Behaviour of biofilm systems under varying hydrodynamic conditions.

Heterotrophic biofilms were cultivated in long-term experiments in biofilm tube reactors. During the biofilm cultivation the substrate loading of glucose was kept constant while the hydrodynamic conditions were changed stepwise. To describe the behaviour of the biofilm structure under these varying flow conditions the mass transfer and transport at the bulk/biofilm interface and inside the biofilm was investigated with oxygen microelectrodes. Furthermore, the biofilm density was used to describe the biofilm compactness before and after the change of the hydrodynamic condition. The obtained results show that the biofilm density and also the substrate flux decreased with decreasing flow velocity in the bulk phase. Additionally the slope of the oxygen concentration profiles decreased and the thickness of the concentration boundary layer increased. On the other hand, increasing the flow velocity in the bulk phase led both to a higher biofilm density and a higher maximum substrate flux. The biofilm surface became more homogenous and the thickness of the concentration boundary layer decreased. The time for adaptation of the biofilm structure after changing the hydrodynamic conditions ranged between 1 and 3 weeks.     

Electron mobility in an AlGaN/GaN two-dimensional electron gas. I. Carrier concentration dependent mobility

The transport properties of two-dimensional electron gas (2-DEG) at the AlGaN/GaN interface were studied by characterizing the 2-DEG mobility dependence on carrier concentration, n/sub s/, and temperature. High-quality AlGaN/GaN heterostructures were grown, and heterostructure field effect transistors (HFETs) using a Fat FET geometry were fabricated. Measurements of 2-DEG mobility were performed by magnetoresistance and capacitance-conductance. In order to understand the dominant transport factors, the mobility was modeled using different scattering mechanisms and compared to our results. It is found that mobility dependence on n/sub s/ shows a bell-shape behavior over the whole temperature range. For low n/sub s/ the mobility is dominated by Coulomb interaction from interface charge, and at high n/sub s/ the mobility is dominated by interface roughness. Using previously reported experimental values of interface charge and interface roughness in our modeling, we show good agreement with mobility measurement results. Scattering from interface states in AlGaN/GaN heterostructures, seems to be related to the high polarization field in the heterointerface. At temperatures higher than 200K polar optical phonon scattering dominates the transport, yet both interface charge and roughness affect the mobility at the low and high n/sub s/, respectively.     

Vasoactive intestinal polypeptide (VIP) innervation of rat spleen, thymus, and lymph nodes

In the thymus, VIP-positive (+) fibers were found in the capsular/septal system, cortex, and medulla. In the spleen, VIP+ nerves coursed along large arteries and central arterioles, and in the white pulp, venous/trabecular system, and red pulp. Splenic VIP innervation was more robust in Long-Evans hooded rats than in Fischer 344 rats. VIP+ nerves in mesenteric lymph nodes were found in the cortex, and along the cortical vasculature and medullary cords. No VIP innervation was observed in popliteal lymph nodes. Immunocytes also were VIP+, suggesting that both neural and cellular synthesis of VIP contributes to VIP concentration in lymphoid organs. Surgical sympathectomy did not alter splenic or thymic VIP content, respectively, and VIP innervation of these organs was not altered, suggesting an origin for VIP+ nerves other than the sympathetic nervous system.     

Evaluation of the AnaeroPack system for growth of anaerobic bacteria

Growth of anaerobic bacteria in the AnaeroPack (Mitsubishi Gas Chemical America, Inc., New York, N.Y.) anaerobic atmosphere generation systems, both the AnaeroPack jar and pouch and the AnaeroPack in a GasPak jar were considered equivalent to or better than growth obtained in the corresponding GasPak jar or pouch system (Becton Dickinson Microbiology Systems, Cockeysville, Md.) for 89 (86%) of the 103 anaerobes tested. There were a total of 26 discrepancies after 48 h of incubation, with 16 discrepancies unresolved after 96 h of incubation. The AnaeroPack jar and pouch never failed to reduce the anaerobic indicator. The AnaeroPack systems are easy to use and performed at least as well as or better than the BBL GasPak systems for growth of anaerobic bacteria.     

Molecular analysis of ligand binding to the second cluster of complement-type repeats of the low density lipoprotein receptor-related protein. Evidence for an allosteric component in receptor-associated protein-mediated inhibition of ligand binding

The low density lipoprotein receptor-related protein (LRP), a member of the low density lipoprotein receptor gene family, mediates the cellular uptake of a diversity of ligands. A folding chaperone, the 39-kDa receptor-associated protein (RAP) that resides in the early compartments of the secretory pathway inhibits the binding of all ligands to the receptor and may serve to prevent premature binding of ligands to the receptor during the trafficking to the cell surface. To elucidate the molecular interactions that underlie the interplay between the receptor, RAP, and the ligands, we have analyzed and delineated the binding sites of plasminogen activator inhibitor-1 (PAI-1), tissue-type plasminogen activator (t-PA).PAI-1 complexes, RAP, and the anti-LRP Fab fragment Fab A8. To that end, we have generated a series of soluble recombinant fragments spanning the second cluster of complement-type repeats (C3-C10) and the amino-terminal flanking epidermal growth factor repeat (E4) of LRP (E4-C10; amino acids 787-1165). All fragments were expressed by stably transfected baby hamster kidney cells and purified by affinity chromatography. A detailed study of ligand binding to the fragments using surface plasmon resonance revealed the presence of three distinct, Ca2+-dependent ligand binding sites in the cluster II domain (Cl-II) of LRP. t-PA.PAI-1 complexes as well as PAI-1 bind to a domain located in the amino-terminal portion of Cl-II, spanning repeats E4-C3-C7. Adjacent to this site and partially overlapping is a high affinity RAP-binding site located on repeats C5-C7. Fab A8, a pseudo-ligand of the receptor, binds to a third Ca2+-dependent binding site on repeats C8-C10 at the carboxyl-terminal end of Cl-II. Next, we studied the RAP-mediated inhibition of ligand binding to LRP and to Cl-II. As expected, we observed a strong inhibition of t-PA.PAI-1 complex and Fab A8 binding to LRP by RAP (IC50 congruent with 0.3 nM), whereas in the reverse experiment, competition of t-PA. PAI-1 complexes and Fab A8 for RAP binding to LRP could only be shown at high concentrations of competitors (>/=1 microM). Interestingly, even though the equilibrium dissociation constants for the binding of RAP to LRP and to Cl-II are similar, the binding of the ligands to Cl-II is only prevented by RAP at concentrations that are at least 2 orders of magnitude higher than those required for inhibition of ligand binding to LRP. Our results favor models that propose RAP-induced allosteric inhibition of ligand binding to LRP that may require LRP moieties that are located outside Cl-II of the receptor.