Journal of Applied Physiology
Vol. 82, No. 2,
pp. 667-677,
February 1997
CONTROL OF BREATHING, CIRCULATION, AND TEMPERATURE
Extended models of the ventilatory response to sustained
isocapnic hypoxia in humans
Pei-Ji
Liang,
Daphne A.
Bascom, and
Peter A.
Robbins
University Laboratory of Physiology, Parks Road, Oxford OX1 3PT,
United Kingdom
ABSTRACT
INTRODUCTION
METHODS
RESULTS
DISCUSSION
ACKNOWLEDGEMENTS
FOOTNOTES
REFERENCES
ABSTRACT
Liang, Pei-Ji, Daphne A. Bascom, and Peter A. Robbins.
Extended models of the ventilatory response to sustained isocapnic hypoxia in humans. J. Appl. Physiol. 82(2): 667-677, 1997.
The purpose of this study was to examine extensions of a model
of hypoxic ventilatory decline (HVD) in humans. In the original model (model I) devised by R. Painter, S. Khamnei, and P. Robbins
(J. Appl. Physiol. 74: 2007-2015, 1993
[Medline]
), HVD is modeled
entirely by a modulation of peripheral chemoreflex sensitivity. In the
first extension (model II), a more complicated dynamic is used
for the change in peripheral chemoreflex sensitivity. In the second
extension (model III), HVD is modeled as a combination of
both the mechanism of Painter et al. and a component that is
independent of peripheral chemoreflex sensitivity. In all cases, a
parallel noise structure was incorporated to describe the stochastic
properties of the ventilatory behavior to remove the correlation of the
residuals. Data came from six subjects from a study by D. A. Bascom, J. J. Pandit, I. D. Clement, and P. A. Robbins (Respir. Physiol.
88: 299-312, 1992). For model II, there was a significant
improvement in fit for two out of six subjects. The reasons for this
were not entirely clear. For model III, the fit was again
significantly improved in two subjects, but in this case the subjects
were those who had the most marked undershoot and recovery of
ventilation at the relief of hypoxia. In these two subjects, the
chemoreflex-independent component contributed ~50% to total HVD.
In the other four subjects, the chemoreflex-independent component
contributed ~10% to total HVD. It is concluded that in some
subjects, but not in others, there may be a component of HVD that
is independent of peripheral chemoreflex sensitivity.
sustained isocapnic hypoxia; hypoxic ventilatory decline; peripheral chemoreflex sensitivity
INTRODUCTION
THE VENTILATORY RESPONSE to sustained hypoxia is
biphasic: there is an initial rapid increase in ventilation, which is
then followed by a slow decline (7, 18). This slow decline is known
variously as hypoxic ventilatory decline or depression (HVD) or hypoxic
ventilatory "roll-off."
In anesthetized animals, HVD may be independent of the peripheral
chemoreflex sensitivity, since 1) in anesthetized cats, the
peripheral chemoreflex sensitivity to CO2 is unchanged
during HVD induced by central hypoxia (16); 2) in anesthetized
cats, the rapid ventilatory response at the onset and relief of hypoxia is almost symmetrical (4); and 3) respiratory depression during hypoxia has been a consistent finding in anesthetized animals that have
undergone peripheral chemodenervation (12).
In conscious humans, however, HVD may arise predominantly through an
alteration of peripheral chemoreflex sensitivity. The evidence for this
is as follows: 1) the rapid ventilatory response at the relief
of sustained hypoxia is much smaller than the rapid response at the
onset of the period of hypoxia (6, 7, 9); 2) the reintroduction
of hypoxia after a brief relief from sustained hypoxia will cause a
ventilatory response with a smaller magnitude compared with the first
exposure to hypoxia (3, 8); and 3) brief exposures to
additional hypoxia during the development of HVD elicit progressively
smaller ventilatory responses as the HVD develops (2).
On the basis of the above findings, Painter et al. (13) developed a
mathematical model to describe HVD during sustained hypoxia in humans
in which HVD arises as the result of a progressive decline in
peripheral chemoreflex sensitivity. The ventilatory response to
sustained hypoxia and the asymmetrical magnitudes of the ventilatory
on- and off-transients at the onset and relief of hypoxia are both
described well by this model. However, as noted by Painter et al., this
model fails to describe very well the ventilatory behavior after the
step out of hypoxia in cases in which there may be some undershoot and
subsequent recovery of the ventilatory response. One possible cause is
that the assumptions about the dynamics are too simple. Another
possible cause of the undershoot and recovery sometimes observed at the
relief of hypoxia might be the existence of an additional component of
HVD in conscious humans, which is independent of peripheral chemoreflex
sensitivity, as has been described in the studies relating to
anesthetized animals.
The purpose of the present study was to explore extensions to the model
of Painter et al. First, we wished to explore whether the dynamics of
the model were too simple. Second, we wished to explore whether there
is an additional component for HVD that is not related to the
peripheral chemoreflex sensitivity. In particular, we wished to
determine 1) whether either extension would improve the fit of
the model to the data at the relief of hypoxia and 2) in the
case of the model with the additional component for HVD, what
proportion of HVD would be attributed to the component that is
independent of the peripheral chemoreflex sensitivity.
In the original model of Painter et al., the parameter estimation was
performed with a simple least squares fitting technique (this
corresponds to a measurement-only noise model). With respiratory data,
use of this technique generally results in residuals that are
correlated, and this can make statistical comparisons between different
models difficult. To overcome this, a parallel noise structure was used
in conjunction with the deterministic models to remove this
correlation. The noise model was fitted by using a Kalman filter
algorithm.
METHODS
Data
Data were taken from a previous study performed in our laboratory (3).
Each experiment lasted 40 min. End-tidal PO2
(PETO2) was held at 100 Torr for the first 10 min, at 50 Torr for the next 20 min,
at 100 Torr for the next 5 min, and at 50 Torr for the final 5 min.
End-tidal PCO2
(PETCO2) was kept constant throughout the experiment at 2-3 Torr above the subject's natural value. Minute ventilation (
E) was measured
breath by breath. Data were available from six subjects, with three to
six repeats of the protocol on each subject.
Both the strength of the stimulus
(PETO2 = 50 Torr) and
background PETCO2 were the
same as for the data used by Painter et al. (13). However, the data
differ in the sense that the protocol used to generate the data modeled
in the present study was prolonged to allow for the reintroduction of
hypoxia to provide a second on-transient. In the data modeled by
Painter et al., there was no second on-transient. This second
on-transient may help to discriminate between a component of HVD that
arises through modulation of peripheral chemoreflex sensitivity and a
component that does not act via such a mechanism.
Models
Model of Painter et al. (13) (model I).
The model of Painter et al. can be written in the form
|
(1)
|
|
(2)
|
|
(3)
|
where
c and
p
represent the central and peripheral chemoreflex contributions to
E, respectively. In Eq. 2,
Tp denotes the time constant for the rapid
peripheral chemoreflex response; (1
S) is the hypoxic stimulus,
where S represents the arterial oxygen saturation as used by Painter et
al. as
|
(4)
|
dp
is the peripheral time delay; kp is a nonnegative
peripheral offset; and gp represents the
peripheral chemosensitivity to hypoxia, which is a variable determined
by a first-order dynamic process described by Eq. 3. In Eq. 3, Th denotes the time constant associated with the
development of HVD; g100 denotes the steady-state chemoreflex sensitivity in hyperoxia when S = 1.0; and gh
denotes the ratio of the sensitivity decrease to the decrease in S. Both g100 and gh are constrained to be
positive.
In the original formulation, Painter et al. (13) used a parameter
kh, whereas in the present formulation the parameter
g100 has been used. The relationship between these two
parameters is given by
|
(5)
|
There were two reasons for preferring our revised
parametrization of the model by Painter et al. First, g100,
the hypoxic sensitivity after exposure to hyperoxia, is a more
intuitive parameter than kh in a physiological sense.
Second, gh and kh appeared to be highly
correlated in the study of Painter et al., whereas there appeared to be
much less correlation between gh and gh + kh ( g100, see Table 1 in Ref. 13).
Assuming that both saturation S and gain gp
remain constant throughout the breath, these differential equations can
be solved to provide a set of difference equations that can be written
as
|
(6)
|
|
(7)
|
|
(8)
|
where
tn refers to the time of the nth breath.
Model incorporating second-order dynamics for gp (model
II).
In the model of Painter et al. (13), a first-order dynamic was chosen
for gp. To explore whether this choice of
dynamic was too simple, a more complicated dynamic was chosen to
determine whether such a change could provide a significant improvement in the fit. The particular dynamic chosen was second-order, and, in a
sense, it represents the next level of sophistication that could be
introduced. The model can be written
as
|
(9)
|
|
(10)
|
|
(11)
|
|
(12)
|
where
I is an intermediate variable, and TI is the time
constant for this additional process.
Assuming, as before, that saturation and gp remain constant
throughout a breath, the difference equations
become
|
(13)
|
|
(14)
|
|
(15)
|
|
(16)
|
Model incorporating additional component for HVD (model
III).
The original model of Painter et al. (13) describes the whole of the
hypoxic ventilatory decline as arising from a modulation of peripheral
reflex sensitivity. The object of this extended model is to introduce a
component of HVD (
d) that may be
independent of the peripheral chemoreflex. This model can be written as
|
(17)
|
where
|
(18)
|
where
c and
p
have the same meaning as for model I; gd is a
nonpositive gain term, which is constant, independent of S; and
Td is a time constant. Again, assuming the saturation
remains constant throughout a breath, a difference equation for the new component can be written as
|
(19)
|
The time delay for this component is assumed to be the same
as for the sensitivity-related component dp.
Fitting Technique
Simple least squares parameter estimations.
The approach to estimating parameter values adopted by Painter et al.
(13) was to use a simple least squares fitting technique. With this
technique, the objective function to be minimized
is
|
(20)
|
where
Emeas denotes the measured
value and
Edet is the
deterministic output from the model. This fitting procedure was initially used for the model by Painter et al. to examine the effects
of incorporating a more complicated noise model (see
RESULTS, Fitting Technique).
Parameter estimation by using a Kalman filter.
One problem associated with estimating the parameters of the
deterministic models is that successive breaths are not independent (14). On the basis of a previous study of breathing during steady levels of stimulation (10), the stochastic behavior was modeled by
using a parallel noise process of the form
|
(21)
|
|
(22)
|
where
x(n) and y(n) are the system state
and observation for the parallel noise component at the nth
breath, respectively; f is the system gain; and
v(n) and w(n) are mutually
independent white Gaussian noise processes with means of zero and a
constant variance ratio of
Rv/Rw, respectively. Thus the
model output (
Eout) for the
ventilatory response to the stimulus can be written as the sum of the
deterministic component
Edet
and the stochastic component
x
|
(23)
|
To
determine an estimate for the stochastic component
x(n), a Kalman filter algorithm was employed. The
prediction and update values for the system state of the noise
component were calculated as follows
|
(24)
|
|
(25)
|
and the prediction and update of a modified variance (10)
are given by
|
(26)
|
|
(27)
|
where
|
(28)
|
is the Kalman gain at the (n + 1)th breath.
The physiological parameters of the deterministic models along with the
two parameters of the stochastic model ( f,
Rv/Rw) can now be estimated
by minimizing the sum of the squared prediction errors of the model,
which is given by
|
(29)
|
where
Emeas denotes the measured
value.
Minimization process.
The simple least squares objective function (Eq. 20) and the
objective function for the Kalman filter (Eq. 29) were
minimized by using a standard Numerical Algorithms Group (Oxford, UK)
subroutine (E04FDF) that finds an unconstrained minimum of a sum of
squared residuals. The fitting procedure was repeated over a range of fixed values for dp for each data set. The value for
dp corresponding with the lowest sum of squared error was
regarded as the optimal value for dp for the data set.
In the study from which the data are taken (3), the authors report that
the speed of the initial ventilatory response to the rapid changes of
PETO2 appeared to be different at the
different stages in the protocol. Thus, instead of fitting a single
value for the fast time constant Tp, separate values for
the time constant were fitted for the onset, relief, and the second
on-transient of the hypoxic stimulus (Tp1,
Tp2, and Tp3, respectively).
Goodness of fit.
The improvement of the fit with the extended models, as compared with
the original model, was assessed using an F-ratio test on the
sum of squared prediction errors (1). The F statistic is given
by
|
(30)
|
where
RSS1 and df1 refer to the residual sum of
squares and the degrees of freedom, respectively, for the original
model; and RSS2 and df2 refer to the residual
sum of squares and the degrees of freedom, respectively, for the
extended model. Tests were conducted on a subject-by-subject basis, and
so the sum of squares and degrees of freedom were accumulated across
the individual repeats of the protocol and fits of the model on each
individual subject.
Parameter values for each subject.
Overall parameter values for each subject for each model were obtained
by using a technique employed by Swanson and Bellville (15) in their
study of modeling the ventilatory responses to CO2. First,
an idealized stimulus of 5-min euoxia
(PETO2 = 100 Torr), 20-min hypoxia
(PETO2 = 50
Torr), 5-min euoxia (PETO2 = 100 Torr), and,
finally, 5-min hypoxia (PETO2 = 50 Torr) was used to generate model ventilatory responses from each individual parameter set associated with each individual experimental repeat of
the protocol (the time duration for each breath was idealized as 3 s).
For each subject, this gave between three and six sets of calculated
responses to the idealized stimulus (one response corresponding to each
individual parameter set obtained from a single experimental record).
The responses were then averaged to give the average responses for that
subject to the idealized stimulus. Next, a single set of parameters was
estimated from the average response to this idealized stimulus (no
noise model is necessary, as there is no noise). This set of parameters
is taken as the overall estimate for that particular subject and model.
Sensitivity Analysis
To determine whether the parameters of the model were theoretically
identifiable, a sensitivity analysis was undertaken.
Model data were generated for the input function associated with the
protocol. The more complex extended model (model III) was
used with a set of physiologically reasonable parameter values (actually, the parameter values determined for subject 758) and a breath duration of 3 s. The model parameters were then estimated repeatedly for the data set, with the exception that one of the parameters would be fixed, in turn, to the value used to generate the
data and then to values ranging from 80 to 120% of this value (except
for kp, where a range of 0.0-0.02 was used, since its value is close to zero). The sum of squared residuals could then be
plotted against the value of the fixed parameter. If the parameter is
not identifiable, then the plot should be flat, whereas if the value of
the parameter affects the fit, then the plot should have a definite
minimum (zero) at the parameter value used to generate the data.
RESULTS
Sensitivity Analysis
The results for the sensitivity analysis are shown in Fig.
1. For all parameters, a minimum (zero) for
the sum of squared residuals can be observed at the parameter value
used to generate the data set. This indicates that all the parameters
are theoretically identifiable in the model with the input function
used to generate the data. However, the sensitivity of the sum of
squared residuals to variations in parameter value varies considerably
for the different parameters, and in some cases the sensitivity plots
are quite asymmetric. The importance or lack of it of these features is difficult to gauge.
Fig. 1.
Sensitivity analysis for parameters of model III. x-Axis,
percentage variations in parameter value from that used to generate the
model response (except for kp, where range of real values is shown); y-axis, sum of squared residuals. See text for
definitions.
[View Larger Version of this Image (19K GIF file)]
Fitting Technique
The effect on the residuals of incorporating the noise model in the
Kalman filter technique is illustrated in Fig.
2. A large degree of autocorrelation is
seen in the residuals from the simple least squares fitting process,
which appears to have been almost totally removed by incorporating the
parallel noise structure. Results from the portmanteau test
demonstrated that all 31 sets of residuals from the simple least
squares fitting algorithm were significantly nonwhite, with P
values close to zero, whereas only 5 out of 31 sets of residuals from
the model using a Kalman filter algorithm were found to be nonwhite.
These five sets of nonwhite residuals were still much less correlated
than the ones from the simple least squares fitting technique.
Fig. 2.
Autocorrelation functions (ACF) for the residuals. Top, model I
fitted with a simple least squares fitting technique; next, from
top to bottom, models I, II, and III fitted by
using a Kalman filter. Values are averages across entire data set.
[View Larger Version of this Image (16K GIF file)]
Average parameter values from both the simple least squares fitting
technique and the Kalman filter algorithm are shown for the model by
Painter et al. (13) in Table 1. In general,
the parameter estimates from the two techniques appear quite similar. However, for the time constants associated with the rapid on-transients (Tp1,
Tp3), the Kalman filter algorithm
consistently yielded lower values than did the simple least squares
fitting procedure. For the time constant for the hypoxic ventilatory
decline Th, the reverse was true, with the values from the
Kalman filter algorithm being consistently higher than those from the
simple least squares fitting procedure. Consistent effects across all
the six subjects are significant at the level P < 0.05 (sign
test) and suggest some element of bias in estimating these values with
a simple least squares fitting routine.
Table 1.
Parameter values estimated by using least squares fitting
technique and by using a Kalman filter for each subject for model I
| Subject No. |
c, l/min
|
g100, l/min |
gh, l/min
|
kp |
Tp1, s
|
Tp2, s |
Tp3,
s |
Th, s |
dp, s
|
|
| Least squares |
| 743
|
12.7 |
139 |
295 |
0.06 |
48.1 |
5.3 |
33.9 |
205
|
0 |
| 758 |
8.8 |
79 |
272 |
0.05 |
51.2 |
3.2 |
56.8
|
296 |
0 |
| 766 |
6.6 |
92 |
433 |
0.01 |
24.7 |
4.7
|
11.5 |
759 |
0 |
| 796 |
14.7 |
59 |
244 |
0.06
|
17.9 |
1.6 |
3.9 |
299 |
1 |
| 818 |
18.7 |
257
|
1,436 |
0.02 |
8.9 |
6.7 |
33.4 |
344 |
0
|
| 824 |
15.0 |
222 |
804 |
0.02 |
27.1 |
30.9
|
19.5 |
312 |
0 |
| Kalman
filter |
| 743 |
14.4 |
136 |
273 |
0.04 |
31.2
|
4.8 |
26.7 |
273 |
0 |
| 758 |
10.2 |
84 |
335 |
0.03
|
46.8 |
3.9 |
56.3 |
315 |
0 |
| 766 |
6.5 |
88 |
407
|
0.01 |
15.6 |
5.7 |
5.8 |
832 |
0 |
| 796 |
12.7 |
50
|
165 |
0.11 |
2.5 |
1.2 |
0.8 |
380 |
3 |
| 818 |
18.3
|
249 |
1,006 |
0.03 |
6.3 |
4.1 |
18.7 |
392 |
2
|
| 824 |
16.0 |
210 |
729 |
0.01 |
12.3 |
16.3 |
12.1
|
359 |
0 |
|
|
See text for symbol definitions.
|
|
Model Comparison
Figure 3 shows one example of the
respiratory data together with the model fits for the three models.
(Model fits for the model by Painter et al. (13) when using the simple
least squares fitting procedure are not shown, as the appearance was
essentially identical to the appearance of the results for the
deterministic component with the use of the Kalman filter algorithm.)
Figure 3, left, shows the fit for model I developed by
Painter et al. (13), Fig. 3, center, shows the fit for
model II, which has second-order dynamics for gp,
and Fig. 3, right, shows the fit for model III, which
incorporates the additional component of HVD, independent of
chemoreflex sensitivity. Figure 3, bottom left (which shows the
deterministic component of the output for model I)
illustrates clearly for this particular data set that the simpler model
of Painter et al. can describe most of the experimental record
reasonably well, but that the model does not reflect particularly well
the transient undershoot in ventilation at the relief of the stimulus.
This aspect of the fit does not seem to be improved by model
II, but the introduction of the extra chemoreflex-insensitive component of model III greatly improves the fit to this part of the record.
Fig. 3.
A comparison between original model and extended models for 1 set of
experimental observations. Left panels, Model I; center panels,
model II; and right panels, model III. Top panels show experimental input (end-tidal PO2 and
PCO2); middle panels illustrate model
prediction and residuals with a Kalman filter (solid line for model
outputs and dots for experimental observations); bottom panels
illustrate deterministic component of the model and associated residuals (solid lines for calculated values and dots for experimental observations).
E, minute ventilation.
[View Larger Version of this Image (30K GIF file)]
Figure 4 shows average data and model fits
for each subject for model I, Fig.
5 shows these data for model II,
and Fig. 6 shows these data for model
III. These were calculated from the individual data sets and model
fits by interpolating the data every 3 s and then averaging across all
the individual responses for each subject. The average of the residuals
sequences for each subject was calculated in the same way, and the 95%
confidence intervals (calculated as ±1.96 SE) were plotted along with
the averaged ventilatory output. For much of the response, the outputs of all three models are very similar. However, for the two subjects (subjects 758, 796) who show the greatest undershoot and
recovery at the relief of hypoxia, model III appears to
describe this process more accurately than do the other two models.
Fig. 4.
Ventilatory responses and model fit for model I for all
subjects (averaged over 3-s intervals). Top section for each
subject (identified by no. on top right) shows averaged
experimental data (dots) and the deterministic component of model
response (lines); bottom section for each subject shows the
95% confidence intervals for associated residuals.
[View Larger Version of this Image (20K GIF file)]
Fig. 5.
Ventilatory responses and model fit for model II for all
subjects (averaged over 3-s intervals). Top section for each
subject (identified by no. on top right) shows averaged
experimental data (dots) and the deterministic component of model
response (lines); bottom section for each subject shows the
95% confidence intervals for associated residuals.
[View Larger Version of this Image (19K GIF file)]
Fig. 6.
Ventilatory responses and model fit for model III for all
subjects (averaged over 3-s intervals). Top section for each
subject (identified by no. on top right) shows averaged
experimental data (dots) and the deterministic component of model
response (lines); bottom section for each subject shows the
95% confidence intervals for associated residuals.
[View Larger Version of this Image (19K GIF file)]
When model II is compared with model I, F-ratio tests
on the sum of squared prediction errors revealed that there was no
significant improvement in fit for four out of the six subjects but
there was an improvement in fit for the other two (subjects 766, 824). Careful inspection of Figs. 4 and 5 suggests that there may
have been some improvement in the fit during the on-transients, but no
improvement was observed during the recovery from hypoxia, where visual
inspection suggests the fit is least good.
When model III is compared with model I, F-ratio tests
revealed that there was, again, no significant improvement in fit for four out of the six subjects but that for the two other subjects (subjects 758, 796) model III fitted significantly
better than model I. Visual inspection of Figs. 4 and 6
suggests that for these two subjects the undershoot and recovery in
ventilation were most marked and that model III did
produce an apparent improvement in fit to this portion of the response.
A whiteness test (portmanteau test) on the prediction errors showed
that 26 out of 31 sequences could be accepted as white for model
I, 27 out of 31 sequences for model II, and 28 out of 31 sequences for model III. Thus fitting a stochastic component to
the data makes the use of an F-ratio test possible without the
complications of trying to correct the degrees of freedom for
correlation present within the residuals.
Overall parameter values for each subject for each model are shown in
Table 2. For all three models, the time
constants for the rapid ventilatory response to the onset and
the relief of hypoxia (Tp1, Tp2,
and Tp3) are faster than the time constant for the slow change in the peripheral chemoreflex sensitivity Th. In most cases, the time constant for the rapid
ventilatory response at the relief of hypoxia (Tp2)
appears faster than those for the rapid ventilatory response at the
onset of hypoxia (Tp1 and Tp3).
However, this effect does not reach statistical significance overall.
Table 2.
Parameter values estimated by using a Kalman filter for each subject
for each model
| Subject No. |
c, l/min
|
g100, l/min |
gh, l/min
|
kp |
Tp1, s
|
Tp2, s |
Tp3,
s |
Th, s |
gd, l/min
|
Td, s |
TI, s
|
dp, s |
f
|
Rv/Rw |
P Value
(F Ratio) |
|
| Model I
|
| 743 |
14.4 |
136 |
273 |
0.04 |
31.2 |
4.8 |
26.7
|
273 |
|
|
|
0 |
0.74 |
2.39 |
| 758 |
10.2 |
84
|
335 |
0.03 |
46.8 |
3.9 |
56.3 |
315 |
|
|
|
0
|
0.65 |
3.01 |
| 766 |
6.5 |
88 |
407 |
0.01 |
15.6
|
5.7 |
5.8 |
832 |
|
|
|
0 |
0.81 |
0.59 |
| 796
|
12.7 |
50 |
165 |
0.11 |
2.5 |
1.2 |
0.8 |
380
|
|
|
|
3 |
0.81 |
1.02 |
| 818 |
18.3 |
249 |
1,006
|
0.03 |
6.3 |
4.1 |
18.7 |
392 |
|
|
|
2 |
0.67
|
1.78 |
| 824 |
16.0 |
210 |
729 |
0.01 |
12.3
|
16.3 |
12.1 |
359 |
|
|
|
0 |
0.87 |
0.53
|
| Model II |
| 743 |
18.8
|
121 |
189 |
0.01 |
29.3 |
3.9 |
19.4 |
141
|
|
|
141 |
0 |
0.75 |
3.49 |
NS |
| 758 |
10.9
|
68 |
238 |
0.02 |
40.4 |
2.9 |
39.6 |
101
|
|
|
239 |
0 |
0.65 |
3.00 |
NS |
| 766 |
6.8
|
70 |
226 |
0.0 |
15.5 |
5.2 |
4.5 |
287 |
|
|
287
|
0 |
0.77 |
0.65 |
<0.05 |
| 796 |
13.0 |
48 |
148
|
0.09 |
5.7 |
3.9 |
1.2 |
293 |
|
|
0.2 |
1 |
0.81
|
1.03 |
NS |
| 818 |
19.6 |
207 |
727 |
0.02
|
5.1 |
3.2 |
13.3 |
279 |
|
|
88 |
2 |
0.68 |
2.48
|
NS |
| 824 |
17.1 |
184 |
549 |
0.01
|
12.3 |
14.5 |
10.3 |
168 |
|
|
168 |
0 |
0.84
|
0.47 |
<0.05 |
| Model
III |
| 743 |
20.2 |
136 |
281 |
0.0 |
27.8
|
4.1 |
23.5 |
328 |
12.4 |
300 |
|
0 |
0.77
|
1.94 |
NS |
| 758 |
12.5 |
135 |
352 |
0.0
|
46.1 |
15.0 |
53.3 |
324 |
55.4 |
52 |
|
0
|
0.60 |
4.12 |
<0.05 |
| 766 |
7.2 |
91 |
431 |
0.0
|
20.4 |
5.4 |
6.9 |
869 |
4.5 |
232 |
|
0 |
0.72
|
0.74 |
NS |
| 796 |
16.7 |
102 |
252 |
0.0
|
11.5 |
1.9 |
5.4 |
499 |
53.1 |
22 |
|
3 |
0.76
|
1.25 |
<0.05 |
| 818 |
18.5 |
248 |
1,009 |
0.03
|
6.2 |
2.8 |
18.7 |
395 |
0.0 |
|
|
2 |
0.67
|
1.80 |
NS |
| 824 |
19.0 |
213 |
723 |
0.0
|
16.1 |
32.6 |
12.9 |
319 |
16.9 |
738 |
|
0
|
0.81 |
0.59 |
NS |
|
|
NS, not significant. See text for other definitions.
|
|
For model II, in five out of six subjects, the parameter values
for TI and Th are of the same order of
magnitude (for three subjects, the values for TI and
Th are the same). In only one subject (subject 796)
are the values radically different. In this one subject, the very low
value for TI compared with Th means that the
dynamic for gp is very close to first order, but
for the other five subjects this seems not to be true. This alteration in dynamic has had consistent (albeit often small) effects on the other
parameter values of the model. In particular, when model II is
compared with model I,
c is
consistently increased and g100 and gh
consistently decreased across all the subjects.
Turning to the parameters for model III, some effect was
attributed to the extra component of the model by the fitting process in five out of six subjects. The values estimated for both
gd and Td were quite variable among the
different subjects. Table 3 shows the
percentage contributions to HVD of the component acting via modulation
of the peripheral chemoreflex sensitivity
p and the component that is independent
of the peripheral chemoreflex (
d) for
each subject. These figures were obtained by calculating the
steady-state values for
p and
d under conditions of a sustained steady
PETO2 of 100 Torr and under
conditions of a sustained steady PETO2 of
50 Torr. For
p, this was done by setting
the derivatives of Eqs. 2 and 3 to zero and obtaining
an explicit expression for
p, and, for
d, by setting the derivative of Eq. 18 to zero and obtaining an explicit expression for
d. The averaged contributions
calculated across all the six subjects were 73.8% for the
component acting via the peripheral chemoreflex and 26.2% for the
peripheral chemoreflex-insensitive component.
When we compared parameter values across all models, one striking
feature we noticed was the consistent nature of the differences in
value for kp. For five out of six subjects, the value for
kp for model II was smaller than for model
I, and for five out of six subjects, the value for kp
was smaller for model III compared with model II. For
model I, a positive value for kp was obtained for
all six subjects; for model II, a positive value was obtained for five out of six subjects; but for model III, a positive
value was only obtained for one out of the six subjects.
Physiologically, kp represents the component of peripheral
chemoreflex drive that is present in high oxygen, and this suggests
that model I attributes a higher proportion of the total
ventilation to peripheral chemoreflex drive in euoxia than does
model II, and that model II attributes a higher
proportion than does model III. This is confirmed by inspection
of Table 3, where the contributions of each component to ventilation
have been calculated for each of the models in euoxia. The mean
contributions to ventilation by the peripheral chemoreflex drive are
significantly different among models, being highest with model
I and lowest with model III (analysis of variance, P < 0.05). In the case of model III, the reduction
of total ventilation by
d is small in
euoxia, as would be expected by the fact that the saturation is close
to 1.
DISCUSSION
Fitting Technique
In the study by Painter et al. (13), no model of the noise structure
was employed, whereas in the present study both a simple least squares
fitting procedure and a simple state-space model for a parallel noise
process were explored. A suitable noise model allows the inherent
correlation between successive breaths to be included in the model and
results in residuals that are overall white or close to white. This is
useful when comparing the overall quality of fit between different
models. This approach has been adopted by others for modeling the
ventilatory response to CO2 (5). The ability of the
particular state-space model chosen to describe ventilatory variability
has been demonstrated previously (10), and this result is supported by
the observation that 26-28 out of 31 sets of residuals could be
accepted as white on the basis of a portmanteau test in the present
study, whereas all the residuals' sequences from the simple least
squares fitting technique were highly correlated.
It is of some interest to determine whether the values for the
stochastic component of the model ( f,
Rv/Rw) were similar to those
obtained from a previous study under conditions of steady chemical
stimulation (10). From this previous study, the mean ± SE values for
f and Rv/Rw were 0.69 ± 0.06 and 0.95 ± 0.13, respectively, for the resting data and 0.81 ± 0.03 and 0.44 ± 0.11, respectively, for the data during exercise. The mean
values for f and Rv/Rw in the
present study were 0.76 ± 0.04 and 1.55 ± 0.41, respectively, for
model I; 0.75 ± 0.03 and 1.85 ± 0.53, respectively, for
model II; and 0.72 ± 0.03 and 1.74 ± 0.53, respectively,
for model III. Thus the mean values for f in the present study
lay between the values for rest and exercise from the previous study,
whereas the values for Rv/Rw
appeared to be a little higher. When the values obtained from the fits
for the three different models of the present study were compared,
analysis of variance showed that there was no significant difference in
the estimated value of Rv/Rw
between the three models (P > 0.05), but there was a
significant difference between the estimated values of f for the
different models (P < 0.05). One interpretation of this is
that when the model structure varies, the residual correlation that has
to be explained by the stochastic process ( f ) varies too,
but not necessarily the estimate for
Rv/Rw.
Model Comparison
Comparisons among the models may be drawn in a number of ways. First,
the question may be asked whether the extended models produce any
statistically significant improvement in the fit, compared with the
original model of Painter et al. (13). This can be determined both by
examining the overall sum of squared residuals and by inspection of the
confidence intervals for the ensemble-averaged residuals over the time
course of the protocol. Second, some physiological judgment may be
exercised in terms of whether the estimated parameter values are likely
to be consistent with other known features of the respiratory system.
In statistical terms, for model II, two subjects (subjects
766, 824) showed a significant reduction in the sum of squared residuals, as compared with model I. These subjects do not
appear to have any particularly distinguishing features in terms of
their response to the hypoxic protocol. In addition, a direct visual comparison of the model fit between model II and model
I did not suggest much by way of difference between them. Overall,
it is difficult to be certain exactly why these two subjects show a significant improvement in fit, but we feel that it is most likely to
be related to differences during and immediately after the onset of
hypoxia. The model does not appear to improve the fit to the period
immediately following the relief from hypoxia, which was one of the
specific purposes of the study.
For model III, again only two subjects (subjects 758, 796) showed a significant reduction in the total sum of squared
residuals when compared with model I. These two subjects
consistently showed an apparent undershoot and then recovery of
ventilation at the relief of hypoxia in all the individual experimental
repeats of the protocol. In other subjects, an undershoot followed by
recovery was either not observed or appeared inconsistently in some,
but not all, of the repeats. Inspection of the plots of the model fit
and ensemble-averaged residuals over time shows that it is during the
period following the relief from hypoxia that the models are most
distinct. We conclude that the use of model III may
significantly improve the fit in some subjects, who show a reasonable
degree of undershoot and recovery of ventilation after the relief of hypoxia, but that this is not the case for all subjects.
The two subjects in whom the fit of model III was a significant
improvement over the original model of Painter et al. (13) had the two
largest magnitudes for the gain term gd of the additional chemoreflex-independent component. In these two subjects, slightly over
50% of HVD (mean 56%) was attributed to the peripheral
chemoreflex-independent component. In the other four subjects, the
value was very much smaller, with a mean value of 11%. Again, this
emphasizes the importance of intersubject differences.
For the two subjects with a substantial contribution to ventilation
from the peripheral chemoreflex-independent compartment, the time
constants associated with this compartment were rather fast (22 and 50 s) and are consistent with the comments of Bascom et al. (3) that the
baseline ventilation appears to recover more quickly than does the
peripheral chemoreflex sensitivity. These values do not really
correlate well with the sorts of values previously obtained for the
development of HVD in anesthetized animals [onset of HVD
149.7 ± 8.5 (SE) s; offset of HVD 105.5 ± 10.1 s (17)]. Thus,
on the basis of data from these two subjects, it would appear that this
peripheral chemoreflex-insensitive component cannot really be equated
simply with a chemoreflex-insensitive form of HVD observed in
anesthetized animals, as postulated in the introductory part of this
paper. However, for the other three subjects in whom some component of
the ventilatory response was attributed to the peripheral
chemoreflex-independent term, the time constants were all somewhat
longer than those associated with HVD in anesthetized animals. Overall,
we feel that it would be unwarranted to draw any very firm conclusions
from these values.
One notable feature that differs among the models is the parameter
estimates determined for kp. Physiologically,
kp is a parameter relating to the contribution of the
peripheral chemoreflex to ventilation in hyperoxia when the arterial
blood is fully saturated. We consider that the positive values for
kp in the original model of Painter et al. (13) may be
necessary to fit the slightly lower level of euoxic ventilation seen
after the relief of hypoxia, when compared with the original baseline
ventilation. In model III, this feature of the data can be
modeled via the additional term
d. Which
of these approaches in a physiological sense is correct is difficult to
determine. Although there is some evidence to suggest that the
peripheral chemoreflex is inactivated by hyperoxia in humans (11), in
which case model III might represent the physiology better, it
is also possible that positive values of kp might simply
represent some nonlinearity of the response of the peripheral
chemoreflex to saturation in this range.
ACKNOWLEDGEMENTS
This work was supported by The Wellcome Trust. P.-J. Liang was
supported by a Run Run Shaw studentship.
FOOTNOTES
Address for reprint requests: P. A. Robbins, University Laboratory of
Physiology, Parks Road, Oxford OX1 3PT, UK.
Received 11 October 1995; accepted in final form 24 September
1996.
REFERENCES
| 1.
|
Armitage, P.,
and
G. Berry.
Statistical Methods in Medical Research (2nd ed.). Oxford, UK: Blackwell Scientific, 1987.
|
| 2.
|
Bascom, D. A.,
I. D. Clement,
D. A. Cunningham,
R. Painter,
and
P. A. Robbins.
Changes in peripheral chemoreflex sensitivity during sustained, isocapnic hypoxia.
Respir. Physiol.
82:
161-176,
1990.
[Medline]
|
| 3.
|
Bascom, D. A.,
J. J. Pandit,
I. D. Clement,
and
P. A. Robbins.
Effects of different levels of end-tidal PO2 on ventilation during isocapnia in humans.
Respir. Physiol.
88:
299-312,
1992.
[Medline]
|
| 4.
|
Berkenbosch, A.,
and
J. DeGoede.
Actions and interactions of CO2 and O2 on central and peripheral chemoreceptive structures.
In: Neurobiology of the Control of Breathing. New York: Raven, 1986, p. 9-17.
|
| 5.
|
DeGoede, J.,
and
A. Berkenbosch.
Dynamic end-tidal forcing technique: modelling the ventilatory response to carbon dioxide.
In: Modeling and Parameter Estimation in Respiratory Control. New York: Plenum, 1989, p. 59-69.
|
| 6.
|
Easton, P. A.,
and
N. R. Anthonisen.
Carbon dioxide effects on the ventilatory response to sustained hypoxia.
J. Appl. Physiol.
64:
1451-1456,
1988.
[Abstract/Free Full Text]
|
| 7.
|
Easton, P. A.,
L. J. Slykerman,
and
N. R. Anthonisen.
Ventilatory response to sustained hypoxia in normal adults.
J. Appl. Physiol.
61:
906-911,
1986.
[Abstract/Free Full Text]
|
| 8.
|
Easton, P. A.,
L. J. Slykerman,
and
N. R. Anthonisen.
Recovery of the ventilatory response to hypoxia in normal adults.
J. Appl. Physiol.
64:
521-528,
1988.
[Abstract/Free Full Text]
|
| 9.
|
Khamnei, S.,
and
P. A. Robbins.
Hypoxic depression of ventilation in humans: alternative models for the chemoreflexes.
Respir. Physiol.
81:
117-134,
1990.
[Medline]
|
| 10.
|
Liang, P.-J.,
J. J. Pandit,
and
P. A. Robbins.
Statistical properties of breath-to-breath variations in ventilation at constant PCO2 and PO2 in humans.
J. Appl. Physiol.
81:
2274-2286,
1996.
[Abstract/Free Full Text]
|
| 11.
|
Miller, J. P.,
D. J. C. Cunningham,
B. B. Lloyd,
and
J. M. Young.
The transient respiratory effects in man of sudden changes in alveolar CO2 in hypoxia and in high oxygen.
Respir. Physiol.
20:
17-31,
1974.
[Medline]
|
| 12.
|
Neubauer, J. A.,
J. E. Melton,
and
N. H. Edelman.
Modulation of respiration during brain hypoxia.
J. Appl. Physiol.
68:
441-451,
1990.
[Abstract/Free Full Text]
|
| 13.
|
Painter, R.,
S. Khamnei,
and
P. Robbins.
A mathematical model of the human ventilatory response to isocapnic hypoxia.
J. Appl. Physiol.
74:
2007-2015,
1993.
[Abstract/Free Full Text] |
| 14.
|
Priban, I. P.
An analysis of some short-term patterns of breathing in man at rest.
J. Physiol. Lond.
166:
425-434,
1963.
|
| 15.
|
Swanson, G. D.,
and
J. W. Bellville.
Step changes in end-tidal CO2: methods and implications.
J. Appl. Physiol.
39:
377-385,
1975.
[Abstract/Free Full Text]
|
| 16.
|
Van Beek, J. H. G. M.,
A. Berkenbosch,
J. DeGoede,
and
C. N. Olievier.
Effects of brain stem hypoxaemia on the regulation of breathing.
Respir. Physiol.
57:
171-188,
1984.
[Medline]
|
| 17.
|
Ward, D. S.,
A. Berkenbosch,
J. DeGoede,
and
C. N. Olievier.
Dynamics of the ventilatory response to central hypoxia in cats.
J. Appl. Physiol.
68:
1107-1113,
1990.
[Abstract/Free Full Text]
|
| 18.
| Weil, J. V., and C. W. Zwillich. Assessment of ventilatory
responses to hypoxia and hypercapnia in man. Chest. 70, Suppl.: 124-128, 1976.
|
0161-7567/97 $5.00
Copyright © 1997 the American Physiological Society