By G E W Wolstenholme
Chapter 1 Chairman's advent (pages 1–2): C. G. Caro
Chapter 2 Interstitial Fluid Pressure?Volume Relationships and Their law (pages 3–24): Arthur C. Guyton
Chapter three idea of movement and delivery methods in Pores and Porous Media (pages 25–48): J. R. Philip
Chapter four alternate of gear via Capillary partitions (pages 49–66): Eugene M. Renkin
Chapter five The Mechanics of the crimson phone when it comes to Its provider functionality (pages 67–84): Alan C. Burton
Chapter 6 movement in slim Capillaries from the point of view of Lubrication concept (pages 85–104): M. J. Lighthill
Chapter 7 The move Behaviour of Particulate Suspensions (pages 105–129): S. G. Mason and H. L. Goldsmith
Chapter eight stream of Human Blood in Glass and Plastic Fibres: A Filmed learn (pages 130–135): E. W. Merrill, H. J. Meiselman, E. R. Gilliland, T. okay. Sherwood and E. W. Salzman
Chapter nine The optimal Elastic homes of Arteries (pages 136–152): M. G. Taylor
Chapter 10 Pressure?Flow family in Small Blood Vessels (pages 153–171): C. G. Caro, M. F. Sudlow, T. H. Foley and A. Ur
Chapter eleven pace Distribution and Transition within the Arterial method (pages 172–202): D. L. Schultz, D. S. Tunstall?Pedoe, G. de J. Lee, A. J. Gunning and B. J. Bellhouse
Chapter 12 The Distribution of gasoline circulate in Lungs (pages 203–214): J. Mead
Chapter thirteen Behaviour of Airborne debris within the breathing Tract (pages 215–235): Bernard Altshuler
Chapter 14 Turbulent movement and Particle Deposition within the Trachea (pages 236–255): P. R. Owen
Chapter 15 Pulmonary Capillary movement, Diffusion air flow and gasoline alternate (pages 256–276): John B. West, Jon B. Glazier, John M. B. Hughes and John E. Maloney
Chapter sixteen Diffusive and Convective circulate of gasoline within the Lung (pages 277–297): L. E. Farhi
Chapter 17 normal dialogue (pages 298–301):
Chapter 18 Chairmen's remaining comments (pages 302–304): C. G. Caro and M. J. Lighthill
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Extra info for Ciba Foundation Symposium - Circulatory and Respiratory Mass Transport
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Guyton: One could also expect even more negative interstitial fluid pressure in the lung than elsewhere, because the capillary pressure is lower; this may be why we record lung interstitial fluid pressures as low as - 16 mm. Hg in a few animals. This is much lower than we ever record in other tissues. Cumming: This would accord with the clinical observations of the resorption of pleural exudates. West:The relevant capillary pressure in the lung will depend on the part of the lung where you implant the capsule, being lowest at the top and highest at the bottom of the lung.
29, 593-597). Your calculation is valid if you assume an equilibrium, but we may not have an exact equilibrium and the lungs may be gaining water from the upper respiratory tract, contrary to the usual textbook statements. Guyton: Just as Starling’s equilibrium in the capillary has to take into account the fluid that becomes lymph, we have to consider the net exchange of fluid in the lung. One can calculate from available data that the amount of non-equilibrium at the peripheral capillary due to lymphatic flow is normally less than 0 5 mm.