Step 1:
The general equation for displacement in simple harmonic motion is:
\[
y = A \sin(2 \pi t + \phi)
\]
where \( A \) is the amplitude, \( t \) is the time, and \( \phi \) is the phase angle.
At \( t = 0 \), the displacement \( y = 2 \, \text{m} \). Thus, at \( t = 0 \), we have:
\[
y = A \sin(\phi) = 2
\]
This gives us the first equation:
\[
A \sin(\phi) = 2 \quad \text{(Equation 1)}
\]
Step 2:
The velocity in simple harmonic motion is given by:
\[
v = A \cdot 2 \pi \cdot \cos(2 \pi t + \phi)
\]
At \( t = 0 \), the velocity is \( v = 4 \, \text{ms}^{-1} \), so:
\[
v = A \cdot 2 \pi \cdot \cos(\phi) = 4
\]
This gives us the second equation:
\[
A \cdot 2 \pi \cdot \cos(\phi) = 4 \quad \text{(Equation 2)}
\]
Step 3:
Now we have two equations to solve:
1. \( A \sin(\phi) = 2 \)
2. \( A \cdot 2 \pi \cdot \cos(\phi) = 4 \)
Dividing Equation 2 by Equation 1:
\[
\frac{A \cdot 2 \pi \cdot \cos(\phi)}{A \sin(\phi)} = \frac{4}{2}
\]
\[
\frac{2 \pi \cos(\phi)}{\sin(\phi)} = 2
\]
\[
\frac{\cos(\phi)}{\sin(\phi)} = \frac{2}{2 \pi} = \frac{1}{\pi}
\]
Thus, \( \tan(\phi) = \pi \), so \( \phi \approx 45^\circ \).
Thus, the phase angle is \( \phi = 45^\circ \).