By G E W Wolstenholme
Chapter 1 Chairman's creation (pages 1–2): C. G. Caro
Chapter 2 Interstitial Fluid Pressure?Volume Relationships and Their legislation (pages 3–24): Arthur C. Guyton
Chapter three concept of move and delivery tactics 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 pink cellphone with regards to Its service functionality (pages 67–84): Alan C. Burton
Chapter 6 movement in slim Capillaries from the viewpoint of Lubrication idea (pages 85–104): M. J. Lighthill
Chapter 7 The stream 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 research (pages 130–135): E. W. Merrill, H. J. Meiselman, E. R. Gilliland, T. okay. Sherwood and E. W. Salzman
Chapter nine The optimal Elastic houses of Arteries (pages 136–152): M. G. Taylor
Chapter 10 Pressure?Flow relatives in Small Blood Vessels (pages 153–171): C. G. Caro, M. F. Sudlow, T. H. Foley and A. Ur
Chapter eleven speed Distribution and Transition within the Arterial approach (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 fuel move in Lungs (pages 203–214): J. Mead
Chapter thirteen Behaviour of Airborne debris within the respiration Tract (pages 215–235): Bernard Altshuler
Chapter 14 Turbulent circulate and Particle Deposition within the Trachea (pages 236–255): P. R. Owen
Chapter 15 Pulmonary Capillary movement, Diffusion air flow and fuel alternate (pages 256–276): John B. West, Jon B. Glazier, John M. B. Hughes and John E. Maloney
Chapter sixteen Diffusive and Convective flow of gasoline within the Lung (pages 277–297): L. E. Farhi
Chapter 17 normal dialogue (pages 298–301):
Chapter 18 Chairmen's last feedback (pages 302–304): C. G. Caro and M. J. Lighthill
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Additional resources for Ciba Foundation Symposium - Circulatory and Respiratory Mass Transport
38,288-298. HONERT, T. H. VAN DEN (1948). Discuss. ,3, 146-153. JACOBSON, H. (1860). Arch. Anat. , 80-112. , and USSING, H. H. (1953). Acta physiol. , 28, 60-76. KOV~SZNAY, L. S. G. (1948). Proc. Camb. phil. math. phys. , 44,58-62. KUHN,W. (1951). Z . , 55,207-217. LANDIS, E. , and PAPPENHEIMER, J. R. (1963). In Handbook ofPhysiology, Section 2: Circulation, vol. 11,pp. 961-1033, ed. Hamilton, W. F. and DOW,P. C. : American Physiological Society. J. , and POPLE,J. A. (1951). Proc. R. SOC. A, 205,155-162.
3b). Evidently the longitudinal spread of the dispersion would, in this case, be proportional to the time since the initial state. Molecular diffusionmodifies the longitudinal dispersion process profoundly, Fig. 3c gives a simplified picture of this. The convective motion sets up radial concentration gradients in the tube which, in a gross sense, produce diffusive transport outward downstream of the centre of gravity and inward transport in the upstream region. In both regions diffusion tends to move material into parts of the cross-section where the convective motion is directed back towards the centre of gravity.
We may get a first intimation of the difference in character between tube flow and medium flow by considering the fate of a small parcel of fluid moving through each system. In the tube the parcel possesses a constant linear velocity throughout, while in the medium it is subject to accelerations which continuously change both the magnitude and direction of its velocity. This vital difference finds quantitative expression in the 1,000 to 1 ratio of the critical Reynolds numbers for failure of linearity of the two systems (Muskat, 1937; Goldstein, 1938).