The initial adsorption kinetics in stagnant flow of both rigid spherical po
ly(propylene imine) dendrimers as well as of flexible branched poly(ethylen
e imine) with similar building-blocks on glass are quantitatively described
as Smoluchowski-Levich convective-diffusion-controlled up to concentration
s C-b approximate to 10 mg/L using a sticking probability beta, defined as
the ratio between the experimental adsorption rate and the theoretical pred
iction. This parameter beta accounts for the nonideality of the substrate:
There is only a limited amount of surface sites in the glass get-layer avai
lable for adsorption, and this affects the collision efficiency. beta is on
the order of 0.03 for the small spheres and 0.8 for the flexible polyelect
rolyte, perfectly in line with the expectation that the flexible polyelectr
olyte, able to conform along the surface, has a much higher chance of findi
ng a site within its contact area than the small dendrimers. At higher conc
entrations, the experimental data no longer show the predicted linear conce
ntration dependence. Whereas for parallel plate flow studies in the literat
ure the breakdown can be related to the neglect of transient concentration
effects in mass transport using the Smoluchowski-Levich approach, for stagn
ant flow, such a simple relation does not exist. It is calculated for the l
atter setup that the time scales needed for the concentration to settle thr
oughout the cell would be longer for the larger poly(ethylene imine) than f
or the dendrimers. This is in contrast with the experimentally observed tre
nd: time scales over which deviations between the Smoluchowski-Levich appro
ximation and the data occur are longer for the faster diffusing dendrimers
than for PEI, and the breakdown can thus at least not directly be related t
o transient concentration terms. It is suggested that the large difference
in the sticking probability of these different types of materials on glass
has to be taken into account in a complete numerical analysis of the mass t
ransport equation, especially at short time scales.