Authors: Syeda Farheen Zaidi, Asim Shaikh, Daniyal Aziz Khan, Salim Surani, Iqbal Ratnani
Categories: Minireviews, Acute respiratory distress syndrome, Driving pressure, Mechanical ventilation, Mortality, Positive end-expiratory pressure, Ventilator induced lung injury
Source: World Journal of Critical Care Medicine
Authors: Syeda Farheen Zaidi, Asim Shaikh, Daniyal Aziz Khan, Salim Surani, Iqbal Ratnani
Driving pressure (∆P) is a core therapeutic component of mechanical ventilation (MV). Varying levels of ∆P have been employed during MV depending on the type of underlying pathology and severity of injury. However, ∆P levels have also been shown to closely impact hard endpoints such as mortality. Considering this, conducting an in-depth review of ∆P as a unique, outcome-impacting therapeutic modality is extremely important. There is a need to understand the subtleties involved in making sure ∆P levels are optimized to enhance outcomes and minimize harm. We performed this narrative review to further explore the various uses of ∆P, the different parameters that can affect its use, and how outcomes vary in different patient populations at different pressure levels. To better utilize ∆P in MV-requiring patients, additional large-scale clinical studies are needed.
Core Tip: Driving pressures (∆P) of < 15 have demonstrated the greatest benefit in mortality. It is most utilized in patients with acute respiratory distress syndrome (ARDS). Some large-scale randomized controlled trials are currently underway; their results will dictate the outcomes of certain ∆Ps under specialized conditions, such as the feasibility of reducing ∆P in ARDS patients on mechanical ventilation and the impact of lateral positioning on ∆P. It is clear, however, that careful implementation of ∆Ps can greatly improve outcomes.
Driving pressure (∆P) is a fundamental element in mechanical ventilation. Its primary function is to overcome the elastic forces of the pulmonary system. It is derived from the difference between end-inspiratory airway pressure, commonly known as the plateau pressure (Pplat), and positive end-expiratory pressure (PEEP) in the absence of spontaneous respiration[1-4].
∆P is derived from the ventilator and serves as a function of respiratory compliance and tidal volume. It reflects the pressure difference within a singular breath and is one of the major parameters implicated in lung stress[5,6]. Recent studies have shown a plausible association between ∆P and improved survival in patients with acute respiratory distress syndrome (ARDS)[5,7-13]. Even though it is commonly used across critical care centers around the globe, it is a measure that requires further introspection to harness its predictive potential and guide safe and effective ventilation.
This review article discusses the dynamics of mechanical ventilation and explores the role of ∆P, its significance in recent studies, and the resulting implications for future research.
Mechanical ventilation allows gas exchange and attenuates increased work of breathing in the setting of an acute compromise of the respiratory system. The mechanics are expressed through indices such as pressure, flow, volume, resistance, work of breathing, and compliance, which directly influence lung volumes, functional residual capacity, and the resulting gas exchange[5].
Physiologically, the respiratory circuit works as a negative pressure system. On inspiration, the diaphragm is pushed down, and negative pleural cavity pressure is generated. A net negative pressure in the airway serves as a suction for air to be brought into the lungs. The negative pressure then, in turn, decreases the right atrial pressure and generates a similar suction effect in the inferior vena cava, which results in an increase in venous return[14].
During mechanical ventilation, however, this physiology is altered, and a positive pressure is transmitted into the pulmonary system instead. This leads to a more positive pressure in the pleural space and less of that suction effect. This positive pressure is also exerted on the right atrium, which leads to a decrease in venous return and preload. The net impact is a reduced cardiac output due to the underfilling of blood in the left heart and low mean arterial pressures[15]. An understanding of the effects of artificial ventilation is important to guide management in patients and adjust for the consequences.
The baby lung concept was coined by Gattinoni and Pesenti[16] after they observed computed tomography scans of patients with ARDS or acute lung injury. They noticed that the total aerated lung tissue of these patients held dimensions of 300-550 g, similar to a 5-6-year-old child. They proposed that the ARDS lung is not stiff but, in fact, functionally small-suggesting that the elasticity of the lung is most likely intact and that the lung tissue may change dimensions after recruitment maneuvers such as prone positioning. They highlighted that gentle lung treatment should thus be employed to avoid baro-volutrauma inflicted by standard aggressive resuscitative strategies. This theory has gained traction as further research on ARDS has supported their findings, and the discovery and application of ∆P in research has improved outcomes[17]. In general, a tailored approach to ventilation is required to match a patient’s variable physiology to reduce the chances of ventilator-induced lung injury (VILI).
The forces that impede ventilation include non-elastic or respiratory system resistance, which occurs when gas flows within the airway circuit, and elastic resistance, which occurs in the absence of gas flow in the circuit[18]. Examples of non-elastic resistance include frictional resistance to gas flow, viscoelastic resistance from the deformation of thoracic tissues, and finally, the inertia of gas flow and tissue movement[18]. While small levels of impedance do not always mean underventilation of lung tissues, higher levels of impedance require higher ∆Ps for effective ventilation. These forms of resistance can be reflected in the *(*Resistance R = Δ pressure/flow).
The elastic resistance comprises of resistance exerted by the chest wall and lung tissue, along with resistance exerted by the surface forces at the alveolar gas-liquid interface. The elastic resistance can be used to derive total compliance of the lung and the chest wall[18]. These forms of resistance can be represented by the following (Compliance Crs = Δ volume/Δ pressure), [Elastance (EL) ELrs = Δ pressure/Δ volume = 1/C].
As a rule, high levels of compliance, and therefore lower levels of EL, allow for less effective mechanical ventilation at lower ∆Ps. Hence, in certain conditions that alter these mechanics, such as in emphysema, which leads to higher compliance, increased levels of ∆P are required to maintain adequate levels of ventilation.
Airway pressure is equal to alveolar pressure in the resting state and depicts the pressure generated to overcome the retractive elastic forces of the pulmonary system. It is reflected in the following equation[19,20]; (airway pressure = flow x resistance + alveolar pressure).
Airway pressure dictates the ∆Ps required for adequate ventilation in all patients. Higher alveolar pressures and general airway resistance require increasing levels of ∆P to maintain effective ventilation.
Pplat is the pressure exerted by the ventilator into the alveoli and small airways of the lung. It is calculated during an inspiratory pause of 0.5-1 s on the ventilator when the respiratory muscles are relaxed. This pressure approximates the mean peak alveolar pressure[21,22]. As noted previously, resting high Pplats are incorporated in ∆P calculations in order to identify requirements for overcoming inside pressures.
Transpulmonary pressure (PTP) is the distending pressure of the lungs and is derived by calculating the difference between the pressure within the alveoli (PALV) and the pleural pressure (PPL)[23]. The transpulmonary pressure is described by the following (PTP = PALV - PPL).
∆P is derived from the difference between Pplat and PEEP. It is essentially the pressure required to open the alveolar sacs. Since static lung compliance (Cstat) is derived from the formula; Tidal volume/(Pplat-PEEP), ∆P is derived as an inverse function of respiratory system compliance (Crs). The higher the ∆P, the lower the compliance of the lung and, therefore, an increased risk of volutrauma. Henceforth, ∆P is the foundational pillar of mechanical ventilation. Adequate ∆P levels are needed for effective air delivery to overcome resistances, high inner pressures, and losses during ventilation. It is described by the following equations[24]: (ΔP = Pplat - PEEP), (ΔP = VT/Crs).
Transpulmonary ∆P (ΔPpL) can be defined as the difference between the PTP at end inspiration and end-expiration.
Peak pressure is the maximum recorded pressure at the end of inspiration in the presence of airflow. Peak pressure is dependent on tidal volume, respiratory rate, and airflow[14,20].
Intrinsic peak expiratory pressure reflects the pressure exerted by the residual volume in the lung due to incomplete exhalation. It can be calculated by doing an expiratory pause and measuring the end-expiratory pressure[14].
Lung stress refers to the pressure required to distend the lung against the counterforce exerted by the chest wall. Stress is depicted best by PTP, which is the difference between airway pressure (Paw) and PPL. Its formula is represented by (Paw-PPL).
Despite its high predictability, PTP is not frequently used due to the difficulty of calculation, and Pplat is thus used as an alternative. Pplat is reflective of alveolar pressure when the airflow is zero and is calculated during an inspiratory pause on the ventilator when the respiratory muscles are relaxed.
Lung strain is directly related to lung stress and refers to the change in lung volume when compared to its volume during regular respiration[20,23,25].
Tidal volume is the amount of air exchanged during ventilation at rest and is matched by ideal body weight or approximations based on the patient’s disposition[14]. Tidal volume follows a proportional relationship with ∆P in mechanical ventilation. Higher tidal volumes increase ∆Ps. This can be modified as needed.
PEEP or extrinsic PEEP is the end-expiration pressure that is delivered by mechanical ventilation to prevent the lung from collapsing. It is important to maintain the patency of the small airways and alveoli. This, in turn, increases lymphatic flow and allows adequate drainage of the lung. Therefore, lower levels of PEEP increase ∆Ps.
The rate of ventilation is set to achieve target levels of carbon dioxide according to the patient’s metabolic demands[14]. Respiratory rate is a component of mechanical power (MP) along with ∆P. These levels can be changed depending on ventilation requirements and desired MP metrics.
Mechanical energy (EnergyL) refers to various forms of energy transferred after each ventilatory cycle and can be derived simply through Pplat (ΔPL) and the EL of the lung. It is described in the following formula(s): (EnergyL = ΔPL 2/EL), [(EnergyL = ΔV2 × [(0.5 × ERS + RR × (1 + I:E)/60 × I:E × Raw ) + ΔV × PEEP)].
MP refers to the EnergyL multiplied by the rate of respiration, thus reflecting the EnergyL transferred per minute from artificial ventilation. This value captures both static and dynamic metrics that influence respiration[26]. MP has recently emerged as a novel and promising predictor of VILI. While its incorporation clinically is yet to be widened, it has shown promise. Maintaining lower rates of MP by considering the dynamic metrics it incorporates, can reduce rates of VILI. The formula of MP is reflected as [MP = (EnergyL x RR) or RR W=RR ∫0 VT PawdV∫]
In recent years, the understanding behind VILI has rapidly expanded from a limited perspective of pressures, volumes, and tidal cycles to an understanding of forces and their interplay in periods of stress and strain while being subjected to different forms of energy and power. The value of ∆P has recently gained traction in research and practice due to key findings demonstrating the impact of high ∆Ps, resulting in low compliance and increased risk of volutrauma. Ultimately lead to higher morbidity and mortality in patients requiring artificial ventilation-particularly in cases of ARDS.
A meta-analysis by Amato et al[3] analyzed 9 randomized controlled trials and demonstrated that in intensive care settings, ARDS patients with elevated ∆Ps of 15 cm H2O were positively associated with higher mortality (relative risk, 1.41; 95%CI: 1.31 to 1.51; P < 0.001), (relative risk, 1.36; 95%CI: 1.17 to 1.58; P < 0.001), after every 1 standard increment in ΔP (approximately 7 cm of water). This result was despite the protective range of tidal volumes and Pplat[3]. A ∆P less than 15 cm H2O was considered to be a safe threshold to guide ventilation in ARDS patients and decrease mortality[3]. This study, despite its limitations, provided a significant understanding of the delicate role ∆Ps can play in the management of ARDS and the intricate and precise difference the slightest of modifications can make.
In addition, the large observational cohort study to understand the global impact of Severe Acute Respiratory failure (LUNG-SAFE), a multicenter, international study, was conducted to identify the incidence of ARDS in intensive care units but also to collect information about the associated ventilatory management, therapies, and outcomes. The multivariate analyses concluded that high peak pressures, higher Pplats, high ∆Ps of > 14 cm H2O, and low PEEP were associated with increased mortality in these patients[27].
This notion gained additional strength when Bellani et al[28], in their retrospective study, also demonstrated that a higher ∆P was associated with higher mortality rates. Chiumello et al[2] revealed that ARDS patients with higher than threshold values of ∆P experienced lung stress and thus were likely to experience more ventilator-associated lung injury due to cyclic stretch. It can, therefore, be inferred that the ∆P reflects the stress on the lungs and that outputs like tidal volumes should be adjusted for ∆P instead of traditional measures. Similarly, PEEP can be adjusted to accommodate the loss of airway recruitment, increased levels of stress and strain, and the resulting increase in ∆P. A higher PEEP will improve lung compliance and attenuate the high ∆Ps resulting from lung inhomogeneity[29,30].
Villar et al[31] provided evidence that ∆P was related to an increase in hospital mortality despite optimized protective ventilation. In addition, Urner et al[32] assessed the dose-effect relationship between ∆P and survival. A hazard ratio of 1.064 (95%CI 1.057-1.071) was seen with a daily increment of ∆P. A higher mortality was noted with ∆P levels of ≥ 15 cm H2O, even if present for brief period. Furthermore, a higher ∆P level had a greater increase in mortality when compared to PaO2/FiO2 or other metrics of oxygenation.
While it has emerged as a promising metric to help attenuate events of VILI, despite reliable estimation of lung pressures, ∆P alone may not provide an accurate measure of risk. The process of VILI occurs due to a complex interplay of various forces, therefore multiple parameters need to be accounted for and addressed when managing mechanical ventilation in these cases.
∆P is measured in two ways. Firstly, in the setting of an absence of spontaneous breathing, an end-inspiratory hold of a few seconds on the ventilator provides the value of Pplat. The ∆P can be derived from the following formula (Pplat-PEEP). This method can be vulnerable to oversimplification and bias when auto-PEEP is significant and not accounted for. It can also be erroneous when clinical leaks such as bronchopleural fistulas or micro leaks are found in the apparatus or tubing. These errors can result in second-by-second variability in Pplat values. A way to counter this discrepancy is to shift the ventilator to volume control mode and set a shorter inspiratory pause of 0.3 s. This method will provide consistent measures of Pplat and thus more reliability due to shorter occlusion periods[33].
Foti et al[34] described the method of calculating ∆P in static conditions with pressure support ventilation. The derivation of Pplat is performed after an end-inspiratory hold and respiratory muscle relaxation [when the pressure generated by the ventilator (Paw) reaches a plateau] This method was proven by Akoumianaki et al[35] to overestimate Pplat and ∆P due to confounding by expiratory muscle activity. Another potential problem that distorts an accurate read of the Pplat is reverse triggering, wherein a patient initiates inspiratory effort during the middle or end of a passive inspiration by the ventilator. This is a form of ventilator desynchrony that tends to occur when a patient is weaning off sedation or paralysis. This results in an underestimation of Pplat due to a misleading drop in end-inspiratory pressures[36].
Therefore, in the case of spontaneous breathing, the derivation of ∆P becomes slightly more complex, as the patient component of respiratory effort needs to be accounted for, which is essentially driving the breath. Therefore, the pressure applied by the ventilator (Pplat-PEEP) needs to be added to the pressure generated by the respiratory muscles; i.e., PPL. The PPL can be accurately estimated through esophageal manometry, and this dynamic measurement is called the PL swing. The swing describes the ∆P for insufflation of the lung and generation of flow representing the overall change in PPL[37]. Therefore, during spontaneous breathing, the formula of ∆P changes to the ∆P = (Pplat-PEEP + ∆PPL).
Another important value Bertoni et al[38] investigated was the ∆Pocc (occluded inspiratory airway pressure), also known as the Pes swing. This value emerged from performing an expiratory hold to ascertain the patient’s inspiratory effort. The deflection depicts the change in PPL. This was described as dynamic PPL. The equation to describe dynamic PPL Predicted dynamic PPL= [∆PLdyn - (Ppeak - PEEP) - 0.66 x ∆ Pocc]. In addition to this, Telias et al[39] also showed the value of the airway occlusion pressure (P0.1) metric that is measured in the first 100 ms. of an occlusion. This metric was used to accurately detect inspiratory effort and low ventilatory drive. P0.1 can also be used to ascertain high values of dynamic.
In ARDS, the lung becomes less compliant, resulting in a reduced proportion of recruitable tissue that can be ventilated. This was best illustrated by the previously described baby lung concept[16]. These alterations thus require modulation of ventilatory techniques to account for the loss of lung volume, such as adjusting tidal volume with compliance and increasing PEEP to target ∆P[3]. As discussed earlier, many studies have described the role of ∆P in patients with ARDS. The strong association of cyclical stretch and lung stress correlates with ∆P and overall survival in ARDS.
Blondonnet et al[40] analyzed ∆P at baseline and at 24 h in patients who had developed ARDS. The analysis showed that both baseline ∆P and respiratory rate were significantly lower. ∆P greater than 16.5 cm H2O was predictive for ARDS development and vice versa. Similarly, Haudebourg et al[11] demonstrated that ∆P-targeted ventilation in patients with moderate to severe ARDS improved ventilatory parameters such as increased tidal volumes, lower MP requirement, and reduced respiratory rate. In addition, Guérin et al[7], in their study, showed that ∆P was more strongly associated with survival as compared to PEEP and tidal volume in ARDS patients. While many studies have highlighted the role of ∆P and its influence on outcomes, some studies suggest otherwise.
One such study by Romano et al[41] compared limiting ∆P with standard lung protective measures during ventilation of patients with ARDS. The tidal volume was set according to ideal weight; 4-8 mL/kg and a ∆P of 10 or the lowest possible was applied. The comparison group was ventilated according to the ARDSNet protocol with adjustments made in tidal volume based on Pplat. It was seen that both the ∆P and tidal volumes were lower in the ∆P-limited group as opposed to the conventional group, although there was no effect on outcomes.
Extracorporeal membrane oxygenation (ECMO), an external circuit to directly oxygenate the blood and remove carbon dioxide, was unveiled in the 1970s, but its use took off in more recent years, increasing to a whopping 433% since 2006[42]. ECMO is used to rest the lungs and decrease stress, strain, and intensity experienced in mechanical ventilation. It provides cardiac, respiratory, or cardiorespiratory support when needed. Ultra-low tidal volumes are employed, and various strategies are used to achieve this. Current guidelines for mechanical ventilation with ECMO, target Pplat and tidal volumes corrected for ideal body weight[43].
A study by Gupta et al[44] analyzed ∆Ps pre- and post-ECMO initiation to compare how high and low ∆Ps influence mortality and outcomes. In this study, 46% of patients had increased ∆Ps and higher drops in PEEP post-ECMO initiation. The study also showed a significantly longer length of ECMO stay in patients, perhaps due to poor parameters influencing clinician decision of weaning. High ∆P in ECMO was seen as a strong predictor of 30-d mortality in both adjusted and unadjusted analyses of patients receiving ECMO in both groups.
Magunia et al[45] showed in their study of patients receiving VV-ECMO that survivors had increased compliance levels and lower ∆Ps as compared to non-survivors. Similarly, Chiu et al, in their study of patients with severe ARDS on ECMO, showed that the cut-off point between survivors and non-survivors was a 33% change in ∆P within the first 12 h with a sensitivity of 78% and a specificity of 67.9%[46].
In the study by Del Sorbo et al[47], the effects of changing ∆P were correlated with various variables. A linear relationship was demonstrated between the change in ∆P and the concentration of certain inflammatory mediators that correlate with VILI in lung epithelial cells. This finding suggests a strong predictive potential for VILI if ∆P is utilized adequately in these patients.
In the surgical setting, there is a high likelihood of pulmonary complications, particularly in thoracic surgery, due to direct injury of lung tissues and open ventilation of one lung. This results in a heightened immune response and increased pulmonary vascular permeability, resulting in ARDS[48].
Blank et al[49] analyzed the ∆P and tidal volumes of patients undergoing thoracic surgery with two or one-lung ventilation and found that ∆P was a risk factor for overall postoperative morbidity with an odds ratio of 1.034 (97.5%CI. 1.001 to 1.068). In a meta-analysis of surgical patients, Neto and colleagues demonstrated a positive correlation between postoperative respiratory complications in patients with higher ∆Ps with an odds ratio of 1.16 for each 1 cm H2O increase in ∆P. No significant associations were found with tidal volume, and PEEP was only influential if it altered the ∆P[50].
In a cohort study conducted by Mathis et al[51] of cardiac patients undergoing surgery, modified ∆P was independently associated with decreased pulmonary complications. However, it was not clear whether active control of ∆P would result in improved outcomes, and the method of controlling or reducing ∆P was not particularly defined in their study.
Park et al[52] randomized patients who were receiving elective thoracic surgery into two ventilatory groups. One group was ventilated with standard measures of low tidal volumes, a peep of 5 cm H2O, and tailored maneuvers to increase recruitment were utilized as needed. Low tidal volumes were used in the second group, but PEEP was titrated according to the desired ∆P. Postoperative pulmonary complications were higher in the first conventional group (12.2%) as compared to the second group, where ∆P was titrated (5.5%). The incidence of ARDS was also elevated in the first group (5 patients) as opposed to the second group (0 patients). Despite the impressive findings, there was no impact on the development of ARDS by day 7, nor was there any decrease in the length of intensive care unit (ICU) and hospital stay.
In the setting of chronic obstructive pulmonary disease, there is increased air trapping, obstruction, and elevated airway resistance. This leads to an increase in end-expiratory lung volume and an increase in end-expiratory alveolar pressure- also referred to as intrinsic peep. It is thus necessary to utilize an end-expiratory and inspiratory hold to accurately generate compliance and therefore ∆P[53]. Although specific studies on COPD patients and the role of ∆P in their ventilation have not been captured, COPD patients require monitoring to ensure the emptying of lung air and thus, PEEP is primarily adjusted.
Obese patients typically have higher chest wall EL, low or more negative PTPs, and lower compliance. Due to the variability of these values, a true reflection of ∆P cannot be obtained accurately. In obese patients, transpulmonary ∆P is more reliable, but more studies are required to better explain these assumptions[54]. De Jong et al[55] studied the relationship between ∆P during the first day of ventilation and 90-d mortality in 100 obese patients and 262 non-obese patients with ARDS but found no association between ∆P and mortality in obese patients. A limitation of the study was the reliance on body mass index as a measure of obesity and body fat percentage was not accounted for.
In pregnancy, the physiology of the respiratory symptom is altered. Due to the chemical effects of progesterone and prostaglandins E1 and E2, bronchodilation occurs. Prostaglandin F2alpha, however, can increase airway resistance and constrict bronchial smooth muscles. In addition, due to uterine distension, the diaphragm is elevated, and there is an increase in end-expiratory abdominal pressure (Pga). The PPL also increases, leading to a reduction in expiratory residual volume (ERV) and functional residual capacity (FRC) due to early closure of small airways. The chest height also becomes shorter and ERV is 8%-40% lower during the second half of pregnancy. The tidal volume and occlusion pressure also increase, reflecting a need for adjustment for ventilation[56,57].
Respiratory failure in pregnancy is rare, occurring in 1 in 10000 pregnancies, but its incidence has increased, particularly since coronavirus disease 2019 (COVID-19)[58]. A study by Vasquez et al[59] showed that respiratory mechanics in pregnant females remained similar to the general population that required ventilation in cases of COVID. In a study by Lapinsky et al[60], they conducted a retrospective analysis of the impact of COVID-19 on mechanical ventilation parameters. In the case of ∆Ps, survivors had an average of < 14 cm H2O, and non-survivors had higher ∆Ps. Post-delivery, there was an increase in the PaO2/FiO2 ratio, but there was no change in static compliance or ∆P.
The first pediatric study to assess ∆P in mechanically ventilated children was conducted by Schelven et al[13] In their study, they demonstrated higher disease severity, MV indication, and an increase in extubation time in patients with higher ∆P[1]. Similarly, a retrospective study by Rauf et al[9] assessed the effects of ∆P on morbidity and mortality in children admitted to the ICU with ARDS. The study divided the children into two groups; one with ∆P of 15 cm H2O in the first hour and the other with lower than 15 cm H2O ∆P. It was seen that children with lower pressures had significantly lower morbidity in ARDS. A study by Yehya et al[61], however, suggested that ∆P in children with ARDS was not an independent predictor of mortality. It is worth noting that ∆P was not accurately defined in either of these studies.
Aging can result in an alteration of lung physiology through increased pro-inflammatory and fibrotic factors. Decreased chest wall compliance and higher levels of air trapping are noted due to the loss of lung tissue, which ultimately leads to a reduction in FEV1[62]. No study has specifically explored the effects of aging on ∆P. Theoretically, it is assumed that it would increase ∆P due to the change in compliance. It is clear that elderly patients are far more susceptible to higher morbidity and mortality in the ICU setting, and several studies have reported age as a strong predictor for mortality[63-66].
Cardiac failure due to structural and functional causes frequently results in pulmonary edema, which requires mechanical ventilation strategies. In a fluid-filled lung, the lung's compliance dramatically decreases, and the resistive forces increase. The lung behaves in a similar way to ARDS due to the pulmonary edema and, therefore, holds the same pathological changes in mechanics.
In an observational study by Yang et al[67], they analyzed 632 patients with heart failure who required invasive ventilation. It was found that higher ∆Ps above a threshold of 14.27 cm H2O were found to be independently associated with increased in-hospital mortality if patients were ventilated over 48 h. With each increment of 1 cm H2O of ∆P, an increased odds ratio of 1.12 in the risk of in-hospital mortality was observed. In contrast, Schmid et al’s study showed that there was no association with mortality in non-ARDS patients, including patients with heart failure and other cardiac-related diseases[10]. A summary of the cumulative findings of ∆P in special populations is shown in Table 1.
A cohort study by Goodwin et al[68] examined electronic health records to ascertain the importance of ∆P and EL in influencing clinical outcomes. The study assessed various factors in 2334 homogenous patients with respiratory failure in the ICU. After adjustment for covariates, exposure to ∆Ps > 15 cm H2O was associated with a 19% increased risk (1.19; CI 1.07-1.33) of mortality and 1.5 fewer ventilator-free days as compared to controls. Increased respiratory EL of > 2 cm H2O/mL/kg was also associated with a 13% increase in the risk of mortality without any impact on the length of stay or ventilatory-free days. This study established a time-weighted averaging method to derive exposure of ∆P and other metrics to give a consistent reading of ∆P and its resulting influence[2].
∆P and EL have been shown by numerous studies as predictors of reduced lung function, increased stress, and a high likelihood of VILI. Employing LUNG-SAFE ventilation strategies has expanded from lowering tidal volume to acceptable thresholds of plateau ∆Ps and reducing ventilation frequency. Currently, values of Pplat of 30 cm H2O and ∆P of 15 cm H2O are considered the upper limit. Intervention is thus necessary to tailor ventilatory care[69-71].
Many studies have provided significant insight into the relevance of ∆P as a detrimental factor in guiding ventilation. These studies have demonstrated this by showcasing high numbers of adverse events in the setting of elevated ∆P. It is worth noting that these studies are not without limitations, with many of them lacking causality. Therefore, there is a need for more comparative analyses to better predict the validity of ∆P when compared to other parameters such as PEEP, EL, tidal volume, MP, etc. A standardized method of quantifying ∆P is also crucial to ensure accuracy, and a protocol should be introduced for clinicians to follow if they plan to conduct further research on the impact of ∆P. The adjunct of additional modalities, such as Electrical Impedance Tomography (EIT) and Ultrasound, will further improve validity and give valuable insight[27]. ∆P in ECMO should also be utilized and studied to extract valuable findings.
It is common in studies to derive ∆Ps during passive ventilation, but efforts should be made to explore ∆Ps in the presence of spontaneous breathing. This will deliver additional comparative data and assess whether there are any shifts in ∆P while revealing additional metrics that may directly or indirectly influence results. The newer generation of ventilators should also be introduced when feasible-to guide clinicians in accounting for all the dynamic and static forces at play so that they can determine attributable risk. Further research on ARDS can benefit from using measurements such as esophageal manometry, as transpulmonary ∆P is a more accurate representation of the force being applied to the lung. An effort should be made to conduct more studies that include different pathologic states that lead to ARDS and clarify any variations in ∆P and ventilatory parameters.
In addition, more randomized controlled trials are needed to better understand the usefulness of ∆P in practice, establish causality, and determine its impact on long- and short-term outcomes. Further exploration of the impact of ∆P in various subsets of populations with varying etiologies is also needed. Basic science and physiological studies assessing the variability of pressures, lung volumes, oxygenation, and deformation of respiratory cells are needed to gain a more causal, sophisticated glance into cellular stress and strain[5].
Some up-and-coming trials that may provide further insight into the prospects and usefulness of ∆P were researched. Upon searching the term ‘∆P’ in clinicaltrials.gov, many promising studies emerged that aim to elaborate on the role of ∆P in various situations. A few of them are described as follows.
∆P limited ventilation for Patients With ARDS [ART-2-Trial ID: NCT02365038]; a multicenter pilot randomized control trial that is assessing the feasibility of limiting ∆P during ventilation of ARDS patients in one arm and employing the standard ventilatory guidance by ARDS Network strategy in the control arm. The tidal volume will be adjusted 3-8 mL/kg PBW to get target values of 13 cm H2O in ∆Ps calculated day 1 and day 3 of randomization.
Mechanical ventilation based on ∆P in lateral position (Trial ID: NCT04455789) A randomized, controlled, double-blind study of 60 patients undergoing total hip replacement surgery. The aim is to investigate the effects of different positions on ventilation utilizing traditional lung protective parameters in the control arm and a low ∆P arm. They aim to assess hemodynamic and respiratory values and overall postoperative outcomes.
∆P during general anesthesia for open abdominal surgery (Trial ID: NCT03884543). A randomized multicenter double-blinded control trial to assess whether the application of high peep during mechanical ventilation to maintain low levels of ∆P helps prevent complications compared to standard low peep strategies. The study targets patients undergoing abdominal surgery who are at intermediate to high risk of pulmonary complications based on the ARISCAT score. These studies and many others hold strong promise in showing an appropriate application of ∆P and its impact in various settings.
∆P has proven to be a highly significant metric when ventilating patients, particularly in ARDS. Adjusting for ∆P has shown improved clinical outcomes and fewer incidences of VILI. Considerations should be made to improve the accuracy of measurements and monitoring. Ongoing research should enhance our understanding of ∆P and how to best harness its potential in providing tailored, safe, and effective ventilation[3,4].