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Diamond transport properties

In the modem era, this basic phenomenology of coupled water transport has been confirmed in a variety of tissues. For example, Diamond [2-4] studied the transport properties of the fish gallbladder. In his experiments the gallbladder was excised from the fish and suspended in a relatively large bath so that the composition of both luminal and (serosal) bath solutions could be controlled. Volume transport out of the lumen was manifest as weight loss of the gallbladder lifted out of the bath. Fig. 1 shows the results of a study of the effect of osmotic gradients on transepi-... [Pg.311]

West G.D., Diamond G.G., Holland D., Smith M.E., Lewis M.H. Gas transport mechanisms through sol-gel derived templated membranes. J. Membr. Sci. 2002 203 53-69 Wu J.C.S., Sabol H., Smith G.W., Flowers D.L. Characterization of hydrogen-permselective microporous ceramic membranes. J. Membr. Sci. 1994 96 275-287 Xomeritakis G., Naik S., Braunbarth C.M., Cornelius C.J., Pardey R., Brinker C.J. Organic-templated silica membranes I. Gas and vapor transport properties. J. Membr. Sci. 2003 215 225-233... [Pg.1366]

Containers less than bulk must bear the red diamond-shaped "FLAMMABLE LIQUID" label. Bulk containers must display the red "FLAMMABLE" placard in association with the UN1090 identification. Fire is the main ha2ard in emergencies resulting from spills. Some manufacturers provide transportation emergency response information. A listing of properties and ha2ard response information for acetone is pubHshed by the U.S. [Pg.96]

Compared to conventional (macroscopic) electrodes discussed hitherto, microelectrodes are known to possess several unique properties, including reduced IR drop, high mass transport rates and the ability to achieve steady-state conditions. Diamond microelectrodes were first described recently diamond was deposited on a tip of electrochemically etched tungsten wire. The wire is further sealed into glass capillary. The microelectrode has a radius of few pm [150]. Because of a nearly spherical diffusion mode, voltammograms for the microelectrodes in Ru(NHy)63 and Fe(CN)64- solutions are S-shaped, with a limiting current plateau (Fig. 33a), unlike those for macroscopic plane-plate electrodes that exhibit linear diffusion (see e.g. Fig. 18). The electrode function is linear over the micro- and submicromolar concentration ranges (Fig. 33b) [151]. [Pg.253]

C. E. Nebel, Transport and Defect Properties of Intrinsic and Boron-Doped Diamond MiloS Neslddek, Ken Haenen and Milan VanSSek, Optical Properties of CVD Diamond Rolf Sauer, Luminescence from Optical Defects and Impurities in CVD Diamond... [Pg.198]

Activation and conductivity at room temperature are problems that can be addressed by the incorporation of other electronic structures that increase carrier transport. Crystal morphology is an important parameter in the boron doping process to determine uncompensated acceptors (Aa-Ad) for different crystal facets as a function of doping concentration. The temperature coefficient of resistance for a CVD diamond film can be changed by boron doping. As conductivity depends on the crystal phase, the combined electromechanical properties can be exploited in sensor applications both for resistive temperature detectors and for pressure transdu-cers. " As electrical conductivity is related linearly with boron concentration, a better-controlled process may allow for the development of better semiconductor devices improving crystal quality and operating limits. ... [Pg.692]

Carbon (element No. 6 in the periodic table) forms a variety of materials, including graphite, diamond, carbon fibers, charcoal, as well as newly discovered nanocarbon materials, such as fullerene, graphene, carbon nanotube, and graphene nanoribbon (GNR). Even though all are composed of the same atoms, different carbon materials can show very different physical and chemical properties, including electrical transport, optical and thermal properties, and chemical reactivity, depending on their structures. [Pg.1]

The classical approach of conduction does not include the above time lag concept or the wavelike response. It expects a delta function-like response of temperature without any time lag with respect to the applied heat pulse. In the classical approach, we use phenomenological models which do not require any knowledge of the mechanism of energy transport or the microstructure of the solids. Fourier s law of heat conduction uses thermal conductivity as a material property which is a function of temperature. This thermal conductivity depends on the microstructure of the solids, which the thermal conductivity data does not show. For example, thermal conductivity of diamond can span an order of magnitude depending on the type of microstructure obtained by chemical vapor deposition. Thermal conductivity of natural... [Pg.303]


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See also in sourсe #XX -- [ Pg.595 ]

See also in sourсe #XX -- [ Pg.595 ]




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