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ABSTRACT |
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We previously observed an increase in minute ventilation (
E) with
resistive unloading (He-O2 breathing) in healthy elderly subjects
with normal pulmonary function. To investigate the effects of resistive unloading in elderly subjects with mild chronic airflow limitation (FEV1/FVC: 61 ± 4%), we studied 10 elderly men and women 70 ± 3 yr of age. These subjects performed graded cycle ergometry to exhaustion, once breathing room air and once
breathing a He-O2 gas mixture (79% He, 21% O2).
E, pulmonary
mechanics, and PETCO2 were measured during each 1-min increment in work rate. Data were analyzed by paired t test at rest, at
ventilatory threshold (VTh), and during maximal exercise.
E was
significantly (p < 0.05) increased at VTh (3.4 ± 4.0 L/min or 12 ± 15% increase) and maximal exercise (15.2 ± 9.7 L/min or 22 ± 13% increase) while breathing He-O2. Concomitant to the increase in
E, PETCO2 was decreased at all levels (p < 0.01), whereas
total work of breathing against the lung was not different. We
concluded that
E is increased during He-O2 breathing because of
resistive unloading of the airways and the maintenance of the relationship between the work of breathing and exercise work rate.
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INTRODUCTION |
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The mechanisms for a sustained hyperventilatory response
(i.e., increased
E) to breathing a low density gas mixture of
helium and oxygen (He-O2) during exercise remain unclear. It
has been suggested that the increase is related to decreased
airflow turbulence at high ventilatory rates (1, 2), to reflex
mechanisms (3), to stimulation of irritant receptors (4), and to
decreased mechanical ventilatory constraints (5). Recently, it
was suggested that only women who experience expiratory
flow limitation during exercise have a sustained hyperventilatory response to He-O2 breathing (6). These new data suggest
that the decrease in turbulent airflow and subsequent reduction in pulmonary resistance play a much lesser role on the
ventilatory response to He-O2 breathing than expiratory flow
limitation. If removal of expiratory flow limitation is critical to
sustained hyperventilation with He-O2 breathing, we thought
that older subjects with mild chronic airflow limitation, who
have both age-related and disease-related declines in pulmonary function and substantial ventilatory constraints during
exercise (7, 8), including extensive expiratory flow limitation,
might show relatively large increases in
E with He-O2 breathing. Furthermore, we proposed that examination of this population may also provide further insight into the mechanisms by
which
E is increased by He-O2 breathing, if the increase in
E with He-O2 breathing is dependent on the magnitude of
expiratory flow limitation during exercise. Thus, the purpose
of the present study was to determine the effect of He-O2
breathing on
E and respiratory mechanics during exercise in
older subjects with mild chronic airflow limitation.
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METHODS |
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Subjects
Volunteers were recruited through local advertisements. None of the subjects had a history of asthma, cardiovascular disease, or musculoskeletal abnormalities that would preclude maximal exercise, or had participated in regular vigorous exercise during the previous 6 mo. In accordance with the Institutional Review Board, all details of the study were discussed with the volunteers, and informed consent was obtained. All qualified participants were familiarized to exercise on the cycle ergometer and instructed to avoid exercise, food, caffeine, and smoking for at least 2 h prior to exercise testing.
Volunteers were accepted for study if their FEV1 was < 79% of predicted and/or their FEV1/FVC ratio was < 74%. No subject had a significant change in spirometry with inhaled bronchodilators. Many of the subjects were unaware of their reductions in pulmonary function until screened for the study, and, therefore, none of the subjects was receiving medications for their breathing. Two subjects were current smokers (1 M, 2 packs/d; 1 W, 1 pack/d), and all 10 subjects had a history of smoking (mean ± SD; 42 ± 13 yr; 65 ± 41 pack-years; 8 ± 8 yr since quitting for eight subjects).
Pulmonary Function
All subjects had standard spirometry, lung volume, and diffusing capacity determinations (Model 6200 body plethysmograph; SensorMedics, Yorba Linda, CA). Pulmonary function was performed according to guidelines of the American Thoracic Society (9). ATS standards were also used for the evaluation of pulmonary impairment (10). Predicted values were based on norms by Knudson and coworkers (11) and Enright and colleagues (12).
Resting Respiratory Mechanics
Maximal flow-volume loops and pressure-volume loops were measured in a pressure-corrected, volume-displacement body plethysmograph to eliminate the gas compression artifact (SensorMedics 6200). Transpulmonary pressure (Ptp) was estimated using an esophageal balloon placed approximately 45 cm from the nostril (13). Isovolume-pressure flow (IVPF) curves were constructed (14) and used to determine the minimum pressure necessary to obtain maximal flow (Pcrit) as described previously (5). IVPF curves were also determined with He-O2 breathing with the use of multiple graded vital capacities, which were performed prior to the He-O2 exercise test. Maximal expiratory flow was increased with He-O2 breathing, but Pcrit was not significantly different between room air and He-O2 breathing (data not shown). These Pcrit data were used solely to confirm expiratory flow limitation during exercise (see below).
Gas Exchange Measurements
Measurements of oxygen uptake (
O2) and carbon dioxide production (
CO2) were made with the use of a custom gas exchange system
that was computerized. However, in the He-O2 tests, it was not possible to measure gas exchange because of the deleterious effects of helium on mass spectrometer operation. Ventilatory threshold (VTh)
was determined from a combination of gas exchange methods (15,
16). VTh was designated as the work rate that was most congruent
among the different threshold determination methods. End tidal CO2
(PETCO2) was measured when breathing room air as well as when
breathing He-O2 with the use of the Poet TE CO2 monitor (Model
602/11; Criticare systems Inc., Waukesha, WI).
Breathing Mechanics
Expiratory and inspiratory flow was measured continuously during the exercise tests as described previously (5). An esophageal balloon was placed as described above for measurements of Ptp during the second and third maximal exercise tests (5). Maximal flow-volume and pressure-volume loops were determined at rest while the subjects were seated on the cycle ergometer just before the baseline measurements, and within 2 min after terminating exercise to determine if exercise had induced bronchodilation or bronchoconstriction, which none of the subjects experienced.
Inspiratory capacity (IC) was measured at rest and during exercise to determine placement of tidal flow-volume loops within the maximal flow-volume loop as described previously (5). End-expiratory lung volume (EELV) was estimated from measurement of IC and reported as a percentage of TLC. End-inspiratory lung volume was calculated (EILV = EELV + VT) and expressed as a percentage of TLC.
Inspired Gas Mixtures
During rest and exercise, inspired gas was provided from a large inspiratory reservoir as described previously (5). The bag was filled with either room air or 21% O2, and the balance He, which was humidified similar to that of room air as in prior studies (5, 17). External resistance (i.e.; valve, tubing, and pneumotachographs) was matched between the room air and He-O2 conditions (5, 17). By matching external apparatus resistance, the He-O2 effect was restricted to the respiratory airways.
Study Protocol
After screening, which included pulmonary function tests, an electrocardiogram, and practice on the cycle ergometer, all subjects performed three maximal exercise tests. The first was a preliminary exercise test to clear subjects for further participation in the study. The second and third tests were performed while they breathed either room air or a gas mixture of 21% O2 and 79% He. The order of these tests were randomized and the subjects were blinded to which gas mixture they were breathing.
Exercise Protocol
All the exercise tests followed the same sequence of procedures. Testing began with the subjects seated on the cycle ergometer while baseline measurements were made. After 3 min of baseline measurements, the subjects performed graded cycle ergometry on an electronically braked cycle ergometer (Model CPE 2000; MedGraphics, St. Paul, MN). Exercise began at 10 W for the women or 20 W for the men and was incremented by 10 or 20 W, respectively, every minute until the subjects stopped because of exhaustion, or the test was stopped because they could not keep the pedal rate at a frequency above 50 rpm. Heart rate was monitored continuously through the use of a 12-lead electrocardiogram (Model CS-100; Schiller, Baar, Switzerland), and blood pressure was monitored with the use of an automated system (Model 4240; Suntech, Raleigh, NC). Arterial saturation was monitored at rest and continuously throughout the first exercise test by pulse oximetry (Model 3700; Ohmeda, Boulder, CO). Ratings of perceived exertion (Borg 20 point scale) and breathlessness (Borg 10 point scale) were taken with the use of the procedures outlined by the American College of Sports Medicine (18) and were recorded at each work rate during the exercise test.
Data Analysis
VT, f,
E, and exercise tidal flow-volume and pressure-volume loops
were determined with the use of an interactive computer program developed in this laboratory, as described previously (5). Pulmonary resistance was computed on a breath-by-breath basis with multiple linear regression by the method of least squares for the whole breath as
described in Method 1 by Officer and colleagues (19). Resistance was
estimated from Ptp and flow on 5 to 10 breaths preceding the measurement of IC, and then averaged. The mechanical work of breathing
against the lung was estimated per breath from the area enclosed by
the dynamic tidal Ptp-volume loop with addition of that portion of a
triangle describing work that fell outside the tidal pressure-volume
loop when plotting Ptp and volume (i.e., part of inspiratory elastic
work) (20), and then averaged. The work of breathing was then further partitioned into resistive and elastic components. Expiratory flow
limitation was defined as the percentage of VT (%VT) where tidal expiratory flow impinged on maximal expiratory flow and where Ptp simultaneously exceeded Pcrit. Data were analyzed at rest, at VTh, and
during maximal exercise. The slope of
E versus work rate was calculated on all the points between rest and VTh and between VTh and
maximal exercise for the room air and He-O2 exercise tests. If the R2
was not greater than 0.85 (i.e., indicating the fit of the data by least
squares regression), then the subject's data were dropped from the
group analysis of ventilatory response. Below VTh, one subject was
dropped when breathing room air and two subjects were dropped
when breathing He-O2; above VTh no subjects were dropped from
analysis. The individual slopes were then averaged and used as indicators of ventilatory response below and above VTh. Work rate was
used in the determination of ventilatory response instead of
CO2 as
previously described (5, 17) so that comparisons could be made between the room air and the He-O2 tests, where it was not possible to
make gas exchange measurements.
The difference between means was tested with the use of paired t tests at rest, at VTh, and during maximal exercise. Relationships among physiologic variables were analyzed by Pearson's correlation coefficients.
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RESULTS |
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Subjects
There were six men and four women with a mean age of 70 ± 3 yr (mean ± SD) who participated in the study (height, 170 ± 10 cm; weight, 74 ± 14 kg). Pulmonary function data are presented in Table 1, which are consistent with mild chronic airflow limitation. Maximal exercise values are presented in Table 2 for the
preliminary graded exercise test, room air, and He-O2 tests. Exercise capacity was normal in these subjects based on
O2 and
HR as a percentage of the age- and sex-predicted normal. Also,
E/MVV ratio was not noticeably elevated. Exercise capacity
was not different with breathing He-O2. Likewise, RPE and
RPB were not different when breathing He-O2.
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Ventilation at Rest, VTh, and Maximal Exercise
E (L/min) at rest, VTh, and maximal exercise when breathing
room air and He-O2 are shown in Figure 1, where
E is plotted against work rate (W).
E was significantly higher at VTh (p < 0.05) and maximal exercise (p < 0.001) when breathing He-O2 (22 ± 13% increase at maximal exercise). The increase in
E
during maximal exercise with He-O2 breathing was due to a
significant (p < 0.01) increase in VT (approximately 12% increase) (Table 3). Along with the increase in
E with He-O2
breathing, there was a significant (p < 0.001) decrease in
PETCO2 at rest, VTh, and maximal exercise (Table 3). The decrease in PETCO2 supports the tendency for sustained hyperventilation when breathing He-O2, even during maximal exercise.
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Ventilatory Response to Exercise
The ventilatory response to exercise below VTh increased from 0.39 ± 0.08 to 0.47 ± 0.11 L/min/W when breathing He-O2, but failed to reach significance (p = 0.0521) (Figure 1). The ventilatory response to exercise above VTh was significantly greater (p < 0.01) when breathing He-O2 (0.74 ± 0.18) as compared with breathing room air (0.60 ± 0.15).
Breathing Mechanics
There was no expiratory airflow limitation at rest with either
room air or He-O2 breathing. At VTh and maximal exercise,
expiratory flow limitation was not significantly different between breathing conditions, although
E was significantly
higher during maximal exercise with He-O2 breathing (Table
3). Six subjects had expiratory flow limitation at VTh while
seven had expiratory flow limitation at maximal exercise when
breathing either room air or He-O2. EELV was significantly
lower when breathing He-O2 at rest, at VTh, and during maximal exercise (Table 3), which is similar to previous findings
and appears to be related to increased maximal expiratory flow and decreased expiratory airflow limitation (5, 17). EILV
between room air and He-O2 was not different at any level (Table 3). Pulmonary resistance (cm H2O/L/s) was reduced at
rest (
0.63 ± 0.92,
15 ± 21%, p = 0.0583), VTh (
0.66 ± 0.79,
19 ± 17%, p < 0.05), and during maximal exercise
(
0.87 ± 0.45,
30 ± 9%, p < 0.001) when breathing He-O2
(Table 3). External resistance as calculated from oral pressure
and flow was not different at any level between the room air
and He-O2 tests, which demonstrates that matching of the external resistance between room air and He-O2 was accomplished (data not shown).
The total work of breathing against the lung was unchanged from that of room air at rest, VTh, and maximal exercise when breathing He-O2, despite a significantly greater
E
at VTh and maximal exercise (Figure 2). Also, at a given absolute work rate (e.g., 20, 40, 60, and 80 W), the total work of
breathing against the lung was not changed (data not shown).
When the total work of breathing was partitioned into elastic
and resistive components at maximal exercise, the elastic work
of breathing was increased (p < 0.05), probably because of the
higher
E and VT. The resistive work of breathing was not significantly different at maximal exercise. At rest and VTh, neither the elastic nor the resistive work of breathing against the
lung were different. Peak expiratory pressure was not changed
at rest, VTh, or maximal exercise by breathing He-O2. It would
appear that at a given level of exercise, respiratory effort
against the lung was unchanged by He-O2 breathing. The similarity of RPE and RPB between room air and He-O2 breathing would also support this observation (Table 3).
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Correlations
To determine if the decrease in pulmonary resistance with He-O2 breathing was associated with the increase in
E, we correlated the change in resistance at rest with the change in
E at
maximal exercise. This yielded a poor correlation (r =
0.18)
but an interesting plot. When this plot was examined further,
it was observed that there was a close relationship between
the decrease in resistance and the increase in
E when men
and women were plotted separately (Figure 3) (for the men, r =
0.82 and p < 0.05; and for the women, r =
0.997 and p < 0.01). Reporting the change in
E with He-O2 breathing as a
percent of
E during maximal exercise breathing room air did
not change these relationships for the men or women, nor did
it change the significance of these relationships. Furthermore, numerous attempts to normalize the change in
E between
the women and men relative to body size, baseline pulmonary
function, and exercise tolerance did not yield a significant correlation when the men and women were analyzed as one
group. This suggested that there was a difference in the increase in
E with He-O2 breathing during exercise between
the women and men.
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Therefore, we examined
E and resistance with He-O2
breathing between the men and women. In the men, the increase in
E in L/min was significantly higher only at maximal
exercise (20 ± 9 and 7 ± 4 L/min, respectively, p < 0.05); although, as a percent change,
E at maximal exercise was not
significantly different between the men and women (28 ± 13 and 14 ± 9%, respectively). The change in pulmonary resistance at rest, in cm H2O/L/s or percent change, was not different between the men and women; although, pulmonary resistance in cm H2O/L/s was significantly higher in the women at
rest and during exercise both when breathing room air and
He-O2 (data not shown; p < 0.05). Thus, the larger increase in
E with He-O2 breathing during exercise in the men was probably related to the fact that the men simply had a larger absolute
E at maximal exercise than did the women (52 ± 7 versus 76 ± 14 L/min; p < 0.05), which is probably related to the
fact that the men are larger and have a larger absolute exercise capacity. This seems reasonable since for a larger absolute
E there would be greater turbulence and the potential for
greater resistive unloading with He-O2 breathing. This possibility is supported when
E with room air breathing is correlated
with the increase in
E with He-O2 breathing over all 30 points (10 subjects at rest, VTh, and maximal exercise; R2 = 0.59, p < 0.001). This finding suggests that the increase in
E
with He-O2 breathing was at least partially related to the magnitude of
E when breathing room air, which was greater in the men at maximal exercise.
To further investigate the relationship between the decrease in pulmonary resistance and the increase in
E when
breathing He-O2, the
E when breathing He-O2 was plotted
against a predicted
E for He-O2 breathing (predicted
E He-O2). The predicted
E for He-O2 breathing was calculated:
Predicted
E He-O2 =
E room air × (RRA/RHe-O2), where
RRA is the breathing circuit resistance at a specified flow rate
and RHe-O2 is the breathing circuit resistance at the same specified flow rate. This resistance ratio was calculated from the
breathing circuit pressure-flow curves for room air and He-O2
before resistance matching. These curves are shown in Figure 4 for the breathing circuitry (includes tubing, valve, and pneumotachographs). The decreases in resistance were obtained at
selected flow rates that were similar to the mean expiratory
flow rates (VT/TE, L/s) observed at rest (0.33 L/s), VTh (0.91 L/s), and maximal exercise (2.05 L/s) when breathing room air
(also see Table 3). At these flow rates, resistance was decreased by 18, 21, and 22%, respectively. Predicted
E for He-O2 breathing is plotted against observed
E when breathing
He-O2 (Figure 5). The R2 of this relationship was 0.97 (p < 0.001) and there was no significant difference between the
means of predicted
E He-O2 and observed
E He-O2. This
close relationship suggests that the increase in
E with He-O2
breathing can be predicted by simply knowing the change in
pressure-flow characteristics with He-O2 and the
E when
breathing room air.
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In contrast to the decrease in resistance at rest, the magnitude of expiratory flow limitation during maximal exercise
when breathing room air was not significantly correlated with
the change in
E with He-O2 breathing. But, when expiratory
flow limitation was correlated to the increase in
E over all
points (10 subjects at rest, VTh, and maximal exercise, 30 points total), there was a significant (p < 0.01) but weak relationship (R2 = 0.32) between the two. This relationship suggests that the magnitude of expiratory flow limitation explains
only a small part of the increase in
E with He-O2 breathing during exercise. Furthermore, expiratory flow limitation tended
to be larger in the women at VTh and maximal exercise, although these differences failed to reach significance in such
small sample sizes (data not shown). Also, the increases in
peak expiratory flow (PEF) 20 ± 5%, p < 0.01) and flow at
50% of the forced vital capacity (FVC) (44 ± 11%) when
breathing He-O2 were not significantly correlated with the
change in
E at maximal exercise. Nor was the increase in
PEF with He-O2 breathing, or the increase in flow at 50% of the FVC significantly correlated with the change in pulmonary resistance at rest with He-O2 breathing. This suggests that the increase in
E during maximal exercise when breathing He-O2
was more related to the decrease in pulmonary resistance at
rest than to the increase in maximal expiratory flow.
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DISCUSSION |
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The major findings of this study were twofold. One, the increase in
E when breathing He-O2 was largely explained by
the decrease in pulmonary resistance at rest and could be predicted by the model presented in this study. Two, the total work
of breathing against the lung was not decreased at VTh or maximal exercise, although pulmonary resistance was decreased
with He-O2 breathing. This indicates that at a given exercise
work rate He-O2 breathing does not always produce a decrease
in the work of breathing against the lung, as commonly assumed,
and that respiratory effort against the lung remains constant per
work rate with room air and He-O2 breathing. Contrary to previous findings (6), we observed that expiratory airflow limitation during exercise breathing room air only partially explained
the increase in
E with He-O2 breathing.
Hyperventilatory Response with He-O2 Breathing
The increase in
E during maximal exercise with He-O2 breathing was similar to that reported previously by the author (5, 17) and by others (2, 3, 21, 22) for younger and older men and
women with normal pulmonary function (24 + 11% increase). Also the increase in percent
E was similar to that reported for patients with severe chronic airflow limitation (23) and for
normal subjects at raised atmospheric pressures (24). Thus, the relative increase in
E with He-O2 breathing appears to be consistent over many populations, including younger and older members with normal pulmonary function and patients with
mild-to-severe chronic airflow limitation, as well as in those in
different environmental conditions (21, 22). This is important
because it suggests that pulmonary function and expiratory
flow limitation during exercise are probably not great influences on the ventilatory response to He-O2 breathing (see EXPIRATORY FLOW LIMITATION below).
The results of this study also suggest that the increase in
E
with He-O2 breathing is directly proportional to the decrease in resting pulmonary resistance and can be predicted from
simple pressure-flow characteristics of He-O2. The relationship between
E with He-O2 breathing and predicted
E with
He-O2 breathing is very strong support for this conclusion
(Figure 5). The more moderate correlation between the magnitude of
E during maximal exercise when breathing room
air and the increase in
E with He-O2 breathing is further support that the increase in
E during exercise when breathing
He-O2 is the result of resistive unloading of the airways and
the magnitude of
E as suggested by others (25).
The slope of the ventilatory response to exercise above
VTh with He-O2 breathing was also increased as previously
reported by the author (5) (0.89 ± 0.22 versus 0.74 ± 0.18 L/
min/W) and other investigators (1) (Figure 1). This increase
in slope indicates that the effect of resistive unloading on
E
becomes greater as the ventilatory output is increased above
VTh. This observation suggests that as ventilatory output is increased, turbulent flow is also increased; and as such, the effect of resistive unloading becomes greater, which has been
suggested by others (25). Below VTh, where ventilatory output is lower,
E was increased very little, which is consistent
with the above statements and with the findings of others as
well (2, 3, 5, 17). Also, for the subjects with chronic airflow
limitation in the present study, the ventilatory response to exercise below VTh, before marked flow limitation, was similar
to that of other subjects 65 to 75 yr of age with normal pulmonary function (Figure 6A). Above VTh, when expiratory flow
limitation was pronounced, their ventilatory response to exercise when breathing room air was slightly lower as compared
with the ventilatory response of other subjects 65 to 75 yr of
age with normal pulmonary function (Figure 6A). But with
He-O2 breathing, the present subjects' ventilatory response to
exercise above VTh was restored to a level similar to that of
those 65 to 75 yr of age with normal lung function breathing room air (Figure 6B). This supports the contention that increased mechanical ventilatory constraints attenuate the ventilatory response to exercise above VTh, as suggested previously by the author (5) and by others (6, 26).
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Furthermore, our data suggest that the increase in
E with
He-O2 breathing is less in women than in men at maximal exercise. However, there are too few men and women to adequately
address the findings related to sex, and they are reported with
caution. However, the percent increase in
E with He-O2 breathing in the older women with mild chronic airflow limitation studied here was similar to that reported by McClaran and colleagues
(6) for younger women with normal pulmonary function.
Work of Breathing
The total work of breathing against the lung was not decreased
at rest, VTh, or maximal exercise with He-O2 breathing. This observation is consistent with previous work in older subjects with normal pulmonary function (5). Others have assumed that the work of breathing against the lung was reduced with He-O2 breathing during exercise, but few have actually measured the work of breathing (27). The results of the present study suggest that respiratory effort against the lung, as reflected by the total
mechanical work of breathing against the lung, remained unchanged for a given exercise work rate; and as a result of the decreased pulmonary resistance,
E was increased progressively as the unloading effect of He-O2 became greater with
heavy-to-maximal exercise. Thus, for a given level of exercise,
it appears to be more important to maintain the same level of
work of breathing against the lung than to maintain a specific
level of
E, or for that matter, PETCO2. This is in agreement
with the conclusions of others (27), and appears true for
subjects with mild chronic airflow limitation as well as for
younger and older subjects with normal pulmonary function.
Expiratory Flow Limitation
It has been suggested that the increase in
E with He-O2
breathing occurs only when flow limitation is present, at least in young women (6). McClaran and colleagues (6) reported that in a study of women, only those with flow limitation during room air exercise increased their
E during exercise with
He-O2 breathing. This finding would suggest that ventilatory
capacity was increased, as defined by an increase of the maximal expiratory flow-volume envelope, to such an extent that
the women were able to increase
E during maximal exercise
by as much as 14% while incurring less flow limitation than
obtained during exercise with room air breathing (6). Of the
10 subjects in the present study, seven had expiratory flow limitation during maximal exercise when breathing room air (34 ± 4%VT) and breathing He-O2 (36 ± 6%VT). They had an average increase in
E of 26 ± 13% with He-O2 breathing. Three
subjects with no flow limitation had an average increase in
E
of 14 ± 11% during maximal exercise with He-O2 breathing. When examined relative for the women (data not shown), it
was found that the increase in
E (14 ± 9%) with He-O2
breathing and the magnitude of expiratory flow limitation (27 ± 18%VT) with room air was similar to that reported by McClaran and colleagues (6) for young women with normal pulmonary function. However, there was no significant correlation
between the magnitude of expiratory flow limitation during
the room air test and the increase in
E during the He-O2 test.
Also, there was no difference in the increase in maximal expiratory flow with He-O2 breathing between the flow-limited
and non-flow-limited subjects. Overall, the subjects in the
present study increased both maximal expiratory flow and
E
with He-O2 breathing, and expiratory flow limitation stayed approximately the same with He-O2 breathing as with room
air breathing, which has been reported previously in both
younger and older men and women with normal pulmonary
function (5, 17) and is now reported for men and women with
mild chronic airflow limitation. Unfortunately, there are very
few studies that have measured expiratory flow limitation with
He-O2 breathing in which to compare these results.
Influence of Mechanical Constraints
On the basis of the results of the present study, it remains unclear how important mechanical ventilatory constraints, specifically expiratory flow limitation, are to the increase of
E
with He-O2 breathing. It is certainly possible that decreasing
expiratory flow limitation could cause some reflex modulation
of expiration, and, as a result, produce an increase in
E when
maximal expiratory flow is increased with He-O2 breathing (3,
30, 31). Alternatively, as in the present study, the increase in
E could be related to the reduction in pulmonary resistance,
which resulted in increases in
E in both flow-limited and non-flow-limited subjects in this study. Nevertheless, it is reasonable, and in agreement with McClaran and colleagues (6), that
expiratory flow limitation could potentially "inhibit"
E during heavy exercise, just as increased pulmonary resistance appeared to attenuate
E in the present study. However, rather
than by inhibitory feedback to a highly integrated controller mechanism, expiratory flow limitation and increased pulmonary resistance could simply impede
E while ventilatory regulation (i.e., respiratory drive) remained the same (28). The
finding that the relationship between the work of breathing
and exercise work rate was unchanged by resistive unloading
of the airways suggests that the regulation of
E is unchanged
by He-O2 breathing. Thus, the increase in
E with He-O2
breathing is simply the result of decreased respiratory impedance, which becomes greater as
E becomes higher. It also
suggests that the drive for breathing during exercise is more
related to the intensity of exercise and to the work of breathing (i.e., feed forward control and peripheral feedback from
the exercising limbs) than
E or pulmonary gas exchange (i.e.,
PETCO2), which can be altered by changes in respiratory impedance. These results have important implications for patients with pulmonary disease regarding the possible mechanisms by which the ventilatory response to exercise may be
increased or decreased during exercise.
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Footnotes |
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Correspondence and requests for reprints should be addressed to T. G. Babb, Ph.D., Institute for Exercise and Environmental Medicine, 7232 Greenville Ave., Dallas, TX 75231. E-mail: tonybabb{at}TexasHealth.org
(Received in original form August 6, 1999 and in revised form November 15, 2000).
Acknowledgments: The writer wishes to thank Darren DeLorey and Brenda Wyrick for their assistance throughout the various stages of this project. He also wishes to acknowledge the help of Penny Palumbo Gardner with data reduction and graphics, to express his appreciation to Dr. Benjamin Levine for his medical support of this project.
Supported by Grant NIA-AG-11805 from the National Institutes of Health.
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