Table 3.
Maneuver (n) | Gain | Phase | ||||||||||
---|---|---|---|---|---|---|---|---|---|---|---|---|
‐CO 2 | +CO 2 | ‐CO 2 | +CO 2 | |||||||||
ICC | Lower bound | Upper bound | ICC | Lower bound | Upper bound | ICC | Lower bound | Upper bound | ICC | Lower bound | Upper bound | |
SinTilt (Hz)(8) | ||||||||||||
0.042 | 0.288 | −0.250 | 0.774 | 0.407 | −0.405 | 0.848 | 0 | −0.524 | 0.629 | 0.318 | −0.490 | 0.816 |
0.067 | 0.453* | −0.072 | 0.842 | 0.717* | 0.105 | 0.936 | 0.348 | −0.093 | 0.783 | 0.587 | −0.132 | 0.901 |
0.1 | 0.804* | 0.362 | 0.956 | 0.950* | 0.791 | 0.990 | 0.333* | −0.024 | 0.757 | 0.679* | 0.093 | 0.924 |
0.167 | 0.778* | 0.277 | 0.950 | 0.751* | 0.175 | 0.944 | 0.788* | 0.293 | 0.953 | 0.815* | 0.345 | 0.960 |
PB (Hz) (7) | ||||||||||||
0.1 | 0.616 | −0.073 | 0.909 | 0.529 | −0.241 | 0.885 | 0.380 | −0.290 | 0.828 | 0.203 | −0.681 | 0.780 |
0.167 | 0.042 | −0.751 | 0.707 | 0 | −0.984 | 0.597 | 0.738* | 0.163 | 0.941 | 0.533 | −0.236 | 0.887 |
0.25 | 0 | −0.870 | 0.329 | 0 | −1.307 | 0.409 | 0.275 | −0.533 | 0.800 | 0 | −0.902 | 0.649 |
Rest 0.1 Hz | ||||||||||||
Supine (8) | 0.424 | −0.325 | 0.836 | 0.585* | −0.027 | 0.886 | 0.320 | −0.444 | 0.797 | 0.222 | −0.580 | 0.761 |
HUT 30° (7) | 0.145 | −0.746 | 0.785 | 0.044 | −0.904 | 0.755 | 0.142 | −0.772 | 0.786 | 0 | −1.037 | 0.659 |
HUT 70° (8) | 0.641* | 0.011 | 0.906 | 0.598* | −0.054 | 0.893 | 0.502* | −0.057 | 0.851 | 0.009 | −0.574 | 0.625 |
Intraclass correlation coefficients (agreement) during sinusoidal tilt (eight subjects), paced breathing at 30° HUT (PB) (seven subjects) and resting recordings in three body positions (7–8 subjects) who participated a second time almost a year after the first. Values are calculated separately for gain and phase and for each of the stimulus frequencies during SinTilt, PB, and rest, respectively (*indicates P ≤ 0.05). Inclusion of the absolute PETCO2 level during each stimulus as covariate in the ANOVA model increased ICC during SinTilt considerably. During PB only at 0.167 Hz and without PETCO2 in the model, a significant ICC could be determined. In the resting recordings, only at HUT 70° significant ICC values were present in both gain and phase. Values of 0 indicate that no valid ANOVA model was found. (Lower‐ and upper bounds are the 95% confidence limits.)