Step 1: Split the motion into two phases.
The particle starts at 12 m/s to the right and decelerates at 2 m/s\(^2\) to the left. It first slows down, stops, then reverses direction. Time to stop: \( 0 = v_0 - at_1 \Rightarrow t_1 = \frac{12}{2} = 6\text{ s} \).
Step 2: Distance covered while slowing down.
Using \( v^2 = v_0^2 - 2as_1 \), at the stopping point \( v=0 \), so \( s_1 = \frac{v_0^2}{2a} = \frac{144}{4} = 36\text{ m} \) to the right.
Step 3: Motion in the remaining time.
The particle now starts from rest and accelerates to the left for the remaining \( t_2 = 10 - 6 = 4\text{ s} \). Distance covered: \( s_2 = \frac{1}{2}at_2^2 = \frac{1}{2}(2)(16) = 16\text{ m} \) to the left.
Step 4: Find the net position.
\[ S = s_1 - s_2 = 36 - 16 = 20\text{ m} \]
\[ \boxed{S = 20\text{ m}} \]