Step 1: Expression for \(S\).
\[
S(\omeg(A) = \frac{\alpha \omega}{\tau + \rho \omega}.
\]
Here, \(\alpha, \tau, \rho>0\) and \(\omega>0\).
Step 2: Differentiate to check monotonicity.
Treating \(\omega\) as a continuous variable:
\[
\frac{dS}{d\omega} = \frac{(\alph(A)(\tau + \rho \omeg(A) - (\alpha \omeg(A)(\rho)}{(\tau + \rho \omeg(A)^2}.
\]
Simplify numerator:
\[
\frac{dS}{d\omega} = \frac{\alpha \tau + \alpha \rho \omega - \alpha \rho \omega}{(\tau + \rho \omeg(A)^2}
= \frac{\alpha \tau}{(\tau + \rho \omeg(A)^2}.
\]
Step 3: Sign of derivative.
Since \(\alpha, \tau, \rho, \omega>0\), both numerator and denominator are positive. Hence:
\[
\frac{dS}{d\omega}>0.
\]
Therefore, \(S\) is a strictly increasing function of \(\omega\).
Step 4: Behavior as \(\omega \to \infty\).
As \(\omega \to \infty\),
\[
S(\omeg(A) \to \frac{\alpha}{\rho},
\]
a finite asymptote, but the increase is monotonic from \(0\) upwards.
\[
\boxed{S \text{ increases as } \omega \text{ increases.}}
\]