In simple harmonic motion (SHM), the acceleration \( a \) at a displacement \( x \) from the mean position is given by:
\[
a = \omega^2 x
\]
where \( \omega \) is the angular frequency. Given:
- \( x = 10 \, \text{cm} = 0.1 \, \text{m} \),
- \( a = 0.4 \, \text{ms}^{-2} \).
Substituting the values:
\[
0.4 = \omega^2 \times 0.1 \quad \Rightarrow \quad \omega^2 = \frac{0.4}{0.1} = 4 \, \text{s}^{-2}
\]
The maximum acceleration in SHM occurs at the amplitude \( A \), and is given by:
\[
a_{\text{max}} = \omega^2 A
\]
Given the amplitude \( A = 30 \, \text{cm} = 0.3 \, \text{m} \), substitute \( \omega^2 = 4 \):
\[
a_{\text{max}} = 4 \times 0.3 = 1.2 \, \text{ms}^{-2}
\]
So, the maximum acceleration of the particle is 1.2 ms\(^{-2}\).