Ventilator-induced lung injury and lung mechanics
Review Article

Ventilator-induced lung injury and lung mechanics

Jason H. T. Bates1, Bradford J. Smith2

1Department of Medicine, University of Vermont Larner College of Medicine, Burlington, VT, USA; 2Department of Bioengineering, University of Colorado Denver, Anschutz Medical Campus, Aurora, CO, USA

Contributions: (I) Conception and design: JH Bates; (II) Administrative support: None; (III) Provision of study materials or patients: None; (IV) Collection and assembly of data: None; (V) Data analysis and interpretation: None; (VI) Manuscript writing: All authors; (VII) Final approval of manuscript: All authors.

Correspondence to: Dr. Jason H. T. Bates. Department of Medicine, University of Vermont College of Medicine, 149 Beaumont Avenue, Burlington, VT 05405-0075, USA. Email: jason.h.bates@uvm.edu.

Abstract: Mechanical ventilation applies physical stresses to the tissues of the lung and thus may give rise to ventilator-induced lung injury (VILI), particular in patients with acute respiratory distress syndrome (ARDS). The most dire consequences of VILI result from injury to the blood-gas barrier. This allows plasma-derived fluid and proteins to leak into the airspaces where they flood some alveolar regions, while interfering with the functioning of pulmonary surfactant in those regions that remain open. These effects are reflected in commensurately increased values of dynamic lung elastance (EL), a quantity that in principle is readily measured at the bedside. Recent mathematical/computational modeling studies have shown that the way in which EL varies as a function of both time and positive end-expiratory pressure (PEEP) reflects the nature and degree of lung injury, and can even be used to infer the separate contributions of volutrauma and atelectrauma to VILI. Interrogating such models for minimally injurious regimens of mechanical ventilation that apply to a particular lung may thus lead to personalized approaches to the ventilatory management of ARDS.

Keywords: Over-distension; recruitment and derecruitment; computational model; surfactant function; acute respiratory distress syndrome (ARDS)


Submitted Mar 06, 2018. Accepted for publication Jun 11, 2018.

doi: 10.21037/atm.2018.06.29


Introduction

Ventilator-induced lung injury (VILI) represents an ever-present danger for patients in respiratory failure, particular those with acute respiratory distress syndrome (ARDS) (1-3). This danger arises from the fact that mechanical ventilation is, first and foremost, a mechanical event; whereas the normal healthy lung is well able to stand the stresses and strains imposed by mechanical ventilation, it can mean irreparable and eventually fatal further damage for the already injured lung. Such an unfortunate outcome, however, follows not only from the reduced physical durability of the injured lung as a result of some infectious or chemical insult. Lung injury is invariably accompanied by alterations in the mechanical properties of the lung itself (4-6). Consequently, the microscale stresses applied to the parenchyma during ventilation of the injured lung are frequently greatly elevated compared to those experienced by the normal lung (7,8), with commensurate consequences for tissue integrity and the biologic processes that are invoked in the face of injury.

By the same token, altered lung mechanics can be highly indicative of, and indeed specific to, the nature and degree of lung injury (4). This means that ongoing monitoring of lung mechanical function during mechanical ventilation has the potential to warn caregivers of impending VILI, and even to serve as the feedback signal by which ventilation can be regulated so as to minimize VILI progression while continuing to provide life support (9). In order to serve such a function, however, it is necessary to have an understanding of the link between the stresses and strains of mechanical ventilation, reflected in measurable pressures and flows at the airway opening, and the underlying VILI mechanisms. Accordingly, the goal of this review is to bring these factors together in a way that provides a unifying framework for potentially optimizing the use of mechanical ventilation in managing the injured lung.


Alterations of lung mechanics in VILI

The lung is, by functional necessity, a readily deformable structure that expands to transport air along a branching airway system from the narrow tracheal opening to the enormous surface area of the blood-gas barrier. In so doing, the pressures generated to produce inspiration must overcome the flow resistance of the airway tree and the viscoelastic recoil of the parenchymal tissue and chest wall. A significant component of this recoil arises a consequence of surface tension forces at the alveolar air-liquid interface (10). The balance of forces involved is conventionally written in terms of a simple equation of motion based on the notion that, on the macroscale, the lung behaves like a single compartment:

where P(t) is driving pressure relative to that at functional residual capacity (FRC), is flow at the tracheal opening, V(t) is lung volume relative to FRC, RL is lung resistance (which includes both airway and tissue resistances), and EL is lung elastance (the inverse of lung compliance). The lung is, of course, vastly more complicated than this. Nevertheless, the simple model expressed by Eq. [1] captures much of its overall dynamic mechanical behavior during both normal spontaneous respiration and mechanical ventilation (11). From the perspective of lung mechanics, the most important consequences of VILI are reflected in its effects on EL, which is a measure of the elastic stiffness of the lung parenchyma. It must be remembered, however, that the tissues of the lung are highly viscoelastic, which means that a substantial (if not the major) component of RL arises from viscous dissipation of energy within the tissues of the respiratory system as opposed to streams of gas flowing along airway conduits (11).

There are a variety of microscale structures that contribute to the determination of organ-scale EL, and that can become altered in acute lung injury. One is the network of extracellular matrix proteins (mostly collagen and elastin) depicted in Figure 1, which provide the parenchyma with its structural integrity (12,13) and which can become stiffened as a result of the fibroproliferation that is a common sequellum of ARDS (14-16). This network occupies the interstitium of the blood-gas barrier, which is located between the endothelial and epithelial cell layers that provide most of the barrier function separating blood from the alveolar airspace. Also in this interstitial space are various cell types and fluid. Expansion of the fluid volume is a ubiquitous occurrence in the injured lung because blood plasma, often with associated plasma proteins, moves across the leaky endothelium to produce interstitial pulmonary edema (17). The resulting congestion of the interstitial space can lead to a stiffening of the parenchyma, and thus an elevation in EL, but studies of experimental hydrostatic edema have shown that this elevation, while certainly measureable, is relatively modest in clinical terms (18).

Figure 1 Scanning electron micrograph of the collagen fiber network in a rat lung (A) showing the alveolar entrances (AE) and helical collagen structure characteristic of low inflation levels. The elastic fibers network (B) crisscross at the point where three alveolar entrances (*) meet and are sparse in the alveolar septa. Reproduced with permission from Toshima et al. (12).

By far the most severe mechanical consequences of acute lung injury occur when edematous material arising from the vasculature breaches the epithelial barrier and accumulates in the airspaces. This potentially has two key consequences. One is simple displacement of air, which effectively reduces lung volume and so increases EL accordingly (19). The more important consequence, however, occurs when the edematous material interferes with the functioning of pulmonary surfactant in the aerated regions, which is readily accomplished by the plasma proteins via their competition at the air-liquid interface with surfactant (20-22). The resulting elevation in surface tension can dramatically increase EL and thus the pressure required to ventilate the lung. Elevated surface tension can also prevent inspiratory pressures from prying apart the walls of alveoli and airways that have come into apposition at the end of expiration (atelectasis) (23) or from eliminating plugs of fluid that have formed to occlude small airways (24-26). Lung regions that are isolated from ventilation in this way are said to be derecruited, and are thus unable to take part in gas exchange. Increased surface tension due to accumulation of plasma fluid and proteins thus increases EL both by causing derecruitment of lung units and by increasing the intrinsic stiffness of those units that remain open. The result is that the effective volume of the lung is reduced, so ventilation is delivered to what has been termed a ‘baby lung’ (19). The most important of these two effects, however, appears to be derecruitment, perhaps because lung injury is a heterogeneous process in which derecruitment occurs in those regions where surface tension is elevated while other regions are relatively spared.

The importance of derecruitment for ARDS and VILI is unequivocal, but what to do about it remains controversial. On the one hand, reversing derecruitment by applying larger inflation pressures to the lung would seem to make sense because this would increase the gas exchanging capacity of the lungs (4,27-29). On the other hand, increased inflation pressures have clear potential to cause physical damage to the lung tissues, particularly when the lung is already injured. Indeed, in some severely injured lungs, the regions that are derecruited, or flooded with edema, may be so recalcitrant to being reopened (30) that their recruitment would require pressures sufficient to cause immediate pneumothorax. Whether to try to recruit collapsed lung—the so-called “open lung approach”—or leave it derecruited is thus a key question that continues to vex the clinical community (31). Promising results with the open-lung approach in animal models have been obtained [e.g., (32)], but recent studies in patients have been inconclusive (33,34). It thus remains a puzzle as to why a strategy that appears to be based on such sound physiological principles should not be resoundingly successful in the clinic. Addressing this question begins with an understanding of the physical factors that determine recruitment and derecruitment.

The first-order view of recruitment and derecruitment is that they are functions of pressure (35-37). That is, a particular region of the lung, when closed, has a pressure, Po, above which it will open. Conversely, the same unit, when open, has a pressure, Pc, below which it will close. It is generally accepted that Pc < Po, implying there is a region of pressure, Pc < P < Po, within which closed lung will not open and open lung will not close. A distribution of values for PO and Pc throughout the lungs means that recruitment and derecruitment are continuous processes over some range of P (38,39). This gives rise to the notion that the pressures of mechanical ventilation should strive to exceed most of this range, or at least to exceed the range of values of Pc once the lung has been maximally recruited by a deep inflation (DI). This is not always possible since the ranges of Po and Pc may exceed pressures that can be safely applied, quite apart from the difficulties of reliably determining where these ranges lie for a given lung. Nevertheless, motivated by this notion, various strategies for identifying the “best positive end expiratory pressure (PEEP)” for a given injured lung have been devised based on analyses of measured pressure-volume relationships (40-43) or assessments of lung aeration from CT images (44,45). Such strategies have led to improvements in oxygenation, but the Holy Grail of reduced mortality has so far remained elusive (46).

One of the reasons why the clinical management of recruitment and derecruitment has been challenging may be that these phenomena are not, in fact, simply functions of pressure. They are also functions of time. In other words, once the pressure in a region of open lung descends to a level at which it may close, derecruitment does not happen instantaneously but rather manifests over some finite period of time. The reasons for this time dependence are complex in their intricate details but, broadly speaking, derecruitment involves fluid movement at the micro level. For example, the liquid layer coating the walls of a small airway is transported axially by a surface-tension induced Rayleigh-Plateau instability (47) into annular rings that eventually neck inward to occlude the airway lumen and draw the airway walls inward and expand the collapse region (48-52). Likewise, fluid displaced from a filled alveolus by inspired air takes time to flow back into and refill the alveolus once again. The processes involved in recruitment of closed lung units, which are roughly the reverse of those just described, also take time to manifest once pressures rise above the threshold at which recruitment can potentially occur. In vitro experiments and computational fluid dynamics have shown that the rates at which these processes take place are described by the dimensionless capillary number Ca = µU/γ that represents the balance between the viscosity of the lining fluid (µ), the surface tension at the air-liquid interface (γ), and the velocity (U) of a finger of air as it propagates along a collapsed tube (53-56). At the low Ca characteristic of the small airways and alveoli the surface tension forces dominate and viscous effects play a relatively minor role in the dynamics of recruitment and derecruitment.

The dynamic nature of recruitment and derecruitment means that the benefits of a recruitment maneuver are transient (27). The immediate benefits of recruiting the lung with a DI are evident in the reduction in EL that ensues. During a subsequent period of regular ventilation at a modest tidal volume, however, EL will gradually rise toward an elevated plateau. The level of this plateau and the rate at which it is approached are modest in a normal lung, but both can be dramatic in severe lung injury. In the latter case, studies using in vivo microscopy (57), lung stereology (58), and micro-CT in experimental animals (28) have shown that post-DI changes in EL correlate strongly and inversely with the fraction of open lung, while measurements of oxygenation support a similar conclusion in human subjects (59). It is not clear that derecruitment entirely explains the post-DI rise in EL in normal lungs, since this may also be due to transient changes in the distribution of surfactant and its surface tension lowering effects, or the gradual folding of alveolar septa (60), but the effect in this case is modest and thus unlikely to be of clinical importance. In any case, understanding the dynamics of recruitment and derecruitment is crucial for accurately predicting the long-term consequences of a given ventilation strategy, particularly if it involves recruitment maneuvers (61). The issue to be addressed regarding the use of recruitment maneuvers is thus not “if”, but “how often”.

Acute lung injury is invariably accompanied by increases in EL, which means that mechanical ventilation with a given minute ventilation results in commensurately increased stresses exerted on the parenchymal tissues. In other words, the same volume of inspired air is forced into an effectively smaller ‘baby lung’ (19), which leads to increased distension of the septal walls. This places the injured lung in danger of succumbing to a positive feedback cycle in which these elevated tissue stresses cause VILI, which worsens the stresses, which then accelerates the rate of injury development in a vicious cycle that is often ultimately fatal (62). There are currently no medical treatments for mitigating either the endothelial or epithelial leak that characterizes VILI, so the primary goal in managing the injured lung must be to ventilate in a way that minimizes VILI development in the hope that the patient’s own reparative machinery will prevail. Since EL is so dramatically affected by lung injury and its recruitment status, understanding what we can learn about VILI mechanisms from the way that EL changes over time in any given patient is crucial for designing optimal management strategies.

Making the most of EL as a marker of VILI requires some kind of mathematical model that allows it to be related in a quantitative fashion to relevant physiological mechanisms. At perhaps the simplest level, the amount of lung volume loss resulting from derecruitment can be equated inversely to the observed increase in EL (63). Exploiting this idea has led to a model of recruitment and derecruitment dynamics in which opening and closing of airspaces take place when pressure exceeds or falls below specified critical values, but with time delays that are accounted for using an empirical construct termed a virtual trajectory (37,38,61,64,65). Although not originally designed to represent any physical mechanism in particular, virtual trajectories are nevertheless reminiscent of the way that fluid plugs move along airways under the influence of an applied pressure until they have deposited enough of their material on the airway wall to finally disintegrate (25,66). In any case, models of distributions of airspaces built around this idea have been shown to describe experimental data rather accurately, and in particular to support the notion that increasing surface tension is the preeminent mechanical consequence of severe acute lung injury (38). Combined with representations of nonlinear tissue elasticity encompassing the idea of an injury threshold for overdistension, mathematical models appear to be usefully predictive of the relative contributions of volutrauma and atelectrauma in VILI (9,61).


Mechanisms of VILI

EL not only provides a means of monitoring the injury status of the lungs, it also mediates the generation of VILI by modulating the potentially injurious stresses and strains that are applied to the lung parenchymal tissues during mechanical ventilation. There are two apparently distinct biomechanical mechanisms by which these phenomena can cause VILI, known respectively as volutrauma and atelectrauma.

Volutrauma refers to the tissue damage caused by the excessive stretching of tissues that occurs when the lung is over-inflated, a concept that makes intuitive sense given that even an organ as expansile as the lung has a threshold volume above which structural failure ensues (67-71). Importantly, it is not high pressures per se that causes this type of injury, even though high pressures are required to produce large inflation volumes; experiments with chest strapping have demonstrated that VILI is reduced when high pressures are prevented from causing inflation, which is why the term barotrauma is no longer used in this context (69). The clinical success of protective ventilation strategies based on the use of low tidal volume (72) would seem to bear these ideas out.

Atelectrauma refers to the injury caused by the repetitive re-opening of closed lung units, something that can happen if regions of the lung become derecruited with each expiration and then recruited again during the next inspiration (5,65,73). Injury from atelectrauma is commonly ascribed to shear forces, which are those operating tangentially to the epithelium (i.e., in the axial direction relative to the airway) as apposed surfaces are peeled apart. However, in vitro studies (55,56,74) supported by detailed computational modeling (23,54,75-82) suggest that the culprit forces actually act normally to the surface (i.e., radial to the airway) and that cell injury is caused by the large axial gradient in these normal forces that occurs during the passage of the air-liquid interface (56) as depicted in Figure 2. Interestingly, injury and pressure gradients are more severe as the advancing air-liquid interface moves more slowly due to thinning of the residual fluid film left on the airway wall. In any case, it is clear that movement of high surface tension air-liquid interfaces over epithelial surfaces is highly damaging (77,83), and indeed can cause cellular necrosis after only a small number of passages.

Figure 2 Hypothetical fluid-mechanical stress (red arrows) during the reopening of a collapsed, fluid-occluded (blue) airway as the air-liquid interface moves from left to right. The stress at the airway wall is applied to the epithelial lining (green insets) causing cell death. Adapted with permission from Bilek et al. (55).

A substantial amount of research in animal models of VILI during the 80s and 90s showed that VILI is accompanied by disruption of both the epithelial and endothelial barriers, and is correlated with the amount of pulmonary edema the accumulates as a result (69,84-86). Much of this earlier work focused on the role of over-distension, the importance of atelectrauma only becoming fully apparent somewhat later. In this regard, work from our laboratory in recent years has shown that initially normal mice do not develop VILI within 4 hours from over-ventilation alone; the animals either maintain normal lung function or, if tidal volume is excessive, succumb to a sudden pneumothorax (5,87). They also do not develop VILI when ventilated at zero PEEP provided tidal volume is also modest. Progressive VILI only develops when the mice are ventilated at zero PEEP simultaneously with a very large tidal volume (5). This combination of inspiratory and expiratory pressures leads to widespread disruption of the blood-gas barrier (Figure 3) and a progressive degeneration of lung mechanical function (65) due to accumulation of proteinaceous edema in the airspaces (87). In fact, under these conditions the rate of VILI development can be conveniently titrated by choice of tidal volume (65). Once VILI is underway, however, it continues to progress when ventilation is switched to either zero PEEP or high tidal volume alone (5), demonstrating that what is safe for the healthy lung may not be safe for a lung that is already injured.

Figure 3 Scanning electron micrograph depicting an undamaged alveolar surface (right panel) and fragmented alveolar epithelium (left panel) caused by two hours of ventilation at high tidal volumes and zero end expiratory pressure. Reproduced with permission from Hamlington et al. (88).

There thus appears to be a complex relationship between over-distension, recruitment, and existing injury that determines whether a given mode of mechanical ventilation will further injure a given lung. Exactly what this relationship is remains a matter of ongoing research, but a specific question that arises in this context is why atelectrauma and volutrauma appear to be synergistic in the production of VILI in the normal lung. One possibility involves the role of so-called “stress concentrators”, which arise when an atelectatic region of the lung borders on a region of normal parenchyma (7,13,89,90). Because the atelectatic region is unable to receive any of the applied ventilation, so long as it remains derecruited, the adjacent normal region is at risk of being over-distended. In particular, at the border of these two regions the alveolar walls are stretched to an exaggerated degree by being constrained to adhere to the region of non-expansile atelectasis as illustrated in Figure 4. Strain and stress are thus concentrated in these alveolar walls, making them particularly susceptible to mechanical failure. Such failure, even at isolated locations throughout the lung, is sufficient to instigate the process of alveolar leak from the vasculature that starts the inexorable march toward full-blown VILI. Of course, this explanation requires the presence of some small degree of alveolar leak to begin the process, but this might be caused by levels of over-distension and repetitive recruitment that do not themselves lead to measurable changes in overall lung function (i.e., in EL). Stress concentrators, being inherently heterogeneous in nature, may also be more likely to exist in animals larger than mice and in humans where the effects of the gravitational gradient on regional differences in lung mechanics are more pronounced (91).

Figure 4 The collapse or flooding of an alveolus (blue) leads to increased distension of the adjacent septa (red).

Another possible explanation for volutrauma-atelectrauma synergy is suggested by our recent study of how VILI affects the size of the leak in the blood-gas barrier. By injecting three different sizes of fluorescently-labelled dextran molecules into mice having varying degrees of VILI and then observing the appearance of each molecule in bronchoalveolar lavage fluid (BALF) (Figure 5), we determined that the holes in the blood-gas barrier appear to follow a power-law distribution (92). That is, there are a large number of very small holes, a small number of large holes, and the intermediate sized holes number such that the histogram of hole sizes is approximately linear in a log-log plot. The significance of this finding lies in the fact that it can potentially be explained by a rich-get-richer mechanism. That is, whereby VILI begins with the generation of small holes, and this initial injury then progresses by the enlargement of these holes in a way that favors holes that are already large (e.g., large holes might correspond to weaker than average areas of the barrier that are particularly susceptible to becoming perforated). Taking this idea a step further leads to the notion that repetitive recruitment might be responsible for the initial creation of holes in the barrier because of its direct action on the epithelium, while subsequent hole enlargement is caused by over-distension. This theory (92) can only be considered speculative at present, but it offers a convenient explanation for why volutrauma and atelectrauma are required together to produce significant VILI, why volutrauma alone is able to exacerbate existing VILI, and why VILI is so difficult to deal with once it is underway. It also potentially explains recent exciting results using preemptive airway pressure release ventilation (APRV) in a large animal model of sepsis (57,93-96) showing that VILI is avoided provided that the duration of pressure release employed is extremely short (a small fraction of a second). The reason may be that this does not allow sufficient time during expiration for any airspaces to actually close (61), thereby eliminating the possibility for atelectrauma to occur. The result is maintenance of an intact alveolar epithelium and avoidance of airway edema despite severe septic shock in the rest of the animal (97). APRV applied in a similar manner in human patients is also showing promise as a means of avoiding the worst ravages of VILI in ARDS (98).

Figure 5 Permeability of the blood-gas barrier (ratio of fluorescent label in BALF versus serum) for three different sized dextran molecules following intravenous injection in mice. Control animals were not subjected to mechanical ventilation and ventilated animals received pressure-controlled ventilation with an end-inspiratory plateau pressure of 37.5 cmH2O. The ZEEP/Short group was ventilated with zero end-expiratory pressure for approximately 30 min. The ZEEP/Mid group was ventilated with zero PEEP for approximately 60 min. The PEEP3 group was ventilated with a positive end-expiratory pressure of 3 cmH2O for approximately 120 min. The ZEEP/2xH group was ventilated with zero PEEP until lung stiffness (H) had risen to twice its baseline value. Used with permission from Hamlington et al. (92).

Another important consideration is where the leak manifests in the blood-gas barrier. Computational modeling of a sheet of cells stitched together by tight junctions shows that the total area of leak that develops as the sheet is stretched is similar to the way that lung function worsens when failure occurs at the cell-cell junctions (99). On the other hand, extensive ultrastructural studies of the blood-gas barrier in animal models of VILI have revealed denudation and blebs in the endothelial and epithelial surfaces, indicating damage to the cells themselves (69,84,100-103). Such damage of the alveolar epithelial surface by high tidal volume ventilation at zero end-expiratory pressure is shown in Figure 3. Wherever these leaks occur, however, they are also presumably capable of being repaired to some extent; not all patients with ARDS and/or VILI die, so recovery from damage must be possible in some cases. It has been shown, for example, that tears in the cell membrane can spontaneously re-anneal in a matter of minutes (104). More profound injury involving cellular necrosis requires that Type II alveolar epithelial cells transdifferentiate to replace Type I epithelial cells and this process occurs over a much longer timescale (105) but is still well within the body’s reparative repertoire.

Finally, VILI has longer-term consequences than simply physical damage to and repair of the components of the blood-gas barrier. The upregulation of inflammatory mediators as a result of this damage can be extensive when injury is widespread and severe (106-111), and can itself have adverse downstream consequences for other parts of the body. Indeed, multi-organ failure resulting from an overwhelming inflammatory response of this nature, known as biotrauma (112), is frequently the ultimate cause of death in ARDS (16).


Mechanics-guided minimization of VILI

The current standard of care for mechanical ventilation in ARDS, derived from the landmark ARDSnet trial in 2000 (2), is essentially an exercise in open-loop control. That is, it employs the one-size-fits-all strategy of striving for a tidal volume of 6 mL/kg ideal body weight in all patients (72). Strong cases can be made for the consideration of other factors that have obvious and strong physiologic rationales, such as choice of PEEP and use of recruitment maneuvers. High-frequency oscillatory ventilation (113-116), variable tidal volume ventilation (117-121), or even liquid ventilation (122-124) have also been investigated extensively, all seemingly based on sound physiologic principles. Despite some positive effects on some physiologic outcomes such as oxygen, however, none has so far demonstrated a benefit in terms of the all-important outcome of reduced mortality. So-called protective (low-tidal volume) ventilation, along with the recent addition of prone positioning (125), thus continues to constitute the rather meagre underpinnings of evidence-based medicine in the management of ARDS. There nevertheless remains a general sentiment in the field that we can do better than this, particularly since the current ARDS mortality rate is still alarmingly high despite marked improvements over the past couple of decades.

One possible explanation for the failure of so many clinical trials of apparently well-founded approaches to ARDS management is the heterogeneity of the condition. ARDS patients vary greatly in the severity and regional distribution of their lung injury (126), the effectiveness with which recruitment maneuvers open collapsed regions of the lung (30), and the ease with which they can be oxygenated. It would seem somewhat obvious that this should be countered with management strategies that are tailored to the specific needs of the individual patient. These needs would have to be measured in each patient, of course, and then used to guide individualized treatment in a closed-loop paradigm. In fact, this is not a new idea, being best exemplified by attempts to determine optimal PEEP in a given patient from measurements of their lung pressure-volume relationships (127,128).

We recently generalized the concept of closed-loop control of mechanical ventilation of the injured lung by investigating some simple candidate injury cost functions with which to define the degree of VILI produced by a given regimen of mechanical ventilation (9). Figure 6 shows a predicted injury cost function based on the product of volutrauma and atelectrauma occurring during the respiratory cycle. Also shown are the positions of experimentally investigated combinations of tidal volume and PEEP that were shown to vary in their capacities to produce VILI in initially healthy mice. The injurious combinations are shown by black X’s while the safe combinations are indicated by white circles. These cost functions were defined in terms of a predictive mathematical model of the lung that estimates both tissue over-distension and repetitive recruitment based on applied pressures and flows. We have taken a similar approach in estimating intra-tidal recruitment and tissue distension from ongoing measurements of airway pressures and flow measured during specialized maneuvers designed to reveal these two phenomena at work (63). Specifically, observing how pressure increases as lung volume is raised to high levels reveals information about the volume-dependence of EL, which in turn can be related to putative thresholds of over-distension above which injury starts to occur. Conversely, observing how EL varies throughout the respiratory cycle reveals the extent to which recruitment of lung units may be occurring with each ventilated breath (129). A convenient way of gaining both types of information simultaneously is provided by the relationships between pressure, volume, and flow observed during variable tidal volume ventilation, since here both the time and amplitude dependence of the lung is being interrogated on an ongoing basis (130). Although this approach awaits clinical validation, in principle brief periods of variable tidal volume ventilation can be used to parameterize numerical models that are then used to predict the amount of volutrauma and atelectrauma generated during other forms of mechanical ventilation so as to determine which may be least injurious.

Figure 6 Predicted lung injury cost function for an initially healthy mouse consisting of the product of volutrauma and atelectrauma. Black ‘X’ indicates in vivo experiments that produced lung injury, white circles demarcate in vivo experiments that were non-injurious. The white line describes a ‘safe region’ of ventilation. Adapted from Hamlington et al. (92).

Conclusions

Lung mechanics reflected in EL and its changes over time contain much useful information about the injury status of the lung, particular when measurements are made in association with maneuvers that interrogate the behavior of the mechanical lung over sufficiently wide ranges of amplitude and time. These measurements afford the opportunity, in principle, to identify mechanical models of the lung that embody the essential mechanisms responsible for volutrauma and atelectrauma. Such models can then be used as virtual laboratories within which searches for optimal ventilation strategies can be made, opening the way to a rationalized approach to personalized management of ARDS.


Acknowledgements

Funding: This work was supported by the National Institutes of Health [grant numbers HL-124052 and R00 HL128944].


Footnote

Conflicts of Interest: JH Bates is a member of the Advisory Board of and a minor shareholder in Oscillavent. BJ Smith has no conflicts of interest to declare.

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Cite this article as: Bates JH, Smith BJ. Ventilator-induced lung injury and lung mechanics. Ann Transl Med 2018;6(19):378. doi: 10.21037/atm.2018.06.29