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Transport experimental

Table 1 summarizes several of the experimental methods discussed in this chapter. A need exists for new or revised methods for transport experimentation, particularly for therapeutic proteins or peptides in polymeric systems. An important criterion for the new or revised methods includes in situ sampling using micro techniques which simultaneously sample, separate, and analyze the sample. For example, capillary zone electrophoresis provides a micro technique with high separation resolution and the potential to measure the mobilities and diffusion coefficients of the diffusant in the presence of a polymer. Combining the separation and analytical components adds considerable power and versatility to the method. In addition, up-to-date separation instrumentation is computer-driven, so that methods development is optimized, data are acquired according to a predetermined program, and data analysis is facilitated. [Pg.122]

Miller, C.L., Day, T.A., Bennett, J.L. and Rax, R.A. (1996) Schistosoma mansoni L glutamate-induced contractions in isolated muscle fibers evidence for a glutamate transporter. Experimental Parasitology 84, 410—41 9. [Pg.385]

Further demonstrations of this sort of counterflow phenomenon for many different substrates in virtually every type of cell have been used as functional hallmarks of carrier-mediated transport. Experimental demonstration of this effect precludes transport being mediated either by simple diffusion or by fixed pores in the membrane. In reviewing 20 years of experimental work related to the carrier hypothesis, LeFevre (1975) lists a number of key functional properties of carrier mediated transport, all of which have stood the test of the subsequent 20 years. These include saturation of transport with increased substrate concentration and associated phenomena such as competition between similar substrates, high rates of unidirectional transport, and countertransport. Also covered are flux coupling (including trans effects and cotransport), chemical specificity, inhibition by protein-specific reagents, hormonal regulation, and a steep dependence of the rate of transport on temperature (included only to bemoan its common inclusion in textbooks ). [Pg.250]

Uglem, G. L. Prior, D. J. (1980). Hymenolepis diminuta chloride fluxes and membrane potentials associated with sodium-coupled glucose transport. Experimental Parasitology, 50 287-94. [Pg.362]

Friedman PA (2000) Mechanisms of renal calcium transport. Experimental Nephrology 8,343-50. [Pg.424]

Skaggs, T.H., Wilson G.V., Shouse P.J., and Leij F.J., 2002. Solute transport experimental methods, in Methods of Soil Analysis, Part 4, Physical Methods, Dane, J.H. and Topp, G.C., Eds., Soil Science Society of America, Madison, WI, pp. 1381-1402. [Pg.103]

The efficiency of oxidative phosphorylation is determined by the P/O ratio, which is a measure of the molecules of ATP made per pair of electrons carried through the electron transport. Experimentally, researchers isolate mitochondria from cells, then use oxygen electrodes to determine the amount of ATP synthesized per oxygen molecule reduced to water molecules in the last step of the electron transport system. [Pg.2255]

Generation of Charge Carriers and Charge Transport Experimental Methods... [Pg.234]

Generation of Charge Carriers and Charge Transport Experimental Methods 239 8.4.2.1 Intrinsic Charge Carrier Separation... [Pg.239]

Figure 3.7. Test of linear phenomenological equation for mass transport - Experimental values and theoretical values. Figure 3.7. Test of linear phenomenological equation for mass transport - Experimental values and theoretical values.
This general analysis of the chlorine-toluene system based upon first order reacticxi was developed in parallel with a series of experimental measurements (9), in which chlorine was absorbed in toluene in a laminar jet. This absorption device provides remarkable control of surface area and with a flat velocity profile the penetration time is reasonably well defined so that the penetration theory can be directly applied without any uncertainty concerning the complications of convective transport. Experimental mixing cup temperatures for Cl -toluene ranged from i C to 6°C. These can be interpreted as the amount of heat accumulated per unit of Jet surface as the jet plunges into the receiver via the equation... [Pg.199]


See other pages where Transport experimental is mentioned: [Pg.366]    [Pg.91]    [Pg.293]    [Pg.74]    [Pg.75]    [Pg.83]    [Pg.109]    [Pg.18]    [Pg.83]    [Pg.264]    [Pg.38]    [Pg.105]    [Pg.57]   
See also in sourсe #XX -- [ Pg.73 , Pg.84 ]




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