Concept:
In kinematics, the position or displacement of an object is given as a function of time, \(S(t)\).
• The instantaneous velocity \(v(t)\) is defined as the first time-derivative of the displacement function:
\[
v = \frac{dS}{dt}
\]
• When an object is said to “come to rest”, its instantaneous linear velocity drops to exactly zero (\(v = 0\)).
Step 1: Compute the velocity function \(v\)
Given the displacement equation:
\[
S = 72t + 3t^2 - t^3
\]
Differentiating each term with respect to the independent variable \(t\) using the power rule (\(\frac{d}{dt}(t^n) = n t^{n-1}\)):
\[
v = \frac{dS}{dt} = \frac{d}{dt}(72t) + \frac{d}{dt}(3t^2) - \frac{d}{dt}(t^3)
\]
\[
v = 72(1) + 3(2t) - 3t^2
\]
\[
v = 72 + 6t - 3t^2
\]
Step 2: Set the velocity equation equal to zero
To find the exact timestamp when the particle is completely stationary (at rest), equate \(v\) to \(0\):
\[
72 + 6t - 3t^2 = 0
\]
Let us rearrange this into a standard quadratic equation format (\(at^2 + bt + c = 0\)) by multiplying the entire expression by \(-1\):
\[
3t^2 - 6t - 72 = 0
\]
Divide every term by the common coefficient factor of $3$ to simplify the quadratic factorization:
\[
t^2 - 2t - 24 = 0
\]
Step 3: Factorize the quadratic equation
We need two numbers that multiply to give \(-24\) and add together to form \(-2\). These numbers are \(-6\) and \(+4\). Split the middle linear term:
\[
t^2 - 6t + 4t - 24 = 0
\]
Group terms by factoring out common values:
\[
t(t - 6) + 4(t - 6) = 0
\]
\[
(t - 6)(t + 4) = 0
\]
This leaves us with two potential mathematical root solutions for the time variable:
\[
t - 6 = 0 \quad \Rightarrow \quad t = 6 \text{ seconds}
\]
\[
t + 4 = 0 \quad \Rightarrow \quad t = -4 \text{ seconds}
\]
Step 4: Filter out extraneous solutions
Since time elapsed cannot be a negative value in real physical situations (\(t \ge 0\)), we discard \(t = -4\).
Therefore, the single valid time calculation is \(t = 6\) seconds.