Concept:
For a particle moving along a straight line under constant linear acceleration, we can determine its displacement and position using the standard kinematic equations of motion:
\[
S = S_0 + v_0 t + \frac{1}{2}at^2
\]
We must establish a consistent coordinate direction convention: we will define displacement to the right as positive and displacement to the left as negative.
Step 1: Identifying parameters with correct signs.
Let us list the values given in the problem statement and assign signs based on our direction convention:
• Initial reference position coordinate, \( S_0 = 0\text{ m} \)
• Initial velocity vector, \( v_0 = 12\text{ m/s} \) (directed to the right, so it is positive: \( +12 \))
• Acceleration rate, \( a = 2\text{ m/s}^2 \) (directed to the left, acting as a deceleration, so it is negative: \( -2 \))
• Elapsed travel time, \( t = 10\text{ s} \)
Step 2: Substituting values into the kinematic equation.
Substitute these parameters into the constant-acceleration position formula:
\[
S = 0 + (12)(10) + \frac{1}{2}(-2)(10)^2
\]
Step 3: Simplifying individual terms.
Calculate the linear velocity displacement product term:
\[
12 \times 10 = 120\text{ m}
\]
Calculate the acceleration term product:
\[
\frac{1}{2} \times (-2) \times (10)^2 = -1 \times 100 = -100\text{ m}
\]
Step 4: Finding the final net position coordinate.
Combine the calculated terms to find the final position \( S \):
\[
S = 120 - 100 = 20\text{ m}
\]
The final calculated position of the particle at time \( t=10\text{ s} \) is exactly \( 20\text{ m} \). This matches option (C).