1,721,063 research outputs found
The major limitation to exercise performance in COPD is inadequate energy supply to the respiratory and locomotor muscles.
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Effect of hyperinflation and equalization of abdominal pressure on diaphragmatic action
No full textWe tested the hypothesis that the mechanical arrangement of costal (COS) and crural (CRU) diaphragms can be changed from parallel to series when direct or indirect transmission of tension occurs. Ratio of rib cage to abdominal displacement (RC/AB) resulting from separate COS and CRU stimulations were used to measure RC expanding action. Hyperinflation in six dogs caused RC/AB with COS and CRU stimulations to change progressively from 0.53 +/- 0.07 (SE) and 0.03 +/- 0.05 at functional residual capacity (FRC) to -0.48 +/- 0.08 and -0.46 +/- 0.05 at 68% inspiratory capacity, respectively. Liquid substitution of abdominal contents in six other dogs equalized abdominal pressure swings (delta Pab), without changing chest wall elastic properties or geometry, or costal RC/AB (0.35 +/- 0.07 before and 0.33 +/- 0.06 after) but caused crural RC/AB to change from 0.01 +/- 0.05 to 0.31 +/- 0.01. We conclude that hyperinflation changes fiber orientation, allowing direct transmission of tension between COS and CRU, which become linked mechanically in series (the diaphragm acts as a unit with RC deflating action); and equalization of delta Pab causes indirect transmission of tension between COS and CRU, which become linked in series (the diaphragm acts as a unit with RC inflating action)
Chest wall and lung volume estimation by optical reflectance motion analysis.
No full text Cala, S. J., C. M. Kenyon, G. Ferrigno, P. Carnevali, A. Aliverti, A. Pedotti, P. T. Macklem, and D. F. Rochester. Chest wall and lung volume estimation by optical reflectance motion analysis. J. Appl. Physiol. 81(6): 2680–2689, 1996.—Estimation of chest wall motion by surface measurements only allows one-dimensional measurements of the chest wall. We have assessed an optical reflectance system (OR), which tracks reflective markers in three dimensions (3-D) for respiratory use. We used 86 (6-mm-diameter) hemispherical reflective markers arranged circumferentially on the chest wall in seven rows between the sternal notch and the anterior superior iliac crest in two normal standing subjects. We calculated the volume of the entire chest wall and compared inspired and expired volumes with volumes obtained by spirometry. Marker positions were recorded by four TV cameras; two were 4 m in front of and two were 4 m behind the subject. The TV signals were sampled at 100 Hz and combined with grid calibration parameters on a personal computer to obtain the 3-D coordinates of the markers. Chest wall surfaces were reconstructed by triangulation through the point data, and chest wall volume was calculated. During tidal breathing and vital capacity maneuvers and during CO2-stimulated hyperpnea, there was a very close correlation of the lung volumes (Vl) estimated by spirometry [Vl(SP)] and OR [Vl(OR)]. Regression equations of Vl(OR) ( y) vs. Vl(SP) ( x,btps in liters) for the two subjects were given by y = 1.01 x − 0.01 ( r = 0.996) and y = 0.96 x + 0.03 ( r = 0.997), and by y = 1.04 x + 0.25 ( r = 0.97) and y = 0.98 x + 0.14 ( r = 0.95) for the two maneuvers, respectively. We conclude spirometric volumes can be estimated very accurately and directly from chest wall surface markers, and we speculate that OR may be usefully applied to calculations of chest wall shape, regional volumes, and motion analysis. </jats:p
Pleural pressure from abdominal to pulmonary rib cage: sweep of the lung border
No full textPleural pressure was measured by a capsule placed in the superior part of right 8th or 9th intercostal space of dogs in left lateral posture. Transit of lung border was observed through endothoracic fascia at sides of the capsule. During inspiration the capsule membrane faced sequentially: diaphragm, lung border, lung; vice versa during expiration. Pressure on the diaphragm at end expiration was -5.3 +/- 0.5 cm H2O, reflecting outward recoil of the rib cage. At transit of lung border during inspiration (bor. I) a marked negative pressure spike occurred; a smaller spike occurred at expiratory transit (bor. E). These spikes should reflect pleural liquid pressure at lung border. At bor. I lung volume and radial displacement of rib 9 or 10 were greater during active than passive ventilation, whereas at bor. E they were similar under both conditions. Hence, during spontaneous inspiration displacement of lung border lags behind lung and rib expansion. Speed of lung border (assessed from duration of negative spike) ranged from 0.8 to 2.3 cm/sec during spontaneous breathing. On average it was similar at bor. I and bor. E, while air flow was greater at bor. I
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