Abstract
The principal function of the circulatory system is to transport molecules, both nutritive and informational, to the various tissues of the body. In trying to understand this process, early physiologic experiments (Pappenheimer et al., 1951; Landis and Pappenheimer, 1963; Renkin, 1964) established that the exchange process was mediated by a semipermeable “membrane.” That is, molecular exchange between the blood and tissue spaces takes place across a selective barrier that on the one hand allows the free exchange of molecules less than 45 Å in diameter (Landis and Pappenheimer, 1963) and on the other hand restricts the movement of larger diameter molecules (Garlick and Renkin, 1970; Landis and Pappenheimer, 1963). The discontinuous nature of molecular transport across this “membrane” has been explained by assuming that exchange occurs through pores of two general classes: small pores (diam. ∼90 Å; freq. 15–20/µm2) and large pores (diam. ∼500–700 Å; freq. 1/15–20 µm2) (Landis and Pappenheimer, 1963; Simionescu et al., 1976a; Lassen and Trap-Jensen, 1970). This theory has been developed in recent years to explain the differing permeabilities of the various vascular compartments; more permeable compartments such as those found in the liver and adrenal cortex have more pores of both classes, whereas relatively impermeable compartments such as those found in the brain (Crone and Lassen, 1969; Simionescu et al., 1976a) have fewer pores.
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Anderson, R.G.W. (1981). Cell Surface Membrane Structure and the Function of Endothelial Cells. In: Schwartz, C.J., Werthessen, N.T., Wolf, S. (eds) Structure and Function of the Circulation. Springer, Boston, MA. https://doi.org/10.1007/978-1-4615-7927-4_4
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