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ABSTRACT |
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In the study reported here, we partitioned the mechanics of the respiratory system into lung and
chest-wall components, using the rapid occlusion technique in seven patients with severe emphysema before lung-volume-reduction surgery and 3 mo later. Patients showed improvements in 6-min
walk (p < 0.01) and dyspnea (p < 0.05). The resistances of the respiratory system and chest wall were not altered by surgery. Ohmic airway resistance did not change, but the component of lung resistance (
RL) due to viscoelastic behavior (stress relaxation) and time-constant inhomogeneities (pendelluft) decreased in six patients (p < 0.03). Dynamic elastance of the lung (Edyn,L) decreased after surgery (p < 0.02), whereas dynamic elastance of the chest wall did not change. The ratio of dynamic intrinsic positive end-expiratory pressure (PEEPi) to static PEEPi, which also reflects viscoelastic
properties and time-constant inhomogeneities, increased after surgery (p < 0.05). The decrease in
dyspnea was related to the decrease in Edyn,L (r = 0.81, p = 0.03), and tended to be related to the decrease in
RL (r = 0.71, p = 0.07). In conclusion, lung-volume-reduction surgery decreased dynamic
pressure dissipations caused by stress relaxation and time-constant inhomogeneities within lung tissue, and it had no effect on the static mechanical properties of the chest wall.
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INTRODUCTION |
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Following lung-volume-reduction surgery, patients with emphysema show improvement in dyspnea, exercise tolerance, and airflow obstruction (1). Although the mechanism of benefit is largely unknown, recent reports suggest that improvements in lung elastic recoil (2), airway conductance (4), and diaphragmatic function (5) may play a role.
Hyperinflation, a hallmark of emphysema, causes breathing to occur at an unfavorable position on the pressure-volume curve of both the lung and the chest wall, leading to an increase in the work of breathing (6). Other factors contributing to the increase in respiratory work include increases in airway resistance, lung-tissue resistance, time-constant inequality within the lung (pendelluft), pressure losses in the viscoelastic units of the lung (stress relaxation), and intrinsic positive end-expiratory pressure (PEEPi) (7). It is conceivable that the benefit of lung-volume-reduction surgery is due to alterations in one or more of these factors.
In a group of patients with emphysema undergoing lung-volume-reduction surgery, we partitioned the mechanics of the total respiratory system into the lung and chest-wall components. Partitioning was achieved by passive ventilation and the rapid airway occlusion technique, which also allowed us to differentiate between the contributions to total respiratory system resistance of ohmic airway resistance and viscoelastic behavior/time-constant inhomogeneities, and to fractionate total dynamic elastance into the components derived from static elastance and additional elastic pressure stored in viscoelastic units (8). To the best of our knowledge, this is the first detailed breakdown of respiratory-system mechanics with an examination of the effect of lung-volume-reduction surgery on each individual component.
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METHODS |
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Patients
We studied six men and one woman (age 62 ± 4 yr [mean ± SE]) with severe airflow limitation and roentgenographic evidence of emphysema. These patients were the same patients in whom we concurrently measured respiratory-muscle performance before and after surgery (5). The study was approved by the Human Studies Subcommittee of the Edward Hines Jr. Veterans Administration Hospital, and informed consent was obtained from each patient. Approximately 25% of each lung was resected via a median sternotomy (1). All patients were enrolled in a structured, supervised exercise rehabilitation program for a minimum of 6 wk before and 12 wk after surgery.
Apparatus
Flow was measured with a heated Fleisch pneumotachograph (Hans Rudolph, Kansas City, MO) placed between the mouthpiece and the Y-piece of the external ventilator circuit. Esophageal pressure (Pes) and gastric pressure (Pga) were measured separately with two thin-walled, latex-balloon-tipped catheters (Erich Jaeger, Wurzberg, Germany) coupled to pressure transducers (MP-45; Validyne, Northridge, CA). Airway pressure (Paw) was measured at the mouthpiece with a tap connected to another transducer. Transpulmonary pressure (PL) was obtained by subtracting Pes from Paw. Electromyographic (EMG) activity of the diaphragm was monitored with surface EMG electrodes.
Functional Assessment
Lung volumes were measured by body plethysmography and timed spirometry. The magnitude of dyspnea was quantified with a visual analog scale, on which patients marked their response to the question "How uncomfortable is your breathing?" Six-minute walking distance was performed according to the standard procedure.
Protocol
Data were recorded 1 to 2 wk before and 3 mo after surgery. Each patient was studied in the sitting position while breathing through a mouthpiece, which in turn was connected to a ventilator (7200a; Puritan Bennett, Carlsbad, CA). Passive ventilation was achieved by gradually increasing the backup rate on the ventilator until the patient's inspiratory muscle activity was completely suppressed. Cessation of patient effort was confirmed by the absence of inspiratory phasic EMG activity and negative deflections of Pes and Paw, and by the uniformity of pressure contour and breath-cycle duration (9, 10); cessation of expiratory muscle recruitment was confirmed by the absence of deviations in the Pga tracings. Because of the flow and volume dependency of resistance and elastance, we maintained identical flow and tidal volume (VT) settings in each patient before and after surgery. For the group, a VT of 0.729 ± 0.06 L and a flow of 1.07 ± 0.05 L/s were used. Lung volume, 6-min walking distance, and dyspnea score at rest were also recorded.
Physiologic Measurements
The mechanics of the respiratory system were partitioned into the
lung and chest-wall components using Pes and the constant-flow, rapid-occlusion method (10, 11). The airway opening was occluded at
the end of a passive inflation for a duration sufficient to achieve a
pressure plateau. After the occlusion, there was an immediate decrease in both Paw and PL from a peak value (Ppeak) to a lower initial
value (Pinit), followed by a gradual decrease until a plateau (Pplat) was
achieved; the second decrement is termed
P. Pinit was measured by
back-extrapolation of the slope of the latter part of the pressure tracing to the time of airway occlusion (8).
The maximum and minimum resistances of the total respiratory
system (Rmax,rs and Rmin,rs, respectively), lung (Rmax,L and Rmin,L, respectively), and chest wall (Rmax,w and Rmin,w, respectively) were computed by dividing Ppeak
Pplat and Ppeak
Pinit from the Paw, PL, and
Pes tracings, respectively, by the flow immediately preceding the occlusion (8). The additional resistances of the respiratory system (
Rrs),
lung (
RL), and chest wall (
RW) were calculated as Rmax,rs
Rmin,rs,
Rmax,L
Rmin,L, and Rmax,w
Rmin,w, respectively. Rmin is considered to
reflect ohmic airway resistance (i.e., true airflow resistance in the absence of unequal time constants within the lung) (8).
R reflects the
viscoelastic properties (stress relaxation) of respiratory tissue when the lung is normal, and also includes a significant contribution from gas redistribution between alveoli with high- and low-pressure units (i.e.,
pendelluft) when the lungs are abnormal and inhomogenous (8). Dynamic PEEPi values of the respiratory system (PEEPi,dyn,rs), lung
(PEEPi,dyn,L), and chest wall (PEEPi,dyn,w) were computed as the
change in Paw, PL, and Pes, respectively, generated by the ventilator to
initiate airflow (12). Static PEEPi values of the total respiratory system
(PEEPi,stat,rs), lung (PEEPi,stat,L), and chest wall (PEEPi,stat,w) were measured as the change in Paw, PL, and Pes, respectively, after the airway
was occluded at end-expiration (11). Dynamic elastances of the respiratory system (Edyn,rs), lung (Edyn,L), and chest wall (Edyn,cw) were measured by dividing Pinit
PEEPistat on the Paw, PL, and Pes tracings, respectively, by VT. Static elastances of the total respiratory system
(Est,rs), lung (Est,L), and chest wall (Est,w) were measured by dividing Pplat
PEEPistat on the Paw, PL, and Pes tracings, respectively, by VT.
Data Analysis
Mechanics of the respiratory system, lung, and chest wall before and after surgery were compared through paired t tests. Regression analysis was used to calculate the correlation coefficient between different variables.
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RESULTS |
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Surgery produced improvements in lung function. FVC increased from 2.02 ± 0.12 to 2.46 ± 0.15 L (p < 0.01); FRC decreased from 6.93 ± 0.46 L to 6.28 ± 0.47 L (p < 0.01); and RV decreased from 5.97 ± 0.45 L to 5.23 ± 0.48 L (p < 0.01). Dyspnea at rest, assessed by a visual analog scale, decreased from 57 ± 11 mm to 22 ± 6 mm (p < 0.05), and the distance covered during a 6-min walk increased from 808 ± 115 feet to 1,198 ± 99 feet (p < 0.01).
Mechanical characteristics of the respiratory system, lung,
and chest wall in patients before and after surgery are shown in Table 1.
RL decreased by 59% in six of seven patients (p < 0.03), whereas Rmin,L remained unchanged after surgery (Figure 1). Edyn,L decreased by 24% after surgery (p < 0.02) (Figure 2), and Edyn,rs tended to decrease (p = 0.07). PEEPi,stat,L
decreased by 28% after surgery (p < 0.02), and PEEPi,stat,rs
tended to decrease (p = 0.07). The ratio of PEEPi,dyn,L to
PEEPi,stat,L
reflecting time-constant inequalities and/or viscoelastic pressure losses
increased by almost 60% after surgery (p < 0.05) (Figure 3). Resistance, elastance, and PEEPi
of the chest wall were not altered by surgery. The change in
dyspnea was positively correlated with the change in Edyn,L (r = 0.81), and tended to correlate with the change in
RL (r = 0.71) (Figure 4).
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DISCUSSION |
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Lung-volume-reduction surgery decreased the dynamic pressure dissipations resulting from stress relaxation and time-constant inhomogeneities within lung tissue. The mechanical properties of the chest wall were not altered by the surgery.
Rmax,rs originated almost completely within the lungs, with
minimal contribution from the chest wall (Table 1). The pulmonary flow resistance (Rmax,L) was largely due to airway resistance (Rmin,L), with a smaller additional resistance (
RL) due
to time-constant inequality and viscoelastic pressure dissipations
within the lungs. The resistance values in our patients were
considerably lower than those reported in ventilator-dependent patients with chronic obstructive pulmonary disease
(COPD) (11), presumably because our patients were in a stable condition, without evidence of acute decompensation, and
were breathing through a mouthpiece without an artificial airway. The ohmic resistance of the airway (Rmin,L) was unaffected by surgery, whereas
RL decreased in six of the seven
patients (p < 0.03) (Figure 1). Moreover, the decrease in
RL
was associated with a reduction in dyspnea after surgery (Figure 4). This suggests that the beneficial action of surgery is
mediated in part through a decrease in time-constant inhomogeneity (pendelluft) and/or pressure losses in viscoelastic
units. The decrease in
RL may be a consequence of the decrease in lung volume effected by surgery, since
RL has been
shown to decrease as a function of lung volume (7).
The tendency toward a decrease in Edyn,rs after surgery was
due to a decrease in Edyn,L (Table 1). This decrease in Edyn,L is
in agreement with our parallel study (5), in which an increase in dynamic lung compliance (Cdyn) was observed after surgery. The different values for Edyn,L and Cdyn in the two studies can be explained by the different methodologies employed. Since
the present paper focuses on respiratory mechanics during
passive conditions, Edyn,L was measured with the constant-flow, rapid occlusion technique (8). In contrast, the measurement of Cdyn in our parallel study was obtained during spontaneous breathing (13). Because Estat,L did not change after surgery, the decrease in Edyn,L is likely to have resulted from a
decrease in the additional elastic pressure stored in viscoelastic units of the pulmonary tissues, and/or from time-constant
inhomogeneities within the lung, (i.e.,
EL) (7). Indeed,
EL
(Edyn,L
Estat,L) decreased in six of the seven patients (p < 0.05) (Figure 2). In contrast to our observations, Gelb and colleagues (4) noted an increase in Estat,L after surgery. The discrepancy between the reports is probably because they (4)
studied patients in the operating room immediately after surgery, whereas our study was performed 3 mo after surgery; accordingly, the increase in Estat,L in their patients could have
been due to the effects of anesthesia and/or surgical trauma to
lung tissue. Moreover, the distending pressures were different
in the two studies: Gelb and colleagues (4) measured elastance
at end-expiratory lung volume (EELV), EELV + 0.60 L, and
EELV + 1.0 L, whereas we measured it at EELV + 0.73 L. Of
note, the elastance of the chest wall did not change with surgery in either study.
Surgery produced a decrease in PEEPi,stat,L without a change
in PEEPi,dyn,L (Table 1). Static PEEPi represents the average level of PEEPi in nonhomogeneous lung after equilibration of
alveolar pressure among lung units with varying time constants, whereas dynamic PEEPi represents the lowest regional
value of PEEPi that needs to be overcome to initiate lung inflation. The ratio of PEEPi,dyn,L to PEEPi,stat,L increased after
surgery (Figure 3), and the increase in this ratio tended to correlate negatively (r =
0.61) with
P, which is the secondary
decrease in pressure between the initial drop to the final plateau during an end-inspiratory occlusion (7, 8). This supports
the notion that the ratio of PEEPi,dyn,L to PEEPi,stat,L reflects
time-constant inequalities within the lung and/or increased
viscoelastic pressure losses, as has been suggested by Maltais
and coworkers (12). The combined changes in the ratio of
PEEPi,dyn,L to PEEPi,stat,L,
RL, and
EL suggest that characteristic responses to lung-volume-reduction surgery include a
decrease in time-constant inhomogeneity and viscoelastic
pressure losses in lung tissue.
The amelioration of dyspnea was correlated with improvements in
RL and Edyn,L (Figure 4). The decrease in Edyn,L suggests that breathing took place on a more compliant portion of
the pulmonary pressure-volume curve after surgery; this decrease in operating lung volume could be partly responsible
for the symptomatic improvement following surgery (14). The
second factor associated with the decrease in dyspnea,
RL,
may also be explained by a decrease in lung volume (7). Specifically, the decrease in
RL implies that lung emptying is
more efficient and that flow limitation is somewhat lessened.
As a result, patients need no longer increase their lung volume
to increase expiratory flow. Indeed, EELV probably decreases
in these patients, as suggested by a decrease in PEEPi,stat (Table 1, Figure 3). This decrease in EELV will cause the inspiratory muscles to operate at a more favorable position on the
length-tension curve, with an improvement of pressure-generating capacity, as shown in our parallel study (5). Moreover,
lessening of dynamic collapse may also have contributed to
symptomatic improvement, since compression of the airways
has been shown to contribute to dyspnea, probably through
activation of the upper-airway mechanoreceptors (15).
In conclusion, we found that the decrease in dyspnea achieved by lung-volume-reduction surgery is related to decreases in time-constant inhomogeneities (pendelluft) and in the storage of additional resistive and elastic pressure in the viscoelastic units of the pulmonary tissues.
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Footnotes |
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Correspondence and requests for reprints should be addressed to Amal Jubran, M.D., Division of Pulmonary and Critical Care Medicine, Edward Hines Jr. VA Hospital, Hines, IL 60141.
(Received in original form June 23, 1997 and in revised form January 20, 1998).
Acknowledgments: Supported by grants from the Veterans Administration Research Service and from the American Lung Association of Metropolitan Chicago.
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