For an elastic container, the compliance is the change in volume brought about by a unit change in pressure:
$$C = \frac{\Delta V}{\Delta P}$$
It is the reciprocal of elastance, which is the pressure exerted by the vessel against a given filling volume:
$$\text{Elastance}=\frac{\Delta P}{\Delta V}$$
Dynamic compliance is the apparent compliance that is measured in the presence of gas flow, i.e. during breathing.
$$C = \frac{\Delta V}{\Delta P}$$
$$C_{dyn} = \frac{TV}{PIP - PEEP}$$
This is affected by all the determinants of static compliance, but also by airway resistance and respiratory rate ('frequency dependence'). The latter is because
Static compliance is compliance measured in the absence of gas flow.
The compliance of the respiratory system is composed of the compliance of the chest wall and the compliance of the lung.
In this case, elastances add, not compliances. This is because the change in volume is constant across all the components, and the pressures are additive (consider stuffing one balloon inside another balloon and then inflating both balloons together. The total elastance is naturally the sum of the two balloon's elastances, since both are recoiling against the same volume).
Therefore
$$\text{Elastance}_{Total} = \text{Elastance}_{Lung} + \text{Elastance}_{wall}$$
$$\frac{1}{C_{Total}} = \frac{1}{C_{Lung}} + \frac{1}{C_{wall}}$$
\(C_{Lung}\) and \(C_{wall}\) are both about 200ml/cmH20, so \(C_{total}=200\mathrm{ml\ cmH2O^{-1}}\)
Specific compliance is compliance over FRC. Usual value is \(0.05 \mathrm{cmH2O^{-1}}\). 1cmH20 should drive five percent of FRC. For an adult with a 2L FRC, 1cmH2O should drive a \(\Delta V\) of 100mL (so a pressure support of 5cmH2O should drive a 500mL tidal volume).
Factors increasing \(C_{Lung}\)
Factors decreasing \(C_{Lung}\)
Factors increasing \(C_{Wall}\)
Factors decreasing \(C_{Wall}\)
For any given pressure, the lung volume is higher during expiration than during inspiration. This is due to: