Concept:
The steady, laminar flow of an incompressible, Newtonian fluid (such as simplified blood flow) through a rigid, cylindrical tube of constant cross-section is governed mathematically by Hagen-Poiseuille's Law. The fundamental equation states:
\[
Q = \frac{\pi \cdot \Delta P \cdot r^4}{8 \cdot \eta \cdot L}
\]
where:
• $Q$ = Volumetric fluid flow rate
• $\Delta P$ = Hydrostatic pressure drop across the vessel length
• $r$ = Internal radius of the vessel
• $\eta$ = Dynamic coefficient of fluid viscosity
• $L$ = Total axial length of the vessel segment
Step 1: Translating radius into diameter terms.
The internal radius ($r$) is equal to exactly half of the total vessel diameter ($d$), or $r = \frac{d}{2}$. Substituting this into our fluid equations gives:
\[
Q = \frac{\pi \cdot \Delta P \cdot \left(\frac{d}{2}\right)^4}{8 \cdot \eta \cdot L} = \frac{\pi \cdot \Delta P \cdot d^4}{128 \cdot \eta \cdot L}
\]
Step 2: Evaluating proportional relationships.
From this equation, we can separate the variables into direct and inverse proportionalities:
• Direct Proportionality (Numerator): The flow rate $Q$ is directly proportional to the pressure drop ($\Delta P$) and to the fourth power of the diameter of the vessel ($d^4$).
• Inverse Proportionality (Denominator): The flow rate $Q$ is inversely proportional to the vessel length ($L$) and fluid viscosity ($\eta$).
Evaluating the choices shows that Option (C) correctly identifies the parameters that share a direct proportional relationship with flow rate.