Concept:
In Simple Harmonic Motion (SHM), the acceleration \( a \) of a particle at any instant is directly proportional to its displacement \( x \) from the mean position and acts in the opposite direction. The governing kinematic equation is:
\[
a = -\omega^2 x
\]
where \(\omega\) represents the angular frequency of the system.
To find the magnitude of the maximum acceleration (\( a_{\max} \)), we consider the point where the displacement is at its absolute maximum value. This maximum displacement is defined as the amplitude \( A \) of the oscillation:
\[
a_{\max} = \omega^2 A
\]
Step 1: Extracting the given kinematic parameters from the problem text.
From the question statement, we have:
• Amplitude of oscillation, \( A = 0.1 \text{ m} \)
• Angular frequency, \( \omega = 10 \text{ rad/s} \)
Step 2: Substituting the parameters into the maximum acceleration formula.
Apply the values directly to the equation:
\[
a_{\max} = (10)^2 \cdot (0.1)
\]
Evaluating the square of the angular frequency:
\[
(10)^2 = 100
\]
Now, performing the multiplication:
\[
a_{\max} = 100 \cdot 0.1 = 10 \text{ m/s}^2
\]
Wait, let's re-read the options and calculation carefully:
\( 100 \times 0.1 = 10 \). This corresponds to option (C). Let me correct the answer label in the final block.
Step 3: Final validation of the correct option choice.
Our calculation gives:
\[
a_{\max} = 10 \text{ m/s}^2
\]
This perfectly matches option (C).