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Poiseuille’s Law

Definition

Poiseuille’s Law (or the Hagen-Poiseuille equation) describes the pressure drop required to maintain a steady, laminar flow of an incompressible, viscous fluid through a long, cylindrical pipe of constant cross-section. It dictates the relationship between flow rate, pressure gradient, fluid viscosity, and pipe geometry.

Q=πr4ΔP8ηLQ = \frac{\pi r^4 \Delta P}{8 \eta L} How to read: Volumetric flow rate Q equals pi times radius r to the fourth power, times the pressure difference delta P, all divided by eight times dynamic viscosity eta times the length of the pipe L. Meaning / when to use: Used to calculate the flow rate QQ of a fluid given a specific pressure drop ΔP\Delta P, or vice versa. The most critical feature is the profound r4r^4 dependency.

Why It Matters

This law is the governing principle behind microfluidics, plumbing, and cardiovascular physiology. Because flow rate scales with the fourth power of the radius, a tiny decrease in a tube’s diameter causes a catastrophic drop in flow. In medicine, if plaque reduces an artery’s radius by half, the heart must pump 16 times harder to maintain the same blood flow. Ignoring this non-linear geometric scaling leads to failed engineering designs and fatal medical misdiagnoses.

Core Concepts

  • Fourth Power Dependency (r4r^4): The dominant variable in the equation. Radius matters exponentially more than length, viscosity, or pressure.
  • Laminar Flow Constraint: The law only applies to smooth, layered, non-turbulent flow (low Reynolds number). If the fluid moves too fast and becomes turbulent, resistance spikes and the equation fails.
  • No-Slip Boundary Condition: The fluid velocity is assumed to be exactly zero right at the walls of the pipe, with maximum velocity in the direct center, creating a parabolic velocity profile.
  • Viscosity (η\eta): The internal friction of the fluid. Thicker fluids (like honey) require proportionally more pressure to move than thin fluids (like water).

Connected Concepts