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 conception of stream and delivery strategies in Pores and Porous Media (pages 25–48): J. R. Philip
Chapter four alternate of drugs via Capillary partitions (pages 49–66): Eugene M. Renkin
Chapter five The Mechanics of the pink mobile in terms of Its service functionality (pages 67–84): Alan C. Burton
Chapter 6 movement in slender Capillaries from the point of view of Lubrication concept (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 move of Human Blood in Glass and Plastic Fibres: A Filmed learn (pages 130–135): E. W. Merrill, H. J. Meiselman, E. R. Gilliland, T. ok. Sherwood and E. W. Salzman
Chapter nine The optimal Elastic houses of Arteries (pages 136–152): M. G. Taylor
Chapter 10 Pressure?Flow kinfolk 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 process (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 circulation 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 circulation and Particle Deposition within the Trachea (pages 236–255): P. R. Owen
Chapter 15 Pulmonary Capillary move, 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 stream of gasoline within the Lung (pages 277–297): L. E. Farhi
Chapter 17 common dialogue (pages 298–301):
Chapter 18 Chairmen's final comments (pages 302–304): C. G. Caro and M. J. Lighthill
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Additional info for Ciba Foundation Symposium - Circulatory and Respiratory Mass Transport
J. gen. , 1-15. STARLING, E. H. (1896). J. , 24, 317-330. STOKES,C. G. (1845). Trans. phil. ,8,287-305. TAYLOR, G. I. (1923). Phil. , Ser. 6, 46,671-674. TAYLOR, G. I. (1953). Proc. R. A , 219,186-203. TAYLOR, G. I. (1954). Proc. R. A , 225,473-477. USSMG, H . H. (1952). Adv. , 13,21-65. J . W. (1947). J. Res. narn. Bur. , 38,169-183. WESTHAVER, WHALLEY, E. (1967). A. phys. , 18,205-232. DISCUSSION Safman: One should perhaps issue a warning that a two-dimensional model is not a good approximation for treating diffusion in porous media.
Iii) The velocity profiles deviate strongly from the Poiseuille parabolic profile (and exhibit points of inflexion related to the maxima of and shearing stress away from the wall). < It must be recognized that the somewhat startling nature of Figs. l b and c arises, in part, from the singularities associated with the point source and sink. It appears, however, that a more realistic representation of the entrance and exit flows would leave us with the same qualitative picture in the broader parts of the pore: velocity profiles with points of inflexion, and, associated with these, maxima of vorticity and shearing stress away from the walls and reversal of potential gradients near the walls.
A) -CONVECTION TO LEFT + CONVECTION -CONVECTION $ RIGHT ____c TO LEFT DISPERSION ABOUT C. OFG. c TO LEFT t t I I I t INWARD DIFFUSION OUTWARD DIFFUSION INWARD DIFFUSION OUTWARD DIFFUSION t 34 J. R. e. in the absence of diffusion) the dispersion about the centre of gravity would consist of transport downstream in the central core and of transport upstream in the outer zone adjoining the wall (see Fig. 3b). Evidently the longitudinal spread of the dispersion would, in this case, be proportional to the time since the initial state.