Concept:
The Laplace transform converts time-domain differential models into easily solvable \(s\)-domain algebraic models. The standard integral definition of the Laplace transform for a continuous function \(f(t)\) is:
\[
\mathcal{L}\{f(t)\} = \int_{0}^{\infty} e^{-st} f(t) \, dt
\]
Step 1: Utilizing the standard identity formula.
We use the general identity for polynomial time functions:
\[
\mathcal{L}\{t^n\} = \frac{n!}{s^{n+1}}
\end{cases}
\]
For a linear ramp function, \(n = 1\). Substituting this integer into our standard formula yields:
\[
\mathcal{L}\{t^1\} = \frac{1!}{s^{1+1}} = \frac{1}{s^2}
\]
Step 2: Applying the linearity property.
The linearity property of Laplace transforms states that constants can be factored outside the operator:
\[
\mathcal{L}\{c \cdot f(t)\} = c \cdot \mathcal{L}\{f(t)\}
\]
Given \(f(t) = 3t\), we factor out the constant scalar 3:
\[
\mathcal{L}\{3t\} = 3 \cdot \mathcal{L}\{t\} = 3 \cdot \left(\frac{1}{s^2}\right) = \frac{3}{s^2}
\]
This calculation confirms option (C) as the correct choice.