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The effects of lung afferents denervation on cardiovascular regulation can be assessed on bilateral lung transplantation patients. The high-frequency component of heart rate variability is known to be synchronous with breathing frequency. Then, if heart beat is neurally modulated by breathing frequency, we may expect disappearance of high frequency of heart rate variability in bilateral lung transplantation patients. On 11 patients and 11 matching healthy controls, we measured R-R interval (electrocardiography), blood pressure (Portapres® ) and breathing frequency (ultrasonic device) in supine rest, during 10-min free breathing, 10-min cadenced breathing (0·25 Hz) and 5-min handgrip. We analysed heart rate variability and spontaneous variability of arterial blood pressure, by power spectral analysis, and baroreflex sensitivity, by the sequence method. Concerning heart rate variability, with respect to controls, transplant recipients had lower total power and lower low- and high-frequency power. The low-frequency/high-frequency ratio was higher. Concerning systolic, diastolic and mean arterial pressure variability, transplant recipients had lower total power (only for cadenced breathing), low frequency and low-frequency/high-frequency ratio during free and cadenced breathing. Baroreflex sensitivity was decreased. Denervated lungs induced strong heart rate variability reduction. The higher low-frequency/high-frequency ratio suggested that the total power drop was mostly due to high frequency. These results support the hypothesis that neural modulation from lung afferents contributes to the high frequency of heart rate variability.

The objectives to determine both the contribution to orthostatic intolerance (OI) of calf venous volume during a stand-test, and the effects of a combined eccentric-concentric resistance exercise countermeasure on both vein response to orthostatic test and OI, after 90-day head-down tilt bed-rest (HDT). The subjects consisted of a control group (Co-gr, n = 9) and an exercise countermeasure group (CM-gr, n = 9). Calf volume and vein cross-sectional area (CSA) were assessed by plethysmography and echography during pre- and post-HDT stand-tests. From supine to standing (post-HDT), the tibial and gastrocnemius vein CSA increased significantly in intolerant subjects (tibial vein, +122% from pre-HDT; gastrocnemius veins, +145%; P < 0.05) whereas it did not in tolerant subjects. Intolerant subjects tended to have a higher increase in calf filling volume than tolerant subjects, in both sitting and standing positions. The countermeasure did not reduce OI. Absolute calf volume decreased similarly in both groups. Tibial and gastrocnemius vein CSA at rest did not change during HDT in either group. During the post-HDT stand-test, the calf filling volume increased more in the CM-gr than in the Co-gr both in the sitting (+1.3 +/- 5.1%, vs. -7.3 +/- 4.3%; P < 0.05) and the standing positions (+56.1 +/- 23.7% vs. +1.6 +/- 9.6%; P < 0.05). The volume ejected by the muscle venous pump increased only in the CM-gr (+38.3 +/- 21.8%). This study showed that intolerant subjects had a higher increase in vein CSA in the standing position and a tendency to present a higher calf filling volume in the sitting and standing positions. It also showed that a combined eccentric-concentric resistance exercise countermeasure had no effects on either post-HDT OI or on the venous parameters related to it.

A model of the metabolic internal power (Eint) during cycling, which includes the gravity acceleration (ag) as a variable, is presented. This model predicts that Eint is minimal in microgravity (0 g; g=9. 81 m s-2), and increases linearly with ag, whence the hypothesis that the oxygen uptake (VO2) during cycling depends on ag. Repeated VO2 measurements during steady-state exercise at 50, 75 and 100 W on the cycle ergometer, performed in space (0 g) and on Earth (1 g) on two subjects, validated the model. VO2 was determined from the time course of decreasing O2 fraction during rebreathing. The gas volume during rebreathing was determined by the dilution principle, using an insoluble inert gas (SF6). Average VO2 for subject 1 at each power was 0.99, 1.21 and 1.52 L min-1 at 1 g (n=3) and 0.91, 1.13 and 1.32 L min-1 at 0 g (n=5). For subject 2 it was 0.90, 1.12 and 1. 42 L min-1 at 1 g, and 0.76, 0.98 and 1.21 L min-1 at 0 g. These values corresponded to those predicted from the model. Although resting VO2 was lower at 0 g than at 1 g, the net (total minus resting) exercise VO2 was still smaller at 0 g than at 1 g. This difference reflects the lower Eint at 0 g.

1. Endurance athletes (E) undergo a marked reduction of arterial O2 saturation (Sa,O2) at maximal exercise in normoxia, which disappears when they breathe hyperoxic mixtures. In addition, at a given level of hypoxia, the drop in maximal O2 consumption (VO2,max) is positively related to the individual normoxic VO2,max. 2. These data suggest that the curve relating VO2,max to PI,O2 may be steeper and perhaps less curved in E than in sedentary subjects (S) with low VO2,max values because of the greater hypoxaemia in the latter, whence the hypotheses that (i) the relationship between VO2,max and PI,O2 may be set by the shape of the oxygen equilibrium curve; and (ii) the differences between E and S may be due to the different position on the oxygen equilibrium curve on which these subjects operate. These hypotheses have been tested by performing a systematic comparison of the VO2,max or Sa,O2 vs. PI,O2 relationships in E and S. 3. On ten subjects (five S and five E), VO2,max was measured by standard procedure during cycloergometric exercise. Sa,O2 was measured by finger-tip infrared oximetry. Arterialized blood PO2 (Pa,O2) and PCO2 (Pa,CO2) were determined in 80 microliters blood samples from an ear lobe. The subjects breathed ambient air or a N2-O2 mixture with an inspired O2 fraction (FI,O2) of 0.30, 0.18, 0.16, 0.13 and 0.11, respectively, VO2,max was normalized with respect to that obtained at the highest FI,O2. 4. The relationships between Sa,O2 or normalized VO2,max and FI,O2 (or PI,O2) had similar shapes, the data for E being systematically below and significantly different from those for S. Linear relationships between Sa,O2 and normalized VO2,max, statistically equal between E and S, were found. 5. We conclude that the relationships between either VO2,max or Sa,O2 and FI,O2 (or Pa,O2) may indeed be the mirror images of one another, implying a strict link between the decrease of VO2,max in hypoxia and the shape of the oxygen equilibrium curve, as hypothesized.