In Simple Harmonic Motion (SHM), the velocity \( v \) is related to the displacement \( x \) and the amplitude \( A \) by the equation:
\[
v = \omega \sqrt{A^2 - x^2}
\]
Where:
- \( \omega \) is the angular frequency,
- \( x \) is the displacement at any point in time,
- \( A \) is the amplitude of the motion.
From the given data:
- When \( x = 4 \, \text{cm} \), \( v = 10 \, \text{cm/s} \),
- When \( x = 5 \, \text{cm} \), \( v = 8 \, \text{cm/s} \).
We can use these two pieces of information to form two equations and solve for \( \omega \) and \( A \).
For \( x = 4 \, \text{cm} \) and \( v = 10 \, \text{cm/s} \):
\[
10 = \omega \sqrt{A^2 - 16}
\]
For \( x = 5 \, \text{cm} \) and \( v = 8 \, \text{cm/s} \):
\[
8 = \omega \sqrt{A^2 - 25}
\]
Now, solving these equations:
From the first equation:
\[
\omega = \frac{10}{\sqrt{A^2 - 16}}
\]
Substitute into the second equation:
\[
8 = \frac{10}{\sqrt{A^2 - 16}} \cdot \sqrt{A^2 - 25}
\]
Simplifying, we find \( A \) and \( \omega \), which allows us to calculate the periodic time \( T = \frac{2\pi}{\omega} \).
After solving, we find that the periodic time \( T = \pi \) sec.