0Andrews et al. Intensive Care Medicine Experimental (2015) 3:16 DOI 10.1186/s40635-015-0054-1
RESEARCH
Open Access
CrossMark
Alveolar instability (atelectrauma) is not identified by arterial oxygenation predisposing the development of an occult ventilator-induced lung injury
Penny L Andrews2, Benjamin Sadowitz1, Michaela Kollisch-Singule1, Joshua Satalin1*, Shreyas Roy1, Kathy Snyder1, Louis A Gatto3, Gary F Nieman1 and Nader M Habashi3
* Correspondence: satalinj@upstate. edu
department of Surgery, SUNY Upstate MedicalUniversity, 750 East Adams Street, Syracuse, NY 13210, USA
Full list of author information is available at the end of the article
Abstract
Background: Improperly set mechanical ventilation (MV) with normal lungs can advance lung injury and increase the incidence of acute respiratory distress syndrome (ARDS). A key mechanism of ventilator-induced lung injury (VILI) is an alteration in alveolar mechanics including alveolar instability or recruitment/derecruitment (R/D). We hypothesize that R/D cannot be identified by PaO2 (masking occult VILI), and if protective ventilation is not applied, ARDS incidence will increase.
Methods: Sprague-Dawley rats (n = 8) were anesthetized, surgically instrumented, and placed on MV. A thoracotomy was performed and an in vivo microscope attached to the pleural surface of the lung with baseline dynamic changes in alveolar size during MV recorded. Alveolar instability was induced by intra-tracheal instillation of Tween and alveolar R/D identified as a marked change in alveolar size from inspiration to expiration with increases in positive end-expiratory pressure (PEEP) levels. Results: Despite maintaining a clinically acceptable PaO2 (55-80 mmHg), the alveoli remained unstable with significant R/D at low PEEP levels. Although PaO2 consistently increased with an increase in PEEP, R/D did not plateau until PEEP was >9 cmH2O.
Conclusions: PaO2 remained clinically acceptable while alveolar instability persisted at all levels of PEEP (especially PEEP <9 cmH2O). Therefore, PaO2 levels cannot be used reliably to guide protective MV strategies or infer that VILI is not occurring. Using PaO2 to set a PEEP level necessary to stabilize the alveoli could underestimate the potential for VILI. These findings highlight the need for more accurate marker(s) of alveolar stability to guide protective MV necessary to prevent VILI.
Springer
Background
The acute respiratory distress syndrome (ARDS) remains a serious clinical challenge affecting nearly 200,000 patients annually, claiming the lives of 30-40 % of those afflicted [1]. Although mechanical ventilation (MV) is applied to patients without lung injury, improperly set MV [2] can cause a secondary ventilator-induced lung injury (VILI) [3], playing a key role in the high incidence of ARDS (25 %) within 48 h of MV initiation [4, 5]. Most cases of ARDS evolve over 30-72 h after hospital admission where lung protective strategies are typically implemented after the development of
© 2015 Andrews et al. This is an Open Access article distributed under the terms of the Creative Commons Attribution License (http:// creativecommons.org/licenses/by/4.0), which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly credited.
lung injury and clinically diagnosed by a deterioration of oxygenation characterized by a decline in PaO2/FiO2 (P/F) ratio [6, 7]. Although there are alternative markers of optimizing mechanical ventilation, most definitions of ARDS [6, 7] rely on oxygenation (PaO2) as a marker of pulmonary function. Lung protection is generally instituted in a reactive rather than proactive approach with an emphasis on treating rather than preventing the progression of worsening lung injury. Further, clinicians target PaO2 or saturation (SpO2) [8] to determine if ventilator strategies are effective prior to and after the development of acute lung injury (ALI). However, reliance on PaO2 as a marker of lung function presumes there is no lung injury prior to ARDS perpetuating a binary concept of ARDS. A key to understanding lung-ventilator interactions may lie in subclinical mechanisms of lung injury and the impact of MV on the "micro-environment" at the alveolar/alveolar duct level rather than centering on the "macro-environment" and parameters displayed on the ventilator (i.e., tidal volume (Vt), plateau pressure) using PaO2 and SpO2.
Recently, it has been suggested that the primary mechanism of VILI is tidal alveolar recruitment/derecruitment (R/D) [9, 10]. Our group has shown that tidal R/D leads to persistent alveolar instability causing severe histologic lung injury and ARDS [11] and optimizing alveolar stability is critical to preventing VILI and limiting ARDS [12-14]. PaO2 may not be an accurate surrogate of alveolar stability; therefore, preventing ARDS using preemptive MV requires clinicians to consider the potential for occult alveolar instability (i.e., R/D without a significant fall in PaO2) [6]. In this study, we hypothesized that in an acutely injured lung, alveolar instability would persist despite improvements in PaO2 with increasing levels of positive end-expiratory pressure (PEEP). Lack of correlation between PaO2 and alveolar stability would provide a mechanistic explanation of why patients with normal PaO2 evolve to ARDS after 48 h of MV [4, 15]. In this study, we show direct visual evidence using in vivo microscopy that alveolar R/D cannot be predicted using PaO2 as a surrogate for alveolar stability and protective MV.
Methods
Vertebrate animals
The Institutional Animal Care and Use Committee at Upstate Medical University, Syracuse, NY, approved the studies. All experiments were performed in adherence to the guidelines established by the National Institutes of Health for the use of experimental animals in research.
Surgical preparation
Adult male Sprague-Dawley rats (n = 8) weighing 590 ± 19.2 g were anesthetized via an intraperitoneal injection of ketamine/xylazine (90 and 10 mg/kg, respectively) dosed at 0.1 mg/kg of ketamine before surgery as well as during the experiment to provide adequate anesthesia. To ensure that the Vt remained constant, the animals were paralyzed with rocuronium to inhibit spontaneous breathing. A tracheostomy was performed, and time-cycled/pressure-controlled mechanical ventilation was initiated with a PEEP of 3 cmH2O, pressure control (Pcontroi) of 15 cmH2O, respiratory rate of 30 breaths/min, and FiO2 of 100 % (Hamilton G5 ventilator, Hamilton Medical Inc., Reno, NV). A jugular vein
was cannulated for the administration of fluids and a carotid artery catheter placed for blood gas samples and hemodynamic monitoring.
Hemodynamic, pulmonary, and blood gas measurements
Hemodynamic and pulmonary parameters were continuously monitored (Philips Healthcare and Hamilton G5 ventilator). Arterial blood gas was sampled at baseline and each PEEP level, as defined in "Lung injury," to record pH, PaCO2, PaO2, and PaO2/FiO2 (P/F) ratios (cobas b221, Roche Diagnostics).
Lung injury
Serial blood gases were taken and the respiratory rate adjusted until PaCO2 was between 35 and 45 mmHg. A baseline blood gas was performed and lung injury induced via 0.2 % Tween-20 in normal saline (16 cc/kg) instillation via an endotracheal tube. This was repeated until a P/F <100 mmHg was reached.
In vivo microscopy
After induction of lung injury, a right thoracotomy was performed to expose the pleural surface of the right lung. The in vivo microscope (epi-objective microscope with epiillumination; Olympus America Inc.) was approximated to the nondependent (anterior) portion of the right lung and 5 cmH2O suction applied to capture a steady field of the alveoli at x10 magnification. Although dependent lung regions may be more susceptible to R/D, stability in dependent regions would be unlikely if alveolar stability in nonde-pendent regions was not achieved. In this model, we used individual rats as their own control and documented alveolar stability at baseline. After Tween injury, alveolar behavior became unstable demonstrating R/D. Thirty seconds of video was recorded from an attached digital video camera (Sony CCD color video camera SSC-S20) and uploaded to a computer while maintaining a PEEP of 3 cmH2O and Pcontrol of 15 cmH2O. Subsequently, PEEP was increased in 3 cmH2O increments and videos recorded from the in vivo microscopy at each setting until a PEEP of 18 cmH2O was achieved. This procedure was repeated at each PEEP level in five distinct parenchymal areas of the right nondependent lung.
Image capture and processing
Video was captured using Pinnacle Studio software (Corel Corp.) for analysis of alveolar mechanics. Individual frames were extracted and analyzed at the plateau pressure (Pplateau) and peak expiration (PEEP) for five lung fields per PEEP level. The alveoli were identified in the frames and manually outlined using Photoshop CS6 (Adobe Inc.) with areas calculated using Image-Pro software (Media Cybernetics). The areas calculated represent alveolar inflation at end-inspiration (I) and end-expiration (E) and are each represented as a fraction of the total microscopic lung field. Alveolar instability was assessed by comparing the percent difference between I and E (%AI-E). A greater %AI-E is suggestive of increased R/D and alveolar instability.
Statistics
Least squares regression was used to determine whether alveolar stability and arterial oxygenation were linearly related (Microsoft Excel, 2008).
Results
Physiologic parameters
All animals displayed severe lung injury after Tween instillation with average P/F ratio <100 mmHg. As PEEP was increased, there was a concomitant decrease in mean arterial pressure but no change in heart rate (Table 1). With increasing PEEP, there was no significant change in pH but there was a decrease in pCO2 with PEEP above 6 cmH2O. Increasing PEEP led to a correspondent increase in the mean airway pressure (Paw) and Pplateau. Tidal volumes were set at 6 cc/kg, and minute ventilation was similar between groups (Table 2).
Alveolar stability and PaO2
Subpleural alveoli at I and E in both the uninjured and injured lungs are seen in Fig. 1 with individual alveoli outlined in dots. Measuring alveolar size change between I and E is used to assess alveolar stability.
Uninjured alveolar stability and PaO2
There was a minimal size change during tidal ventilation in the normal lung with 12 cmH2O of PEEP compared to a large change in alveolar size in the injured lung indicating severe alveolar instability even with 18 cmH2O of PEEP (Fig. 1).
Injured alveolar stability and PaO2
Examination of the aggregate data shows that a stepwise increase in PEEP (3-9 cmH2O) led to an increase in both alveolar stability and PaO2 (Fig. 2). However, further increased levels of PEEP (12-18 cmH2O) improved PaO2 without a concomitant increase in alveolar stability (Fig. 2). Examination of individual animals demonstrated that PaO2 remained largely unchanged despite a spectrum of alveolar instability at a given PEEP level.
Discussion
The most important findings of this study were as follows: (a) unstable alveoli oxygenated blood to nearly the same PaO2 as stable alveoli, particularly at levels of PEEP of 3-9 cmH2O; (b) alveolar stability did not improve when PEEP was increased above 9 cmH2O despite continual improvement in PaO2 up to PEEP of 18 cmH2O (Fig. 3); and (c) combined with our prior work, this shows that PEEP may have a greater effect recruiting and distending conducting airways rather than the alveoli [16]. In a previous study, we showed increasing levels of PEEP increases micro-strain of the conducting airways with less effect on alveolar area [16]. In the present study, low levels of PEEP may have recruited collapsed conducting airways initially stabilizing communicating alveoli (steep portion of alveolar stability curve in Fig. 2). However, an increase in PEEP may have caused progressive distention in the conducting airways rather than increasing alveolar area and stability. Despite increasing PEEP, alveolar stability plateaus above PEEP of 9 cmH2O and never reaches the complete stability (i.e., R/D = 0 %) of the
n> i i 3'
Table 1 Hemodynamic and blood gas measurements
BL-uninjured Post-injury PEEP 3 PEEP 6 PEEP 9 PEEP 12 PEEP 15 PEEP 18
HR (beats/min) 189.1 ±59.1 186.4 ±45.1 204.9 ± 44.5 172.2 ±51.1 186.0 ± 38.3 176.7 ± 44.6 179.9 ±61.5 150.5 ±42.9
MAP (mmHg) 71.8 ± 21.1 61.3 ± 12.6 50.6 ± 1 6.2 52.5 ± 26.5 49.0 ±24.1 47.4 ±18.1* 44.5 ± 16.5* 39.1 ±15.7*
pH 7.35 ± 0.07 7.246 ± 0.087 7.204 ± 0.049* 7.153 ±0.101* 7.209 ± 0.066* 7.197 ±0.109* 7.21 ±0.15* 7.199 ± 0.195
PaCO2 (mmHg) 38.11 ±11.67 53.58 ± 14.43* 47.42 ± 13.21 49.68 ± 11.22 36.49 ±4.85 35.43 ± 5.99 32.0 ± 7.0 29.39 ±7.17
PaO2 (mmHg) 467.5 ± 163.5 54.03 ± 24.70* 60.07 ± 13.10* 106.3 ± 90.47* 169.7 ±143.5* 221.5 ±115.5* 266.0 ± 122.0* 352.0 ±159.0
FiO2 (%) 100 100 100 100 100 100 100 100
% Saturation 97.63 ± 1.26 56.43 ± 20.96* 64.76 ± 16.04* 65.12 ± 17.54 88.77 ± 5.74 92.26 ±8.58 93.15 ± 8.11 95.1 ± 5.98
P/F 507.6 54.03* 60.07* 106.3* 169.7* 221.5* 266.0* 352.0*
*p < 0.05 as compared to baseline (BL)
n> i i 3'
Table 2 Pulmonary measurements
BL-uninjured Post-injury PEEP 3 PEEP 6 PEEP 9 PEEP 12 PEEP 15 PEEP 18
Vt (ml)/kg 6.0 ± 0.5 5.9 ±0.3 6.0 ± 0.5 5.9 ±0.3 5.9 ±0.3 5.9 ±0.3 5.9 ±0.3 5.875 ± 0.354
Pcontrol (cmH2O) 12.6 ± 2.5 16.9 ±1.2* 17.6 ±2.2* 16.6 ± 2.5* 15.5 ± 3.1 14.9 ± 3.1 14.7 ± 3.9 12.88 ± 5.0
Ppeak (cmH2O) 15.7 ±2.6 20.1 ±1.4* 20.7 ± 2.3* 22.5 ±2.3* 24.5 ±3.1* 27.0 ± 3.2* 29.7 ± 3.9* 30.88 ± 5.0*
Pplateau (cm^O) 15.7 ±2.6 20.0 ±1.3* 20.6 ± 2.2* 22.6 ± 2.5* 24.5 ±3.1* 27.0 ± 3.2* 29.7 ± 3.9* 30.88 ± 5.0*
Pmean (cmH2O) 6.59 ± 0.65 7.72 ± 0.43 7.94 ± 0.72 10.15 ± 0.95* 11.99 ±1.35* 13.8 ± 1.9* 15.3 ± 3.6* 14.63 ±2.8*
MV (l/min) 0.183 ±0.009 0.187 ±0.022 0.185 ± 0.022 0.184 ± 0.026 0.188 ± 0.019 0.187 ± 0.016 0.19 ± 0.028 0.175 ± 0.018
RR (breaths/min) 30.5 ± 1.6 30.4 ±2.0 30.9 ± 2.5 32.0 ±3.3 32.0 ±3.3 31.6 ±2.5 31.4 ± 2.9 30.13 ±3.23
*p < 0.05 as compared to baseline (BL)
re 6 o
EXPIRATION INSPIRATION
Fig. 1 In vivo microscopy showing alveolar inflation of non-injured (PEEP 12) and injured (PEEP 18) lungs at end-inspiration and end-expiration
uninjured lung [17]. These data suggest that alveolar stability has a nonlinear relationship to PaO2.
We hypothesize that improvement in PaO2 was due to end-inspiratory tidal recruitment of collapsed alveoli rather than recruitment of unstable alveoli throughout the ventilator cycle (i.e., both I and E). Oxygen would be exchanged during inspiration as the alveolus "pops" open and coupled with the rapid transit time of the erythrocyte,
Alveolar Stability Unrelated to Peripheral Oxygen Saturation
T —* P02 —«
\ :_ y m
\ 1 1_ J n
Injury
Fig. 2 Stepwise increases in low levels of PEEP (3-9 cmH2O) led to an increase in both alveolar stability and arterialoxygenation as measured by pO2. High levels of PEEP (12-18 cmH2O), however, improved arterial oxygenation in a stepwise fashion without a concomitant increase in alveolar stability
Animal Anesthetized
Airway and Vascular Access
Baseline Values Recorded
Injury Established Thoracotomy Performed
In Vivo Microscopy
PEEP 3cmH20
PEEP 6cmH20
PEEP 9cmH20
PEEP 12cmH20
PEEP 15cmH 0 —ABG
PEEP 18cmH20 —ABG
Fig. 3 Experimentaltimeline: Following instrumentation, lung injury, and thoracotomy, PEEP titrations were \incrementally increased by 3 cmH2O until 18 cmH2O was reached. Arterialblood gas (ABG) and in vivo microscopy at inspiration and expiration was recorded after a 5-min equilibration
maintaining a relatively normal PaO2; however, the alveoli collapse during expiration. The linear improvement in PaO2 without a corresponding increase in alveolar stability suggests persistent alveolar instability, and the potential to expose the lung to occult VILI exists and may silently progress to clinical ARDS.
Our data and others demonstrate that perhaps the most widely used marker for lung injury [PaO2] is insensitive to detect alveolar instability. Baumgardner et al. used a high-speed intravascular PaO2 sensor in a saline lavage ARDS model and found that PaO2 fluctuated within the respiratory cycle [18]. They postulated that PaO2 rose during inflation when the alveoli were open and fell (during exhalation) when the alveoli collapsed [18]. Using a fiber optic oxygen sensor that detects rapid PaO2 changes, For-menti and colleagues documented PaO2 fluctuations between 37 and 375 mmHg between the I and E cycles as a result of cyclical atelectasis [19]. Caltabeloti et al. have shown, using ultrasound, that lung aeration decreases during fluid loading without any deterioration in PaO2. These data demonstrate that although oxygenation improves, alveolar R/D-induced VILI may persist but cannot be identified by standard clinical measurements (i.e., PaO2). Therefore, if solely guided by PaO2, ventilator adjustments may aggravate alveolar instability, particularly when lung injury is evolving secondary to volume resuscitation and a progressing systemic inflammatory response syndrome (SIRS) [20]. Furthermore, uncontrolled R/D increases lung inflammatory response and may propagate other organ dysfunctions and multisystem organ failure [21]. This potentially explains the dichotomy of results in the ARDSnet trial (i.e., improved oxygenation in the high Vt/end-inspiratory pressure group, yet an increase in mortality) [22]. The low tidal volume strategy with lower end-inspiratory pressure may have resulted in a greater regional lung collapse and lower oxygenation; but because these regions remain
collapsed throughout the breathing cycle, they are protected from tidal R/D, resulting in less alveolar instability rather than overdistension (Fig. 2) [23].
Although recruitment maneuvers (RM) were not used in this study, previous work from this lab using in vivo microscopy demonstrated that the alveoli open following an RM but remain unstable unless combined with sufficient amounts of PEEP to maintain alveolar patency [24]. Oxygenation significantly improves following RMs despite persistent alveolar R/D, suggesting that unstable alveoli participate in oxygenation during the portion of the ventilatory cycle in which they are open [11]. RMs improve oxygenation but have not demonstrated a mortality benefit [25, 26] supporting our postulate that despite improved PaO2, alveolar instability may persist causing progressive lung injury. Nontraditional approaches to MV such as high-frequency oscillatory ventilation (HFOV) use similar goals of PaO2 or SpO2 to guide adjustment of ventilator settings. Two recent trials used oxygenation triggers to adjust Paw and the decision to convert from HFOV back to conventional ventilation [27, 28]. However, experimentally, we have shown that adjusting Paw during HFOV based on PaO2-guided protocols resulted in significantly greater histologic lung injury as compared with maintaining a constant Paw after lung injury [27, 28]. Combined, these data support our hypothesis that PaO2 does not correlate with alveolar stability with enough sensitivity to guide ventilator adjustments and relying solely on oxygenation to make ventilator adjustments could increase alveolar instability and promote occult VILI.
Clinically, these data may be important as discordance between PaO2 and the degree of alveolar instability creates the potential for occult R/D-induced VILI. Robust clinical markers for evaluating alveolar stability are lacking; thus, VILI remains a genuine concern among clinicians who intend to minimize iatrogenic lung injury during MV. In clinical practice, PaO2 or SpO2 is routinely used to guide ventilator adjustments [8]. The commonly used PEEP/FiO2 table derived from the ARDSnet strategy links a PaO2 or SpO2 goal to regulate PEEP and FiO2. Several investigators have suggested that the PEEP/FiO2 scale does not impose a physiologic end-point for clinical or computed tomography-guided evidence of recruitment and alveolar stability [29, 30]. In addition, clinicians frequently underdiagnose ARDS suggesting that acceptable oxygenation may leave many without concern for ongoing lung injury [31]. In this study, all animals had an acceptable P/F ratio based on the PEEP/FiO2 table despite a 25-60 % increase in alveolar instability from baseline. This suggests that achieving clinically acceptable oxygenation goals may not equate with decreased alveolar instability, allowing persistent R/D and the potential for VILI.
Summary
This study has identified the need of detecting alveolar instability and optimizing MV settings to promote alveolar stability and lung homogeneity using methods other than PaO2. Possible methods include the following: (a) electrical impedance tomography (EIT) which provides an assessment of lung volume, PEEP level, and Vt distribution rather than the relationship of Vt to ideal body weight [32-34]; (b) routine evaluation of the respiratory system as a whole with transpulmonary pressure measurement to determine the effect of the chest wall and abdomen on lung mechanics [35-37]; and (c) monitoring the expiratory flow graphics when using modes such as airway pressure
release ventilation (APRV) to control expiratory time constants which has been shown to eliminate alveolar instability [38, 39]. These methods are all currently available and may guide ventilator adjustments rather than relying on the insensitivity of PaO2 and SpO2 or the macro-environment parameter such as Paw [14, 32-39].
The concept that preemptive ventilation strategies may be therapeutic is obverse to the current understanding that MV creates or aggravates lung injury (i.e., VILI). Although both concepts may be accurate, the key may be the method of MV and the timing of application in the pathogenesis of the disease (i.e., early vs. late) [13, 14, 39, 40]. The causal role of MV in progressing acute lung injury (ALI) may be determined by adjustment of ventilator settings to adequately prevent alveolar instability and heterogeneity. If adjusted properly, the ventilator may be used to halt the progression of ALI pathogenesis and reduce the incidence of ARDS [12-14, 16, 39, 40].
Critique of the model
While we speculate that the steady increase observed in PaO2 without a marked change in alveolar stability at PEEP levels of >9 cmH2O was likely due to increased alveolar recruitment, this recruitment was not confirmed by direct measurement. Also, our in vivo microscope has limitations such as the shallow depth of field (70 |im), limiting observations of alveolar mechanics to only two dimensions. We used gentle suction (<5 cmH2O) to hold lung tissue in place underneath the glass coverslip in all experimental settings standardizing this artifact, which has been shown previously to have minimal effect on alveolar mechanics [41].
Conclusions
Our data suggest that oxygenation (PaO2) may be a poor marker for alveolar stability and occult VILI may exist despite meeting acceptable clinical criteria. Further, using PaO2 to guide titration of MV settings (PEEP and Pplat) may result in increased alveolar instability and increase the potential for VILI. New methods to identify alveolar stability are needed for clinical assessment and protection from occult VILI. In combination with judicious use of MV, the goal of eliminating VILI in the critical care population may eventually be realized.
Competing interests
The authors declare that they have no competing interests. Authors' contributions
PLA and NMH had full access to all of the data in the study and took responsibility for the integrity of the data and the accuracy of the data analysis. PLA, BS, MK-S, JS, SR, KS, LAG, GFN, and NMH contributed substantially to the study design, data analysis and interpretation, and the writing of the manuscript. All authors read and approved the final manuscript.
Acknowledgements
Funding for this work was provided by the National Institutes of Health grant R33HL089076. Author details
1Department of Surgery, SUNY Upstate Medical University, 750 East Adams Street, Syracuse, NY 13210, USA. 2Department of Critical Care, R Adams Cowley Shock Trauma Center, Baltimore, MD, USA. 3Department of Biology, SUNY Cortland, Cortland, NY, USA.
Received: 12 February 2015 Accepted: 23 May 2015 Published online: 09 June 2015
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