Morphometry of the extremely thin pulmonary blood-gas barrier in the chicken lung

The gas exchanging region in the avian lung, although proportionally smaller than that of the mammalian lung, efficiently manages respiration to meet the high energetic requirements of flapping flight. Gas exchange in the bird lung is enhanced, in part, by an extremely thin blood-gas barrier (BGB). We measured the arithmetic mean thickness of the different components (endothelium, interstitium, and epithelium) of the BGB in the domestic chicken lung and compared the results with three mammals. Morphometric analysis showed that the total BGB of the chicken lung was significantly thinner than that of the rabbit, dog, and horse (54, 66, and 70% thinner, respectively) and that all layers of the BGB were significantly thinner in the chicken compared with the mammals. The interstitial layer was strikingly thin in the chicken lung ( approximately 86% thinner than the dog and horse, and 75% thinner than rabbit) which is a paradox because the strength of the BGB is believed to come from the interstitium. In addition, the thickness of the interstitium was remarkably uniform, unlike the mammalian interstitium. The uniformity of the interstitial layer in the chicken is attributable to a lack of the supportive type I collagen cable that is found in mammalian alveolar lungs. We propose that the surrounding air capillaries provide additional structural support for the pulmonary capillaries in the bird lung, thus allowing the barrier to be both very thin and extremely uniform. The net result is to improve gas exchanging efficiency.     

Ultrastructural appearances of pulmonary capillaries at high transmural pressures.

Electronmicroscopic appearances of pulmonary capillaries were studied in rabbit lungs perfused in situ when the capillary transmural pressure (Ptm) was systematically raised from 12.5 to 72.5 +/- 2.5 cmH2O. The animals were anesthetized and exsanguinated, and after the chest was opened, the pulmonary artery and left atrium were cannulated and attached to reservoirs. The lungs were perfused with autologous blood for 1 min, and this was followed by saline-dextran and then buffered glutaraldehyde to fix the lungs for electron microscopy. Normal appearances were seen at 12.5 cmH2O Ptm. At 52.5 and 72.5 cmH2O Ptm, striking discontinuities of the capillary endothelium and alveolar epithelium were seen. A few disruptions were seen at 32.5 cmH2O Ptm (mostly in one animal), but the number of breaks per millimeter cell lining increased markedly up to 72.5 cmH20 Ptm, where the mean frequency was 27.8 +/- 8.6 and 13.6 +/- 1.4 (SE) breaks/mm for endothelium and epithelium, respectively. In some instances, all layers of the blood-gas barrier were disrupted and erythrocytes could be seen moving into the alveolar spaces. In about half the endothelial and epithelial breaks, the basement membranes remained intact. The average break lengths for both endothelium and epithelium did not change significantly with pressure. The width of the blood-gas barrier increased at 52.5 and 72.5 cmH2O Ptm as a result of widening of the interstitium caused by edema. The cause of the disruptions is believed to be stress failure of the capillary wall. The results show that high capillary hydrostatic pressures cause major changes in the ultrastructure of the walls of the capillaries, leading to a high-permeability form of edema.     

Increased fragility of pulmonary capillaries in newborn rabbit

The pulmonary capillaries of neonatal lungs are potentially vulnerable to stress failure because of the complex changes in the pulmonary circulation that occur at birth. We perfusion fixed the lungs from nine anesthetized newborn rabbits at capillary transmural pressures (P(tm)) of 5 +/- 5, 10 +/- 5, and 15 +/- 5 cmH(2)O. Normal microscopic appearances were seen at P(tm) values of 5 +/- 5 and 10 +/- 5 cmH(2)O, but massive airway edema was observed in lungs perfused at a P(tm) of 15 +/- 5 cmH(2)O. Consistent with this, no disruptions of the alveolar epithelium were observed at P(tm) values of 5 +/- 5 cmH(2)O, but mean values of 0.11 and 1.22 breaks/mm epithelium were found at P(tm) of 10 +/- 5 and 15 +/- 5 cmH(2)O, respectively (P < 0.05 for 5 +/- 5 vs. 15 +/- 5 cmH(2)O). These pressures are in striking contrast to those in the adult rabbit in which, by a similar procedure, a P(tm) of 52.5 cmH(2)O, is required before stress failure is consistently seen. We conclude that stress failure of pulmonary capillaries in newborn rabbit lungs can occur at P(tm) values of less than one-third of those that are required in adult lungs.     

Morpho-functional analysis of lung tissue in mild interstitial edema

Mild pulmonary interstitial edema was shown to cause fragmentation of interstitial matrix proteoglycans. We therefore studied compartmental fluid accumulation by light and electron microscopy on lungs of anesthetized rabbits fixed in situ by vascular perfusion after 0.5 ml.kg(-1).min(-1) iv saline infusion for 180 min causing approximately 6% increase in lung weight. Morphometry showed that a relevant portion (44%) of extravascular fluid is detected early in the alveolar septa, 85% of this fluid accumulating in the thick portion of the air-blood barrier. The arithmetic mean thickness of the barrier increased in interstitial edema from 1.06 +/- 0.05 (SE) to 1.33 +/- 0.06 microm. The harmonic mean thickness increased from 0.6 +/- 0.03 to 0.86 +/- 0.07 microm, mostly due to thickening of the thin portion causing an increase in gas diffusion resistance. Despite some structural damage, the air-blood barrier displays a relatively high structural resistance providing a safety factor against the development of severe edema. It is suggested that the increase in extra-alveolar perivascular space occurs as a consequence of fluid accumulation in the air-blood barrier.     

Pressure-flow behavior of pulmonary interstitium

A method to measure the pressure-flow behavior of the interstitium around large pulmonary vessels is presented. Isolated rabbit lungs were degassed, and the air spaces and vasculature were inflated with a silicon rubber compound. After the rubber had hardened the caudal lobes were sliced into 1-cm-thick slabs. Two chambers were bonded to opposite sides of a slab enclosing a large blood vessel and were filled with saline containing 3 g/dl albumin. The flow through the interstitium surrounding the vessel was measured at a constant driving pressure of 5 cmH2O and at various mean interstitial pressures. Flow decreased with a reduction of mean interstitial pressure and reached a limiting minimum value at approximately -9 cmH2O. The pressure-flow behavior was analyzed under the assumptions that the interstitium is a porous material described by a single permeability constant that increases with hydration and that the expansion of the interstitium with interstitial pressure was due to the elastic response of the surrounding rubber compound. This resulted in an interstitial resistance (reciprocal of permeability constant) of 1.31 +/- 1.03 (SD) cmH2O.h.cm-2 and a ratio of interstitial cuff thickness to vessel radius of 0.022 +/- 0.007 (SD), n = 11. The phenomenon of flow limitation was demonstrated by holding the upstream pressure constant at 15 cmH2O and measuring the flow while the downstream pressure was reduced. The flow was limited at downstream pressures below -10 cmH2O.     

Perialveolar interstitial resistance and compliance in isolated rat lung

We have developed a method to characterize fluid transport through the perialveolar interstitium using micropuncture techniques. In 10 experiments we established isolated perfused rat lung preparations. The lungs were initially isogravimetric at 10 cmH2O arterial pressure, 2 cmH2O venous pressure, and 5 cmH2O alveolar pressure. Perialveolar interstitial pressure was determined by micropuncture at alveolar junctions by use of the servo-null technique. Simultaneously a second micropipette was placed in an alveolar junction 20-40 microns away, and a bolus of albumin solution (3.5 g/100 ml) was injected. The resulting pressure transient was recorded for injection durations of 1 and 4 s in nonedematous lungs. The measurements were repeated after gross edema formation induced by elevated perfusion pressure. We model the interstitium as a homogeneous linearly poroelastic material and assume the initial pressure distribution due to the injection to be Gaussian. The pressure decay is inversely proportional to time, with time constant T, where T is a measure of the ratio of interstitial tissue stiffness to interstitial resistance to fluid flow. A linear regression was performed on the reciprocal of the pressure for the decaying portion of the transients to determine T. Comparing pressure transients in nonedematous and edematous lungs, we found that T was 4.0 +/- 1.4 and 1.4 +/- 0.6 s, respectively. We have shown that fluid transport through the pulmonary interstitium on a local level is sensitive to changes in interstitial stiffness and resistance. These results are consistent with the decreased stiffness and resistance in the perialveolar interstitium that accompany increased hydration.     

High lung volume increases stress failure in pulmonary capillaries.

We previously showed that when pulmonary capillaries in anesthetized rabbits are exposed to a transmural pressure (Ptm) of approximately 40 mmHg, stress failure of the walls occurs with disruption of the capillary endothelium, alveolar epithelium, or sometimes all layers. The present study was designed to test whether stress failure occurred more frequently at high than at low lung volumes for the same Ptm. Lungs of anesthetized rabbits were inflated to a transpulmonary pressure of 20 cmH2O, perfused with autologous blood at 32.5 or 2.5 cmH2O Ptm, and fixed by intravascular perfusion. Samples were examined by both transmission and scanning electron microscopy. The results were compared with those of a previous study in which the lung was inflated to a transpulmonary pressure of 5 cmH2O. There was a large increase in the frequency of stress failure of the capillary walls at the higher lung volume. For example, at 32.5 cmH2O Ptm, the number of endothelial breaks per millimeter cell lining was 7.1 +/- 2.2 at the high lung volume compared with 0.7 +/- 0.4 at the low lung volume. The corresponding values for epithelium were 8.5 +/- 1.6 and 0.9 +/- 0.6. Both differences were significant (P less than 0.05). At 52.5 cmH2O Ptm, the results for endothelium were 20.7 +/- 7.6 (high volume) and 7.1 +/- 2.1 (low volume), and the corresponding results for epithelium were 32.8 +/- 11.9 and 11.4 +/- 3.7. At 32.5 cmH2O Ptm, the thickness of the blood-gas barrier was greater at the higher lung volume, consistent with the development of more interstitial edema. Ballooning of the epithelium caused by accumulation of edema fluid between the epithelial cell and its basement membrane was seen at 32.5 and 52.5 cmH2O Ptm. At high lung volume, the breaks tended to be narrower and fewer were oriented perpendicular to the axis of the pulmonary capillaries than at low lung volumes. Transmission and scanning electron microscopy measurements agreed well. Our findings provide a physiological mechanism for other studies showing increased capillary permeability at high states of lung inflation.     

Alveolar liquid pressures in newborn and adult rabbit lungs

To study the effects of lung maturation and inflation on alveolar liquid pressures, we isolated lungs from adult and newborn rabbit pups (1-11 days old). We used the micropuncture technique to measure alveolar liquid pressure at several transpulmonary pressures on lung deflation. Alveolar liquid pressure was greater than pleural pressure but less than airway pressure at all transpulmonary pressures. Alveolar liquid pressure decreased further below airway pressure with lung inflation. At high transpulmonary pressure, alveolar liquid pressure was less in newborn than in adult lungs. To study the effects of edema, we measured alveolar liquid pressures in newborn lungs with different wet-to-dry weight ratios. Alveolar liquid pressure increased with progressive edema. In addition, we compared alveolar liquid and perivenular interstitial pressures in perfused newborn lungs and found that they were similar. Thus alveolar liquid pressure can be used to estimate perivenular interstitial pressure. We conclude that the transvascular pressure gradient for fluid flux into the interstitium might increase with lung inflation and decrease with progressive edema. Furthermore, this gradient might be greater in newborn than adult lungs at high inflation pressures.     

Effects of electric charge on hydraulic conductivity of pulmonary interstitium

The hydraulic conductivity of pulmonary interstitium was measured in a short isolated segment of interstitium surrounding a large pulmonary artery (1-3 mm diam) of the rabbit. The flow rate of the following solutions was measured sequentially: normal saline, polycation protamine sulfate (0.08 mg/ml), cationic dextran (0.1 or 1.5%) or anionic dextran (0.1 or 1.5%), and hyaluronidase (testes, 0.02%) solution. The pH of all solutions was adjusted to 7.35-7.40. The ratios of the flow of protamine sulfate and cationic dextran to that of saline averaged 2.3 +/- 0.92 (SD, n = 7) and 3.0 +/- 1.2 (n = 6), respectively. The anionic dextran-to-saline flow ratio averaged 0.72 +/- 0.28 (n = 13). Flow increased in the presence of positively charged molecules and decreased in the presence of negatively charged molecules. At a lower pH of 5.0-6.0, only 0.1% cationic dextran had an effect on interstitial conductivity. Thus pulmonary interstitium at physiological pH has the properties of a negatively charged membrane. The increased interstitial conductivity caused by the positively charged molecules was not observed after treatment with hyaluronidase. These effects of electric charge on interstitial conductivity were partly attributed to the presence in the interstitium of negatively charged hyaluronan.     

Effect of pancreatic and leukocyte elastase on hydraulic conductivity in lung interstitial segments.

Elastase-induced changes in flow were used to quantify the degradation of lung interstitial elastin. Degassed rabbit lungs were inflated with silicon rubber via airways and vessels. The lungs were cut into 1-cm-thick sections. Two chambers were bonded to each section to enclose the interstitium surrounding an arterial segment. Flow of albumin solution (0-5 g/dl) between the chambers was followed by that of the albumin solution with 0.25 g/dl pancreatic elastase solution. Driving pressure was 5 cmH(2)0, and mean interstitial pressure was either 0 or 10 cmH(2)O. Elastase caused an increase in flow in approximately 70% of the interstitial segments and a reduction in flow in the remaining segments. The elastase-induced response in flow was independent of both albumin concentration and mean interstitial pressure. Leukocyte elastase (5 units/dl) produced flow responses similar to those of 0.25 g/dl pancreatic elastase. The increased flow of leukocyte elastase was reduced by a subsequent flow with 0.25 g/dl pancreatic elastase but enhanced by a subsequent flow with a 10-fold lower concentration. A change in the order of the elastase flows reversed the concentration-dependent responses. This behavior suggests a complex interaction among the interstitial fibers after degradation by pancreatic and leukocyte elastase. Endogenous elastase-induced increases in interstitial permeability might affect blood-lymph barrier permeability, whereas elastase-induced cessation of flow might be related to the alveolar septal wall destruction observed in emphysema.     

Electron microscopic study of the open circulatory system of the shrimp,Caridina japonica. I. Gill capillaries

The ultrastructure of the phyllobranchiate type gill of the shrimp, Caridina japonica, was studied. The most characteristic feature of the open circulatory system of Cardina is the vascular lumen of the gill capillaries which is considered to be the interstitial space. The following observations substantiate this view: (1) a thin fibrous layer forms the innermost structure of the walls of gill capillaries and is in direct contact with the blood stream; (2) filaments in the fibrous layer are assumed to correspond to the reticular fibers in the interstitial space of the alveolar wall of mammals; (3) the absence of the endothelium as well as the endothelial basal lamina which are the essential structural components of the closed circulatory system in vertebrates. The gill epithelium contains intermediate, septate and tight junctions. The first two form a junctional complex near the apical cell border and may function as a permeability barrier by occluding the intercellular space as well as functioning in electrical coupling and cellular adhesion. The tight junction is spot-like and may serve no role in the function of the permeability barrier.     

Longitudinal distribution of pulmonary vascular pressures as a function of postnatal age in rabbits.

The major purpose of this study was to determine whether the longitudinal distribution of pulmonary vascular pressures changes with postnatal age in rabbits. Using the direct micropuncture technique, we measured pressures in 20- to 80-microns-diam arterioles and venules in isolated lungs of rabbits of different postnatal ages. To determine the contribution of vasomotor tone, we added the vasodilator papaverine to the perfusate of some lungs of each age group. We compared vascular pressures measured at blood flow rates chosen to approximate in vivo cardiac outputs. In untreated lungs, the resistance across 20- to 80-microns-diam microvessels decreased from 12- to 72-h-old (0.022 +/- 0.009 cmH2O.min.kg.ml-1) to 5- to 15-day-old rabbits (0.008 +/- 0.007 cmH2O.min.kg.ml-1) and remained at this lower level in adults (0.013 +/- 0.008 cmH2O.min.kg.ml-1). In contrast, in papaverine-treated lungs, the resistance across 20- to 80-microns-diam microvessels did not change between 12- to 72-h-old (0.007 +/- 0.005 cmH2O.min.kg.ml-1) and 5- to 15-day-old rabbits (0.005 +/- 0.002 cmH2O.min.kg.ml-1) but increased between 5- to 15-day-old and adult rabbits (0.014 +/- 0.007 cmH2O.min.kg.ml-1). Thus vasomotor tone contributed to the postnatal change in the distribution of vascular pressures across lungs of rabbits.     

Invited review: pulmonary capillary stress failure.

The pulmonary blood-gas barrier is an extraordinary bioengineering structure because of its vast area but extreme thinness. Despite this, almost no attention has been given to its mechanical properties. The remarkable area and thinness come about because gas exchange occurs by passive diffusion. However, the barrier also needs to be immensely strong to withstand the very high stresses in the capillary wall when capillary pressure rises during exercise. The strength of the thin region of the barrier comes from type IV collagen in the basement membranes. When the stresses in the capillary walls rise to high levels, ultrastructural changes occur in the barrier, a condition known as stress failure. Physiological conditions that alter the properties of the barrier include severe exercise in elite human athletes. Animals that have been selectively bred for high aerobic activity, such as Thoroughbred racehorses, consistently break their pulmonary capillaries during galloping. Pathophysiological conditions causing stress failure include high-altitude pulmonary edema and overinflation of the lung, which frequently occurs with mechanical ventilation. Remodeling of the capillary wall occurs in response to increased wall stress in diseases such as mitral stenosis. The barrier is able to maintain its extreme thickness with sufficient strength as a result of continual regulation of its wall structure. How it does this is a central problem in lung biology.     

Radial organization of interstitial exchange pathway and influence of collagen in synovium.

The synovial intercellular space is the path by which water, nutrients, cytokines, and macromolecules enter and leave the joint cavity. In this study two structural factors influencing synovial permeability were quantified by morphometry (Delesse's principle) of synovial electronmicrographs (rabbit knee), namely interstitial volume fraction Vv.1 and the fraction of the interstitium obstructed by collagen fibrils. Mean Vv.1 across the full thickness was 0.66 +/- 0.03 SEM (n = 11); but Vv.1 actually varied systematically with depth normal to the surface, increasing nonlinearly from 0.40 +/- 0.04 (n = 5 joints) near the free surface to 0.92 +/- 0.02 near the subsynovial interface. Tending to offset this increase in transport space, however, the space "blocked" by collagen fibrils also increased nonlinearly with depth. Bundles of collagen fibrils occupied 13.6 +/- 2.4% of interstitial volume close to the free surface but 49 +/- 4.8% near the subsynovial surface (full-thickness average, 40.5 +/- 3.5%), with fibrils accounting for 48.6-57.1% of the bundle space. Because of the two counteracting compositional gradients, the space available for fibril-excluded transport (hydraulic flow and macromolecular diffusion) was relatively constant > 4 microns below the surface but constricted at the synovium-cavity interface. The space available to extracellular polymers was only 51-53% of tissue volume, raising their effective concentration and hence the lining's resistance to flow and ability to confine the synovial fluid.     

Myocardial interstitial Cajal-like cells (ICLC) in caveolin-1 KO mice

We compared, by transmission electron microscopy (TEM), the ultrastructure of interstitial Cajal-like cells (ICLC) in normal mammalian myocardium versus caveolin-1 null mice. TEM showed that myocardial ICLCs of caveolin-1-deficient mice retain their main ultrastructural characteristics, for example, location among cardiomyocytes, close vicinity to nerves and/or blood capillaries, specialized cell-to-cell junctions, presence of 2–3 typical processes, which are very long (several tens of micrometres), but are very thin (0.1–0.2 μm) and moniliform. However, the most striking modification of myocardial ICLC in caveolin-1 KO mice was the absence of caveolae . Beyond this main observation, three other findings could be reported: (1) the absence of caveolae in capillary endothelium, (2) persistence of (some) caveolae at the level of cardiomyocte sarcolemma or vascular smooth muscle cell sarcolemma and (3) (un)expected ultrastructural modifications such as increased thickness of capillary basement membrane and increased autophagy of several cardiomyocytes.     

Type I cell-like morphology in tight alveolar epithelial monolayers

The pulmonary alveolar epithelium separates air spaces from a fluid-filled interstitium and might be expected to exhibit high resistance to fluid and solute movement. Previous studies of alveolar epithelial barrier properties have been limited due to the complex anatomy of adult mammalian lung. In this study, we characterized a model of isolated alveolar epithelium with respect to barrier transport properties and cell morphology. Alveolar epithelial cells were isolated from rat lungs and grown as monolayers on tissue culture-treated Nuclepore filters. On Days 2-6 in primary culture, monolayers were analyzed for transepithelial resistance (Rt) and processed for electron microscopy. Mean cell surface area and arithmetic mean thickness (AMT) were determined using morphometric techniques. By Day 5, alveolar epithelial cells in vitro exhibited morphologic characteristics of type I alveolar pneumocytes, with thin cytoplasmic extensions and protruding nuclei. Morphometric data demonstrated that alveolar pneumocytes in vitro develop increased surface area and decreased cytoplasmic AMT similar to young type I cells in vivo. Concurrent with the appearance of type I cell-like morphology, monolayers exhibited high Rt (greater than 1000 omega.cm2), consistent with the development of tight barrier properties. These monolayers of isolated alveolar epithelial cells may reflect the physiological and morphological properties of the alveolar epithelium in vivo.     

Morphology and morphometry of the normal lung of the adult vervet monkey (Cercopithecus aethiops)

The lungs of four adult specimens of the vervet monkey (Cercopithecus aethiops) have been examined by transmission and scanning electron microscopy. A morphometric evaluation of the structural components directly involved in gas exchange has been carried out and the data have been modelled to estimate the anatomical diffusing capacity of the lung. The upper air-conducting airways of the lung were lined by an epithelium characterized by ciliated cells among which were dispersed goblet cells. The alveolar surface was lined by squamous type I pneumocytes and cuboidal type II granular pneumocytes. The blood-gas (tissue) barrier consisted of an epithelial cell, a common basal lamina, and an endothelial cell in the thin parts of the interalveolar septum. In the thicker parts of the septum, an interstitial space interposed between the basal laminae of the epithelial and endothelial cells contained supportive elements such as collagen, elastic tissue, and fibrocytes. The alveoli, the blood capillaries, and septal tissue composed 73%, 16%, and 11%, respectively, of the parenchyma. The harmonic and arithmetic mean thicknesses of the blood-gas (tissue) barrier were 0.311 micron and 1.048 microns; the surface area of the blood-gas (tissue) barrier per unit body weight was 50 cm2g-1, and the surface density was 117 mm2.mm3-1. The weight-specific total morphometric diffusing capacity was 0.11 mlO2 (sec.mbar.kg)-1. In comparison, the pulmonary morphometric characteristics of vervet monkey lung were superior to those of the other primates (Macaca irus, M. mulatta, and Homo sapiens) for which equivalent data are available. The gas-exchange potential of the lungs of the nonhuman primates as revealed by morphometric studies surpasses that of man, a feature that can be attributed to the relatively less energetic human lifestyle.     

Ovulation and the mechanism of follicle rupture

Summary The rabbit Graafian follicles are encircled by a capillary network between the theca interna and the avascular membrana granulosa. After injection of an ovulatory dose of human chorionic gonadotrophin (HCG) the theca interna cells showed an increase in the amount of smooth endoplasmic reticulum, lipid droplets and mitochondria with tubular cristae. In addition, considerably more junctions, similar to the abutment nexuses of granulosa cells were found; annular nexuses also appeared. At 4 hours after injection of HCG a prominent oedema was evident in the theca interna layer, particularly in the apical region.Small fenestrations in the endothelium of the blood capillaries increased in amount after HCG injection, and close to the time of ovulation, large gaps or perforations, 1–3 in diameter, were found in the thin, distended part of the endothelial cells. The surrounding basement membrane became fragmented and partly lost, so that a seemingly free passage from the capillary lumen to the interstitium was eventually established. Leakage of fluid, causing interstitial oedema, presumably proceeds until the pressure in the pericapillary interstitium has risen to the pressure in the capillaries. Some hours before and up to ovulation the pericapillary interstitium has also broad communications with the cavity of the follicles. Therefore, both pressure and fluid can be passed from the capillaries-via the interstitium-to the follicle antrum. However, influx of fluid with subsequent follicle expansion and ovulation-at constant pressure-does not occur until the tensile strength of the follicle wall has decreased.This investigation was supported by grants from the Swedish Medical Besearch Council (Projects No. B72-12X-78-07A, B73-12X-78-08B and B74-12X-78-09C). The technical assistance of Miss Ingalis Fransson, Miss Kerstin Nilsson, and Mrs. Ulla-Britt Westman is greatly appreciated.     

Regulation of brain water during acute hyperosmolality in ovine fetuses, lambs, and adults.

In adult rats, when plasma osmolality increases, water flows across the blood-brain barrier down its concentration gradient from brain to plasma, and brain volume deceases. The brain responds to this stress by gaining osmotically active solutes, which limit water loss. This phenomenon is termed brain volume (water) regulation. We tested the hypothesis that brain volume regulation is more effective in young lambs and adult sheep than in fetuses, premature lambs, and newborn lambs. Brain water responses to acute hyperosmolality were measured in the cerebral cortex, cerebellum, and medulla of fetuses at 60 and 90% of gestation, premature ventilated lambs at 90% of gestation, newborn lambs, young lambs at 20-30 days of age, and adult sheep. After exposure of the sheep to increases in systemic osmolality with mannitol plus NaCl, brain water content and electrolytes were quantified. The ideal osmometer is a system in which impermeable solutes do not enter or leave in response to an osmotic stress. There were significant differences from an ideal osmometer in the cerebral cortex of fetuses at 90% of gestation, cerebral cortex, and cerebellum of newborn lambs, and cerebral cortex, cerebellum, and medulla of young lambs and adult sheep; however, there were no differences in the brain regions of fetuses at 60% of gestation and premature lambs, cerebellum and medulla of fetuses at 90% of gestation, and medulla of newborn lambs. We conclude that 1) brain water loss is maximal and brain volume regulation impaired in most brain regions of fetuses at 60 and 90% of gestation and premature lambs; 2) brain volume regulation develops first in the cerebral cortex of the fetuses at 90% of gestation and in the cerebral cortex and cerebellum of newborn lambs, and then it develops in the medulla of the lambs at 20-30 days of age; 3) brain water loss is limited and volume regulation present in the brain regions of young lambs and adult sheep; and 4) the ability of the brain to exhibit volume regulation develops in a region- and age-related fashion.     

Biosynthesis of prostaglandins and thromboxane B2 by fetal lung homogenates

The conversion of arachidonic acid to prostaglandins (PG's) and thromboxane B2 (TXB2) was investigated in homogenates from fetal and adult bovine and rabbit lungs. Adult bovine lungs were very active in converting arachidonic acid (100 microgram/g tissue) to both PGE2 (10.7 microgram/g tissue) and TXB2 (6.2 microgram/g tissue. Smaller amounts of PGF2alpha (0.9 microgram/g) and 6-oxoPGF1alpha were formed. Homogenates from fetal calf lungs during the third trimester of pregnancy were quite active in converting arachidonic acid to PGE2, but formed very little TXB2, PGF2alpha or 6-oxoPGF1alpha. Homogenates from rabbit lungs converted arachidonic acid (100 microgram/g) mainly to PGE2, both before and after birth. The amount of PGE2 formed increased during gestation to a maximum of about 6 microgram/g tissue at 28 days of gestation. It then decreased to a minimum (1.5 microgram/g) which was observed 8 days after birth, followed by an increase to about 4 microgram/g in older rabbits.