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Changes in microvascular fluid filtration capacity during 120 days of 6° head-down tilt
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     1 Clinic of Anaesthesiology and 4 Institute of Surgical Research, University of Munich, 81366 Munich, Germany;

    2 Department of Paediatrics, Imperial College School of Medicine, London SW10 9NH, Great Britain;

    3 Institute of Biomedical Problems, Moscow 123007, Russia

    ABSTRACT

    We used venous congestion strain gauge plethysmography (VCP) to measure the changes in fluid filtration capacity (Kf), isovolumetric venous pressure (Pvi), and blood flow in six volunteers before, on the 118th day (D118) of head-down tilt (HDT), and 2 days after remobilization (Post). We hypothesized that 120 days of HDT cause significant micro- and macrovascular changes. We observed a significant increase in Kf from 3.6 ± 0.4 × 103 to 5.7 ± 0.9 × 103 ml · min1 · 100 ml1 · mmHg1 (+51.4%; P < 0.003), which returned to pretilt values (4.0 + 0.4 × 103 ml · min1 · 100 ml1 · mmHg1) after remobilization. Similarly, Pvi increased from 13.4 ± 2.1 mmHg to 28.9 ± 2.8 mmHg (+105.8%; P < 0.001) at D118 and was not significantly different at Post (12.4 ± 2.6 mmHg). Blood flow decreased significantly from 2.3 ± 0.3 to 1.3 ± 0.2 ml · min1 · 100 ml tissue1 at D118 and was found elevated to 3.4 ± 0.7 ml · min1 · 100 ml tissue1 at Post. We believe that the increased Kf is caused by a higher microvascular water permeability. Because this may result in edema formation, it could contribute to the alterations in fluid homeostasis after exposure to microgravity.

    keywords:microgravity; fluid filtration capacity; microvascular permeability; head-down tilt

    INTRODUCTION

    COSMONAUTS AND ASTRONAUTS returning from a prolonged period in microgravity frequently show orthostatic dysregulation, which can cause cardiovascular instability and collapse of the subject in response to a postural challenge (2, 10, 14). A 6° head-down tilt (HDT) is an established model of simulated weightlessness (18). Profound fluid shifts occur within hours of exposure to both microgravity and simulated microgravity environments, with an initial cephalic fluid shift causing relative hypervolemia in the upper part of the body (9, 22). This was found to be counteracted by a compensatory fluid loss over the ensuing week, resulting in a 14-16% reduction in plasma volume (8). Thereafter, plasma volume remained relatively constant, and hematocrit stabilized at a lower value as part of the well-documented space-related anemia (22). The initial edema, which is always observed in both simulated and true microgravity, may be due to changes in the forces described by the Starling equation (16). However, to date, there have been no reports of systematic investigations into changes in the microvascular permeability coefficients, the osmotic reflection coefficient (), and the hydraulic permeability during microgravity exposure.

    We sought to address these questions by using a venous congestion strain gauge plethysmography (VCP) technique and protocol (13) that enables assessment of changes in both microvascular and compliance characteristics of lower limbs. We studied fluid filtration capacity (Kf), an index of microvascular water permeability, and isovolumetric venous pressure (Pvi), which we used to describe the dynamic balance of Starling forces at the microvascular interface. Altered vascular compliance was also thought to be a factor that might contribute to the control of local transvascular forces. Venous compliance has been shown to increase during the first 3-4 wk of HDT (7), as well as after exposure to actual microgravitation (21). However, subsequent studies showed that, after an initial increase in compliance, the value started to decrease after a transient plateau phase when the HDT period was increased to 6 wk (18). We hypothesized that 120 days of continuous 6° HDT causes significant micro- and macrovascular changes, namely an increase in microvascular permeability, a decrease in arterial blood flow, and, contrary to previous reports, also a decrease in venous compliance in the calves of human volunteers.

    METHODS

    The study was approved by the local ethical committee of the Russian Space Agency and the Institute of Biomedical Problems, Moscow, responsible for the medical care of cosmonauts. The experiments were part of a joint research activity of the Russian Space Agency, the European Space Agency, the Japanese Space Agency, and the German Space Agency.

    The investigations were performed on six healthy 25- to 42-yr-old male volunteers (age 30.8 ± 7.5 yr, weight 79.5 ± 7.1 kg, height 180.7 ± 5.2 cm; means ± SE) who gave written, informed consent. Subjects were selected from more than 300 volunteers after an extended physical examination procedure as used by the Russian Space Agency before entering a volunteer into the cosmonaut training program.

    All subjects were under permanent medical supervision during the 6-mo period encompassing the 120-day test. After the control period of 7 days, all subjects were placed on a modified hospital bed, which sustained 6° HDT. This position was strictly maintained throughout the 120 days, including sleep, food intake, and daily hygiene, with the exception of a few experiments requiring an upright position. VCP measurements were conducted 7 days before the start of the HDT, on the 118th day of the 120-day HDT, and 2 days after remobilization.

    VCP. We used a computer-assisted strain gauge plethysmography technique and a small cumulative pressure step protocol to determine Kf from the relationship between congestion cuff pressure and fluid filtration into the limb (13). The studies were bilateral and the strain gauges (measurement accuracy < 5 μm) fixed onto the limbs at a site of known circumference. The gauges were then pre-tensioned such that the calibration procedure, comprising application of cumulative, known, small (~2 mm) increases and decreases in length, gave a uniform and repeatable signal. The gauges were then rebalanced in the Wheatstone bridge circuit at this ideal tension. After an equilibration period of 15 min, the venous congestion cuff, placed around the thigh, was inflated by using six to eight small (8.0-mmHg) cumulative pressure steps. The highest congestion pressure used did not exceed the subjects' diastolic blood pressure.

    Determination of Kf and venous compliance. Kf and venous compliance were determined by using the method previously described by Gamble et al. (13). When cuff pressure is increased, by small cumulative steps, to a value in excess of the subject's existing venous pressure at the level of the strain gauge, a rapid volume change is recorded, which achieves a steady-state value [asymptotic volume (Va)] at each pressure. Va reflects filling of the compliant vessels of the limb. Each compliance response to a small pressure step can, typically, be described by an exponential function, with a time constant <13 s (4, 13). Once the congestion pressure also exceeds the value required to induce net fluid filtration, the volume increase comprises two components: the rapid initial compliance function together with a slow, steady-state volume change attributable to fluid filtration. The analysis program uses an exponential fitting routine, which allows us to distinguish between the two components. When the vascular compliance data are plotted with respect to applied pressure, a curvilinear relationship is usually seen, which reflects the compliance of the low-pressure vessels and the surrounding tissue. The relationship between cuff pressure and fluid filtration is linear, once the existing balance of the Starling forces is exceeded. The slope of this function is the Kf, and the intercept represents the Pvi, the cuff pressure that has to be applied to induce net fluid filtration into the tissue (13). This pressure intercept, which is the product of the and plasma colloid osmotic pressure, is equivalent to the effective osmotic pressure at the microvascular interface in the calf.

    Arterial blood flow (a) to the limb was determined from the initial slope of the volume response to a large pressure step (>33 mmHg). Blood flow was routinely measured before and then after completion of the small cumulative pressure step protocol (12).

    Brachial arterial blood pressure and heart rate, oxygen saturation, end-tidal CO2, respiration rate, skin temperature, and room temperature were measured every 2 min throughout the protocol by using a Siemens SC 9000 monitor (Siemens, Munich, Germany) to ensure a comparable physiological state at the different measurement points. At the end of the study, all data were saved to disk for subsequent off-line analysis.

    Measurements were obtained 7 days before (D0) and on the 118th day of 6° HDT (D118) as well as 2 days after remobilization (Post).

    Statistical analysis. Data are given as mean values ± SE. We obtained bilateral measurements of Kf, Pvi, and a, of which the mean value was taken as an individual data point for each subject.

    Statistical comparisons of data were made by using the repeated-measures analysis of variance (RmA) for multiple comparisons, with the D118 and Post values from each study being compared against their own D0 value. Significance was assumed at P < 0.05.

    RESULTS

    The baseline hemodynamic data obtained in the supine position, which are given in Table 1, show that no significant changes in heart rate; systolic, mean, and diastolic blood pressure; or respiration rate and oxygen saturation were seen at the three stages of the study. End-tidal CO2, however, was significantly lower after 118 days HDT (Table 1).

    VCP. After 118 days of HDT, there was a significant reduction in calf circumference (P < 0.001; RmA). However, after only 2 days of remobilization, the calf circumference had returned to a value that was not significantly different from the pre-HDT control value (Table 2). Limb a decreased significantly from 2.3 ± 0.3 to 1.3 ± 0.2 ml · min1 · 100 ml tissue1 at D118 and was found elevated to 3.4 ± 0.7 ml · min1 · 100 ml tissue1 2 days after remobilization (Fig. 1).

    Figure 2 illustrates the individual changes in vascular compliance that occurred after 118 days of HDT. It also shows the restitution of this function after only 2 days of remobilization. A quantitative assessment of these changes was obtained by comparing the Va that occurred at the pressure closest to 50 mmHg during the cumulative pressure step protocol in each study. The means ± SE of the Va and corresponding congestion cuff pressure data are given in Table 2. Whereas the D118 value was significantly less than that at D0 (P < 0.01; RmA), D0 and Post values were not significantly different from one another.

    We observed a significant increase in Kf from 3.6 ± 0.4 × 103 to 5.7 ± 0.9 × 103 ml · min1 · 100 ml1 · mmHg1 (+51.4%; P < 0.003) at D118 which decreased to 4.0 ± 0.4 × 103 ml · min1 · 100 ml1 · mmHg1 2 days after remobilization (Fig. 3). Pvi also increased from a value of 13.4 ± 2.1 mmHg before HDT to 28.9 ± 2.8 mmHg (+105.8%; P < 0.001) at D118 and decreased to 12.4 ± 2.6 mmHg at 2 days post-HDT (Fig. 4). Thus, within 2 days of remobilization, both Kf and Pvi values were not significantly different from the D0 control values.

    There was no significant correlation between Kf, a, and Pvi at any of the time points measured.

    DISCUSSION

    Our data showed that, after 118 days, HDT steady-state peripheral arterial blood flow and venous compliance were decreased and both Kf and Pvi were elevated. However, all measured parameters showed an almost complete restitution 2 days after the return from simulated microgravity.

    Kf and Pvi. Kf, the filtration capacity, is the product of the total surface area available for fluid filtration per 100 ml soft tissue and the permeability of the microvessels per unit surface area. It describes the increase in fluid filtration after a local elevation of microvascular hydrostatic pressure induced by a venous congestion pressure cuff (13). Pvi is the equilibrium pressure at the microvascular interface, which has to be exceeded to achieve net fluid filtration. It is equivalent to the product of plasma colloid osmotic pressure and the coefficient () that describes the effective microvascular permeability to proteins. The relationship between these parameters is described by the Starling equation (20)

    (1)

    where Jv is the fluid filtration, P represents the hydrostatic and the colloid osmotic (oncotic) pressures, and the subscripts c and t the intraluminal and interstitial microvascular environments, respectively. In the light of Eq. 1, the higher Kf values found on the 118th day, in the present study, could be caused by 1) an increased microvascular permeability to water (filtration coefficient, Kf), 2) an increased surface area available for fluid filtration, or 3) a decreased lymphatic flow.

    By contrast, the observed changes in Pvi could be attributed to 1) a decrease in microvascular permeability to proteins, i.e., an increase in the protein reflection coefficient () or 2) either a systemic or a local increase in plasma oncotic pressure.

    Leach et al. (17) used increased microvascular permeability to water to explain the discrepancy in the fluid balance of astronauts after their exposure to microgravity environments. Many factors have been shown to cause such changes, in particular free oxygen radicals, activated leukocytes or thrombocytes, and a variety of mediators like tumor necrosis factor- and interleukins. The data from this study presented by Chouker et al. (3) confirms this hypothesis, and we believe, in agreement with Leach et al., that an increased permeability to water is the most likely cause of the observed increased Kf. Other mechanisms, however, also have to be considered.

    Because Kf is the product of the mean permeability per unit surface area and the total surface area available for filtration, an increase in the available area is a theoretical cause for the higher Kf after 118 days. In an earlier publication (11), our laboratory provided evidence that, in healthy supine controls, the microvascular surface area available for filtration assessment was not influenced by challenges giving rise to extremes of vasomotor control. We deduced that, in healthy controls, the whole microvascular surface was available for assessment using this technique. Studies have shown that, after 30 days of HDT, leg volume decreased by 9.9%; half of this could be attributed to the muscle compartment (7, 15). Nuclear magnetic resonance investigations corroborated these observations, showing a decrease in muscle mass of 8.2 ± 1.2% in control subjects, compared with only 5.8 ± 1.5% in a group using countermeasures. These changes correlated well with observations on venous distensibility that were made on the same subjects (18). It is now well established that calf muscle mass decreases in both real as well as simulated weightlessness, and the significant reduction in calf circumference during exposure to HDT and hypokinesia found in this study is in good agreement with previous reports. With respect to the changes in Kf, however, it is noteworthy that in animal experiments the number of capillaries decreased in skeletal muscle during the exposure to microgravity (15). Thus the surface area available for fluid filtration decreases, resulting in a lower measured Kf. With this in mind, the increased Kf at the 118th day can therefore not be explained by the changes in surface area but most likely represent an underestimation of the true increase in microvascular permeability. Because no morphometric data are currently available on the change in the actual number of microvessels perfused in humans after exposure to microgravity, more experiments are needed to confirm this hypothesis.

    A decrease in lymphatic flow is another mechanism that might contribute to the measured increased net fluid flux, as described by Kf. The basic limb lymph flow during rest is known to be very low indeed. Moreover, the changes that might occur in response to factors that could upregulate it, like the application of a venous congestion pressure, may take hours to reach a new steady state (1). Although unlikely, the contribution of a reduced lymphatic flow to the measured increase in Kf has to be considered and could in part explain the rapid normalization of the Kf value after remobilization.

    Pvi. There have been no direct measurements of the plasma protein permeability coefficient during prolonged exposure to either real or simulated microgravity environments. In the present study, venous plasma oncotic pressure was not measured. Hsieh et al. (16), however, showed that plasma oncotic pressure increased from 23 to 30 mmHg after 14 days of 6° HDT. Because we have previously shown that an increased plasma oncotic pressure causes a similar change in Pvi (5), we believe that this may be the main cause for the elevated Pvi found at D118. Moreover, we have postulated that high values of Pvi may be associated with factors giving rise to a simultaneous decrease in microvascular plasma flow and an increase in the filtration force of the hydrostatic pressure of the intraluminal environment. Such changes might be brought about by venular leukocyte-endothelial interaction, leading to a flow-limited exchange, which results in a high local oncotic pressure (6) and hence a high Pvi.

    Venous compliance. There have been a number of studies on the changes in venous compliance after periods of 6° HDT. It has been shown that compliance increases during the first weeks of both HDT and actual weightlessness (7, 19). Louisy et al. (19) investigated the venous outflow dynamics after 41 days of HDT. They found that, after an increase in venous compliance by 67% of the prebedrest value, the compliance decreased after the 26th day of HDT to a value that was only slightly higher than that obtained pretilt. Louisy et al. suggested that studies on longer periods of HDT were necessary to clarify the late changes in venous compliance that they had observed. We did not investigate the early changes in venous compliance; our data, however, support the contention that the late decrease in venous compliance described by Louisy et al. continues, and, on the 118th day, venous distensibility is in fact reduced compared with control values. Louisy et al., using an optoelectronic sensor, also showed that leg volume decreased rapidly within 24 h of imposing HDT and continued to decrease in the ensuing 3 wk to a 13% reduction on the 41st day of HDT. They speculated that the initial change in leg volume may be due to a cephalic intravascular fluid shift followed by changes in interstitial and later intracellular fluid volume. The decrease in leg volume only correlated with the changes in venous compliance during the first phase of the study period (up to day 28). This observation supports our contention that there may be a time-related change in venous compliance during simulated microgravity. Orthostatic intolerance after prolonged exposure to microgravity has been frequently attributed to the increase in venous compliance (7, 19). Our observation and those of Louisy et al., however, suggest that this may not be the case for periods of more than 40 days. After this period, other mechanisms, like the cardiovascular deconditioning syndrome or the suggested reduction in venous smooth muscle tone, may play a more important role (19).

    Changes in arterial blood flow after 118 days of 6° HDT. In a 41-day HDT study, Louisy and co-workers (19) showed that arterial blood flow decreased from 2.1 to 1.1 ml · min1 · 100 ml tissue1 on the 40th day to reach a significantly higher value of 2.8 ml · min1 · 100 ml tissue1 on the third day of remobilization. We also found a reduction in arterial blood flow after 118 days of HDT; moreover, the values reached a significantly higher level after the volunteers had resumed normal daily activity. The absolute values obtained in both studies were comparable but low with respect to previous reported values in healthy volunteers (12). We suspect that remaining immobile in a 6° HDT for 118 days results not only in muscular atrophy but also in a downregulation of the skeletal muscle blood flow of the leg. Because we found no obvious correlation between the changes in Kf and blood flow, we assume that the changes in the macro- and microcirculation occur independently from each other.

    Limitations of the study. In this study, no representative control group was included. This was due to the extreme nature of the study but limits the results because the observed changes in microvascular parameters could also be due to alterations in the experimental conditions over time. Although great care was undertaken to not change the study environment and conditions, this could, however, not be wholly excluded because of the length of the study period.

    In summary, the present study provides evidence that profound microcirculatory changes occur during simulated microgravity. The increase in Kf and Pvi, as well as the decrease in venous compliance, may play a role in the fluid shift and the orthostatic dysregulation encountered after exposure to microgravity. In addition, because cosmonauts and astronauts are exposed to a high radiation load, which is known to increase microvascular permeability, the routine measurement of the permeability values characterized by Kf and seems a valuable procedure for the assessment of the microcirculatory risks associated with these procedures. This appears to be of even greater relevance in view of long-term missions planned both by the NASA and the Russian Space Agency.

    ACKNOWLEDGEMENTS

    This study was supported by Deutsches Zentrum für Luft- und Raumfahrt Grant 50-WB9654 and by Siemens AG, Germany.

    FOOTNOTES

    Address for reprint requests and other correspondence: F. Christ, Clinic of Anaesthesiology, Ludwig Maximilians Univ. Munich, 81366 Munich, Germany (E-mail: frank.christ@ana.med.uni-muenchen.de).

    The costs of publication of this article were defrayed in part by the payment of page charges. The article must therefore be hereby marked "advertisement" in accordance with 18 U.S.C. Section 1734 solely to indicate this fact.

    Received 15 April 2001; accepted in final form 27 July 2001.

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