Step 1: Understanding the Concept:
In classical kinematics, the instantaneous velocity of a moving body is defined precisely as the time derivative of its position or displacement vector.
To find the exact time when the body briefly comes to rest, we must calculate the velocity function and explicitly set it equal to zero.
Step 2: Key Formula or Approach:
The instantaneous velocity $v$ is derived from the displacement $x$ using basic differential calculus: $v = \frac{dx}{dt}$.
Once the generalized expression for $v$ is obtained, solve the algebraic equation $v(t) = 0$ for time $t$.
Step 3: Detailed Explanation:
The given displacement function with respect to time is:
\[ x = -\frac{3}{4}t^2 + 12t + 3 \]
Differentiate this entire equation with respect to $t$ to find the instantaneous velocity $v$:
\[ v = \frac{d}{dt} \left( -\frac{3}{4}t^2 + 12t + 3 \right) \]
Applying basic power rule differentiation:
\[ v = -\frac{3}{4}(2t) + 12(1) + 0 \]
\[ v = -\frac{3}{2}t + 12 \]
To precisely find when the velocity becomes absolute zero, we set $v = 0$:
\[ -\frac{3}{2}t + 12 = 0 \]
Rearranging the simple linear equation:
\[ \frac{3}{2}t = 12 \]
\[ t = 12 \times \frac{2}{3} \]
\[ t = \frac{24}{3} = 8\text{ s} \]
Step 4: Final Answer:
The velocity of the moving body drops to zero exactly after $8\text{ s}$.