The displacement \( x \) is given by:
\[
x = A \sin(\omega t)
\]
where \( A \) is the amplitude, and \( \omega \) is the angular frequency.
- The velocity \( v \) is the time derivative of displacement:
\[
v = \frac{dx}{dt} = A \omega \cos(\omega t)
\]
The velocity leads the displacement by a phase of \( \frac{\pi}{2} \).
- The acceleration \( a \) is the time derivative of velocity:
\[
a = \frac{dv}{dt} = -A \omega^2 \sin(\omega t)
\]
The acceleration lags the velocity by a phase of \( \frac{\pi}{2} \), and thus, lags the displacement by a phase of \( \pi \).
Thus, displacement lags both velocity and acceleration by the phases of \( \frac{\pi}{2} \) and \( \pi \), respectively.