Step 1: Understanding the Question:
We are given a position function $S(t)$ with constants $a$ and $b$. Using the kinematic boundary conditions (comes to rest at $t = 4\ \text{sec}$ when $S = 16\ \text{m}$), we need to find the constant acceleration of the particle.
Step 2: Key Formula or Approach:
Velocity ($v$) is the first derivative of distance with respect to time, and acceleration ($A$) is the second derivative:
$$ v = \frac{\text{d}S}{\text{d}t}, \quad A = \frac{\text{d}v}{\text{d}t} $$
Step 3: Detailed Explanation:
Given displacement equation:
$$ S = a t^2 + b t + 6 $$
Differentiating once to get the velocity function:
$$ v = \frac{\text{d}S}{\text{d}t} = 2at + b $$
Differentiating a second time to determine acceleration:
$$ A = \frac{\text{d}v}{\text{d}t} = 2a $$
Now let's apply our boundary conditions at $t = 4\ \text{s}$:
• The particle is at position $S = 16$:
$$ 16 = a(4)^2 + b(4) + 6 \implies 16a + 4b = 10 \quad \text{--- (Equation 1)} $$
• The particle comes to rest ($v = 0$):
$$ 0 = 2a(4) + b \implies b = -8a \quad \text{--- (Equation 2)} $$
Substitute Equation 2 into Equation 1:
$$ 16a + 4(-8a) = 10 $$
$$ 16a - 32a = 10 \implies -16a = 10 \implies a = -\frac{10}{16} = -\frac{5}{8} $$
Now substitute the value of $a$ back into our acceleration formula:
$$ A = 2a = 2 \times \left(-\frac{5}{8}\right) = -\frac{5}{4}\ \text{m/sec}^2 $$
Step 4: Final Answer:
The acceleration of the particle is $- \frac{5}{4}\ \text{m/sec}^2$, which matches option (D).