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Measurement regimes

in which paths from an isotherm at temperature Tj to an isotherm at T2 arrive at the same point, P, in the pressure-composition space from very different starting points, according to the constraint. [Pg.177]

Pressure-composition isotherms may be constructed under an isochoric constraint by adding hydrogen aliquots to the system and measuring the hydrogen absorption or desorption stepwise, or under an isobaric constraint by actively controlling the pressure over the sample to a constant value while the sample absorbs or desorbs. [Pg.177]

2 Delineation of isochoric, isobaric and isoplethic approaches to the same point P on a pressure-composition isotherm at temperature 72, starting from an isotherm at a higher temperature T.  [Pg.178]

3 Isochoric approach to equilibrium compared to a real isobaric isotherm for the LaNi5-H2 system in which the gas pressure was increased then decreased by a few kPa under active pressure control to within a few Pa. The point at which the isochore is tangent to the isobaric curve defines the isochoric isotherm, which therefore lies below the isobaric isotherm. The experimental data are from Gray (1992). [Pg.179]

A fourth regime worthy of consideration is constant molar flow, particularly for investigating the kinetics of hydrogen absorption and desorption. In this case a flow controller could be used to control and measure the flow of gas to the sample cell (but see also Section 7.7) with the pressure in the sample cell used as a measure of the chemical potential required to force the hydrogenation reaction at the measured rate. [Pg.179]


Another conductivity mechanism could be suggested for LB films of this polymer with Ag+ cations. Such cations can accept or release electrons easily, so in the layer of such cations the conductivity could be caused by electron transitions between the ions with different degrees of oxidation. With tunneling microscopy an anomaly in the dl/dV(V) curves near zero bias was discovered for the LB films in Ag form with an odd number of layers there was a conductivity peak some 150-200 mV wide (Figure 7.4, Curves 1, 3) but no anomaly for these same films with an even number of layers (Figure 7.4, Curve 2). For LB films with an odd number of layers the ordered superstructure of the scale 11.5 x 11.5 x lO cm has been found in a conductivity dl/dV (x,y) measurement regime. The scale of such a structure corresponds to 3 x 2 surface reconstruction (Figure 7.5). [Pg.106]

Figure 7.S. Photo of the surface of LB film of three layers in the conductivity dI/dV(x,y) measurement regime dimension is 70 x 74 x 10 8cm gray range of brightness corresponds to relative units U = -50 mV, / = 0.8 nA, 17 = 50 mV... Figure 7.S. Photo of the surface of LB film of three layers in the conductivity dI/dV(x,y) measurement regime dimension is 70 x 74 x 10 8cm gray range of brightness corresponds to relative units U = -50 mV, / = 0.8 nA, 17 = 50 mV...
In a similar way to mediators, enzymes may be covalently bound to electrode surfaces, thus giving enzyme-chemically modified electrodes (ECME). When enzymes and mediators are coimmobilized, addition of auxiliary substances during the measuring process can be avoided a reagentless measuring regime becomes feasible (Fig. 19). [Pg.31]

The great number of patents and publications and of available commercial analyzers indicate the leading position of amperometric glucose sensors. These sensors allow a simple measuring regime and make use of the advantages of Faradaic electrode processes, such as independence of buffer capacity, linear concentration dependence, and high sensitivity in substrate measurement. [Pg.93]

In conjunction with appropriate measuring regimes not only does a much wider range of analyte species becomes in this way accessible to measurement by the bioelectroanalytical approach also the selectivity and sensitivity of the biosensor may be enhanced through the appropriate choice of the coupling strategy [2,14],... [Pg.5739]

A subtle, but very effective option to shift a thermally almost silent interaction (low enthalpy output) into a well-measurable regime opens up when supramolecular binding involves the simultaneous transfer of protons. Of course, the participation and couphng to protonation equilibria requires strong buffers to maintain a fixed proton concentration however, if the main event releases (or takes up) protons, they must react also with the buffer species. The observable enthalpy output A/Aobs results from the overlay of the intrinsic heat of the supramolecular interaction AH up, the change in the protonation state of the partners on... [Pg.364]

Represents one of the most common measurement regimes in which the deformation rate is set to a constant value, de/dt = const, and the force, F, necessary to keep the sample in equilibrium is measured with a dynamometer. If this force is measured in reference to the initial cross section of the... [Pg.204]


See other pages where Measurement regimes is mentioned: [Pg.233]    [Pg.237]    [Pg.5]    [Pg.116]    [Pg.26]    [Pg.443]    [Pg.102]    [Pg.225]    [Pg.292]    [Pg.177]    [Pg.178]    [Pg.189]    [Pg.189]    [Pg.200]    [Pg.441]    [Pg.444]    [Pg.16]    [Pg.399]    [Pg.58]    [Pg.1129]    [Pg.5732]    [Pg.173]    [Pg.441]    [Pg.624]    [Pg.246]    [Pg.273]    [Pg.350]    [Pg.98]   


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Flow regime measurements

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