Pleural pressure theory revisited: a role for capillary equilibrium
Original Article

Pleural pressure theory revisited: a role for capillary equilibrium

Aaron R. Casha1,2, Roberto Caruana-Gauci3, Alexander Manche1, Marilyn Gauci4, Stanley Chetcuti5, Luca Bertolaccini6, Marco Scarci7

1Department of Cardiothoracic Surgery, Mater Dei Hospital, Malta; 2Faculty of Medicine, Medical School, 3Metamaterials Unit, Faculty of Science, University of Malta, Malta; 4Department of Anaesthesia, Mater Dei Hospital, Malta; 5Cardiovascular Center, University of Michigan, Ann Arbor, Michigan, USA; 6Thoracic Surgery Unit, Sacro Cuore Don Calabria Research Hospital, Verona, Italy; 7Department of Thoracic Surgery, University College London Hospital, London, UK

Contributions: (I) Conception and design: AR Casha; (II) Administrative support: AR Casha; (III) Provision of study materials or patients: All authors; (IV) Collection and assembly of data: All authors; (V) Data analysis and interpretation: All authors; (VI) Manuscript writing: All authors; (VII) Final approval of manuscript: All authors.

Correspondence to: Aaron R. Casha, MD, PhD. Medical School, University of Malta, Mater Dei Hospital, Msida, Malta. Email:; Marco Scarci, MD. Department of Thoracic Surgery, University College London Hospital, London, UK. Email:

Background: Theories elucidating pleural pressures should explain all observations including the equal and opposite recoil of the chest wall and lungs, the less than expected pleural hydrostatic gradient and its variation at lobar margins, why pleural pressures are negative and how pleural fluid circulation functions.

Methods: A theoretical model describing equilibrium between buoyancy, hydrostatic forces, and capillary forces is proposed. The capillary equilibrium model described depends on control of pleural fluid volume and protein content, powered by an active pleural pump.

Results: The interaction between buoyancy forces, hydrostatic pressure and capillary pressure was calculated, and values for pleural thickness and pressure were determined using values for surface tension, contact angle, pleural fluid and lung densities found in the literature. Modelling can explain the issue of the differing hydrostatic vertical pleural pressure gradient at the lobar margins for buoyancy forces between the pleural fluid and the lung floating in the pleural fluid according to Archimedes’ hydrostatic paradox. The capillary equilibrium model satisfies all salient requirements for a pleural pressure model, with negative pressures maximal at the apex, equal and opposite forces in the lung and chest wall, and circulatory pump action.

Conclusions: This model predicts that pleural effusions cannot occur in emphysema unless concomitant heart failure increases lung density. This model also explains how the non-confluence of the lung with the chest wall (e.g., lobar margins) makes the pleural pressure more negative, and why pleural pressures would be higher after an upper lobectomy compared to a lower lobectomy. Pathological changes in pleural fluid composition and lung density alter the equilibrium between capillarity and buoyancy hydrostatic pressure to promote pleural effusion formation.

Keywords: Pleural pressures; capillarity; biomechanics; basic research

Submitted Sep 18, 2016. Accepted for publication Mar 12, 2017.

doi: 10.21037/jtd.2017.03.112


Pleural fluid exists as a thin film under sub-atmospheric pressure, in the range of 5 cm water pressure (1), and is even lower than atmospheric pressure at the lung apex compared to the base (2).

Pleural fluid acts as a lubricant reducing lung friction at the surface (3). The vertical gradient of pressure within the pleura is less than predicted from its hydrostatic pressure (4). There occurs a circulation of pleural fluid with fluid exudation from the parietal pleura and fluid absorption occurring maximally at the parietal pleura basally, at the mediastinal pleura (5).

The explanation for these pleural fluid phenomena has been controversial with various models proposed. These include hydrostatic equilibrium (6,7), viscous flow (4,8) and pleural pumping (9-12). These models have specific predictions regarding how pleural pressure is developed. Contrary to the hydrostatic model, experimental evidence shows that the vertical pressure gradient in the pleural space is less than 1 cmH2O/cm height; though proponents claimed that points of contact between the pleural surfaces reduced lung surface pressures, thus explaining pleural pressures (13).

In the viscous flow model, Lai-Fook states that the “surface pressure expanding the lung, equal and opposite to the pressure expanding the chest wall, is transmitted hydraulically across the pleural space with the surface pressure equal to the pleural liquid pressure, and is the major determinant of the pleural liquid pressure. The difference between the vertical gradient in pleural surface pressure and the hydrostatic value drives a viscous flow of pleural liquid downward in the pleural space, which has no pleural contact” (14). The viscous flow model excludes the presence of a hydrostatic equilibrium and also omits capillary pressures, relying only on transmural pressures generated by the equal and opposing recoils of the lungs and the chest walls.

The pleural lymphatic vessels over the lower parts of parietal pleura have open stomas that drain pleural fluid directly into the lymphatics, where it is actively pumped by smooth muscle in the lymphatic walls aided by skeletal muscle contraction (15). A requirement of the pleural pumping model is that active pumping directly causes the negative pleural pressure (11). However, pumping to such a degree of negative pressure is energy consuming and would probably lead to fluid being drawn across the pleural membranes.

Examples of capillary action are common in nature. For example, when a brush is dipped in water, surface tension forces cause the hairs in the brush to coalesce. Surface tension is the elastic tendency of a fluid surface to acquire the lowest surface-area possible, and is due to the greater attraction or cohesion of water molecules to each other through hydrogen bonds, rather than adhesion to other molecules. Surface tension forces exist without the need for air, for example in capillaries (xylem) in plants and trees. The contact angle is the mean of a range of angles (contact angle hysteresis between advancing and receding contact angles) at which a liquid or vapour meets and is in equilibrium with a solid. The contact angle reflects the strength of the molecular attraction, and allows calculation of surface tension forces.

A model that covers all known facts about pleural pressures, but avoids the pitfalls mentioned above, has not yet been proposed. The concept of capillary forces in the pleural space is attractive since it would immediately imply that pleural pressure is negative and maximal at the apex due to capillarity, that lung and chest wall recoil is equal and opposite, and the concept of flexo-capillarity (capillarity between flexible sheets) implies that contact may be both present and absent (16).

The aim of our theoretical model was the evaluation of the physics of the pleural space in the light of the capillary action that occurs in thin films of fluid between conforming surfaces, assuming equilibrium between the hydrostatic, buoyancy and capillary forces at all levels, with the lung floating in pleural fluid following Archimedes’ hydrostatic paradox. To clinically test this hypothesis, the capillary equilibrium model was used as a prediction model in the scaling of pleural pressures with body size, in the development of pleural effusions, and to assess post-lobectomy temporary pleural pressure changes.


Mathematical analysis of capillary surface interaction aimed at calculating pleural pressure was performed. A systematic literature search was performed. We searched three bibliographic databases (MEDLINE, EMBASE, and the Cochrane Central Register of Controlled Trials) from inception (MEDLINE, 1946; EMBASE, 1974; and Cochrane Central Register of Controlled Trials, 1898) to 1st December 2015, without language restriction. An extensive search strategy using a combination of subject headings (“surface tension”, “contact angle”, “pleura”, “peritoneum”) was constructed to find articles with data about surface tension and contact angles required to calculate capillary forces.

According to previous models, the chest wall was shaped as a wetted surface with consistent physical characteristics, and the lung simplified as a homogenous (17), floating substrate with a contact angle equal to that of the chest wall as all pleural surfaces have a phospholipid coating (18). The lung was modelled as floating according to Archimedes’ hydrostatic paradox (an object with an average density lower than its surrounding fluid can float in a quantity of fluid with less volume than the object itself) (19). The equilibrium of contact across the pleura was modelled as the capillary interaction of near parallel surfaces balanced against buoyancy pressure. An assumption of static equilibrium in the pleural space was made, so the effects of cardiac and respiratory movements on the pleural space were disregarded. The shapes of the lungs and chest wall were taken to be confluent, apart from the borders of the lobes of the lung.



The lung is assumed to be floating in the pleural fluid according to Archimedes’ hydrostatic paradox. The density contrast between the lung and pleural fluid forms the hydrostatic gradient for pleural fluid (Figure 1) (20):

Figure 1 The pleural space. (A) Schematic of pleural fluid column surrounding lung; (B) pressure gradient as a function of pleural space height and fluid thickness. The volume of pleural fluid is a function of the balance of capillary forces pulling the pleural fluid up and the force of gravity acting together with the density contrast between the lung and pleural fluid, tending to pull pleural fluid down. Modified and redrawn after Shepherd 2009 (20).

where g is the acceleration due to gravity, h is the vertical height, and ppleural fluid, plung are the densities of pleural fluid and lung respectively. In this paper, a value of 0.32 g/mL was taken for lung density and 1.025 g/mL for pleural fluid density, with further details shown below.

Lung density or specific density varies in the literature with values ranging from 0.14 g/mL [data on lung mass from Molina et al. (21) and on lung volume from Stocks et al. (22)] and 0.25–0.37 g/mL [data from Garnett et al. (23)]. Normal pleural fluid has a protein concentration of approximately 15 g/L (24), corresponding to a density of 1.034 g/mL (25), but a pleural fluid density of 1.025 g/mL (range, 1.020–1.030 g/mL) has also been reported (26).

There is also a range of values between the differing pleural fluid and lung densities, resulting in a liquid pressure gradient in the pleural space of approximately 0.775 cmH2O/cm height (subtracting 0.250 from 1.025) above lung base when pleural surfaces are confluent. There is however an even wider range of variation in lung and pleural fluid densities in pathological states (Table 1) (23,26) resulting in a wide range of pressure gradients from 0.1–0.9 cmH2O/cm height that matches the range of experimental measurements of the vertical pressure gradient within the pleural space (Table 2) (8,14).

Table 1
Table 1 Variation in lung buoyancy in pathological states.
Full table
Table 2
Table 2 Experimental measurements in a dog model compare with the range of vertical gradient in pleural pressure in humans in the capillary equilibrium model based on an average relative density of 0.775 g/cm3 and the wider range of pathological values.
Full table


The forces acting on the pleural fluid and lung interface are assumed to be in equilibrium, with the lung displacing pleural fluid, and capillary forces retaining a film of pleural fluid (40). The force generated by the weight of the elevated pleural fluid acting against the lung is balanced by the negative pull of the surface tension forces at all levels and the buoyancy pressure generated by the lung floating in the pleural fluid (Figure 1). With the assumed occurrence of equilibrium:

Calculation of capillary pressures and pleural fluid thickness

Confluent plates are pressed together with a capillary force F (41):

where A is the area of contact of the film, d is the distance between the plates at the edge of the film, α is the contact angle between the fluid and the solid, and T is the surface tension of the liquid.

Since pressure is force over area, then capillary pressure (Pc):

Pleural fluid thickness was calculated by substituting from formula (1):

Capillary pressure and hydrostatic pressure calculations were performed using the following parameters: specific gravity of pleural fluid 1.025, pleural fluid contact angle 38°, surface tension of 18 dynes/cm and relative density between the lung and pleural fluid 0.775 g/cm3.

The pleural fluid contact angle of 38° was based on the mean contact angle of a phospholipid extract coated surface of 38.2°±4° (42), contact angle of phosphatidylcholine coated slide of 40° (43), contact angle of lipid-extract-coated slide of 32° (43), and a parietal peritoneal contact angle of 43° and visceral peritoneal contact angle of 47° (44). Surface tension of pleural fluid was assumed to be 18 dynes/cm based on the surface tension of a phospholipid extract of 20±3.4 dynes/cm (42), the surface tension of ten lipid extract samples of 17.2±2.3 dynes/cm (20), direct measurements of surface tension in the lung (45) ranging from 9–20 dynes/cm, and peritoneal surface tension of 17 dynes/cm (43), see Table 3; in contrast, the surface tension of pure water at 37 °C is 74.27 dynes/cm.

Table 3
Table 3 Values for contact angle and surface tension in the literature
Full table

The range of pleural pressures was calculated using relative density 0.65–0.89 g/mL, contact angle 32°–47°, and surface tension 15–23 dynes/cm and reported in Table 4. The predicted range of thickness of pleural capillary film against the height of the fluid showed an asymptotic behaviour (Figure 2), see Eqs. [7] and [8] below. For example, using the mean values of this paper, at a height above lung base of 10 cm, the capillary pressure would be 7.75 cmH2O (Table 4). This calculation approximates well with Lai-Fook’s work on the difference in pleural pressure between lobar margins and costal surfaces in dogs (4) (Figure 3), where at 10 cm above lung base, the difference in pleural pressure between the lobar margin and costal surface was 7 cmH2O.

Table 4
Table 4 Pleural height from the base, and calculated pleural thickness and pressure according to the capillary equilibrium model of pleural pressures. See text for the mean and range of values for relative density, contact angle and surface tension used in the calculation
Full table
Figure 2 Predicted range of thickness of pleural capillary film against the height of the fluid showing asymptotic behaviour, with the results varying according to the normal range of lung and pleural fluid densities. Based on calculations in Table 4.
Figure 3 Pleural fluid pressure measured in the prone dog at both the lobar margin and costal surface demonstrating the difference in pleural pressures. Modified and redrawn after Lai-Fook (4).

The capillary equilibrium model suggests several speculative predictions that could support the validity of this theory.

Scaling with size

In large animals, the vertical height of the lungs would result in a thin pleural film with a high tendency to collapse because of elastocapillary forces: this collapse of the pleural film may be expected over an extended period of time to result eventually in fibrosis of the pleural space, especially apically. This may be an alternative explanation to West’s answer that elephants developmentally obliterate the pleural space, extant in the foetal stage (46), to protect the parietal pleural microvasculature (47).

Effect on development of pleural effusions

The pleural fluid contains protein at a lower level than serum. The higher the protein content, the lower the surface tension of water, and the higher the capillary forces. Lower protein levels result in a drop in capillary forces, which may lead to a lack of adhesion of lung to chest wall with resultant formation of a fluid collection. The phospholipid coating on the pleural surface generates a similar effect on lowering surface tension. Since capillarity and buoyancy pressure are assumed to be in equilibrium:

The pleural fluid thickness is proportional to surface tension (T) and the cosine of the contact angle (cos α), and inversely proportional to buoyancy (the difference in densities).

As the protein content in pleural fluid decreases, the surface tension (T) increases (more hydrophobic) according to formula (8), so pleural fluid thickness increases are encouraging the formation of a transudate effusion: dT.

From formula (8), the thickness of pleural fluid is inversely proportional to the difference in lung and pleural density, or buoyancy:

From Table 1, it is evident that lung buoyancy is maximal in emphysema, suggesting that pleural effusions should not develop in emphysema, where the thickness of pleural fluid should be minimal. This explains why pleural effusions developing in emphysema patients occur only with concomitant congestive heart failure (48), which would decrease buoyancy of the lung and increase pleural fluid thickness. Tight control of the volume and protein content of pleural fluid is required to allow an adequate connection between the lung and the thoracic wall (8). Pathological changes in lung and pleural densities (Table 1) can substantially affect pleural pressure and thickness measurements by altering the equilibrium between capillarity and buoyancy hydrostatic pressure.

Contact between the parietal and visceral pleura

The previous hydrostatic equilibrium model required areas of contact between the parietal and visceral pleura (49), while the viscous flow model postulated the existence of points of contact between the two pleural surfaces possibly through cells present in pleural fluid and microvilli (1,2,14,50). The model described here can work with both the presence and lack of areas of contact; classical capillarity assumes no contact up till a height as predicted by Jurin’s law (that represents the height of rising of a liquid in capillary tubing), but elastocapillarity allows contact between pleural surfaces due to the flexible visceral pleura (51).

Assumptions in model

Lung density was assumed to be uniform, however at the lung base, some areas may act similar to West zone 4, with increased density due to the collapse of the lung structure under its weight. The changes in lung density are partly gravitational, partly due to pressure from the heart and partly by patterns of blood flow within the lung, since blood makes up about 50% of the lung’s weight (17,52,53). The values of the contact angle and surface tension were taken as an average and constant at all points. We also assumed that the protein concentration (which affects the surface tension) is constant throughout the pleural fluid. Static equilibrium in the pleural space and the confluent shape of the lung against the chest wall were other assumptions. The equations used assume the presence of an infinitely small of air in the pleural cavity and are approximations, accurate on flat surfaces whilst the lung is curved.


Any theory for pleural pressure needs to explain certain crucial facts, including that the lung and chest walls exert an equal and opposite recoil pressure (54). It would need to explain the negative values for pleural pressure, and why apical pleural pressure is more negative than at the base. It would also require an explanation for the lower than expected pleural hydrostatic pressure gradient that differs from the hydrostatic pressure gradient at the lobar margins in confluent pleural space, as well as a mechanism explaining how pleural circulation occurs.

In the capillarity equilibrium model, pleural forces press the lung and chest wall together by negative capillary forces, passively based on the molecular attraction of solids and liquids. When ventilation is paused at functional residual capacity, there exists a state of equilibrium. Capillarity develops equal and opposite forces in the chest wall and lung explaining how the reactive forces on the lung and chest wall are equal and opposite. Since the lung is more compliant than the chest wall, capillary forces act to conform the lung to the parietal pleura. The recoil of the lung from the chest wall occurs when the high capillary forces are disrupted in a pneumothorax or hydrothorax.

The pleural fluid, whose volume and composition is tightly controlled by the metabolically-active pleural mesothelial cells (55), yet varies in pathological states, acts as a thin film creating capillary interaction. This model postulates that pleural fluid causes adhesion, effectively coupling lung and chest wall, precisely because the volume of pleural fluid is kept low by active pumping. The pumping action of the chest wall mesothelial cells is necessary to maintain a minimal pleural fluid volume (12,56) and thus support capillary forces in the pleura, which would be lost if the fluid was allowed to accumulate. The capillary forces generate a negative pressure gradient that is maximal at the apex, where the pleural fluid film is thinnest. This proposed model explains the negative value for pleural pressure (57), and why this is maximal at the apex (14).

Why the hydrostatic vertical pleural pressure gradient is higher at pleural borders

The hydrostatic fluid gradient in the pleural space is altered by the presence of lungs that are buoyant in pleural fluid, changing the relative hydrostatic pressure gradient of the pleural fluid. At every level of the pleura, the capillary forces are in balance with the hydrostatic buoyancy force exerted by the lung floating in pleural fluid, based on the relative densities of pleura and lung. This is similar to the contact problem between two immiscible liquids of different densities such as oil and water, as occurs with buoyancy forces in reservoir fluids (20).

Modelling can explain the issue of the less than expected hydrostatic vertical pleural pressure gradient for buoyancy forces between the pleural fluid and the lung floating in the pleural fluid according to Archimedes’ hydrostatic paradox; the solution sketched here is based solely on this explanation. The previous comment by Agostoni (49) that pleural contact occurs is feasible according to the modern theory of flexo-capillarity (16). With flexible walls, the contact between opposite walls enables the liquid to rise virtually to infinity (51).

As a film of pleural fluid exists at the apex (14), the lung can be assumed to be submerged and floating in pleural fluid in a state similar to Archimedes’ hydrostatic paradox. The volume of pleural fluid remaining at a given height in the pleural space is a function of the balance of capillary forces pulling the pleural fluid up and the force of gravity acting together with the density contrast between the lung and pleural fluid, operating to remove the pleural fluid down (40). The capillary-bound pleural fluid comprises a continuous column of pleural fluid, which will have a pressure gradient controlled by the pleural fluid density. The lung will have a pressure gradient controlled by the (lower) lung density (Figure 2). Although lung and pleural fluid coexist in the same localised pleural space, the forces acting on the two are different. The difference in pressure between the lung and pleural fluid increases with height above the free-pleural-fluid level; the free-pleural-fluid level being the level at which the lung pleural fluid interface would theoretically stand in the presence of air (58), with only gravity and buoyancy forces controlling pleural fluid level in this situation. The relationship between capillary and buoyancy forces thus monitors the thickness of the pleural fluid film within the pleural space (20). The lung will float fractionally higher than expected (even though the same total volume of pleural fluid would have been displaced) as in a state of equilibrium, the buoyancy and surface tension forces are equal to the weight of displaced fluid.

At the level of the lobar borders, the lung is not confluent with the chest wall, so there is no thin film arrangement, and capillary forces are much weaker. In this case, the column of fluid acts hydrostatically with a pressure change akin to a manometer with an increase of 1 cmH2O as one moves 1 cm further inferiorly.

Pleural fluid circulation

The formation of pleural fluid is due to exudation mostly from the parietal pleural surface and is absorbed by the diaphragmatic and mediastinal parietal pleura (54). The capillary equilibrium model suggests that the higher rate of pleural fluid formation in the apex is due to the greater negative capillary forces there, resulting in a flow of pleural fluid to the relatively lower-producing areas in the base. The heart acts as a pressure chamber within another pressure chamber, the thorax. Pleural pressure varies from −5 cmH2O at the bottom to −15 cmH2O at the apex whilst pericardial pressure ranges from −10 to +5 cmH2O depending on the stage of the cardiac cycle (59), with pericardial pressures increasing with faster heart rates as occurs with exercise in healthy hearts (60). The high negative apical pleural pressure leads to a basal-to-apical gradient that is effectual only at the mediastinal pleural surface since cardiac motion is only efficient as a pump at the mediastinal surface. An increase in the heart rate is associated with an increase in contractility of the myocardium; at higher heart rates, the diastolic time decreases, so the effective pressure generated within the pericardium rises towards the maximum of +5 cmH2O (61). This increases the forward gradient and causes increased pumping particularly at the lobar edges where the lack of confluence between lung and chest wall allows pleural fluid to be easily disturbed by cardiac contractions and the motions of breathing (ventilator pump), and where the capillary forces are greatly diminished, leading to a fluid flow directed up towards the apex. Absorption occurs into parietal and diaphragmatic lymphatic stomata (62) with those at the level of the diaphragmatic pleura (3) driven by diaphragmatic contraction (15).

Deep respiration with descent of the diaphragm and increase in the thoracic volume makes the intra-thoracic pressure more negative. Intra-pleural pressure is subject to the same change in pressure as measured by intra-esophageal balloon catheter pressure measurements. All this implies that the capillary equilibrium model is consistent with known physiology (14).

Post-lobectomy temporary intrapleural pressure changes

After a lobectomy, there is lung volume loss leading to a temporary increased pleural space that is initially free of fluid but eventually fills with pleural fluid, but with loss of the capillary component of pleural pressure. Pleural pressures in the initial post-operative period measure pleural air pressure with large volume swings, but pleural pressure becomes negative with lessening volume swings as space fills with fluid (63). Once the pleural space fills completely with fluid, the pleural pressure becomes more negative as the pleural space becomes non-confluent, similar to the normal circumstances at the lobar edge where the pleural pressure gradient is higher. The greater the non-confluence between the lung and the chest wall, the more negative the pleural space due to the absence of capillarity (Figure 3). Pleural pressures are higher with an upper lobectomy and normal in the case of a lower lobectomy (64,65). The temporary presence of more apical fluid after an upper lobectomy leads to loss of capillarity since the remaining lower lobe fits imperfectly in the pleural cavity, explaining the higher pleural pressures post-upper lobectomy and the normal ones post-lower lobectomy. Once confluence between the lower lobe and the apex develops, the pleural fluid physiology returns back to normal.

Pathological conditions

Pathological conditions such as emphysema, edema or fibrosis may alter the elastic property of the pulmonary parenchyma. For example, lung fibrosis causes hyperinflation of the lungs. This in turn results in coalescence of the pleural surfaces resulting in a change in the height of capillary rise when compared to normal lungs that can be modelled mathematically by elastocapillarity theory.

Pathology in the form of pleural effusions may also have an effect on this proposed model. Transudative effusions due to heart failure, cirrhosis and nephrotic syndrome etc., occur when there is excessive pleural fluid production exceeding the active resorptive capacity; on the other hand, exudative effusions occur when pleural leaks occur due to pleural damage from trauma, infection, malignancy etc. (3). In both cases the active pleural pump is overwhelmed with the increase in pleural fluid thus diminishing the capillary effect.


Capillary action attracts the parenchymal pleura to the parietal pleura. This force is a passive one, in that it does not entail the use of energy, and results in equal and opposite recoil forces in the lung and chest and is maximal at the apex. This model describes capillary forces as being in equilibrium with hydrostatic and buoyancy forces at all levels. Archimedes’ hydrostatic paradox explains buoyancy forces at confluent costal surfaces and the variation at lobar margins. This hypothesis predicts that pleural effusions cannot occur in pure emphysema; explains pleural pressure changes post-lobectomy; and is consistent with cardiac pumping setting up an upward flow of fluid in the mediastinum along an active pressure gradient. Pathological changes in pleural fluid composition and lung density alter the equilibrium between capillarity and buoyancy hydrostatic pressure to promote pleural effusion formation.


The authors would like to thank the University of Malta for partly supporting this research.


Conflicts of Interest: The authors have no conflicts of interest to declare.

Ethics Statement: All results reported in this study are based on referenced work and the authors did not seek ethics approval since no experiments were carried out for this study and no participants were enlisted.


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Cite this article as: Casha AR, Caruana-Gauci R, Manche A, Gauci M, Chetcuti S, Bertolaccini L, Scarci M. Pleural pressure theory revisited: a role for capillary equilibrium. J Thorac Dis 2017;9(4):979-989. doi: 10.21037/jtd.2017.03.112