Introduction

During neonatal stabilisation at birth, the most frequently used respiratory support device for providing non-invasive ventilation (e.g., continuous positive airway pressure (CPAP) or intermittent positive pressure ventilation (iPPV)) is a T-piece resuscitator. The T-piece generates positive end expiratory pressure (PEEP) or CPAP by providing resistance to the bias gas flow through the expiratory outlet of the T-piece (called the PEEP valve). It then generates positive inflation pressures (PIP) when the PEEP valve is occluded.1,2 The resistance of the PEEP valve is regulated by altering the area of the aperture to achieve a certain CPAP level, but the required area (thus resistance) to achieve this CPAP level depends on the bias gas flow. To achieve the same PEEP/CPAP level, a low bias gas flow (e.g. 6–8 L/min) requires a small aperture with high resistance, whereas higher bias gas flows (e.g. 12–15 L/min) require a larger aperture with a lower resistance.1,3,4 As the infant expires through the PEEP valve, a reduced valve resistance will reduce the expiratory resistance imposed on the infant and thereby increase expiratory flows. When expiration is active, this is thought to reduce the imposed work of breathing (iWOB) (e.g., breathing effort and energy cost).3,4 When a T-piece is compared to other CPAP methods in a simulated setting with an active expiration, it generates a substantially higher iWOB due to the relatively high resistance of the PEEP valve.3,4

Recently, a new low imposed resistance resuscitator with a low iWOB for neonatal stabilisation was introduced using dual flow (e.g., bias flow and jet flow). This device, now commercially available as r-PAP, generates PEEP/CPAP using the jet flow. The turbulence created in the angulated tube opposes expiration and supports inspiration, a phenomenon that is called a fluidic flip. During iPPV the system is occluded in the same manner as a T-piece and the bias flow added to achieve a sufficient total gas flow for an acceptable inspiratory rise time. In this way, the dual flow system is able to generate the same PEEP/CPAP levels as a T-piece, but with a lower imposed resistance during active expiration.5 In addition, the dual flow system is able to generate more stable PEEP level across a range of different lung compliances during iPPV.2 A recently performed multicentre randomised controlled trial6 comparing this dual flow system with a traditional T-piece system (e.g., Neopuff™) in preterm infants reported less delivery room intubation when the dual flow system was used. However, this was an unblinded study and the reason for the differences in intubation rates have not been explained. It could be related to the interface (face mask vs nasal prongs) or other differences such as imposed resistance or more stable CPAP and PEEP levels.

While a resuscitation device that provides a low imposed resistance might provide advantages, there might be benefits from increasing resistance and limiting expiratory flows. Peak flows >500 L/min (equivalent to >~6 L/kg/min) during coughing produced shear stress in airway walls in adults.7 Therefore, reducing peak flows by using a T-piece system could potentially lead to less shear stress and airway epithelial cell damage, particularly in the less compliant immature lung of preterm infants at birth. Limiting flows during resuscitation and stabilisation have not been investigated for iPPV or spontaneous breathing.

A possible compromise might be to use the traditional T-piece system with a higher bias gas flow (e.g., 12 L/min), thereby reducing the imposed resistance and generating more stable PEEP/CPAP pressures, while limiting potentially harmful peak flows. Indeed, we recently investigated the differential effects of a bias gas flow of 12 L/min and 8 L/min in spontaneous breathing preterm infants at birth and showed that increased bias gas flow resulted in a lower inspiratory and expiratory resistance with less inspiratory CPAP fluctuations.1

As resuscitators providing either a low imposed resistance (e.g., r-PAP) or a higher imposed resistance (e.g., Neopuff™), both provide advantages and disadvantages, we aim to investigate i) the differences in peak flows and pressure stability resulting from differences in resistance during intermittent positive pressure ventilation (iPPV) and simulated spontaneous breathing between the r-PAP and Neopuff™.

Methods

An experimental study was performed at The Ritchie Centre, Hudson Institute of Medical Research in Melbourne, Australia to compare a low imposed resistance resuscitator, Inspire r-PAP (Inspiration Healthcare Group, Steenderen, The Netherlands), to a higher imposed resistance resuscitator, Neopuff™ T-Piece resuscitator (Neopuff™ Infant Resuscitator, Fisher & Paykel Healthcare Ltd., Auckland, New Zealand) with various bias gas flows.

The test setting is shown in Fig. 1. A custom made test-lung (Fig. 1), with a FRC of 35 mL, was connected to the respiratory tubing of the Neopuff™ or r-PAP. A disposable Avea Varflex Flow transducer (Carefusion, CA) was placed between the end of the test-lung’s trachea and the respiratory tubing. Three pressure transducers (PD10; DTX Plus Transducer; Becton Dickinson, Singapore) were connected to (1) the intrathoracic space, (2) the lung and (3) the respiratory tubing at the end of the test-lung’s trachea. Flows were recorded digitally using the Polybench physiological software (Applied Biosignals, Weener, Germany) by connecting the flow transducer to a respiratory function monitor (Advanced Life Diagnostics, Weener, Germany). Pressures were recorded digitally using the LabChart data acquisition system via a Bridge Amp (Powerlab, ADInstruments, Sydney, Australia). The Neopuff’s bias gas flow was set to 8, 12 and 15 L/min and the CPAP level was set to 8 cm H2O. For the r-PAP, the GE Giraffe Stand-alone Infant Resuscitation System (GE Healthcare, Rydalmere, Australia) was used to set the bias gas flow and jet flow (as also described in a previous study6). The jet flow was titrated to achieve a CPAP/PEEP level of 8 cm H2O and bias flow was then added to reach a total fresh gas flow of 15 L/min.

Fig. 1: Test-lung.
figure 1

Test-lung (system compliance: 7 mL/cm H2O), which consists of a Draeger test-lung (a) within a Sealed Perspex cylinder with two 3D printed rubber lids (b), which is partly filled with polystyrene foam (c). The test-lung ends in a simulated trachea (d), which is connected to a flow sensor (e) and then to either the Neopuff™ or r-PAP respiratory support system (f). On the other side of the cylinder a suction tube with T-piece (g) is inserted through the lid. niPPV was simulated by occluding and opening the aperture of the respiratory support system whilst spontaneous breathing was simulated by occluding and opening the T-piece of the suction tube. Pressures where measured in the lung (h), the cylinder (i) and the simulated trachea (j).

During iPPV, a positive end expiratory pressure (PEEP) of 8 cm H2O and positive inflation pressures (PIP) of 20 cm H2O were set. During simulated spontaneous breaths, an intrathoracic pressure gradient of 30 cm H2O was generated by occluding the lateral opening of the suction device simulating an active inspiration, while a passive expiration was simulated by re-opening the lateral opening of the suction device. For each group, 20 inflation breaths over 60 s and 20 spontaneous breaths over 60 s were simulated by the resuscitator manually. All pressures were set based on the pressure measurements visible on the RFM.

All inflation breaths and spontaneous breaths were analysed on a breath-by-breath basis to determine PEEP/CPAP level, PIP level, peak inspiratory flow rate (PIFR), PEFR, inspiratory tidal volume (Vti) and the resistance of the T-piece valve (Rv). During simulated spontaneous breathing inspiratory and expiratory CPAP fluctuations (ΔCPAPinsp, ΔCPAPexp) were also assessed. All pressures were measured by the pressure sensor in line (Fig. 1j).

The valve resistance was calculated using a derivation of Ohm’s law (Formula 1, Fig. 2).

$${{{{{{\mathrm{Rv}}}}}}}=\frac{\triangle P}{{{{{{{\mathrm{Qv}}}}}}}}=\frac{{{{{{{\mathrm{Pd}}}}}}}-{{{{{{\mathrm{Pat}}}}}}}}{\,{{{{{{\mathrm{Qb}}}}}}}+{{{{{{\mathrm{Qm}}}}}}}}=\frac{{{{{{{\mathrm{CPAP}}}}}}}-0}{\,{{{{{{\mathrm{Qb}}}}}}}+0}$$
(1)
Fig. 2
figure 2

Closed-loop schematic visualisation of flows, pressures and resistance during spontaneous breathing.

As the r-PAP uses a dual flow system and generates CPAP by a jet of fresh gas instead of a resistor, we were unable to calculate the imposed resistance during ventilation or spontaneous breathing for this device. However, it is known that systems resembling the r-PAP, such as infant flow and the benveniste valve, have a much lower expiratory resistance than a T-piece, even with a bias gas flow of 15 L/min.4

In addition, we measured the CPAP fluctuations during spontaneous breaths in both devices. During inspiration less flow travels through the expiratory outlet resulting in a pressure below the set CPAP (formula 2), while during expiration the flow through the expiratory outlet increases resulting in a pressure above the set CPAP (formula 3).

$$\triangle {{{{{{{\mathrm{CPAP}}}}}}insp}}={{{{{{\mathrm{PEEP}}}}}}}-{{{minimum}}}\,{{{inspiratory}}}\,{{{pressure}}}$$
(2)
$$\triangle {{{{{{\mathrm{CPAP}}}}}}}exp ={{{peak}}}\,{{{expiratory}}}\,{{{pressure}}}-{{{{{{\mathrm{PEE}}}}}}}{{{{{\mathrm{P}}}}}}$$
(3)

The local institutional Research Ethics Committee of the LUMC approved the study protocol and issued a statement of no objection for performing this study.

All statistical analyses were performed with IBM SPSS Statistics version 25 (IBM Software, Chicago, Illinois, 2016). Continuous data are presented as median (IQR) or mean ± SD. Normality was judged based on the inspections of histograms. The Kruskal–Wallis test was used to compare all four groups (r-PAP, NP 8 L/min, NP 12 L/min and NP 15 L/min). In addition, the Mann–Whitney test was used to compare the r-PAP to each group of the Neopuff™. A p-value < 0.05 was considered statistically significant.

Results

Intermittent positive pressure ventilation

The valve resistance of the T-piece was significantly reduced when the bias gas flow in the Neopuff™ was increased from 8 to 15 L/min (NP8 0.86 ± 0.01 vs. NP12 0.62 ± 0.01 vs. NP15 0.46 ± 0.01 cm H2O/L/min, p < 0.001) . As a result, the PIFR and PEFR increased in the Neopuff™, but the peak flows were still significantly lower compared to the peak flows observed in the r-PAP (PIFR: NP8 3.8 ± 0.06 vs. NP12 3.9 ± 0.06 vs. NP15 4.0 ± 0.05, r-PAP 6.0 ± 0.26 L/min, p < 0.001; PEFR NP8 2.4 ± 0.08 vs NP12 3.0 ± 0.02 vs. NP15 3.5 ± 0.06 vs r-PAP 4.6 ± 0.19 L/min, p < 0.001). During iPPV, a pressure overshoot of 3.2 cm H2O was observed in the r-PAP (Table 1 and Fig. 3).

Table 1 Comparing the r-PAP to the Neopuff™ with different bias gas flows during intermittent positive pressure ventilation.
Fig. 3
figure 3

Pressure-flow curves of Neopuff™ T-piece and r-PAP with GE system during positive pressure ventilation.

Simulated spontaneous breathing

When increasing the bias gas flow from 8 to 15 L/min in the Neopuff™, the valve resistance of the T-piece was significantly lower (NP8 0.94 ± 0.01 vs. NP12 0.67 ± 0.01 vs. NP15 0.50 ± 0.01 cm H2O/L/min, p < 0.001). This was consistent with the finding that both the PIFR and PEFR significantly increased following the increase in bias gas flow (PIFR: NP8 3.1 ± 0.06 vs. NP12 3.2 ± 0.06 vs. NP15 3.4 ± 0.06 L/min, p < 0.001; PEFR: NP8 4.9 ± 0.07 vs. NP12 5.2 ± 0.08 vs. NP15 5.7 ± 0.12 L/min, p < 0.001), whereas the inspiratory and expiratory CPAP fluctuation significantly decreased (ΔCPAPinsp: NP8 5.7 ± 0.17 vs. NP12 4.7 ± 0.19 vs. NP15 4.4 ± 0.16 cm H2O, p < 0.001; ΔCPAPexp: NP8 8.8 ± 0.19 vs. NP12 7.2 ± 0.21 vs. NP15 6.3 ± 0.21 cm H2O, p < 0.001)) (Table 2).

Table 2 Comparing the r-PAP to the Neopuff™ with different bias gas flows during simulated spontaneous breathing.

Compared to the Neopuff™, the r-PAP device resulted in significantly higher PIFR and PEFR and had significantly less inspiratory and expiratory CPAP fluctuations (PIFR NP15 3.4 ± 0.06 vs. r-PAP 4.5 ± 0.10 L/min, p < 0.001; PEFR NP15 5.7 ± 0.12 vs. r-PAP 7.3 ± 0.14 L/min, p < 0.001); ΔCPAPinsp: NP15 4.4 ± 0.16 vs. r-PAP 1.1 ± 0.16 cm H2O, p < 0.001; ΔCPAPexp: NP15 6.3 ± 0.21 vs. r-PAP 1.9 ± 0.20 cm H2O, p < 0.001) (Table 2).

Discussion

In this study, we found that increasing the bias gas flow in the Neopuff™ by a factor of 1.88 (i.e., from 8 to 15 L/min) reduced the resistance of the valve by the same magnitude during simulated spontaneous breathing while maintaining the same CPAP level. Reducing imposed resistance led to smaller CPAP fluctuations and higher inspiratory and expiratory peak flows. However, even with a bias gas flow of 15 L/min, the Neopuff™ still had a higher imposed resistance compared to the r-PAP device as well as larger CPAP fluctuations and lower inspiratory and expiratory peak flows. In addition, a pressure overshoot was observed when using the r-PAP during positive pressure ventilation.

This study confirms the results of our previous retrospective study investigating the effect of a higher bias gas flow on valve resistance and imposed expiratory resistance during spontaneous breathing in preterm infants at birth. In the retrospective study, we also observed that increasing the bias gas flow by a factor of 1.5, reduced the imposed inspiratory and expiratory resistance by the same factor.1 However, the retrospective study reported a lower PIFR with similar PEFR, while we observed higher peak flows in an experimental setting during which airway resistance and pulmonary pressures remained similar during the study period. This is also confirmed by Huckstadt et al.,8 who reported an increase in PIFR and PEFR in preterm infants admitted to the NICU when a device administering CPAP with a high expiratory resistance (Babylog 8000) was compared to a low-resistance CPAP device (Infant Flow). The observed differences between in vitro and in vivo measurements at birth might be explained by the fact that airway resistance and pulmonary pressures markedly change during the transition at birth.

Although higher inspiratory and expiratory peak flows were observed in the low imposed resistance resuscitator compared to a higher imposed resistance resuscitator, these peak flows remained <6 L/kg/min when assuming that a FRC of 35 mL correlates to a birthweight of 2 kg.9 However, it should be kept in mind that the driving force for inspiratory and expiratory flow is the pressure gradient between inside and outside of the lung when flow is zero. During simulated spontaneous breathing, this was the difference between the internal pulmonary pressure (~–30 cm H2O) at peak inspiration and the external CPAP level (~8 cm H2O). During iPPV, this was the difference between PIP (~20 cm H2O) and PEEP (~8 cm H2O). As the average pressures generated during the first breaths at birth10 have been recorded at –70 cm H2O and PIP > 20 cm H2O can be used during neonatal stabilisation, the peak flows that occur naturally in infants at birth might be higher than what we observed in this study. Indeed, in our retrospective study1 there were occasional peak flows of >~6 L/kg/min observed during spontaneous breaths on CPAP when the higher imposed resistance resuscitator, Neopuff™, was used. As the peak flow in the low imposed resistance resuscitator will be higher, the incidence of spontaneous breaths or ventilated breaths with peak flows >~6 L/kg/min might be as well. In addition, higher peak expiratory flows increase the deflation rate, which could lead to a loss of FRC due to the lung’s higher momentum as it approaches FRC.1 This effect would even be higher when air accumulates in the abdomen as it would increase abdominal pressure and apply an upward displacement on the diaphragm leading to higher peak flows. This risks increasing the momentum of the lung during deflation, which would cause the lung to deflate to a greater degree, leading to a reduction in FRC. As such, the lower the expiratory resistance, the greater the effect that abdominal air accumulation will have. Future animal studies will be necessary to investigate whether lower peak flows as seen with T-piece systems positively affect FRC and/or reduce shear stress and subsequent airway epithelial cell damage in the fragile lungs of preterm infants at birth. In the meantime, a possible compromise might be to use the traditional T-piece system with a higher bias gas flow, thereby reducing the imposed resistance and generating more stable PEEP/CPAP pressures, while limiting potentially harmful peak flows.

The pressure overshoot observed when using the low imposed resistance resuscitator is in line with results reported in previous studies and related to the pressure release valve in the GE driver. These studies reported spikes above set PIP for both T-piece and r-PAP, ranging from 0.6 to 9.46 cm H2O, in GE and Draeger systems, depending on lung compliance and the set PIP.2,11 As these spikes increase pulmonary pressures above the set PIP and are not obvious unless a respiratory function monitor is used, caregivers using these devices should be aware that they might be providing higher PIP levels than intended. Although the clinical significance of these pressure spikes are unknown, they might be harmful for preterm infants at birth. Indeed, the spikes shown in Fig. 3 are ~200 ms in duration and so when using higher inflation rates (e.g., at 60 inflations per minute) these pressure spikes will form a highly significant component of the inflation time. It is important to note that the pressure spikes above PIP were not observed with the r-PAP device when the designated driver was used.

As this study was a bench test with the purpose to generate rationale, the results should be translated with the appropriate caution to clinical practice. In this study, all variables are controlled, while during the transition at birth airway resistance and pulmonary pressures markedly change. As the r-PAP uses a dual flow system, we were unable to measure the imposed resuscitator resistance of the r-PAP, which made it harder to compare the results with the Neopuff™. However, looking at the pressure and flow values and resistance reported in other papers,3,4,12 the imposed resuscitator resistance of the r-PAP is lower than the imposed resuscitator resistance of the Neopuff™. In addition, as we recorded values at 200 Hz, our measure of PEFR (and the size of the pressure spike) may be an under-estimation, despite the variability between measurements being extremely low.

Conclusion

In a bench test, it seemed that the r-PAP had a lower resistance than the T-piece system (e.g., Neopuff™) even when bias gas flows in the T-piece system were increased to compensate. This resulted in more stable CPAP pressures with higher peak flows when using the low imposed resistance resuscitator. The lower peak flows observed in higher imposed resistance systems such as the Neopuff™ might have advantages by increasing lung function and reducing lung injury and this needs to be further investigated.