Background: Intratracheal pressure (P(trach)) should be the basis for
analysis of lung mechanics. If measured at all, P(trach) is usually as
sessed by introducing a catheter into the trachea via the lumen of the
endotracheal tube (ETT). The authors propose a computer-assisted meth
od for calculating P(trach) on a point-by-point basis by subtracting t
he flow-dependent pressure drop DELTAP(ETT)(V) across the ETT from the
airway pressure (P(aw)), continuously measured at the proximal end of
the ETT. Methods. The authors measured the pressure-flow relationship
of adult endotracheal tubes with different diameters (ID, 7-9 mm) at
different lengths and of tracheostomy tubes (ID, 8-10 mm) in the labor
atory. The coefficients of an approximation equation were fitted to th
e measured pressure-flow curves separately for inspiration and expirat
ion. In 15 tracheally intubated patients under volume-controlled venti
lation and spontaneous breathing, the calculated P(trach) was compared
with the measured P(trach). Results. The authors present the coeffici
ents of the ''nonlinear approximation'': DELTAP(ETT) = K1 . V(K2), wit
h DELTAP(ETT) being the pressure drop across the ETT and K1 and K2 bei
ng the coefficients relating V to DELTAP(ETT). An important result was
an inspiration/expiration asymmetry: the pressure drop caused by the
inspiratory flow exceeds that of the expiratory flow. A complete descr
iption of the pressure-flow relationship of an ETT, therefore, require
s a set of four coefficients: K1I, K2I, K1E, and K2E. The reason for t
his asymmetry is the abrupt sectional change between ETT and trachea a
nd the asymmetric shape of the swivel connector. Comparison of calcula
ted and measured P(trach) in patients gives a correspondence within +/
- 1 cmH2O (mean limits of agreement). The mean root-meansquare (rms) d
eviation is 0.55 cmH2O. Conclusions: P(trach) can be monitored by comb
ining our ETT coefficients and the flow and airway pressure continuous
ly measured at the proximal end of the ETT.