A theoretical model was developed to relate the size selectivity of the glo
merular barrier to the structural characteristics of the individual layers
of the capillary wall. Thicknesses and other linear dimensions were evaluat
ed, where possible, from previous electron microscopic studies. The glomeru
lar basement membrane (GBM) was represented as a homogeneous material chara
cterized by a Darcy permeability and by size-dependent hindrance coefficien
ts for diffusion and convection, respectively; those coefficients were esti
mated from recent data obtained with isolated rat GEM. The filtration slit
diaphragm was modeled as a single row of cylindrical fibers of equal radius
but nonuniform spacing. The resistances of the remainder of the slit chann
el, and of the endothelial fenestrae, to macromolecule movement were calcul
ated to be negligible. The slit diaphragm was found to be the most restrict
ive part of the barrier. Because of that, macromolecule concentrations in t
he GEM increased, rather than decreased, in the direction of flow. Thus the
overall sieving coefficient (ratio of Bowman's space concentration to that
in plasma) was predicted to be larger for the intact capillary wall than f
or a hypothetical structure with no GBM. In other words, because the slit d
iaphragm and GBM do not act independently, the overall sieving coefficient
is not simply the product of those for GEM alone and the slit diaphragm alo
ne. Whereas the calculated sieving coefficients were sensitive to the struc
tural features of the slit diaphragm and to the GEM hindrance coefficients,
variations in GEM thickness or filtration slit frequency were predicted to
have little effect. The ability of the ultrastructural model to represent
fractional clearance data in vivo was at least equal to that of conventiona
l pore models with the same number of adjustable parameters. The main stren
gth of the present approach, however, is that it provides a framework for r
elating structural findings to the size selectivity of the glomerular barri
er.