Time Delays
A capnogram is produced by the sequential analysis of inspired
and expired gas flowing by the mainstream window, which is usually positioned just
proximal to the endotracheal tube or breathing mask, or sampled from a sidestream
sampling site connected to the breathing circuit. In the case of sidestream sampling,
a definite time delay is introduced by the length and volume of the tubing carrying
the sampled gas to the detector. This delay caused by the transfer of the sampled
gas into the reading cell can be minimized by using high flow rates for the sampling
flow and narrow, short tubing assemblies compatible with the position of the equipment
with respect to the patient breathing circuit. After the sampled gas reaches the
sensing cell, an additional delay is introduced by the rise time of each instrument.
The rise time is a characteristic delay induced by the exponential response to a
square front of changing gas concentration, in which CO2
concentration
changes instantaneously from zero to a new steady-state level (CO2ss
).
This can be described by the following exponential equation:
S = CO2ss
· (1 − e−t/τ
)
(24)
In Equation 24, S is the signal at time t, e is the base of natural logarithms (≅2.718),
and τ (tau) is the time constant. When t = τ (i.e., one time constant),
it is possible to calculate that S = 0.63 · CO2ss
(or 63%). This approach is used to measure the speed of response of the circuitry.
It is often presented in clinical instruments as a different fraction of the response,
such as the 10% to 90% response time (≅2.2 τ).
If we assume a square-wave capnogram for argument's sake as the
most difficult for an instrument to follow and assume a time constant of 100 msec
(a frequent value for a clinical instrument), it is theoretically possible to follow
respiratory profiles of CO2
within 5% of the real value (accuracy better
than 5%) up to respiratory rates of 100 breaths/min. In practice, most clinical
capnographs display this accuracy up to 60 breaths/min.[169]
A shared mass spectrometer, with the usually longer sampling line used in the share
configuration, may display significant inaccuracy at respiratory rates of about 40
breaths/min.[171]
The relative duration of inspiration
and expiration (I/E ratio) can also affect the accuracy of the recording instrument.
Standardized respiratory cycle profiles have been used to compare the most commonly
employed clinical instruments.[172]
Sidestream capnographs are susceptible to errors related to gas
diffusion. Radial diffusion of CO2
out of the tubing can cause artificially
low values.[173]
This error is related to the tubing
material and the length of exposure of the sample inside the tubing (i.e., related
to the sample flow rate and tubing length). Polyethylene and Teflon
tubing are much more permeable to CO2
than nylon. Axial diffusion across
the fronts of CO2
-rich boluses traveling along sampling lines can also
smear the upstrokes and the downstrokes of waveforms. This type of diffusion has
a significant effect on the interpretation of end-tidal CO2
at higher
respiratory frequencies.