Correspondence to: A.S. Verkman, Cardiovascular Research Institute, 1246 Health Sciences East Tower, Box 0521, University of California, San Francisco, San Francisco, CA 94143-0521. Fax:415-665-3847 E-mail:verkman{at}itsa.ucsf.edu.
Released online: 13 December 1999
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Abstract |
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The mammalian peripheral lung contains at least three aquaporin (AQP) water channels: AQP1 in microvascular endothelia, AQP4 in airway epithelia, and AQP5 in alveolar epithelia. In this study, we determined the role of AQP4 in airspace-to-capillary water transport by comparing water permeability in wild-type mice and transgenic null mice lacking AQP1, AQP4, or AQP1/AQP4 together. An apparatus was constructed to measure lung weight continuously during pulmonary artery perfusion of isolated mouse lungs. Osmotically induced water flux (Jv) between the airspace and capillary compartments was measured from the kinetics of lung weight change in saline-filled lungs in response to changes in perfusate osmolality. Jv in wild-type mice varied linearly with osmotic gradient size (4.4 x 10-5 cm3 s-1 mOsm-1) and was symmetric, independent of perfusate osmolyte size, weakly temperature dependent, and decreased 11-fold by AQP1 deletion. Transcapillary osmotic water permeability was greatly reduced by AQP1 deletion, as measured by the same method except that the airspace saline was replaced by an inert perfluorocarbon. Hydrostatically induced lung edema was characterized by lung weight changes in response to changes in pulmonary arterial inflow or pulmonary venous outflow pressure. At 5 cm H2O outflow pressure, the filtration coefficient was 4.7 cm3 s-1 mOsm-1 and reduced 1.4-fold by AQP1 deletion. To study the role of AQP4 in lung water transport, AQP1/AQP4 double knockout mice were generated by crossbreeding of AQP1 and AQP4 null mice. Jv were (cm3 s-1 mOsm-1 x 10-5, SEM, n = 712 mice): 3.8 ± 0.4 (wild type), 0.35 ± 0.02 (AQP1 null), 3.7 ± 0.4 (AQP4 null), and 0.25 ± 0.01 (AQP1/AQP4 null). The significant reduction in Pf in AQP1 vs. AQP1/AQP4 null mice was confirmed by an independent pleural surface fluorescence method showing a 1.6 ± 0.2-fold (SEM, five mice) reduced Pf in the AQP1/AQP4 double knockout mice vs. AQP1 null mice. These results establish a simple gravimetric method to quantify osmosis and filtration in intact mouse lung and provide direct evidence for a contribution of the distal airways to airspace-to-capillary water transport.
Key Words: water permeability, airways, transgenic mouse, membrane transport, aquaporin-1
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INTRODUCTION |
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Water transport across epithelial and endothelial barriers in lung is important for fluid absorption in the perinatal lung and for airspace hydration in the adult lung (
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Water permeabilities have been measured across several of the major barriers in lung. Osmotically driven water movement in the in situ sheep lung was determined from the time course of airspace fluid osmolality, measured by direct fluid sampling, in response to instillation of hypertonic saline into the airspaces (
Recent studies in transgenic mice have begun to define the role of aquaporin-type water channels in water transport across the various barriers in the intact lung. Three aquaporins have been localized in lung: aquaporin-1 (AQP1)1 in microvascular endothelia and some pneumocytes (
The purpose of this study was to determine whether AQP4, and thus the distal airways, contribute measurably to water permeability between the airspace and capillary compartments in intact lung. To be able to detect small effects of AQP4 deletion, measurements were compared in AQP1 null mice, which have low lung water permeability, and double knockout mice in which both AQP1 and AQP4 were deleted. For measurement of water transport, a gravimetric method was developed and validated, which provided a simple and accurate approach to quantify both osmotically and hydrostatically driven water transport across the alveolarcapillary barrier and lung microvessels. The gravimetric method complements and provides distinct technical advantages over pleural surface fluorescence methods (see DISCUSSION). Deletion of AQP4 in AQP1 null mice resulted in significantly decreased airspacecapillary water permeability, establishing a role of the airways in lung water transport.
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METHODS |
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Transgenic Mice
Transgenic knockout mice deficient in AQP1 and AQP4 proteins were generated as described previously (
Isolated Lung Perfusion
Mice were killed using intraperitoneal pentobarbital (150 mg/kg). After a midline incision, the trachea was cannulated in situ with polyethylene PE-90 tubing and the pulmonary artery with PE-20 tubing. The left atrium was usually transected to permit fluid exit, but in some experiments the left atrium was cannulated with PE-20 tubing to set pulmonary venous outflow pressure. After securing the cannulae with 3-0 Nylon suture, the heart, lungs, and trachea were removed en bloc and transferred to a fluorescence microscope or gravimetric apparatus (see below). The pulmonary artery was gravity perfused at specified pressures (generally 2025 cm H2O). The time between death and perfusion was generally <7 min with >80% of perfusions being technically successful. For airspace-capillary water permeability measurements (see below), the airspace was filled with 0.5 ml HEPES-buffered Ringer's (HBR: 137 mM NaCl, 2.68 mM KCl, 1.25 mM MgSO4, 1.82 mM CaCl2, 5.5 mM glucose, 12 mM HEPES, 5% bovine serum albumin, pH 7.4, 300 mosM). For microvascular water permeability measurements, the airspace was filled with 0.5 ml of Fluorinert (3-M), a dense, nonviscous, inert water-immiscible perfluorocarbon.
Pleural Surface Fluorescence Measurements
Osmotically driven water movement between capillary and airspace compartments in surface alveoli was measured by a pleural surface fluorescence method (C], where Pf (cm/s) is the osmotic water permeability coefficient, [d(F/Fo)/dt]t = 0 is the initial slope of the relative fluorescence versus time data, S/V (cm-1) is alveolar surface-to-volume ratio (1,600 cm-1), vw (18 cm3/mol) is the partial molar volume of water, and
C is the difference in osmolality between perfusate and airspace fluids.
Gravimetric Apparatus
Figure 1 B shows a schematic of the gravimetric apparatus for continuous measurement of lung weight. The heart/lung block was suspended from a weight transducer (TSD125C; Biopac Inc.) with sensitivity <1 mg. The perfusion inflow tubing was positioned so as not to interfere with weight measurements. The perfusate fluid leaving the transected left atrium or left atrial cannula was drawn away from the heart/lung bloc by a wick to avoid artifactual weight changes arising from droplet formation. The wick consisted of a (2 x 20 mm) strip of waxed weighing paper adherent to the dorsum of the lung. The lower pole of the wick was immersed in fluid in a reservoir that rested on a second weight transducer. Perfusate flow was monitored in every measurement from the increasing reservoir weight. The gravimetric transducers were interfaced to a recorder (MP100A-CE; Biopac Inc.) and PC computer. Data were acquired at a rate of 500 Hz and averaged over 1-s intervals. For temperature control, the heart/lung block was positioned in a custom-designed cylindrical glass chamber (10 cm length, 2.5 cm inner diameter) in a moisturized air atmosphere connected to a circulating water bath. The chamber contained a slot for positioning the perfusion tubing. The gravity-fed perfusion system consisted of reservoirs and valves to permit rapid changes in perfusate fluid composition without transient changes in pressure, or rapid changes in perfusion inflow or outflow pressure. The perfusion tubing proximal to the pulmonary artery insertion point was enclosed in a temperature-jacketed compartment.
Gravimetric Water Permeability Measurements
Osmotically driven water transport between the airspace and capillary compartments was determined from the time course of lung weight in response to changes in pulmonary artery perfusate osmolality. The airspaces were filled with HBR as described above. The hyperosmolar solutions (310600 mOsm) consisted of HBR containing specified amounts of sucrose, glycine, urea, or NaCl; the hypoosmolar solutions (290150 mOsm) consisted of HBR diluted with distilled water. The initial change in lung weight following a maneuver, Jw (mg/s), was determined from the derivative (evaluated at zero time) of a quadratic polynomial fitted to the first 12 min of weight data. Osmotically driven water transport between the capillary and interstitial compartments was measured as described above except that the airspaces were filled with Fluorinert. Hydrostatically driven water transport (filtration) was measured from the time course of lung weight in response to changes in the inflow pressure of the HBR perfusate (to simulate pulmonary arterial hypertension) or in the venous outflow pressure (to simulate left-sided congestive heart failure).
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RESULTS |
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Gravimetric Measurement of Lung Water Permeability
The gravimetric and pleural surface fluorescence methods were compared for determination of airspace-capillary osmotic water permeability, a measurement that can be made by both methods (Figure 2A and Figure B). The pleural surface fluorescence method provides information about the concentration of a fluorophore (proportional to osmolality) in fluid-filled airspaces only very near (<200 µm) the lung surface (
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The gravimetric method measures total lung weight and thus the sum of fluids contained in the airspace, interstitial, and capillary compartments. Averaged information is obtained for the whole lung rather than surface alveoli/vessels, and no exogenous fluorescent probe is used. When the airspace compartment is filled with an isosmolar saline solution, changes in perfusate osmolality result in water movement across endothelial and epithelial barriers, producing changes in interstitial and airspace water content observed as changes in lung weight. Figure 2 B shows representative gravimetric data for the same changes in perfusate osmolality studied by the fluorescence method. Increasing perfusate osmolality to 400 mOsm (left) produced a decrease in lung weight as water is extracted from the extravascular spaces of the lung; decreasing perfusate osmolality to 200 mOsm (right) had the opposite effect. A 100-mg weight calibration was done in every experiment, as well as real-time measurement of perfusate flow. Detailed characterization of the gravimetric method for measurement of airspace-capillary osmotic water transport is provided below in Figure 3 and Figure 4.
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We showed previously that when the airspace compartment is filled with an inert perfluorocarbon (to minimize fluid movement into the airspaces) and perfusate osmolality is changed, information is obtained regarding osmotically driven water transport across the microvascular barrier (
The gravimetric method permits measurements of lung fluid transport in response to hydrostatic pressure gradients, measurements that cannot be carried out by a fluorescence approach. Figure 2 D shows the increase in lung weight in response to a change in pulmonary artery pressure from 8 to 18 cm H2O at a constant pulmonary venous outflow pressure of 5 cm H2O. The perfusate consisted of an isosmolar saline solution throughout. Initially, there was a prompt increase in weight resulting from vascular engorgement, which was generally complete in <10 s. The vascular phase was followed by a linear increase in weight as extravascular lung fluid accumulates. Reduction of perfusion pressure to 8 cm H2O produced a rapid weight decrease, due to decreased vascular engorgement, followed by a slower and not fully reversible decrease in lung weight. Additional characterization of the gravimetric method to measure lung filtration is given in Figure 5.
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Characterization of Lung Water Transport in Wild-Type and AQP1 Knockout Mice
The dependence of osmotically driven water transport on osmotic gradient size and direction was measured from lung weight changes in response to a series of osmotic gradients. The airspace compartment was filled with isosmolar saline and the perfusate fluid was switched between isosmolar and hyperosmolar or hypoosmolar solutions. Figure 3 A shows that the rates and magnitudes of the weight changes were dependent on osmotic gradient size. Changes in lung weight of <10 mg could be measured in response to osmotic gradients as small as 10 mOsm. Averaged initial rates of lung weight change are given in Figure 3 B. There was a linear relationship between water flux and osmotic gradient size, with slope 4.4 x 10-5 cm3 s-1 mOsm-1 at 23°C, indicating that lung water transport is symmetrical and nonrectifying. Figure 3 C shows the dependence of lung weight change on osmotic gradient size. The abscissa is expressed as the dimensionless ratio (300 mOsm/perfusate osmolality - 1), derived from the relationship (300 mOsm)wo = (perfusate osmolality) (wo + w), where wo is the initial weight of fluid instilled into the airspaces and
w is the weight gain. As predicted for a simple osmometer, the lung weight change (
w) varied with 300/mOsm - 1 in a nearly linear manner. A small difference in slope is noted for weight increases versus decreases, which might be related to interstitial and intracellular water accumulation/volume regulation and/or heterogeneity in regional perfusion.
Osmotically driven water permeability was further characterized in terms of effects of osmotic solute size, temperature, and perfusion pressure. Figure 4 A (left) shows similar lung weight kinetics in response to matched osmotic gradients of NaCl, sucrose, glycine, and urea. Averaged water fluxes (Figure 4 A, right) indicate that osmotically driven water transport is independent of osmolyte size, indicating unity reflection coefficients for the solutes studied here. The monophasic time course of lung weight change further indicated that the permeability of each solute across the airspace-capillary barrier is very low. Figure 4 B (left) shows original data from temperature-dependence measurements done on wild-type and AQP1 null mice. Lung water permeability was remarkably decreased (10-fold at 23°C) by AQP1 deletion. Water permeability in wild-type mice was minimally affected by temperature changes in the range 1237°C. The averaged water fluxes are summarized in an Arrhenius plot (Figure 4 B), giving apparent activation energies (Ea) of 2.4 (wild-type mice) and 7.6 (AQP1 null mice) kcal/mol. The higher Ea in AQP1 null mice is consistent with water movement via a rate-limiting lipid- rather than channel-mediated pathway. Figure 4 C shows the effect of pulmonary artery perfusion pressure on changes in lung weight in response to osmotic gradients. A series of such measurements indicated that a pulmonary artery pressure of 18 cm H2O, corresponding to an average flow of 2.5 ml/min, was able to induce maximal (vascular flow-independent) water transport. Figure 4 D shows the effect of increasing left atrial pressure at a constant 20 cm H2O inflowoutflow pressure difference. Although increased pressure resulted in lung water accumulation (see below), osmotic water permeability remained unchanged.
Figure 4 E shows the effect of AQP1 deletion on lung microvascular water permeability in which perfusate osmolality was changed in the presence of fluorinert-filled airspaces. AQP1 deletion produced slowed lung fluid accumulation in response to the osmotic gradient, consistent with a marked reduction in microvascular endothelial water permeability. The increase in lung weight was too small to quantify the residual water permeability after AQP1 deletion.
Figure 5 shows the effect of AQP1 deletion on lung fluid accumulation in response to hydrostatic driving forces. Previously, we reported qualitative differences in lung fluid accumulation with AQP1 deletion when venous outflow pressure was kept at zero (transected left atrium) (
Figure 5 C shows that at a constant outflow pressure of 5 cm H2O, an increase in perfusion pressure from 8 to 18 cm H2O produced a prompt increase in lung weight (vascular engorgement) that is easily distinguished from a nearly linear slower increase in lung weight. The continued accumulation of lung water is probably related to the effective contribution of post-capillary filtration when left atrial pressure is elevated, which more closely recapitulates the in vivo situation. Averaged rate of lung water accumulation was 0.63 ± 0.05 mg/s, giving a filtration coefficient of 4.7 ml min-1 cm H2O-1/100 g wet lung wt. AQP1 deletion produced a slower rate of lung water accumulation (Figure 5 C, right).
The linear increase in lung water accumulation permitted quantitative comparisons of hydrostatically driven edema formation in wild-type versus AQP1 null mice (Figure 5 D). There was a small but significant decrease in lung water accumulation in the null mice, despite the dramatic reduction in osmotically driven water transport seen in Figure 4 B.
Role of AQP4 in Lung Water Permeability
To determine the role of AQP4 in airspace-capillary water transport, osmotic water transport was compared in perfused lungs of wild-type, AQP1 knockout, AQP4 knockout, and AQP1/AQP4 double knockout mice. The AQP1 knockout and AQP1/AQP4 double knockout mice were carefully matched in body weight and the investigator was blinded to mouse genotype until completion of the analysis. Lungs from wild-type, AQP1 knockout, and AQP1/AQP4 double knockout mice were indistinguishable grossly and by light microscopic examination. Survival of the single and double knockout mice was excellent and similar to that of wild-type mice; however, the AQP1 knockout mice generally grew 1013% slower than wild-type mice and the AQP1/AQP4 double knockout mice grew 1520% slower than wild-type mice.
Figure 6 A shows representative original weight recordings for mice of each genotype. Whereas AQP4 deletion had no obvious effect on water transport (compared with wild-type mice), there was a consistent difference in water transport in lungs of AQP1 knockout versus AQP1/AQP4 double knockout mice. A full set of measurements was done on a separate set of mice using the pleural surface fluorescence method with representative recordings shown in Figure 6 B. There was a consistently lower rate of water transport in lungs from the double knockout mice compared with the AQP1 knockout mice, in agreement with the gravimetric data.
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Averaged osmotically driven volume fluxes for individual mice determined from gravimetric and pleural surface fluorescence measurements are summarized in Figure 7A and Figure B, respectively. There was no significant effect of AQP4 deletion in wild-type mice, whereas AQP4 deletion in AQP1 null mice (comparing AQP1 knockout and AQP1/AQP4 double knockout mice) produced a 1.44-fold decrease in water permeability (P < 0.001, gravimetric study; P < 0.05, fluorescence study). Compared with wild-type mice, AQP1 deletion produced a 10-fold decrease in water permeability, and AQP1/AQP4 deletion produced a 15.3-fold decrease.
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DISCUSSION |
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As reviewed in the INTRODUCTION, recent studies have defined the water transporting properties of the permeability barriers in lung. Water permeabilities of the alveolar epithelial and microvascular endothelial barriers are very high as measured in sheep, rat, and mouse lung, whereas the water permeability of isolated distal airways (measured in guinea pig lung) is substantially lower. Technical limitations in the microperfusion methods have precluded the measurement of airway water permeability in mammals other than guinea pig. The role of aquaporin water channels is of considerable interest for lung fluid balance in the perinatal and adult lung, both under normal and pathological conditions. Because there are at present no aquaporin inhibitors for in vivo use, the generation of knockout mice lacking specific aquaporins was undertaken to investigate the role of aquaporins in organ physiology. Transgenic mice lacking AQP1 are unable to concentrate their urine (
The contribution of airway AQP4 to airspace-capillary water permeability was investigated by comparing water transport in mice lacking AQP1 alone versus AQP1 and AQP4 together. It was reasoned that the relatively low lung water permeability in AQP1 null mice might permit the detection of a small incremental effect of AQP4 deletion. AQP1/AQP4 double knockout mice were generated by breeding of mice containing the individual gene deletions. Airspace-capillary water permeability, measured by the established pleural surface fluorescence method as well as a new gravimetric method, was significantly reduced by 1.41.6-fold in AQP1/AQP4 double knockout mice versus AQP1 knockout mice. No significant effect of AQP4 deletion in wild-type mice was found, probably because of the substantially greater basal water permeabilities. The 1.41.6-fold effect of AQP4 deletion on water permeability in the AQP1 null mice suggests an overall contribution of AQP4 to lung water permeability of ~4% (taking into account the 10-fold effect of AQP1 deletion alone). Although this represents a relatively small contribution, it is remarkably greater than that predicted based on estimates that the airways comprise only 1.4% of the total airspace epithelial surface area (
AQP4 expression is strongly upregulated in the neonatal period, a time where rapid absorption of distal airspace fluid occurs and when relatively little AQP1 and AQP5 are expressed (
Because of the complex airspace and microvascular geometry, it is difficult to quantify effective airway versus alveolar surface areas, as well as fluid flow patterns during osmosis. As depicted in Figure 1 A, the pulmonary artery runs with the airways and divides as the airways divide. A capillary bed consisting of AQP1-containing endothelial cells is formed in the alveolar acinar region beyond the terminal bronchiolus. The bronchial artery forms a capillary plexus that supplies the muscle and submucosa of the airways. This plexus communicates with branches of the pulmonary artery and empties into the pulmonary veins. In addition, there is further complexity in terms of heterogeneity in microvasculature and alveolar geometry in different regions of the lung. Thus, the description of lung fluid movement in terms of passage across well-demarcated geometric barriers is probably an oversimplification, underscoring the need for functional studies to quantify barrier properties.
Gravimetry is a classical method to study organ bed capillary filtration that originated more than 50 years ago (
An interesting observation in the hydrostatic edema studies was that interstitial fluid accumulation was strongly dependent on venous outflow pressure. At a venous outflow pressure of zero (transected left atrium), there was mild fluid accumulation that saturated over a few minutes, whereas sustained fluid accumulation occurred when left atrial outflow pressure was maintained at 5 cm H2O. At zero venous outflow pressure, there was limited edema even when pulmonary artery pressure was increased to 45 cm H2O (not shown). These results suggest that the venous component of the microvasculature plays an important role in lung fluid accumulation in response to hydrostatic pressure differences. In addition, the increased venous outflow pressure may promote the maintenance of microvascular bed patency throughout the lung. AQP1 deletion was associated with a small, but significant 1.4-fold decrease in lung fluid accumulation in response to a hydrostatic stress, despite a 10-fold reduction in osmotically driven airspace-capillary water permeability. Therefore, AQP1-independent pathways, probably involving paracellular water transport, play a major role in hydrostatically driven transcapillary water movement.
The gravimetric method provides a simple and quantitative approach to characterize the water permeability properties of microvascular and epithelial barriers. The modifications to the classical gravimetric method introduced here for studies in small animals permit measurements of both osmotic and hydrostatically driven lung water transport across airspace-capillary barriers. The administration of perfluorocarbon into the airspaces permits measurements of transcapillary water movement without the confounding effects of transepithelial fluid movement. The instrumentation for gravimetric measurements in small animals is simple, consisting of 2-mgresolution gravimetric transducers and various reservoirs, values, and heating devices to control and measure perfusate pressure, flow, and composition. Because of the small weight of the mouse lung, care is needed to minimize changes in lung weight arising from solution exiting the lung and evaporative water losses. In contrast to pleural surface fluorescence measurements, gravimetry permits direct assessment of the fluid content of the interstitial compartment, and provides information about all airspaces rather than only those at the pleural surface. The determination of microvascular water permeability does not require complex experimental and analysis methods. The characterization of hydrostatically driven water transport has not been done previously in mice and cannot be done by fluorescence approaches. The simplicity of the gravimetric apparatus and the straightforward interpretation of experimental data should make it attractive to laboratories studying lung fluid transport in transgenic mice and other small animals.
The application of gravimetry to quantify lung water transport is particularly useful for comparative studies, such as in lungs of wild-type versus transgenic mice, and effects of inhibitors and temperature. As mentioned above, the determination of absolute permeability coefficients (in contrast to apparent permeabilities and filtration coefficients) is challenging because of the complex lung anatomy and potential heterogeneity in perfusion efficiency. There are a number of other concerns for quantitative applications of gravimetry. Unstirred layer effects is a consideration for permeability measurements in organ perfusion models (
Although the present study examined the role of AQP4 in lung water transport, it did not provide direct measurements of airway water permeability, nor did it address the broader issue of the role of aquaporins in lung physiology. Methodologies are needed to measure apical and basolateral water permeabilities in distal airways from mice. Studies to address aquaporin physiology in lung are in progress, including measurements of active alveolar fluid clearance in the adult lung, neonatal lung fluid clearance, and lung edema in various injury models such as acid aspiration, congestive heart failure and hyperoxia. These studies are being done using the AQP1 and AQP4 knockout mice, as well as knockout mice with deletions of AQP3 expressed in large airways, and AQP5 expressed in alveolar epithelium. It is notable here that the AQP1/AQP4 double knockout mice, although less robust than wild-type or AQP1 null mice, are able to survive and generally grow well. The residual low water permeability in lung after AQP1 and AQP4 deletion thus appears to be adequate for mice to survive and thrive. Further experiments as described above and using mice containing multiple aquaporin gene deletions will be required to define the role of aquaporins in lung physiology under normal and pathological conditions.
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Footnotes |
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1 Abbreviation used in this paper: AQP, aquaporin.
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Acknowledgements |
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We thank Ms. Liman Qian for transgenic mouse breeding and genotype analysis.
This study was supported by National Institutes of Health grants HL59198, HL51854, DK35124, HL60288, and DK43840, and grant R613 from the National Cystic Fibrosis Foundation.
Note Added in Proof. AQP4 knockout mice also manifest reduced brain edema in response to water intoxication and ischemic stroke (Manley, G.T., M. Fujimora, T. Ma, N. Noshita, F. Feliz, A.W. Bollen, P. Chan, and A.S. Verkman. 2000. Aquaporin-4 deletion in mice reduces brain edema following acute water intoxication and ischemic stroke. Nat. Med. In press).
Submitted: 30 July 1999
Revised: 28 October 1999
Accepted: 1 November 1999
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