Translational Investigation | Published:

Establishing lung gas volumes at birth: interaction between positive end-expiratory pressures and tidal volumes in preterm rabbits

Pediatric Research volume 73, pages 734741 (2013) | Download Citation

Abstract

Background:

We investigated the effects of positive end-expiratory pressure (PEEP) and tidal volume (VT) on lung aeration, pulmonary mechanics, and the distribution of ventilation immediately after birth using a preterm rabbit model.

Methods:

Sixty preterm rabbits (27 d) received volume-targeted positive pressure ventilation from birth, with one of the 12 combinations of PEEP (0, 5, 8, or 10 cmH2O) and VT (4, 8, or 12 ml/kg). Outcomes included functional residual capacity (FRC), peak inflating pressure (PIP), dynamic compliance (Cd), and distribution of ventilation.

Results:

Increasing PEEP from 0 to 10 cmH2O increased FRC by 4 ml/kg, increased Cd by 0.2 ml/kg/cmH2O, and reduced PIP by 5 cmH2O. Increasing VT from 4 to 12 ml/kg increased FRC by 2 ml/kg, increased Cd by 0.3 ml/kg/cmH2O, and increased PIP by 4 cmH2O. No effect of VT on FRC occurred at 0 or 5 PEEP, and no effect of PEEP occurred at VT = 4 ml/kg. At 0 PEEP, increasing VT increased the proportion of gas entering the smaller apical regions, whereas at 10 PEEP, increasing VT increased the proportion of gas entering basal regions, from 47% to 63%.

Conclusion:

Both PEEP and VT have independent, additive effects on FRC, lung mechanics, and the distribution of ventilation during the immediate newborn period.

Main

Approximately 1 in 15 infants receive positive pressure ventilation (PPV) at birth (1). In particular, preterm infants commonly require PPV support as they must clear their airways of liquid and establish and maintain a functional residual capacity (FRC), despite having weak inspiratory efforts. Data to guide recommendations for respiratory support immediately after preterm delivery are needed because of the potential to injure the immature lung (2). PPV with a high tidal volume (VT) causes lung injury (3,4,5,6) as does PPV of poorly aerated lungs (7). Providing positive end-expiratory pressure (PEEP) immediately after birth quickly improves oxygenation (8) and the establishment of an FRC (9). However, the optimal PEEP required during resuscitation of very preterm infants is not known. Similarly, it is not known whether the optimal level of PEEP varies depending on the VT.

The physiological mechanisms involved with lung aeration and the clearance of fetal lung liquid from the airways are complex, and include peripartum factors, epithelial sodium channels, and transepithelial pressure gradients depending on the timing and mode of delivery (10,11,12,13,14,15,16,17,18). However, after birth, spontaneously breathing infants inhale air into their lungs and establish FRC by generating a subatmospheric intrathoracic pressure (19). This creates a pressure gradient that facilitates the movement of liquid across the distal airways into the surrounding tissue (19), from where it is cleared (13,20). Because hydrostatic pressure gradients facilitate lung aeration, we investigated the effect of PEEP and sustained inflations on lung aeration at birth in preterm rabbits (9,21,22) using synchrotron-based imaging techniques (23). These studies demonstrated that both pressure and the time over which the pressure is applied (pressure–time integral) are important for facilitating and maintaining FRC immediately after birth. During newborn resuscitation, clinicians may increase the peak inflating pressure (PIP) to increase the VT if a baby does not respond to inflations at the starting PIP. In this study, we hypothesized that the VT used during resuscitation will also influence FRC accumulation after birth and will have a synergistic effect with PEEP. Specifically, we investigated the interacting effects of PEEP and VT on FRC, ventilation parameters, and the homogeneity of tidal ventilation during the initial inflations after birth in preterm rabbits.

Results

In total, 62 pups were studied although two were ventilated at the wrong settings and were excluded from the analysis, leaving 60 pups (five per group). Imaging data were not available for 3 of 60 pups owing to a failure of the microprocessor-controlled imaging camera, corruption of a data file, or failure of the X-ray shutter to open. The nonimaging data from these pups have been included. Of the 57 pups with video data, all were alive at the end of the experiment as determined by visualization of a heartbeat. All had a detectable heartbeat at the start of the experiment except for one (PEEP = 0 cmH2O, VT = 4 ml/kg), in which no heartbeat could be detected until after the lung had partially aerated. No pups established regular breathing.

The mean (SD) weight of the 60 pups analyzed was 23 (4) g and all were 27 d gestational age, with no differences between groups in weight or birth order. None of the pups developed pneumothoraces during the course of this experiment; this was visualized from the phase contrast X-ray imaging.

Analysis of the data for inflations 40–160 showed that the real-time assessment of VT overestimated the actual VT . This overestimation resulted from a minor bounce in the plethysmograph trace during expiration. Pups in the 4 ml/kg groups received a mean (SD) actual VT of 3 (0.5) ml/kg; the 8 ml/kg group received 6.4 (0.6) ml/kg; and the 12 ml/kg group received 9.9 (0.8) ml/kg. These differences were consistent across groups. PEEP was delivered accurately.

Changes in FRC

The FRC at 40, 80, 120, and 160 inflations (FRC160) is shown in Table 1 and Figure 1. Plethysmograph data from two outliers were excluded because FRC measurements were outside the mean plus three SDs and measurements were not consistent with the imaging data. After 160 inflations, FRC was <3 ml/kg at PEEP 0 and 5 cmH2O irrespective of the VT. FRC increased at PEEP 8 and 10 cmH2O; at these higher PEEPs, VT had an additive effect, with a maximum FRC of 9.6 ml/kg at PEEP 10 and VT = 12 ml/kg. Regression coefficients are shown in Table 2. Overall, the effect of increasing PEEP from 0 to 10 cmH2O was to increase FRC by 4 ml/kg (P < 0.001). Increasing VT from 4 to 12 ml/kg increased FRC by 2 ml/kg (P = 0.01). In this model, to obtain an FRC at inflation 160 of >5 ml/kg, the PEEP needed to be ≥8 cmH2O with a VT ≥ 8 ml/kg.

Table 1: Functional residual capacity
Figure 1
Figure 1

Functional residual capacity (FRC) after 160 inflations. Increasing both positive end-expiratory pressure(PEEP) and tidal volume (VT) resulted in a higher FRC. In all groups, FRC was still increasing after 160 inflations; typical FRC in aerated lung is 15–20 ml/kg. VT, light gray = 4 ml/kg; VT, medium gray = 8 ml/kg; VT, dark gray = 12 ml/kg.

Table 2: Results of linear regression

PIPs

During the experiment, the PIP was altered to deliver the target VT. The PIPs are summarized in Table 3 and Figure 2. The rate of weaning PIP is not shown, but varied considerably between pups. The initial PIP (PIPinit) was 39–42 cmH2O for all groups except where higher VTs were used in the lower PEEP groups. The highest PIP needed was 45 cmH2O in the PEEP = 0 cmH2O, VT = 12 ml/kg group.

Table 3: Peak inflating pressure, mean airway pressure, and dynamic compliance
Figure 2
Figure 2

Maximum peak inflating pressure (PIP) (a) during the initial 40 inflations and (b) after 160 inflations. Increasing both positive end-expiratory pressure (PEEP) and tidal volume (VT) increased aeration and compliance (see Figure 3), and led to reduction in required PIP. The difference in PIP between the 4 and 12 ml/kg groups was ≈4 cmH2O at all PEEPs. VT, light gray = 4 ml/kg; VT, medium gray = 8 ml/kg; VT, dark gray = 12 ml/kg.

Using linear regression (Table 2), the effect of increasing PEEP from 0 to 10 cmH2O was to decrease PIPinit by 2.6 cmH2O (P = 0.01). The effect of increasing VT from 4 to 12 ml/kg was to increase PIPinit by 3.2 cmH2O (P = 0.01).

By inflation 160, the PIP (PIP160) was 10 cmH2O lower than the PIPinit at all levels of PEEP and for all three VT targets. The effect of increasing PEEP from 0 to 10 cmH2O was to reduce PIP160 by 6 cmH2O (P < 0.0001). The effect of increasing the target VT from 4 to 12 ml/kg was to increase PIP160 by 4 cmH2O (P < 0.0001), i.e., at all levels of PEEP, the difference in PIP required to provide a VT of 12 ml/kg was only ≈4 cmH2O higher than that required to provide a VT = 4 ml/kg.

Mean Airway Pressure

Mean airway pressures (MAPs) are reported in Table 3 and Figure 3. The MAP increased with increasing PEEP and increasing VT for both the initial MAP (MAPinit) and the MAP after 160 inflations (MAP160). The effect of VT on MAP, however, was relatively small and was effectively lost at higher PEEP levels.

Figure 3
Figure 3

Mean airway pressure (MAP) (a) during initial inflations and (b) after 160 inflations. MAP reduced ≈5 cmH2O after 160 inflations, with only 3 cmH2O difference between groups. Despite a threefold difference in tidal volume (VT), the effect of VT on MAP160 was small. VT, light gray = 4 ml/kg; VT, medium gray = 8 ml/kg; VT, dark gray = 12 ml/kg. PEEP, positive end-expiratory pressure.

The effect of increasing PEEP from 0 to 10 cmH2O in different groups of pups was to increase the MAPinit by 4.9 cmH2O (P < 0.001). The effect of increasing VT from 4 to 12 ml/kg was to increase the MAPinit by 1.3 cmH2O (P = 0.001), the main effect occurring between 4 and 8 ml/kg.

The effect of increasing PEEP from 0 to 10 cmH2O was to increase the MAP160 by 3.6 cmH2O (P < 0.001). The effect of increasing VT from 4 to 12 ml/kg was to increase the MAP160 by only 1.6 cmH2O (P < 0.001). Regression coefficients are reported in Table 2.

Dynamic Compliance

Dynamic compliance (Cd) is presented in Table 3 and Figure 4. All groups had similarly low initial Cd (Cdinit). The effect of increasing PEEP from 0 to 10 cmH2O was to increase Cdinit by 0.02 ml/kg/cmH2O (P = 0.04). The effect of VT on Cdinit was not statistically significant.

Figure 4
Figure 4

Dynamic compliance (Cd), which was calculated from the tidal volume (VT) and Δpressure (PIP − PEEP). (a) Initial Cd was minimal in all groups. (b) The effect of VT and PEEP was additive and increased Cd by 160 inflations. VT, light gray = 4 ml/kg; VT, medium gray = 8 ml/kg; VT, dark gray = 12 ml/kg. PEEP, positive end-expiratory pressure; PIP, peak inflating pressure.

By 160 inflations, the Cd (Cd160) had increased at all PEEP and VT levels. Regression coefficients are reported in Table 2. The effect of increasing PEEP from 0 to 10 cmH2O was to increase Cd160 by 0.20 ml/kg/cmH2O (P < 0.001). The effect of increasing VT from 4 to 12 ml/kg was to increase Cd160 by 0.30 ml/kg/cmH2O (P < 0.001). Increasing both PEEP and VT independently increased Cd, and the effects of each were additive; the highest compliance (0.57 ml/kg/cmH2O) was measured at the highest PEEP (10 cmH2O) and VT (12 ml/kg).

Distribution of FRC and VT Within the Lung

The gas distribution within the lung was determined from the image data and is reported in Figure 5. Data showing distribution of tidal ventilation in aerated lung from a separate set of experiments is shown for comparison (M.L. Siew, M.J. Wallace, M.J. Kitchen, et al., unpublished data); in those experiments, 72% of VT was distributed to the basal segments of the lungs, which have a larger anatomical volume.

Figure 5
Figure 5

Mean (SE) tidal volume (VT) distribution after 160 inflations. (a) Absolute volume measurements (ml/kg) distributed to the apical and basal regions. (b) Percentage distribution of VT distributed to the apical and basal regions, compared with data from aerated lung with homogenous ventilation. Increasing positive-end expiratory pressure (PEEP) increased VT distribution to the lower lung regions (which have a larger volume and are preferentially ventilated during normal breathing). At lower PEEPs (with lower functional residual capacity (FRC)), increasing VT preferentially increased ventilation of the upper regions. At higher PEEPs (with a higher FRC), increasing VT increased ventilation of the lower regions. (c) Linear regression of the gradients in b at each of the four PEEP settings (gradient = −0.36 PEEP + 1.79 (P = 0.03, R2 = 0.94)). VT, light gray = 4 ml/kg; VT, medium gray = 8 ml/kg; VT, dark gray = 12 ml/kg; black, aerated lung.

At lower PEEPs, more gas entered the apical region of the lung during inflation, whereas more gas entered the basal regions of the lung at PEEP = 10 cmH2O. The effect of increasing PEEP from 0 to 10 cmH2O was to increase the proportion of gas directed to the basal regions from 38% to 55% (P < 0.001).

The effect of increasing VT on the distribution of gas during inflation varied with PEEP. In the PEEP 0 groups, increasing VT resulted in further increased volume to the apical region, reducing the proportion entering the basal region from 48% to 32%. At PEEP 10, increasing VT increased the distribution of tidal ventilation toward the basal region from 47% to 63% (post hoc regression: P = 0.03, R2 = 0.94, Figure 5c).

We did not observe any effect of either PEEP or VT in the relative distribution of FRC (data not shown).

Discussion

The aim of this study was to investigate the effects of different PEEP and target VT levels on FRC and gas distribution in the preterm rabbit lung. We found that increasing PEEP and VT both led to an increase in FRC and dynamic lung compliance. Increasing PEEP also improved the relative distribution of VT within the lung, increasing it to dependent regions, whereas the effect of VT was less clear.

The 2010 International Liaison Committee on Resuscitation guidelines for neonatal resuscitation recommend starting PIPs of 30 cmH2O (20–25 for preterm infants), and that PEEP “should be used if suitable equipment is available” for apneic preterm infants who require PPV (2). However, a specific PEEP level is not recommended, and the guidelines warn that “high levels” of PEEP (8–12 cmH2O) may reduce pulmonary blood flow and increase the risk of pneumothoraces (8,24). These guidelines draw on studies in immature animals in which high VTs at birth were reported to cause lung injury, impair gas exchange, and reduce lung compliance (N.H. Hillman, T.J. Moss, I. Nitsos, A.H. Jobe, unpublished data). There is a lack of evidence for many of these recommendations.

FRC

Although lung aeration is important for gas exchange after birth, uniform aeration and distribution of ventilation are also thought to be important to minimize regional overexpansion and injury (25,26). Our findings indicate that when providing PPV, adequate PEEP and VT are needed to create and establish FRC. For the very immature pups in this experiment, PEEP ≥ 8 cmH2O and VT ≥ 8 ml/kg were required to establish an FRC ≥ 3 ml/kg. We note, however, that the FRC gained during these experiments was less than that observed in spontaneously breathing term rabbit pups (10–15 ml/kg) (27) and term human infants (15–20 ml/kg) (28). Because pups were still continuing to establish FRC after 160 inflations (≈7 min), the FRC clearly had not reached steady state by this time, and it is likely that higher FRCs would have eventually been attained (Table 1).

The effect of increasing VT on FRC depended on PEEP levels: no effect of VT was observed at the lower PEEPs, whereas at 10 PEEP we observed a marked effect of VT on FRC (Table 1 and Figure 1). Similarly, the effect of increasing PEEP on FRC was not evident at a VT of 4 ml/kg, whereas at a higher VT (12 ml/kg) the effect of PEEP on FRC was marked. This indicates that both PEEP and an appropriate VT are required for the rapid accumulation of an appropriate FRC.

VT

We have previously shown that in spontaneously breathing term newborn rabbits, the first few breaths after birth are characteristically large (~15 ml/kg) and gradually reduce to ~7 ml/kg after the first 100 breaths (19). In human neonates, VTs of 6.4 (4.1) ml/kg have been observed in term infants and 6.7 (3.9) ml/kg in preterm infants, although it is unlikely that the very first breaths after birth were recorded in this study (29). In a separate study of babies receiving continuous positive airway pressure at birth, a variety of different respiratory patterns were observed with VT ranging from mean (SD) 3.1 (1.7) to 7.5 (4.2) ml/kg (30). Although evidence is lacking in preterm human infants, spontaneously breathing newborn rabbits appear to use large VTs (≈15 ml/kg) at the onset of air breathing, which gradually decrease with increasing breath number. On the basis of our observations, this would be expected to facilitate FRC recruitment.

Although large VTs facilitate FRC recruitment, they are largely thought to be injurious to the lung in newborn infants receiving respiratory support (31,32). Indeed, only six inflations of 35–40 ml/kg were sufficient to impair the response to surfactant and induce histological evidence of lung injury (3). Our data suggest that the combination of a relatively large VT with little or no PEEP is likely to be even more injurious than when combined with a high PEEP. With no PEEP, the vast majority of the VT was primarily distributed to the smaller apical lobes; this is likely to induce regional overdistension injury in those areas. By contrast, the delivery of a relatively large VT combined with a high PEEP in the initial resuscitation period distributed the air in a similar fashion to that observed in a well-aerated lung.

Clearly, the optimal VTs that should be used during the early stages of resuscitation at birth are unknown. Although an arbitrary range of 4–8 ml/kg is considered to be the optimal VT range to target when ventilating preterm human infants, a recent study has demonstrated that many of the volumes delivered during resuscitation are inadvertently well outside this range (33). It is clear that some spontaneous breathing infants initiate tidal breathing exceeding 8 ml/kg (29,30). In newborn rabbits, VT reduces as aeration occurs (19). During PPV, continued delivery of high VTs is likely to be injurious.

PIPs and Dynamic Pulmonary Compliance

For all levels of PEEP and VT, the PIPs required to initiate lung aeration were high (40–45 cmH2O), which was likely to be due to the initial presence of liquid in the airways rather than any other factor (19,34). However, the PIP required to achieve a set VT markedly and rapidly decreased as soon as the lung began to aerate. During this time, dynamic lung compliance was greatest in pups receiving the largest PEEP (10 cmH2O) and/or VT (12 ml/kg), resulting in much lower PIPs. This reflects more effective airway liquid clearance, resulting in larger lung gas volumes. Although the PIPs required during the initial 40 inflations were higher than those routinely used in human infants, they are not dissimilar to those used in preterm lambs (31). Similarly, previous studies have investigated the effects of PEEP on pulmonary function in preterm lambs and found that lambs ventilated at high PEEP (12 cmH2O) initially had better lung function but all developed pneumothoraces and died within 90 min (35). None of the pups developed pneumothoraces in our study, but they were ventilated for only a relatively short period. Because the characteristics of the lung are very different during the first few minutes after ventilation onset, as compared with when it is fully aerated, continued PEEP of 10 cmH2O may have eventually resulted in pneumothoraces. Therefore, optimal PEEP levels may differ with time after birth.

Distribution of Tidal Ventilation

The distribution of tidal ventilation with increasing VT at different PEEP levels was consistent within a group, but varied between groups. In particular, at PEEP 0, increasing the VT increased the distribution of incoming air into the apical regions of the lung. By contrast, at PEEP 10, increasing the VT increased the distribution of incoming air into the basal regions of the lung. It is possible that this finding explains the marked increase in lung compliance at higher PEEPs and VTs. Given that the basal regions of the lung are much larger and have a greater potential gas volume, we suggest that higher PEEPs effectively allow the incoming tidal ventilation to have access to and ventilate these dependent regions, thereby greatly increasing the ventilated gas volume of the lung.

Thus, it is clinically plausible that by increasing FRC and compliance, the combination of higher PEEPs and VTs during the immediate newborn period promoted a more physiological distribution of tidal ventilation. However, future studies should examine the effect of these strategies on the adequacy of gas exchange and on lung injury.

Limitations and Applicability

This study was designed to examine the physiological principles of establishing FRC soon after birth, and particularly the roles of VT and PEEP. We used a preterm animal model because these relationships cannot ethically be thoroughly examined in human infants. The premature rabbits were sedated, surgically intubated, immersed in warm water (with the head out of the water), and ventilated in an upright orientation, and were not exposed to maternal steroids. As such, these experiments were not intended to replicate clinical practice, but to specifically examine the inter-relationship between VT and PEEP on FRC, lung compliance, and the distribution of tidal ventilation, as these relationships are likely to be similar in humans.

The relatively low FRCs measured during this experiment are likely to result from a number of factors, particularly the extremely immature nature of the neonatal rabbits used (27 d gestational age), and the fact that neither antenatal steroids nor postnatal surfactant were administered. Because we used a relatively long expiratory phase (1.5 s) to facilitate image acquisition, there was likely to be a greater reliance on PEEP, as compared with other factors such as inflation, for maintaining FRC. However, because the same ventilation parameters (except the VT and PEEP changes) were used for all pups, we do not believe this would have biased the results.

Implications for Clinical Practice

Although the physiological principles are likely to be similar in human infants, the ventilation parameters used (e.g., PIPs and PEEPs) may not be directly comparable between preterm rabbits and humans. In performing this volume-targeted strategy with the advantage of an endotracheal tube present at birth, we needed to adjust the initial PIPs quickly, both up and down, particularly over the initial 40 inflations. During ongoing ventilation, a difference in PIP of only ~4 cmH2O increased VT from 4 to 12 ml/kg. This indicates that it may be difficult to achieve specific VTs manually during resuscitation without appropriate volume-targeted devices. Current guidelines for resuscitating preterm infants recommend starting PIPs of 20–25 cmH2O, and adjusting according to clinical response (2). However, because the effects of any particular PIP are highly variable and can change quickly with time, monitoring the VT administered would seem to be important.

Furthermore, the guidelines caution against the use of higher PEEPs, citing animal studies resulting in increased pneumothoraces and reduced pulmonary blood flow. However, these adverse outcomes occurred beyond 30 min of age, after the lungs were initially aerated, and may not be applicable to the immediate newborn period when the lung is partially liquid-filled and its mechanics are very different. Therefore, we suggest that the use of higher PEEPs during the initial resuscitation of extremely preterm neonates should be evaluated further.

Conclusion

The effects of PEEP and VT on lung aeration were examined using a rabbit model of extreme prematurity. Both PEEP and VT have independent but additive effects on FRC recruitment, lung mechanics, and the distribution of ventilation during the immediate newborn period. Specifically, increasing PEEP and VT levels markedly increase FRC, improve lung compliance, and increase the proportion of ventilation entering the larger basal regions of the lung. Future studies should investigate the effects of these strategies on acute lung injury.

Methods

Animal Experiments

All procedures were approved by Monash University and SPring-8 Synchrotron Animal Ethics Committees. Pregnant New Zealand white rabbits were studied at 27 d gestational age (term = 32 d). Antenatal steroids were not used. Anesthesia of the doe was induced using propofol (12 mg/kg bolus, 100 mg/kg/h infusion; Rapinovet, Schering-Plough Animal Health, Millsboro, DE) and maintained with inhaled isofluorane (1–2%) following intubation. Pups were partially delivered sequentially by hysterotomy, retaining a patent umbilical cord and with amniotic membranes over the nose and mouth to prevent air entering the lungs. Pups were sedated with sodium pentobarbitone (Nembutal, 0.1 mg i.p., Abbott Laboratories, North Chicago, IL), and local analgesia was applied to the neck (Xylocaine; 5% lignocaine, AstraZeneca, Södertälje, Sweden) before they were intubated surgically via a tracheostomy using an 18-gauge plastic canula as an endotracheal tube. This was capped to prevent air entering the lungs before PPV commenced. The umbilical cord was cut and the pup placed in a purpose-built water plethysmograph (34) to record respiratory function during imaging. After the experiment, rabbits and their pups were humanely killed using an overdose of sodium pentabarbitone (>100 mg/kg).

Experimental Protocol

Changes in lung volume were measured with a head-out water-filled plethysmograph (prewarmed to 39 °C) as previously described (36). Using a purpose-built, small animal ventilator (Monash University, Clayton, Australia) (37), pups were ventilated initially with a PIP of 35 cmH2O, adjusted to achieve the desired VT. Ventilation was provided at a rate of 24 inflations/min (1.0 s inflation and 1.5 s deflation) for 7 min (160 inflations). These times were used so that images could be acquired during both inflation (three images) and deflation (four images). Imaging was synchronized to the onset of each inspiration to ensure consistent image acquisition through the respiratory cycle. Twelve groups of pups (n = 5 per group) were studied, with different groups receiving one of three different VTs (4, 8, or 12 ml/kg) and one of four different PEEP levels (0, 5, 8, or 10 cmH2O).

Phase Contrast X-Ray Imaging

Phase contrast X-ray imaging techniques were used to measure lung gas volumes and the regional distribution of ventilation within and between successive breaths as previously reported (23). These lung gas volume measurements are accurate to within 25 μl, closely agreeing with plethysmograph measurements (23). The X-ray energy used was 24 keV and the imaging detector was placed 3 m downstream from the pups to optimize the phase contrast effects. Imaging was synchronized with mechanical ventilation using a short exposure time (40 ms), which when combined with relatively long inspiratory (1.0 s) and expiratory (1.5 s) times minimized motion blur. The detector was a Hamamatsu C9300-124F21 CCD camera (Hamamatsu Photonics, Shizuoka Prefecture, Japan) with a 1.8:1 ratio Fiber Optic Taper bonded to the CCD chip (16.2 µm effective pixel size). Radiation exposure to the pup was minimized by the use of a presubject shutter.

Data Collection

Plethysmograph measurements, ventilation parameters, and image timing data were collected at 1,000 Hz using PowerLab ADCs and LabChart Software version 7 (both ADInstruments, Sydney, Australia).

Image Analysis

Distribution of tidal ventilation was determined from image analysis as previously described and validated (23). The position of the pup was tracked using skeletal landmarks and a fiducial marker. Each frame was partitioned into quadrants: vertically through the spine and horizontally at the level of the seventh rib. The proportion of the VT distributed to the apical and basal regions of the lung was calculated and compared with measures separately obtained from fully aerated and homogenously ventilated lungs of pups of similar maturity; mean (SD) FRC 31 (12) ml/kg (M.L. Siew, M.J. Wallace, M.J. Kitchen, et al., unpublished data).

Analysis of Physiological Data

FRC was determined from plethysmograph data after each inflation, and defined as the volume of gas in the lung at end expiration. FRC was determined at 40, 80, 120, and 160 inflations by averaging five consecutive measurements, e.g., the FRC for inflation 80 was calculated by averaging end-expiratory measurements of inflations 78–82.

VT was defined as the volume change for each inflation, and the Δpressure was defined as (PIP − PEEP). MAP was calculated using PIP, PEEP, and the I:E ratio. Cd was determined by dividing the VT by the Δpressure. These parameters were determined as five-point averages for the same inflations as the FRC measurements.

From previous experience of ventilating neonatal rabbits of similar immaturity, we expected to initially increase the PIP to achieve initial tidal ventilation. Most pups did not have a stable VT until 40 inflations, and so data from inflations 40 to 160 were used to define the mean delivered VT. Data from the first 40 inflations were used to determine the PIPinit, defined as the maximum PIP required to achieve initial aeration. MAPinit and Cdinit were calculated at the corresponding inflation.

Statistics

No data were available to determine a sample size calculation. However, based on the expected differences and similar experiments performed previously (9,19,21,22), we used a sample size of five pups per group. Recorded data were analyzed using LabChart (ADInstruments, Sydney, Australia) and Excel (version 2007, Microsoft, Redmond, WA). Statistics were performed using Stata (version IC 10.1; Stata Corp, College Station, TX). A P value of <0.05 was considered to be statistically significant.

We performed linear regression for each major outcome against VT and PEEP. Post hoc, after reviewing the nonlinear effect of VT on the distribution of ventilation into apical and basal lobes at increasing PEEP levels, we performed regression of the gradient of VT distribution at each PEEP setting.

Statement of Financial Support

This project was funded by Australian National Health and Medical Research Council (NHMRC) grant 384100 and supported by the Victorian Government’s Operational Infrastructure Support Program. Travel funding was provided by the International Synchrotron Access Program managed by the Australian Synchrotron and funded by the Australian Government. K.W. is supported by a Monash University International Graduate Scholarship. P.D. and S.H. are in receipt of NHMRC research fellowships. M.K. is the recipient of an Australian Research Fellowship funded by the Australian Research Council.

Disclosure

C.M. is a consultant to Dräger Medical, Lübeck, Germany. This company was not involved with the study design, conduct, data analysis, or preparation of the manuscript and did not contribute financial support.

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Acknowledgements

The authors acknowledge the support of the SPring-8 Synchrotron Radiation Facility, Japan, in providing beam time for these experiments.

Author information

Affiliations

  1. The Ritchie Centre, Monash Institute for Medical Research, Monash University, Melbourne, Australia

    • Kevin Wheeler
    • , Megan Wallace
    • , Arjan te Pas
    • , Melissa Siew
    •  & Stuart Hooper
  2. Newborn Research, Royal Women’s Hospital, Melbourne, Australia

    • Kevin Wheeler
    • , Colin Morley
    • , Peter Davis
    •  & Stuart Hooper
  3. Murdoch Children’s Research Institute, Melbourne, Australia

    • Kevin Wheeler
  4. Department of Obstetrics and Gynaecology, Monash UniversityMelbourne, Australia

    • Megan Wallace
    • , Melissa Siew
    •  & Stuart Hooper
  5. School of Physics, Monash Centre for Synchrotron Science, Melbourne, Australia

    • Marcus Kitchen
    • , Muhammad Islam
    •  & Robert Lewis
  6. Division of Neonatology, Leiden University Medical Center, Leiden, The Netherlands

    • Arjan te Pas
  7. Division of Biological Engineering, Monash University, Melbourne, Australia

    • Andreas Fouras
  8. Department of Obstetrics and Gynaecology, University of Melbourne, Melbourne, Australia

    • Peter Davis

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Correspondence to Kevin Wheeler.

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https://doi.org/10.1038/pr.2013.48

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