help button home button
AJRCCM
HOME HELP FEEDBACK SUBSCRIPTIONS ARCHIVE SEARCH TABLE OF CONTENTS

This Article
Right arrow Abstract Freely available
Right arrow Full Text (PDF)
Right arrow Alert me when this article is cited
Right arrow Alert me if a correction is posted
Services
Right arrow Similar articles in this journal
Right arrow Similar articles in PubMed
Right arrow Alert me to new issues of the journal
Right arrow Download to citation manager
Right arrow reprints & permissions
Citing Articles
Right arrow Citing Articles via HighWire
Right arrow Citing Articles via Google Scholar
Google Scholar
Right arrow Articles by KADITIS, A. G.
Right arrow Articles by MOTOYAMA, E. K.
Right arrow Search for Related Content
PubMed
Right arrow PubMed Citation
Right arrow Articles by KADITIS, A. G.
Right arrow Articles by MOTOYAMA, E. K.
Am. J. Respir. Crit. Care Med., Volume 159, Number 2, February 1999, 389-396

Partitioning of Respiratory System Resistance in Children with Respiratory Insufficiency

ATHANASIOS G. KADITIS, SHEKHAR T. VENKATARAMAN, WALTER A. ZIN, and ETSURO K. MOTOYAMA

Departments of Pediatrics (Division of Pediatric Pulmonology) and Anesthesiology and Critical Care Medicine, University of Pittsburgh School of Medicine and Children's Hospital of Pittsburgh, Pittsburgh, Pennsylvania; and Institute of Biophysics, Federal University of Rio de Janeiro, Rio de Janeiro, Brazil

    ABSTRACT
TOP
ABSTRACT
INTRODUCTION
METHODS
RESULTS
DISCUSSION
REFERENCES

Using end-inspiratory airway occlusion, respiratory system resistance (Rrs) can be partitioned into a flow-resistive component (Rint), and an additional component (Delta R), reflecting viscoelasticity and time constant inequalities. We studied flow and volume dependence of Rrs and its subdivisions (Rint and Delta R) in 13 children, seven mechanically ventilated for pulmonary insufficiency (Group 1; six with parenchymal lung disease; one with lower airway obstruction) and six without primary lung disorder (Group 2). In comparison with healthy children, Rint was increased in the patient with lower airway obstruction and five of six patients without primary lung disorder but in only one of six with parenchymal lung disease. Delta R was increased in all seven patients in Group 1 and in four of six patients in Group 2. The directions of changes in Rint and Rrs with increasing flow (isovolume conditions) and with increasing volume (isoflow conditions) were variable. Delta R decreased exponentially (p < 0.05) with increasing flow in 11 of 13 subjects and increased with increasing tidal volume (VT) in 12 of 13. Thus, Delta R was increased in most children on mechanical ventilation with or without primary lung disease; its volume and flow dependence were opposite to that of airway resistance.

    INTRODUCTION
TOP
ABSTRACT
INTRODUCTION
METHODS
RESULTS
DISCUSSION
REFERENCES

The end-inspiratory airway occlusion method is the combination of the interrupter (1) and elastic subtraction (2) techniques, originally described by von Neergaard and Wirz in 1927. This method was reintroduced by Bates and coworkers recently, for the assessment of respiratory mechanics (3). The results of early studies in anesthetized paralyzed animals (4, 5) were interpreted in terms of a model which separates the flow-resistive component (Rint) from the viscoelastic component (Delta R) of the total respiratory system resistance (Rrs) (6).

Hitherto, the end-inspiratory airway occlusion method has been used in otherwise healthy adults under general anesthesia and in adults with respiratory insufficiency who were on mechanical ventilation (7). We have previously reported values of intrinsic flow resistance and viscoelastic resistance in healthy children under general anesthesia undergoing minor elective surgery (15). Measurements in newborn infants have been presented by other investigators (16). Additionally, in several studies in children with and without lung disease, the midexpiratory airway occlusion technique has been used (17).

In the present study, we applied the end-inspiratory occlusion technique to critically ill, mechanically ventilated pediatric patients with and without primary lung disease. The working hypothesis was that children with parenchymal lung disease would demonstrate an increase in viscoelastic tissue resistance (Delta R) but without changes in airway resistance, as represented by Rint, as seen in adult patients (10). Further, children with lower airway obstruction would have increased Rint and Delta R (14), whereas those on mechanical ventilation without prior lung disease would show essentially normal Rint and Delta R. This study also compared the flow and volume dependence of Rrs and its subdivisions to those found in adult patients.

Technical and theoretical features of the end-inspiratory occlusion method have been extensively reviewed in the literature (3, 7, 21) and are briefly summarized here. After a rapid end-inspiratory occlusion, there is an initial rapid drop in airway pressure proximal to the endotracheal (ET) tube (Pao), representing intrinsic flow resistive component (Rint), mostly caused by airway resistance (Raw). The subsequent slower decrease in Pao is the result of intrinsic viscoelastic resistance (Delta R) of lung and chest wall tissues. Both Rint and Delta R change with changes in constant inspiratory flow (VI) and tidal volume (VT); but the directions of their volume and flow dependence are opposite of each other (7). Delta R has been found to be the major component of Rrs, especially at VI less than 1 L/s in adults (7). Consequently, the direction of flow and volume dependence of Rrs follows changes of Delta R, not those of Rint, as has been assumed in the past (21).

The viscoelastic property of the respiratory system can be explained by the "spring-and-dashpot" model, in which a Maxwell body is added in parallel to the standard (flow) resistance (dashpot or shock absorber, Rint) and static elastance of the total respiratory system (spring, Est) (6, 7). The Maxwell body consists of a second spring (E2) and dashpot (R2) in series. After end-inspiratory airway occlusion, E2 dissipates its stored energy on R2, representing the existence of an additional non-Newtonian resistance (effective resistance, Delta R). Delta R is responsible for the slow decrease in Pao after the end-inspiratory airway occlusion. As the inspiratory time decreases (with high frequency, high inspiratory flow, or smaller VT), most energy offered to the Maxwell body is stored in E2, because R2 has less time to move and dissipate energy. This means lower effective tissue resistance (Delta R) and higher effective tissue elastance (Delta E) for the total respiratory system (21). Viscoelasticity (Maxwell body) explains the frequency dependence of resistance and elastance as well as the stress relaxation properties of the respiratory system (22).

    METHODS
TOP
ABSTRACT
INTRODUCTION
METHODS
RESULTS
DISCUSSION
REFERENCES

Study Subjects

We studied two groups of children on mechanical ventilation in the pediatric intensive care unit (ICU) of the Children's Hospital of Pittsburgh between July and December of 1996. The first group (Group 1) consisted of seven patients who were mechanically ventilated for respiratory failure caused by lung disease. One of the Group 1 patients presented with lower airway obstruction; the remaining six patients had parenchymal lung disease. The subjects in Group 2 were six children without primary respiratory disorder but who were ventilated for decreased levels of consciousness and/or inability to protect their airways from gastric regurgitation. Patient characteristics for each group are summarized in Table 1. Results from these individuals were compared with the data obtained previously from eight healthy children, mechanically ventilated under general anesthesia for elective dental procedures (15).

                              
View this table:
[in this window]
[in a new window]
 

TABLE 1

PATIENT CHARACTERISTICS

All patients were intubated transorally with cuffed ET tubes, sedated with fentanyl, paralyzed with vecuronium administered intravenously, and were placed in the supine position. The Servo 900C ventilator (Siemens-Elema, Sweden) was used. The mode of ventilation was volume control with constant inspiratory flow and with the ventilator settings selected by the pediatric ICU patient care team. All subjects were on positive end-expiratory pressure (PEEP: range, 3 to 10 cm H2O; median, 5 cm H2O).

The study was approved by the institutional review board for human experimentation. Informed consent for participation in the study was obtained from the parents or legal guardians.

Equipment, Procedures, and Data Analysis

Airway opening pressure (Pao) was measured through a side port connected proximal to the ET tube using a pressure transducer (model 267BC; Hewlett-Packard, Palo Alto, CA). VI was measured with a heated pneumotachograph (Fleisch No. 1; Fleisch, Lausanne, Switzerland), inserted between the ventilator circuit and the ET tube, using a Hewlett-Packard 47304A unit. The software used was the ANADAT-LABDAT (RHT InfoDat, Montreal, Canada). VT measurements were obtained by computer integration of flow signals.

The technical aspects of the end-inspiratory airway occlusion technique have been described in detail elsewhere (4, 7). For the period of each experiment, the standard ventilator circuit with the heater and the humidifier was replaced with a short (60 cm) low compliance ventilator tubing (Tygon; Norton Performance Plastics, Akron, OH) connecting the patient directly to the ventilator. This replacement minimized the effects of the compliance and resistance of the ventilator circuit on the mechanics measurements (23). To prevent possible hypoxemia during the experiment, the fraction of inspired oxygen (FIO2) was increased to 10% above the established setting for each patient. Each subject was monitored continuously with a pulse oximeter (Nellcor, Palo Alto, CA), a capnometer (Datex Capnomac Ultima, Helsinki, Finland), and an indwelling arterial catheter (for blood pressure measurements). The continuous gas sampling port, proximal to the pneumotachograph, was closed intermittently during the period of pressure and flow measurements. Before any measurements were carried out, the ventilator circuit and ET tube were examined to eliminate any air leaks.

The rapid end-inspiratory airway occlusion was accomplished by simultaneous closure of both inspiratory and expiratory valves, located within the ventilator, and was maintained for approximately 5 s. The effects of the closure time of the Servo ventilator valve on respiratory mechanics measurements have been previously presented by Sly and coworkers (23). Because no valve closes instantaneously, a small gas volume (Delta V) passes into the respiratory system while the valve is moving to closure, leading to underestimation of the initial and subsequent drops in Pao (Pmax - P1, Pmax - P2, respectively) and, therefore, underestimation of Rint [(Pmax - P1)/VI] and Rrs [(Pmax - P2)/ VI] (4, 23). For the purposes of the present study, the gas volume that passed through the valve during its closure was estimated by integration of the flow signal with respect to time from the moment that flow started to decline until it ceased. Then a correction factor based on Delta V was added to Rint and Rrs (23).

The first assessment of respiratory mechanics with the end-inspiratory occlusion was performed at the baseline ventilator setting. To study the flow dependence of resistance and elastance while the end-inspiratory volume was kept constant (isovolume condition), VI was changed to one level below and one above the baseline setting. To evaluate the volume dependence of respiratory mechanics using a constant inspiratory flow (isoflow condition), VT was varied to one level below and one level above the baseline setting. At each ventilator setting the measurement was repeated three times. Thus, for each individual, a total of five sets of triplicate measurements were obtained. The different flow and volume settings were tried in random order. Patients received at least five regular mechanical breaths between end-inspiratory occlusions.

At the conclusion of each experiment, the flow resistance of the equipment was measured in triplicate at the different VI settings used for the patient. During data analysis the equipment resistance was subtracted from the uncorrected data to obtain Rint and Rrs.

Static intrinsic PEEP (PEEPi) was determined by the end-expiratory airway occlusion technique (24). Est is provided (21) by the equation:
Est=[P<SUB>2</SUB>−(PEEP+PEEP<SUB>i</SUB>)]/V<SC>t</SC>. (1)

To compare patients of different size, all the resistance and elastance measurements were normalized for body weight. Data were presented as mean ± SEM. Resistance and elastance values, under baseline flow and volume conditions, were compared to the values previously obtained from children under general anesthesia (15).

Statistical Analysis

Least square regression analysis (linear or nonlinear) was used to correlate resistance and elastance measurements with changes in VT (under constant VI) and VI (under constant VT) for each subject, as was performed in previous studies (7, 11). The computer statistical package Sigma Stat, version 1.0 (Jandel Scientific, San Rafael, CA) was used. In all cases, p < 0.05 was considered as statistically significant.

    RESULTS
TOP
ABSTRACT
INTRODUCTION
METHODS
RESULTS
DISCUSSION
REFERENCES

Adverse Effects

Data collection for each subject was completed in less than 40 min (median, 30 min; range, 25 to 39 min). During and after the completion of the procedure, none of the patients had significant changes in SaO2, end-tidal CO2, or blood pressure.

Variations in VT and VI

The median percent change in VT used to assess the volume dependence of Rrs and its components was 21% (range 12 to 35%) below and 33% (range 12.5 to 100%) above the baseline VT setting in each patient. The median percent change in VI used to evaluate flow dependence was 34% (range 16 to 34%) below and 65% (range 32 to 65%) above the baseline VI.

Static PEEPi

Five of 13 patients (Subjects 4, 7, 9, 11, and 13) had static PEEPi exceeding 1 cm H2O (median, 2.2 cm H2O; range 1.3 to 6.0 cm H2O).

Rint

The mean values of Rint at baseline ventilator settings are presented in Table 2. Two of 7 patients from Group 1 and five of six patients from Group 2 had Rint values, determined at baseline ventilator settings, higher than the 95% confidence limits which had been obtained in a previous study for healthy children under general anesthesia (15). All individuals with PEEPi had increased Rint.

                              
View this table:
[in this window]
[in a new window]
 

TABLE 2

MEAN (SEM) RintDelta R, AND Rrs VALUES AT BASELINE VENTILATOR SETTINGS

Figure 1 shows values of Rint for each patient in relation to changes in VI or VT. Results under the isovolume, variable inspiratory flow setting were as follows. In Group 1 (with primary lung disease), Rint increased significantly (p < 0.05) with increasing VI in two of seven patients. Rint decreased in one patient (p < 0.05) and did not change in four patients. In Group 2 (without primary lung disorder), Rint significantly increased (p < 0.05) in four of six patients, decreased in one patient (p < 0.05), and remained statistically unchanged in one patient (Figure 1A).


View larger version (18K):
[in this window]
[in a new window]
 


View larger version (17K):
[in this window]
[in a new window]
 
Figure 1.   (A) Rint in relation to changes in V I while VT was kept constant (isovolume conditions) in children on mechanical ventilation with primary lung disease (Group 1: closed circles) and those without primary lung disorder (Group 2: open circles). Data from healthy children (closed squares, dashed line; mean ± SEM) (15) are also included for comparison. (B) Rint in relation to changes in VT while V I was kept constant (isoflow conditions) in the same groups of patients.

Findings under the isoflow, variable VT setting were as follows. In Group 1, Rint did not change with increasing VT in five of seven subjects and significantly decreased (p < 0.05) in two subjects. In Group 2, Rint did not change in four of six subjects and decreased (p < 0.05) in two subjects (Figure 1B).

Delta R

The mean values of Delta R at baseline ventilator settings are presented in Table 2. All patients in Group 1 and four of six patients in Group 2 had Delta R values above the 95% confidence limits for healthy anesthetized children (15). Figure 2 illustrates Delta R in each patient in relation to changes in VI or VT.


View larger version (18K):
[in this window]
[in a new window]
 


View larger version (17K):
[in this window]
[in a new window]
 
Figure 2.   (A) Delta R in relation to changes in V I while VT was kept constant (isovolume conditions) in children on mechanical ventilation with primary lung disease (Group 1: closed circles) and those without primary lung disorder (Group 2: open circles). Data for healthy children (closed squares, dashed line; mean ± SEM) (15) are also included for comparison. (B) Delta R in relation to changes in VT while V I was kept constant (isoflow conditions) in the same groups of patients.

Under isovolume, variable inspiratory flow settings, Delta R decreased exponentially with increasing VI in 11 of 13 patients, according to the equation Delta R = A + B (1 - e-C/VI), where A is a constant attributed to time constant inequalities within the lung and/or chest wall (11) and B and C are constants that describe the viscoelastic properties of the respiratory system (11) (Figure 2A). Constant C is also affected by the VT used. In all of our children, A was not statistically different from 0; this was true even for Patient 7 who had lower airway obstruction, clinically. These findings indicate that the time constant inequality of the lung and chest wall tissues (pendelluft) did not importantly contribute to Delta R (11). In two of 13 patients, Delta R did not change with VI. Under isoflow, variable VT settings, Delta R increased linearly with VT in 12 of 13 patients, whereas it did not change in one patient (Figure 2B).

Rrs

Values for Rrs under baseline ventilator settings are provided in Table 2. All patients had values above the 95% confidence limits of Rrs for healthy anesthetized children (15). Under the constant VT, variable VI setting, Rrs decreased significantly (p < 0.05) with increasing VI in six of 13 patients, following the direction of change of Delta R. In four of these six patients both Delta R and Rint decreased with increasing VI. In three of 13 patients, Rrs increased with increasing VI (p < 0.05) because the increase in Rint was more prominent than the exponential decrease in Delta R. In the remaining four of 13 patients, Rrs did not change with the change in VI. Under the constant VI, variable VT setting, Rrs increased with increasing VT in 11 of 13 subjects following the direction of change of Delta R. In the two remaining subjects, Rrs did not change with increasing VT.

Est

Values of Est at baseline ventilator settings are provided in Table 2. Compared with healthy anesthetized children who were studied previously (15), five of seven patients in Group 1 and two of six patients in Group 2 had increased Est. Patient 1 (Group 1), who was undergoing extracorporeal membrane oxygenation for acute lung injury (ALI) secondary to meningococcal sepsis, had the highest Est value. Figure 3 illustrates Est in relation to changes in VI or VT. With increasing VI under constant VT, Est decreased slightly but significantly (p < 0.05) in 11 of 13 patients and did not change in the remaining two (Figure 3A). With increasing VT under constant VI, Est decreased (p < 0.05) in 10 of 13 subjects and remained unchanged in the rest of them (Figure 3B).


View larger version (15K):
[in this window]
[in a new window]
 


View larger version (15K):
[in this window]
[in a new window]
 
Figure 3.   (A) Est in relation to changes in V I while VT was kept constant (isovolume conditions) in children on mechanical ventilation with primary lung disease (Group 1: closed circles) and those without primary lung disorder (Group 2: open circles). Data for healthy children (closed squares, dashed line; mean ± SEM) (15) are also included. (B) Est in relation to changes in VT while V I was kept constant (isoflow conditions) in the same groups of patients.

    DISCUSSION
TOP
ABSTRACT
INTRODUCTION
METHODS
RESULTS
DISCUSSION
REFERENCES

The constant flow, end-inspiratory occlusion technique has not been used for the evaluation of children in respiratory insufficiency in the ICU. The present investigation has demonstrated the feasibility and safety of this method applied on critically ill patients who are relatively stable hemodynamically. The analysis of Rrs and its flow-resistive (Rint) and viscoelastic (Delta R) components, as well as their flow and volume dependences, can lead to a better understanding of the pathophysiologic nature of respiratory insufficiency. Based on such information, intensive care physicians can more rationally formulate a physiologically sound ventilator treatment strategy.

Methodological Consideration

In the present study, the apparent valve closure time, as judged from the flow signal, was used to correct resistance measurements for the error introduced by the valve closure time (4). The apparent valve closure time is affected by the inspiratory flow and the resistance of the respiratory system and the equipment (including connectors, a pneumotachograph, and an ET tube) (23). Therefore, in the present study, valve closure time might have caused a slight underestimation of Rint and Rrs. Bates and coworkers have shown that Rint may be underestimated by as much as 7% if the valve closure time is 12 ms (25). Sly and coworkers have estimated the mean time for valve closure of the Siemens 900C ventilator to be between 22 and 229 ms; but Rint was underestimated by a mean of 17% using the standard ventilator tubing (23). Kochi and associates have proposed a formula to correct for the underestimation of Rint resulting from gas flowing into the lungs while the valve is being closed (4).

For flow measurements we used a Fleisch No. 1 pneumotachograph, inserted between a Y connector and an ET tube. It has been shown that this connection can lead to an overestimation of flow. A flow of 1.5 L/s can be overestimated by 5% (26); the overestimation becomes progressively greater with increasing flow. The range of VI used in this investigation was 0.06 to 1.1 L/s.

An error can also be introduced when the expiratory pause button of the ventilator is used for the measurement of static PEEPi. This error (underestimation of PEEPi with resultant overestimation of Est) increases when the patient's Est increases or the equipment elastance decreases (27). The high elastance of the ventilator tubings that we used in the present study probably minimized the underestimation of PEEPi.

In our previous study of healthy children under general anesthesia, standard ranges of VI and VT were used and the results were normalized for body weight (15). The same methodological strategy, however, could not be applied to children in the present study. This is because the children were on mechanical ventilation, having a variety of respiratory disorders. Consequently, the ranges of VI and VT studied in each patient varied considerably. In the present study, data from the children with a wide age range (0.5 to 17.7 yr) were compared with the data from healthy children under general anesthesia with a narrower age range (2.3 to 6.5 yr). It should be emphasized that the data of the latter study were used as a general guide for comparison, rather than as control values; one reason being that elastance corrected for lung volume (specific elastance) increases with age or height (17). Additional potential problems with the use of the data of healthy children under general anesthesia as controls for patients in the ICU include the possible effects of anesthetics (bronchodilation) and different gas densities between the two settings. These problems, however, were relatively minor with the children in the previous study, in whom the anesthetic technique used was intravenous propofol with FIO2 of 0.3 in nitrogen. Propofol, unlike inhaled anesthetics, has minimal bronchodilator effect (28); the gas mixture is similar between the two studies. Finally, the patients on mechanical ventilation would undergo changes in respiratory mechanics unrelated to their primary respiratory problems. These changes include autonomic responses to the presence of an ET tube, inflammatory processes secondary to infection, hyperoxia, volutrauma caused by high positive pressure ventilation, and the presence of airway secretions (29).

Special Characteristics of Respiratory Mechanics in Children

Postnatally the lungs develop and grow at an extremely rapid pace in human infants. Although at birth, terminal air sacks are composed mostly of primitive saccules, alveolar formation in the lungs is completed by 18 mo of age (30). Postnatal development of lung parenchyma, however, continues throughout the first decade of life (31). It has been known that, in the neonate, the specific elastance of both the lungs and chest wall are lower (compliance, higher) than those of older children and adults. Furthermore, in the neonate the outward recoil of the chest wall is disproportionately lower than the inward recoil of the lungs (32). Papastamelos and coworkers (33) recently demonstrated that by 9 to 12 mo of age chest wall elastance rapidly increases to the level of lung elastance. Thereafter, elastances of both the chest wall and the lungs continue to increase at the same pace (33).

In awake infants, the extremely compliant chest wall resists the inward recoil of the lungs by tonic contractions of inspiratory muscles that maintain FRC (33). When the sustained tension of the inspiratory muscles of the chest wall is abolished, either by general anesthesia or by muscle relaxants, the balance is shifted and FRC (or relaxation volume, Vr) in infants decreases to 15 to 20% of TLC and results in concomitant airway closure and atelectasis (12, 32). By contrast, in adults, such a reduction in Vr with anesthesia or muscle relaxants amounts to only 9 to 25% of FRC in the awake state (33, 35).

In a recent study involving eight healthy children undergoing general endotracheal anesthesia, all measurements were made after "sighs" (three slow inflations to TLC) to minimize airway closure or atelectasis and to set a consistent volume history (15). In this study, Rint decreased with increasing VT when the inspiratory flow was kept constant (isoflow condition) as seen in studies on anesthetized adults. Unlike in adult studies, however, Rint did not change with VI (isovolume conditions). Flow and volume dependences of Delta R were similar to those of adult patients and their directions were opposite to changes of Rint: Delta R decreased with increasing VI (isovolume studies) whereas it increased with VT (isoflow experiments) (15). Unlike in adults, Rrs did not change with changes in Delta R (15). More important clinically, we found evidence that even under PEEP (5 cm H2O), Vr of the lungs was still well below the level of physiologic FRC or the steepest portion of the pressure-volume (P-V) curve of the respiratory system. It is interesting to note that in a separate study of healthy children under general anesthesia, a PEEP value of 12 cm H2O yielded the maximal value of respiratory system compliance (36). These differences in the characteristics of Rint, Delta R, and Rrs and their flow and volume dependence between adults and children are apparently due to developmental characteristics of the lungs and chest wall in children during their postnatal development and growth.

Rint, Delta R, and Rrs in Children with Respiratory Insufficiency

In the present study, all 13 children with respiratory insufficiency of diverse etiology demonstrated increased Rrs. The end-inspiratory occlusion technique, rarely used to study children in clinical settings, allowed us to further analyze the pathophysiology of respiratory insufficiency.

Most of our patients with primary lung disease and respiratory failure (Group 1) did not show increased Rint, indicating that their primary lung parenchymal pathology did not affect airway patency. Exceptions in this group are two of seven patients with increased Rint (one with status asthmaticus), both of whom also had increased PEEPi, evidence of dynamic hyperinflation (24). High Rint has been documented in some of the studies on adult patients with adult respiratory distress syndrome (ARDS) (11, 12) but not in others (10).

It is important to note that nearly all (5 of 6) children in Group 2, who were without primary respiratory disorder and were mechanically ventilated, demonstrated increased Rint. At the time of the study, none of these patients had clinical evidence of lower airway obstruction. These findings indicate that even the patients who are intubated and put on mechanical ventilation without lung disease in the ICU settings develop lower airway obstruction after an extended period. The only patient in this group who did not have increased Rint (Patient 8) was studied only a few hours after the initiation of mechanical ventilation. Increased Rint may be secondary to increased bronchomotor tone in response to the presence of the ET tube, accumulation of airway secretions, and airway inflammation caused by hyperoxia (37) and volutrauma from lung hyperdistention (38).

In our previous study of healthy children under general anesthesia (15), Rint decreased significantly with increasing VT (isoflow settings), reflecting an increasing airway caliber with VT. On the other hand, Rint did not change significantly with VI (isovolume conditions). Flow and volume dependence of Rint in the present study were variable, reflecting diverse conditions and causes of respiratory insufficiency.

In the present study, Delta R was markedly increased in all patients in Group 1 with acute lung injury/pulmonary edema from the range found in healthy children under general anesthesia. Similar findings were reported in adults with ARDS (10, 11, 13). Delta R was also increased in four of the six patients in Group 2 without primary pulmonary disorders. Of these children, three were also found to have increased Rint. Therefore, time constant inhomogeneity resulting from bronchospasm (39) or increased airway secretions, cell debris, etc. most likely contributed to the increased Delta R (11). The remaining patient (Patient 8) had an elevated Delta R without clinical signs of parenchymal lung disease and with a normal Rint. Because the chest wall importantly contributes to the viscoelastic properties of the respiratory system (8), it is likely that the thoracotomy, which the patient had undergone recently, might have altered the value of Delta R. Delta R decreases with increasing flow; Delta R also decreases with decreasing VT (7). In patients with increased Delta R the work of breathing would be the lowest with rapid shallow respirations. It is of clinical interest to note that the adult patients with ARDS, who failed attempted weaning from mechanical ventilation, developed rapid shallow breathing immediately after the discontinuation of a ventilator, whereas those who survived did not (40, 41). However, tachypnea was not a predictor of success and failure of weaning from mechanical ventilation in a recent study involving 208 children with respiratory failure, although 42% of those who failed the attempted weaning did develop tachypnea (42). The exact mechanism of rapid shallow breathing in ARDS is not well understood (41).

Est in Children with Respiratory Insufficiency

Est represents the elastic property of the respiratory system. Four of six children with parenchymal lung disease had increased Est. A similar observation was made on adult patients with ARDS (10, 11). In the remaining two patients, however, Est was not elevated; these patients were recovering from respiratory insufficiency and were weaned from ventilatory assistance shortly after the measurements. Patient 1, who was undergoing extracorporeal membrane oxygenation (ECMO) for acute lung injury secondary to meningococcal sepsis, had the highest Est value, probably reflecting the severity of his parenchymal lung disease. Patient 7 with status asthmaticus also exhibited increased Est. This patient also had elevated PEEPi, a sign of dynamic hyperinflation. This finding could mean that FRC of this patient was on the upper, stiff portion of the P-V curve of the respiratory system, where Est was increased. Patient 8 also had an elevated Est, most likely as a result of the recent thoracotomy.

In healthy anesthetized adults or adult patients with ARDS, Est did not change with increasing VI (isovolume conditions) but decreased with increasing VT (isoflow conditions) (7, 11). In healthy children under general anesthesia (15) and in most pediatric patients of the present study, Est decreased with increasing VT. These findings probably indicate that Vr was below the steep midportion of the P-V curve of the respiratory system. Est also decreased with increasing VI; the reason is not clear. We speculate that lung inflation with increasing VI may lead to progressive recruitment of previously closed airways or air spaces and result in decreased Est.

    Footnotes

Correspondence and requests for reprints should be addressed to Etsuro K. Motoyama, M.D., Children's Hospital of Pittsburgh, Department of Anesthesiology/ CCM, 3705 Fifth Ave., Pittsburgh, PA 15213.

(Received in original form February 18, 1998 and in revised form August 14, 1998).

Presented in part at the annual international conference of the American Thoracic Society, May 16-21, 1997, San Francisco.

Acknowledgments: The authors thank David Chasey for editorial assistance.

Supported by intramural funds of the Department of Anesthesiology and Critical Care Medicine.

    References
TOP
ABSTRACT
INTRODUCTION
METHODS
RESULTS
DISCUSSION
REFERENCES

1. von Neergaard, K., and K. Wirz. 1927. Die messung der strömungswiederstande in der atemwege des menschen, insbesondere bei asthma und emphysem. Z. Klin. Med. 105: 51-82 .

2. von Neergaard, K., and K. Wirz. 1927. Über eine methode zur messung der lungenelastizität am lebenden menschen, insbesondere beim emphysem. Z. Klin. Med. 105: 35-50 .

3. Bates, J. H. T., P. Baconnier, and J. Milic-Emili. 1988. A theoretical analysis of interrupter technique for measuring respiratory mechanics. J. Appl. Physiol. 64: 2204-2214 [Abstract/Free Full Text].

4. Kochi, T., S. Okubo, W. A. Zin, and J. Milic-Emili. 1988. Chest wall and respiratory system mechanics in cats: effects of flow and volume. J. Appl. Physiol. 64: 2636-2646 [Abstract/Free Full Text].

5. Similowski, T., P. Levy, C. Corbeil, M. Albala, R. Pariente, J.-P. Derenne, J. H. T. Bates, B. Jonson, and J. Milic-Emili. 1989. Viscoelastic behavior of lung and chest wall in dogs determined by flow interruption. J. Appl. Physiol. 67: 2219-2229 [Abstract/Free Full Text].

6. Bates, J. H. T., K. Brown, and T. Kochi. 1987. Identifying a model of respiratory mechanics using the interrupter technique. Proc. Ninth Am. Conf. IEEE Eng. Med. Biol. Soc. 3: 1802-1803 .

7. D'Angelo, E., E. Calderini, G. Torri, F. M. Robatto, D. Bono, and J. Milic-Emili. 1989. Respiratory mechanics in anesthetized paralyzed humans: effects of flow, volume, and time. J. Appl. Physiol. 67: 2556-2564 [Abstract/Free Full Text].

8. D'Angelo, E., F. M. Robatto, E. Calderini, M. Tavola, D. Bono, G. Torri, and J. Milic-Emili. 1991. Pulmonary and chest wall mechanics in anesthetized paralyzed humans. J. Appl. Physiol. 70: 2602-2610 [Abstract/Free Full Text].

9. D'Angelo, E., E. Calderini, M. Tavola, D. Bono, and J. Milic-Emili. 1992. Effect of PEEP on respiratory mechanics in anesthetized paralyzed humans. J. Appl. Physiol. 73: 1736-1742 [Abstract/Free Full Text].

10. Auler, J. O. C. Jr., P. H. N. Saldiva, M. A. Martins, C. R. R. Carvalho, E. M. Negri, C. Hoelz, and W. A. Zin. 1990. Flow and volume dependence of respiratory system mechanics during constant flow ventilation in normal subjects and in adult respiratory distress syndrome. Crit. Care Med. 18: 1080-1086 [Medline].

11. Eissa, N. T., V. M. Ranieri, C. Corbeil, M. Chassé, F. M. Robatto, J. Braidy, and J. Milic-Emili. 1991. Analysis of behavior of the respiratory system in ARDS patients: effects of flow, volume, and time. J. Appl. Physiol. 70: 2719-2729 [Abstract/Free Full Text].

12. Eissa, N. T., V. M. Ranieri, C. Corbeil, M. Chassé, J. Braidy, and J. Milic-Emili. 1991. Effects of positive end-expiratory pressure, lung volume, and inspiratory flow on interrupter resistance in patients with adult respiratory distress syndrome. Am. Rev. Respir. Dis. 144: 538-543 [Medline].

13. Eissa, N. T., V. M. Ranieri, C. Corbeil, M. Chassé, J. Braidy, and J. Milic-Emili. 1992. Effect of PEEP on the mechanics of the respiratory system in ARDS patients. J. Appl. Physiol. 73: 1728-1735 [Abstract/Free Full Text].

14. Guérin, C., M.-L. Coussa, N. T. Eissa, C. Corbeil, M. Chassé, J. Braidy, N. Matar, and J. Milic-Emili. 1993. Lung and chest wall mechanics in mechanically ventilated COPD patients. J. Appl. Physiol. 74: 1570-1580 [Abstract/Free Full Text].

15. Nishio, I., T. Imai, B. Gronert, I. Seki, W. Zin, and E. Motoyama. 1993. Flow and volume dependence of pulmonary mechanics in anesthetized children: effect of sigh and PEEP (abstract). Anesthesiol. 79: 1220A .

16. Storme, L., Y. Riou, R. Logier, J. P. Dubos, N. Kacet, S. Rousseau, and P. Lequien. 1994. A new application of an old method for respiratory mechanics measurements: the passive inflation method in newborn infants during pressure-controlled ventilation. Pediatr. Pulmonol. 18: 244-254 [Medline].

17. Lanteri, C. J., and P. D. Sly. 1993. Changes in respiratory mechanics with age. J. Appl. Physiol. 74: 369-378 [Abstract/Free Full Text].

18. Freezer, N. J., W. Butt, and P. D. Sly. 1991. Pulmonary mechanics and outcome of neonates on ECMO. Pediatr. Pulmonol. 11: 108-112 [Medline].

19. Freezer, N. J., and P. D. Sly. 1993. Predictive values of measurements of respiratory mechanics in preterm infants with HMD. Pediatr. Pulmonol. 16: 116-123 [Medline].

20. Freezer, N. J., C. J. Lanteri, and P. D. Sly. 1993. Effect of pulmonary blood flow on measurements of respiratory mechanics using the interrupter technique. J. Appl. Physiol. 74: 1083-1088 [Abstract/Free Full Text].

21. Milic-Emili, J., F. M. Robatto, and J. H. T. Bates. 1990. Respiratory mechanics in anaesthesia. Br. J. Anaesth. 65: 4-12 [Free Full Text].

22. Nicolai, T., C. J. Lanteri, and P. D. Sly. 1993. Frequency dependence of elastance and resistance in ventilated children with and without the chest open. Eur. Respir. J. 6: 1340-1346 [Abstract].

23. Sly, P. D., J. H. T. Bates, and J. Milic-Emili. 1987. Measurement of respiratory mechanics using the Siemens Servo Ventilator 900C. Pediatr. Pulmonol. 3: 400-405 [Medline].

24. Maltais, F., H. Reissmann, P. Navalesi, P. Hernandez, A. Gursahaney, V. M. Ranieri, M. Sovilj, and S. B. Gottfried. 1994. Comparison of static and dynamic measurements of intrinsic PEEP in mechanically ventilated patients. Am. J. Respir. Crit. Care Med. 150: 1318-1324 [Abstract].

25. Bates, J. H. T., I. W. Hunter, P. D. Sly, S. Okubo, S. Filiatrault, and J. Milic-Emili. 1987. Effect of valve closure time on the determination of respiratory resistance by flow interruption. Med. Biol. Eng. Comput. 25: 136-140 [Medline].

26. Kreit, J. W., and F. C. Sciurba. 1996. The accuracy of pneumotachograph measurements during mechanical ventilation. Am. J. Respir. Crit. Care Med. 154: 913-917 [Abstract].

27. Grootendorst, A. F., G. Lugtigheid, and E. J. van der Weygert. 1993. Error in ventilator measurements of intrinsic PEEP: cause and remedy. Respir. Care 38: 348-350 .

28. Yamakage, M., C. A. Hirshman, and T. L. Croxton. 1995. Inhibitory effects of thiopental, ketamine, and propofol on voltage-dependent Ca2+ channels in porcine tracheal smooth muscle cells. Anesthesiology 83: 1274-1282 [Medline].

29. Marini, J. J.. 1996. Evolving concepts in the ventilatory management of acute respiratory distress syndrome. Clin. Chest Med. 17: 555-575 [Medline].

30. Langston, C., K. Kida, M. Reed, and W. M. Thurlbeck. 1984. Human lung growth in late gestation and in the neonate. Am. Rev. Respir. Dis. 129: 607-613 [Medline].

31. Zeltner, T. B., and P. H. Burri. 1987. The postnatal development and growth of the human lung: II. Morphology. Respir. Physiol. 67: 269-282 [Medline].

32. Agostoni, E.. 1959. Volume-pressure relationships of the thorax and lung in the newborn. J. Appl. Physiol. 14: 909-913 [Abstract/Free Full Text].

33. Papastamelos, C., H. B. Panitch, S. E. England, and J. L. Allen. 1995. Developmental changes in chest wall compliance in infancy and early childhood. J. Appl. Physiol. 78: 179-184 [Abstract/Free Full Text].

34. Dobbinson, T. L., H. I. Nisbet, D. A. Pelton, and E. Levison. 1973. Functional residual capacity (FRC) and compliance in anaesthetized paralyzed children: part II. Clinical results. Canad. Anaesth. Soc. J. 20: 322-333 .

35. Westbrook, P. R., S. E. Stubbs, A. D. Sessler, K. Rehder, and R. E. Hyatt. 1973. Effects of anesthesia and muscle paralysis on respiratory mechanics in normal man. J. Appl. Physiol. 34: 81-86 [Free Full Text].

36. Thorsteinsson, A., A. Larsson, C. Jonmarker, and O. Werner. 1994. Pressure-volume relations of the respiratory system in healthy children. Am. J. Respir. Crit. Care Med. 150: 421-430 [Abstract].

37. Coalson, J. J., V. T. Winter, D. R. Gerstman, S. Idell, R. J. King, and R. A. deLemos. 1992. Pathophysiologic, morphometric, and biochemical studies of the premature baboon with bronchopulmonary dysplasia. Am. Rev. Respir. Dis. 145: 872-881 [Medline].

38. Fukunaga, T., P. Davies, L. Zhang, Y. Hashida, and E. K. Motoyama. 1998. Prolonged high intermittent positive pressure ventilation induces airway remodeling and hyperreactivity in young rats. Lung Cell. Mol. Physiol. 275: L567-L573 . [Abstract/Free Full Text]

39. Bigos, D., J. J. Pérez, and Fontán. 1994. Contribution of viscoelastic stress to the rate-dependence of pulmonary dynamic elastance. Respir. Physiol. 98: 53-67 [Medline].

40. Yang, K., and M. J. Tobin. 1991. A prospective study of indexes predicting outcome of trials of weaning from mechanical ventilation. N. Engl. J. Med. 324: 1445-1450 [Abstract].

41. Jubran, A., and M. J. Tobin. 1997. Pathophysiologic basis of acute respiratory distress in patients who failed a trial of weaning from mechanical ventilation. Am. J. Respir. Crit. Care Med. 155: 906-915 [Abstract].

42. Khan, N., A. Brown, and S. T. Venkataraman. 1996. Predictors of extubation success and failure in mechanically ventilated infants and children. Crit. Care Med. 24: 1568-1579 [Medline].





This article has been cited by other articles:


Home page
Anesth. Analg.Home page
A. G. Kaditis, E. K. Motoyama, W. Zin, N. Maekawa, I. Nishio, T. Imai, and J. Milic-Emili
The Effect of Lung Expansion and Positive End-Expiratory Pressure on Respiratory Mechanics in Anesthetized Children
Anesth. Analg., March 1, 2008; 106(3): 775 - 785.
[Abstract] [Full Text] [PDF]


This Article
Right arrow Abstract Freely available
Right arrow Full Text (PDF)
Right arrow Alert me when this article is cited
Right arrow Alert me if a correction is posted
Services
Right arrow Similar articles in this journal
Right arrow Similar articles in PubMed
Right arrow Alert me to new issues of the journal
Right arrow Download to citation manager
Right arrow reprints & permissions
Citing Articles
Right arrow Citing Articles via HighWire
Right arrow Citing Articles via Google Scholar
Google Scholar
Right arrow Articles by KADITIS, A. G.
Right arrow Articles by MOTOYAMA, E. K.
Right arrow Search for Related Content
PubMed
Right arrow PubMed Citation
Right arrow Articles by KADITIS, A. G.
Right arrow Articles by MOTOYAMA, E. K.


HOME HELP FEEDBACK SUBSCRIPTIONS ARCHIVE SEARCH TABLE OF CONTENTS
Proc. Am. Thorac. Soc. Am. J. Respir. Cell Mol. Biol.
Copyright © 1999 American Thoracic Society