Vol. 94, Issue 2, 576-582, February 2003
Magnitude estimation of inspiratory resistive loads by
double-lung transplant recipients
Weiying
Zhao,
A.
Daniel
Martin, and
Paul W.
Davenport
Department of Physical Therapy and Physiological
Sciences, University of Florida, Gainesville, Florida 32610
 |
ABSTRACT |
The purpose of this study was to
investigate the role of afferent input from the lung and lower airways
in magnitude estimation of inspiratory resistive loads (R). To assess
the role of lung vagal afferents in respiratory sensation, sensations
related to inspiratory R, reflected by subjects' percentage of
handgrip responses (HG%), were compared between double-lung transplant
(DLT) recipients with normal lung function and healthy control (Nor)
subjects. Perceptual sensitivity to the external load was measured as
the slope of HG% as a function of peak mouth pressure (Pm), and the slope of HG% as a function of R, after a log-log
transformation. The results showed that the DLT group had a
similar HG% response, as well as the slopes of log HG%-log Pm and log
HG%-log R, compared with the Nor group. Furthermore, the
ventilatory responses to external loads were also similar between the
two groups. These results suggest that lung vagal afferents do not play
a significant role in magnitude estimation of inspiratory resistive
loads in humans.
respiratory sensation; psychophysics; inspiratory load; load
compensation
 |
INTRODUCTION |
HUMANS CAN PERCEIVE
increases in ventilatory loads during both physiological conditions
(e.g., exercise) and pathological conditions (e.g., asthma, chronic
obstructive pulmonary disease). Load detection and magnitude estimation
are two perceptual processes of respiratory mechanosensation
(5). Magnitude estimation has been studied by using
scaling methods (3, 9, 12, 23-25). Subjects are
usually exposed to a series of suprathreshold loads and asked to
provide an estimate of the magnitude of the load by using numerical
scales or by cross-modality matching with handgrip tension. The
collective results of these studies have shown that increasing load
intensity is associated with increased perceptual estimate about the
load magnitude. There is a linear relationship between the load
magnitude and the perceptual estimate of the load when a log-log
transformation is made. The slope of the line, i.e., the exponent of
the Steven's psychophysical power function, is a measure of the
sensitivity of the subject to the stimulus.
Increases in inspiratory extrinsic load change the pattern of airflow,
volume, and pressure in the respiratory system. These mechanical changes may be sensed by mechanical receptors located in
lung and lower airways, which are innervated by the vagus nerves. However, the relative contribution of lung vagal afferent mechanism in
magnitude estimation of respiratory loads remains controversial. Burki
et al. (3) showed that upper and lower airway anesthesia in normal subjects did not alter the exponents for magnitude estimation of either resistive load (R) or elastic load. However, it is possible that some pulmonary stretch receptors may escape anesthesia because the
anesthetic agents could not penetrate to the smooth muscle. Furthermore, because both upper and lower airway receptors were interrupted by airway anesthesia in the study of Burki et al., it is
difficult to specify the role of lung and lower airway receptors in
magnitude estimation of respiratory loads.
Lung transplantation recipients provide a good model to clarify the
role of lung and lower airway receptors in respiratory sensation
because all of the afferent traffic from receptors located distal to
the surgical anastomosis are interrupted. In contrast to the findings
of Burki et al. (3), Peiffer et al. (20) found that the slope of the linear relationship between the Borg scores
and peak inspiratory mouth pressure (Pm) associated with breathing
against different R values was significantly lower in lung transplant
recipients. However, the difference in the slopes may be a
result of higher Pm and larger Pm range found in those lung transplant
recipients. Furthermore, subjects' perceptual sensitivity to the load
was not compared between the two groups in the study of Peiffer et al.
The purpose of this study was to investigate the role of afferent input
from lung and lower airways in magnitude estimation of inspiratory
resistive loads by recruiting double-lung transplant (DLT) recipients
as a lung denervation model. We hypothesized that the absence of
pulmonary afferents in those DLT recipients would result in a decrease
in load magnitude estimation and perceptual sensitivity to the load,
compared with matched normal (Nor) subjects.
 |
METHODS |
Subjects.
Studies were performed with 10 DLT patients and 12 Nor subjects. All
subjects were Caucasian. The DLT subjects were recruited from the
University of Florida Medical Center. The time since the DLT patients
received transplant surgery varied from 1.5 to 5.5 yr. None of the DLT
subjects had any evidence of current respiratory or neurological
disease, and no evidence of rejection was found in those patients when
they participated in the study. All of the DLT subjects were still on
immunosuppressive agents (Imuran, Prograf, etc.) and steroid
medications (Prednisone, etc.) when they participated in this study.
Forced vital capacity (FVC) and forced expiratory volume in 1 s
(FEV1) were tested for each subject. Subjects with a FVC or
FEV1 <70% of predicted values were excluded from this
study. Only one DLT subject was excluded from this study because of
abnormal lung function (FVC: 60.8% of predicted value; FEV1: 41.9% of predicted value). The Institutional Review
Board of University of Florida reviewed and approved this study. All participants provided informed consent before participating in this study.
Procedures.
Subjects were asked to refrain from strenuous physical activity, large
meals, and caffeine for at least 4 h before the test. All subjects
performed pulmonary function testing in a sitting position. Spirometry
testing conformed to American Thoracic Society Standards.
Standard instructions were given to each subject. All subjects
performed a FVC maneuver. Each test was repeated two to four times with
at least a 1-min rest between each repetition. The results were
contrasted with age- and sex-predicted reference values and were
expressed as a percentage of predictive values.
Background respiratory resistance was measured by using the forced
oscillation method. The subject was seated in front of the apparatus
and breathed "normally" through the mouthpiece, with his or her
cheeks supported by both hands. Approximately 10 tidal breaths were
collected continuously to analyze the resistance by computer (Jaeger
Toennies, Medizintechnikmit System, version 4.5). The test was repeated
at least three times for each subject with a 1-min rest between
repetitions. The average of three acceptable measures was used as the
subject's respiratory system resistance.
Inspiratory muscle strength was measured as the maximal inspiratory
pressure (MIP). Subjects were in a standing position when they
performed the test. After exhaling to residual volume, subjects were
instructed to place their lips around the mouthpiece and inspire as
forcefully as possible with their nose clamped. The test was repeated
until three measurements within 10% variation were obtained. There was
at least a 1-min rest between repetitions. The maximal value obtained
was recorded as the subject's MIP.
During the magnitude estimation experiment, the subject was
seated in a lounge chair in a sound-isolated chamber, separated from
the experimenter and the experimental apparatus. The subject was
instructed to breathe through a mouthpiece connected to a non-rebreathing valve (2600 series, Hans Rudolph) with their nose clamped. The inspiratory port of the valve was connected to the resistive loading manifold. Pm was measured at the center of the non-rebreathing valve and recorded on a polygraph. Inspiratory airflow
was measured with a differential pressure transducer (model MP45,
Validyne) and signal conditioner (model CD316, Validyne) connected to a
pneumotachograph. Inspired volume was obtained by electrical
integration of the airflow signal. Pm, inspiratory airflow, and volume
were recorded on a polygraph (Grass Instruments), stored, and analyzed
on a computer (model 7, Chart, Powerlab AD Instrument). The R
values were sintered bronze disks placed in series in the loading
manifold and separated by stopped ports.
Initially, subjects were asked to breathe normally with eyes closed. A
line was placed on the oscilloscope screen placed in front of each
subject that coincided with the peak inspiratory flow rate with quiet
breathing. This was set as the target flow rate. The subjects then
opened their eyes and breathed while watching the oscilloscope screen.
They were instructed to let their inspiratory airflow signals of each
breath "hit" the target line during the entire experiment.
Occasionally a light was illuminated on top of the oscilloscope during
expiration, cueing subjects that the next inspiration would be loaded.
Subjects estimated the test inspiration each time the light above the
oscilloscope was illuminated. They squeezed the handgrip by using their
dominant hand, according to the degree of difficulty of the perceived
inspiratory effort (sense of effort).
Before the resistive loading sessions, each subject squeezed the
handgrip as hard as possible three times and his or her handgrip response was recorded on the polygraph. All handgrip magnitude estimations were expressed as a percentage of their maximum handgrip responses. A practice session was then presented while informing the
subject of the size of the load ("large" or "small"). After a
rest period, a series of R values (1.64, 2.48, 3.26, 6.95, 11.46, 20.48, and 42.62 cmH2O · l
1 · s)
were presented in a randomized block design during the experimental session. Each loaded breath was separated by two to six unloaded breaths. The load was applied for the entire inspiration. A
total of 10 presentations of each load were presented in two trials with a 5-min rest period between trials. Subjects were monitored by
video camera throughout the study.
Data analysis.
The handgrip response during loaded breathing was divided by the
maximal handgrip response for each subject to obtain the percentage of
handgrip response (HG%). Only the handgrip responses that corresponded
to the load level greater than each subject's detection threshold,
which was predetermined for each subject before the study, were used
for analysis. The HG% was plotted against R magnitude and peak Pm by
using a log-log transformation. The regression line was obtained by
using the method of least squares, and the slopes from each subject
were determined (slope of log HG%-log R and slope of log HG%-log Pm).
Pm, peak volume (Vmax), peak inspiratory airflow, inspiratory duration
(TI), expiratory duration (TE), time to peak
airflow (TP), breathing frequency (f), and minute ventilation
(
E) were recorded for each loaded breath.
A one-tailed t-test was used to compare the slope of the DLT
group with the slope of the Nor group. A two-way repeated-measures ANOVA was performed to estimate the effects of group and different level of loads on the value of HG%, Pm, peak inspiratory airflow, Vmax, TI, TE, f, and
E.
Contrast analysis was performed to compare the effects of different
loads. The P value for each contrast test was
corrected by dividing 0.05 by the total number of contrasts.
The descriptive statistics of all the variables were calculated and
expressed as means ± SE. Significance level was set at 0.05, unless multiple contrast analysis was used.
 |
RESULTS |
The group mean demographic characteristics and pulmonary functions
of all the subjects that participated in this study are shown in Table
1. The DLT and the Nor groups were
comparable in age, height, and weight. Background respiratory
resistance and MIP between the two groups were not significantly
different. Both FVC and FEV1 were significantly lower in
the DLT group than in the Nor group (97.0 ± 4.9% vs. 119.5 ± 5.0% of predictive value and 83.8 ± 6.1 vs. 108.3 ± 3.7% of predictive value, respectively). However, both FVC and
FEV1 were still within normal range in the DLT group.
FEV1-to-FVC ratio was not significantly different between the two groups (88.1 ± 6.0% of predicted value for the DLT group vs. 93.9 ± 2.8% of predicted value for the Nor group;
P = 0.371).
Two-way repeated-measures ANOVA showed no main effects of group for Pm
(Fig. 1), Vmax, peak airflow (Fig.
2), TI, TE, TP, f, and
E. This indicated that the loaded breathing
pattern during magnitude estimation was not significantly different
between the DLT group and the Nor group. All of the above breathing
pattern parameters displayed a significant load effect
(P < 0.05), except TE (P = 0.068). Specifically, as the magnitude of R increased, Pm, Vmax,
TI, and TP increased significantly, whereas airflow, f, and
E decreased. Load and group interaction effects were significant for airflow, TI, and f (P < 0.05). The range of Pm during loaded breathing was not significantly
different between the DLT patients and the Nor subjects (12.22 ± 1.2 vs. 15.14 ± 1.5 cmH2O; P = 0.155), as shown in Fig. 3.

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Fig. 1.
Peak inspiratory mouth pressure (Pm) at different levels
of resistance during loaded breathing in the double-lung transplant
(DLT) group and the normal (Nor) group. Values are means ± SE;
n, no. of subjects.
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Fig. 2.
Peak inspiratory airflow at different levels of
resistance during loaded breathing in the DLT group and the Nor group.
Values are means ± SE; n, no. of subjects.
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Fig. 3.
Group mean of peak inspiratory Pm range in the DLT group
and the Nor group. Values are means ± SE.
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The relationships between the magnitude estimate of breathing
difficulty (represented by HG%) and stimulus intensity (R and Pm) are
displayed in Fig. 4. As the magnitude of
R increased, Pm and HG% increased. For both DLT and Nor subjects, the
peak handgrip response occurred at approximately midinspiration when mouth pressure and inpiratory airflow reached peak. This
suggested that, at higher loads, the subjects generated higher Pm and
squeezed the handgrip harder. The main effect of load on HG% is
significant (P < 0.001). Two-way repeated-measures
ANOVA found no significant difference between the DLT group and the Nor
group in their handgrip response (P = 0.93).

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Fig. 4.
Percentage of the handgrip response (HG%) as a function
of the magnitude of resistive loads (A) and peak inspiratory
Pm (B) after a log-log transformation in the DLT group and
the Nor group. Values are means ± SE.
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The exponents of the power function relationships between load and
estimated magnitude of load, i.e., the slope of log HG%-log R and the
slope of log HG%-log Pm, reflects the sensitivity of the subject to
the load (Fig. 5). The mean slope of log
HG%-log R for the DLT group and the Nor group was 0.39 ± 0.08 and 0.42 ± 0.06, respectively. The mean slop of log HG%-log Pm
for the DLT group and the Nor group was 0.66 ± 0.15 and 0.57 ± 0.07, respectively. There was no significant difference between
the two groups for either slope (P = 0.38 for log
HG%-log R, and P = 0.29 for log HG%-log Pm).

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Fig. 5.
Group mean slope of the log-log relationship between HG%
and resistive loads (A) and between HG% and peak
inspiratory Pm (B) in the DLT group and the Nor group.
Values are means ± SE.
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 |
DISCUSSION |
The results of the present study showed that the DLT and the Nor
groups were both able to target their breathing with a similar loaded
breathing pattern. The handgrip responses were also similar between the
DLT and the Nor group. No significant differences were found in the
sensitivity to inspiratory R values between the two groups. These
results suggest that the ability of the subjects to behaviorally
control their inspiration and to estimate inspiratory R magnitude and
the sensitivity of the subjects to load magnitude were not changed
after lung denervation.
Many studies have examined the relationship between the perceived
magnitude of loads and the intensity of the load (3, 9, 12,
23-25). In the present study, the subjects were asked to
provide an estimate of the magnitude of R by using their handgrip response (HG%). Similar to previous studies, as the load increased, larger handgrip responses were given by all subjects. The sensitivity of the person to the stimulus, i.e., the mean slope, obtained in Nor
subjects in the present study (0.57 ± 0.07 for log Hg%-log Pm,
and 0.42 ± 0.06 for log Hg%-log R, respectively) was lower compared with previous reports, in which the exponents varied from 0.57 to 0.96 (3, 9, 12, 14, 21). The difference might be due to
the difference in the subjects' age, the load range, the scale used to
estimate magnitude, and airflow targeting. The mean age of Nor subjects
in this study was 46.6 ± 4.4 yr, which was older than those
reported in previous studies. Tack et al. (23) studied the
effect of age on magnitude estimation. They found that the exponent for
both inspiratory and expiratory loads was reduced in older subjects,
which was probably due to age-related changes in sensory perception. In
the present study, the R values ranged from 1.64 to 42.62 cmH2O · l
1 · s.
A "range effect" is another possible explanation to account for the
differences in exponent obtained from other studies. This refers to a
general law in psychophysics stating that the higher the range of a
given stimulus, the lower the rate of increase in the intensity of the
induced sensation (19). Therefore, the lower slope found
in this study might be due to a relatively large load range used in the
magnitude estimation task. Moreover, some studies used numerical scales
(e.g., Borg scale) (9, 12, 14), whereas others (including
the present study) used cross-modality matching (e.g., handgrip
response) (3, 21) to estimate load magnitude. Unlike the
Borg scale, for which subjects only needed to select a number from the
Borg scale to match their breathing difficulty, cross-modality matching
method involves a more complicated process. First, the subject has to
detect and quantify the load. Then, the subject has to translate the
respiratory sensation into a handgrip response quantitatively. At the
same time, the subject's sensation arising from their handgrip
squeezing has to be transferred back to the higher brain center to
match the previous sensations about the external load that the
subject breathes against. It is possible that handgrip and Borg
scale magnitude estimates result from two different types of neural
processing. Muza and Zechman (16) compared different
scales in magnitude estimation. The mean exponent and correlation
coefficient obtained from numerical estimates were 1.11 ± 0.16 and 0.94 ± 0.04, respectively, whereas the exponent and
correlation coefficient simultaneously obtained from handgrip matching
was 0.73 ± 0.10 and 0.91 ± 0.05, respectively. Therefore,
the choice of a different scaling method will affect the absolute value
of the exponent. However, both scaling methods have been found to be
able to reflect the effect of the resistive load level, and both
correlated well with load size and Pm in our laboratory (unpublished
observations). The use of handgrip scaling method provides
more information about the subjects' perceptual response (e.g., the
temporal pattern of response). A final explanation about the difference
in exponent among studies might be due to whether or how well airflow
was targeted in those studies. In the present study, even though the
subjects were instructed to reach the peak airflow target during loaded
breathing, airflow still decreased as load magnitude increased (Fig.
2), especially for the three highest loads (11.46, 20.48, and 42.62 cmH2O · l
1 · s).
Therefore, it was possible that the actual impedance of those high
loads was underestimated, which might flatten the regression line when
log HG% was plotted against log R.
Few studies have investigated the role of vagal afferent inputs in
inspiratory load magnitude estimation tasks. Burki et al. (3) found that anesthesia of the upper and lower airways
did not significantly alter the slope between log added resistive load
and log handgrip response. However, it is possible that some pulmonary
stretch receptors may escape topical anesthesia because the anesthetic
could not penetrate to the smooth muscle or because the drug was
carried away rapidly by rich blood flow (2). Moreover, because both upper and lower airway receptors were blunted in their
methods, it is not possible to make a conclusion about the specific
role of lung and lower airway afferents in load magnitude estimation.
Lung transplantation, through a total interruption of afferent nerve
fibers from the lung and lower airways, provides an opportunity to
study the contribution of neural feedback from lung and lower airways
to respiratory sensation. The present study found that the loaded
breathing pattern and handgrip response during the magnitude estimation
experiment were similar between the DLT group and the Nor group. It has
been found in our laboratory that those DLT subjects had a similar
resting breathing pattern compared with Nor subjects (26).
Therefore, the influence of breathing pattern on the subjects'
respiratory perceptual response should be minimal. Both groups showed a
higher handgrip response as load magnitude increased. There were no
significant differences in the slope of log HG%-log Pm (0.66 ± 0.15 in DLT vs. 0.57 ± 0.07 in Nor; P = 0.59) and
the slope of log HG%-log R (0.39 ± 0.08 in DLT vs. 0.42 0 ± 0.06 in Nor; P = 0.76). These results suggest that
lung vagal afferents are not essential to magnitude estimation of
suprathreshold loads. Recently, Peiffer et al. (20)
compared sensations related to inspiratory resistive loaded breathing
in lung transplant recipients and healthy control subjects. In contrast to our results, they found that the slope of Borg scale as a function of peak Pm was significantly lower in lung transplant recipients than
controls (0.63 vs. 1.26; P < 0.01). Although they did
not report the analysis in absolute Borg scale scores between the two
groups, it appeared that the difference in the slope of Borg scale as a
function of Pm was only due to the difference in Pm between the two
groups. Indeed, their lung transplant recipients had a significantly
higher peak Pm and higher individual range of Pm than normal subjects
(10.4 ± 5.6 vs. 4.8 ± 0.96 cmH2O, respectively) during loaded breathing. Therefore, the lowered slope found in lung
transplant patients might result from the higher range of stimulus,
i.e., a range effect (19), instead of from lung
denervation. In the present study, Pm range was not
significantly different between the DLT group and the Nor group
(12.22 ± 1.2 vs. 15.12 ± 1.5 cmH2O,
respectively; P = 0.159), nor was peak Pm (Fig. 1). The
difference in lung transplant subjects' loaded responses between the
present study and that of Peiffer et al. (20) might also be a result of the methodology difference. In their protocol, airflow
was not targeted. Therefore, it is likely that the subject may
underestimate the load magnitude if their inspiratory airflow is
reduced during loaded breathing. Moreover, according to their methods,
inspiratory resistive loads were presented for the duration of two
consecutive inspiratory breaths. It is not known whether their
magnitude estimates come from the first or the second loaded breath.
Load responses will be different for the first breath compared with the
second breath. Furthermore, inspiratory muscle strength was not
measured. Lung transplant recipients usually have weakened respiratory
muscles because of the use of steroid medications and/or deconditioning
after surgery (22). Most studies demonstrated a close
relationship between weak muscle strength and increased respiratory
drive (1, 8). However, weakened inspiratory muscles and
increased drive should increase the intensity of respiratory
sensations, which was opposite to their results. The DLT subjects in
the present study had similar inspiratory muscle strength compared with
the Nor group. Although we did not measure inspiratory drive directly,
it would be reasonable to believe the drive would be similar due to
similar inspiratory muscle strength in these two groups. Therefore, the
impact of inspiratory muscle strength and drive on load magnitude
estimation is minimal in this study.
There is a possible contribution of vagal afferents from receptors
proximal to the anastomosis to the load magnitude estimation in the DLT
subjects. However, the vagal innervaton remaining in the transplanted
patients is a small portion of the vagal innervation in the lower
airway and lung. Therefore, the impact of the remaining vagal input
should be minimal. An important assumption of this study is that DLTs
are, and remain, entirely denervated after surgery. The results of
several investigations performed in animals found reappearance of a
weak Hering-Breuer inflation reflex as early as 5 mo after pulmonary
autotransplantation (6, 15). However, reinervation would
be less likely in the context of human allotransplantation than with
simple reimplantation of an excised lung as in the canine model because
no attempt is made to approximate nerves in DLT patients
(13). In a study investigating the integrity of the cough
reflex, which is mediated mostly by pulmonary receptors, after lung
transplant, Higenbottam and co-workers (10) observed a
significantly diminished cough response to ultrasonically nebulized distilled water for up to 3 yr after lung transplant. More compelling evidence for persistent lung denervation after human lung transplant has been provided by Iber et al. (11). They reported
persistently absent expiratory prolongation after passive lung
inflation during sleep in bilateral lung transplant recipients for a
period of 49 mo after surgery. In contrast to the above findings,
Butler et al. (4) reported that respiratory events (cough
or apnea) and noxious sensations evoked by injections of lobeline (>30
µg/kg) occurred in a few bilateral lung transplantation subjects who were studied >1 yr after transplantation. Their results suggested that
there might be functional reinnervation of the lungs after bilateral
lung transplantation. However, changes in nonpulmonary receptors may
have occurred over time to recover the sensitivity to lobeline in those
patients. In the present study, the time since the patients received
DLT surgery varied from 1.5 to 5.5 yr, with an average of 3.45 yr.
Although we did not test the reinnervation in our patients, it seems
unlikely that reinnervation had occurred on the bais of previous
findings (10, 11). Interestingly, a previous study in our
laboratory showed that the DLT subjects had a significantly elevated
inspiratory R detection threshold as well as Weber fraction
(26). In addition, the activation of cortical neurons by
breathing against mechanical loads has been studied by using the
respiratory-related evoked potential (RREP) method in the DLT subjects
(27). Early-latency RREP components were not affected by
lung denervation, whereas the late-latency RREP component
(P3) was found to be significantly delayed and attenuated
in the DLT subjects. This suggests that lung vagal afferents may play a
role in respiratory load perception. However, the presence of both
early- and late-latency RREP components in DLT patients, as well as the
fact that these DLT patients were able to detect inspiratory R and
magnitude estimate loads similarly to normal subjects, indicates that
lung vagal afferents are not the sole input and they are not essential
to perceptual processing of respiratory mechanical loads. Load
perception is certainly a multimodal process; however, further studies
are needed to investigate the interactions among different afferent
mechanisms in respiratory load perception.
Conclusions.
In summary, we found that the handgrip response and loaded breathing
pattern were similar in the DLT group and the Nor group. Furthermore,
the slopes of log HG%-log Pm and logHG%-log R were also comparable in
the two groups. These findings suggest that neural feedback from the
lung and lower airways does not play a significant role in inspiratory
resistive load magnitude estimation tasks. It is possible that the
relative importance of other potential afferent mechanisms (upper
airway, respiratory muscle, chest wall, etc.) may be altered as one
site is blocked, e.g., lung denervation. Similarly, a nonexclusive role
in respiratory sensation has been previously demonstrated for other
potential paths, such as chest wall (7), phrenic nerve
(17), or upper airway (18), suggesting that
respiratory sensation related to loaded breathing may be due to
multiple and simultaneous sensory inputs.
 |
ACKNOWLEDGEMENTS |
This study was supported by National Heart, Lung, and Blood
Institute Grant HL-47892.
 |
FOOTNOTES |
Address for reprint requests and other correspondence:
P. W. Davenport, Dept. of Physiological Sciences, Box
100144, HSC, Univ. of Florida, Gainesville, FL 32610 (E-mail:
davenportp{at}mail.vetmed.ufl.edu).
The costs of publication of this
article were defrayed in part by the
payment of page charges. The article
must therefore be hereby marked
"advertisement"
in accordance with 18 U.S.C. Section 1734 solely to indicate this fact.
First published October 11, 2002;10.1152/japplphysiol.00564.2002
Received 27 June 2002; accepted in final form 3 October 2002.
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