Step 1: Understanding the Topic:
This problem involves "Laws of Motion," specifically focusing on friction in non-inertial frames. When a trolley accelerates, an object on it experiences a "pseudo force." Friction acts to prevent the object from sliding due to this force.
Step 2: Key Formulas and Approach:
Pseudo Force ($F_p$) = $m \times a$ (acting opposite to acceleration).
Limiting Static Friction ($f_{max}$) = $\mu_s \times N = \mu_s \times m \times g$.
For the box to remain stationary relative to the trolley: $F_p \leq f_{max}$.
Step 3: Detailed Explanation:
Analyze forces: As the trolley accelerates forward with acceleration '$a$', the box (mass $m$) feels a force $ma$ pushing it backward relative to the trolley. To stop this motion, the static friction $f_s$ acts forward.
Find the limit: The box starts to slip when the required force to keep it stationary exceeds the maximum possible friction the surface can provide.
\[ m \cdot a = \mu_s \cdot m \cdot g \]
Simplify: Notice that the mass '$m$' appears on both sides of the equation. Dividing both sides by $m$:
\[ a = \mu_s \cdot g \]
Calculate: Substitute the given values ($\mu_s = 0.12$ and $g = 10 \text{ m/s}^2$):
\[ a = 0.12 \times 10 = 1.2 \text{ m/s}^2 \]
Even though the mass was given as 15 kg, it does not affect the maximum possible acceleration.
Step 4: Final Answer:
The maximum acceleration is 1.2 m/s².