Gas flows from areas of higher to lower pressure. The opposition to this flow is resistance.
In laminar conditions, \(\dot{V} \propto \Delta P\), so resistance is well defined (as the constant of proportionality). This is sometimes called "ohm's law for a pipe" by analogy with the linear electrical resistance seen in circuits.
In turbulent conditions, \(\dot{V} \propto \sqrt{\Delta P}\) and resistance is not well-defined.
Turbulence significantly increases opposition to flow.
In turbulent conditions, \(\dot{V} \propto \sqrt{\Delta P}\)
Reynold's Number is the ratio of a fluid's inertia and viscosity. Turbulence occurs when this quantity is >2000. In a pipe of fixed diameter,
$$Re = \frac{\rho V D}{\mu}$$
where \(\rho\) is density, V is fluid velocity, D is pipe diameter, and \(\mu\) is viscosity.
Confusingly, decreasing diameter would appear to decrease the Reynold's number. But, for a fixed gas flow Q, we have
$$Q = V \cdot \pi \left( \frac{D}{2} \right)^2$$
$$Q = V \cdot \pi \frac{D^2}{4}$$
$$V = \frac{4Q}{\pi D^2}$$
and therefore
$$Re = \frac{\rho 4Q D}{\mu \pi D^2}$$
$$Re = \frac{\rho 4Q}{\mu \pi D}$$
So, if gas flow (minute ventilation) is held constant, then a smaller diameter increases turbulence.
In laminar conditions, \(\dot{V} \propto \Delta P\), or \(\dot{V} = \frac{\Delta P}{R}\)
Resistance to laminar flow is given by the Hagen-Poiseuille equation.
$$R = \frac{8 l \mu}{\pi r ^ 4}$$
Where l is the pipe length, \(\mu\) is the viscosity, and r is the pipe radius.
Lung volume decreases resistance by expanding the airways through radial tension from the elastic tissues.
Airway radius is the most important, and is affected by:
Airway length is increased by circuit components e.g. increased by ETT, decreased by tracheostomy
Gas velocity (\(\therefore\) turbulence) is increased by a short inspiratory time or high respiratory rate.
Gas density (\(\therefore\) turbulence) can be reduced by heliox.
Resistance is much higher in infants.