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Measuring active

Operation and Control. Control of a chromium phosphate conversion coating bath requires monitoring chromium and aluminum concentrations, active fluoride level, and temperature. Coating weight is very sensitive to active, ie, uncomplexed, fluoride. An innovative electrochemical method using a siHcon electrode (25) is employed for measuring active fluoride. A special precaution in chromium phosphate bath operation is the... [Pg.223]

Electrochemical cells may be used in either active or passive modes, depending on whether or not a signal, typically a current or voltage, must be actively appHed to the cell in order to evoke an analytically usehil response. Electroanalytical techniques have also been divided into two broad categories, static and dynamic, depending on whether or not current dows in the external circuit (1). In the static case, the system is assumed to be at equilibrium. The term dynamic indicates that the system has been disturbed and is not at equilibrium when the measurement is made. These definitions are often inappropriate because active measurements can be made that hardly disturb the system and passive measurements can be made on systems that are far from equilibrium. The terms static and dynamic also imply some sort of artificial time constraints on the measurement. Active and passive are terms that nonelectrochemists seem to understand more readily than static and dynamic. [Pg.49]

Following the general trend of looldng for a molecular description of the properties of matter, self-diffusion in liquids has become a key quantity for interpretation and modeling of transport in liquids [5]. Self-diffusion coefficients can be combined with other data, such as viscosities, electrical conductivities, densities, etc., in order to evaluate and improve solvodynamic models such as the Stokes-Einstein type [6-9]. From temperature-dependent measurements, activation energies can be calculated by the Arrhenius or the Vogel-Tamman-Fulcher equation (VTF), in order to evaluate models that treat the diffusion process similarly to diffusion in the solid state with jump or hole models [1, 2, 7]. [Pg.164]

Microactivity Test (MAT) is a small, packed-bed catalytic cracking test that measures activity and selectivity of a feedstock-catalyst combination. [Pg.360]

Thus the rate of change of ip under activation control is much faster than / i, which is under diffusion control, and for the same condition of solution velocity the two rates could become equal at some common temperature, i.e. = ip, and there is no active-passive transition. For many of the systems given in the table this temperature is about 100°C. Above this temperature the measured activation energy is lower and diffusion control is established. [Pg.324]

A condition in which a receptor is unresponsive despite the presence of agonist also referred to as a refractory state . Typically this state is the consequence of prolonged exposure to agonist, and occurs after receptor activation it is a built in mechanism to limit a receptor s effects. Mechanistically the desensitised state differs from the resting, closed state of a receptor because in the latter state, a receptor can respond to agonist. This difference predicts that these states are structurally distinct. The desensitised state may also be stabilised by very low concentrations of agonist, such that no measurable activation of the receptor precedes it. Desensitisation is an intrinsic property of many receptors but can also be influenced by other interactions or modifications, such as phosphorylation. [Pg.421]

It is interesting to mention here that Dewar and Storch (1989) drew attention to the fact that ion-molecule reactions often lack a transition state barrier in theoretical calculations related to the gas phase, but are known to proceed with measurable activation energy in solution. Szabo et al. (1992) made separate calculations at the ab initio Hartree-Fock 3/21 G level for the geometry of the nitration of benzene with the protonated methyl nitrate by two mechanisms, not involving solvent molecules. Both calculations yielded values for the energy barriers. [Pg.44]

This calculated energy difference, as well as those obtained using MINDO/3 by Castenmiller and Buck (1977, 356 kJ mol-1) and with MNDO by Brint et al. (1985, 195 kJ mol-1), are clearly unrealistic when compared with the experimentally measured activation energy (Ea= 114-117 kJ mol-1, see Sec. 8.3). The statement by Castenmiller and Buck is therefore fair Calculations of this kind of model appear to be beyond the scope of the present possibilities. ... [Pg.178]

Another approach was used some years ago by Dewar and Storch (1989). They called attention to solvent effects in ion-molecule reactions which do not yield an activation energy in theoretical calculations related to gas-phase conditions, but which are known to proceed with measureable activation energy in solution. Dewar and Storch therefore make a distinction between intrinsic barriers due to chemical processes and desolvation barriers due to chemical processes. [Pg.182]

Measured activation energies, which are not independent of temperature nor of the acid concentration, vary between 13.3 and 24.2, show a minimum at the acid concentration giving the maximum rate and these fairly low energies for such unreactive substrates are consistent with a highly reactive electrophile. [Pg.13]

Available methods provide measurements of enzyme activity rather than of enzyme concentration. In order that the measured activity be proportional to enzyme concentration, the reaction conditions which include pH, temperature, initial substrate concentration, sample and total volume and reaction time must be held constant and be carefully controlled. [Pg.184]

The measured activity should be directly proportional to enzyme concentration over a practical working range. [Pg.185]

Synergism is calculated by dividing the measured activity (enzyme combinations) by the expected activity (individual activities, data not shown). Values >1 indicate positive synergism. [Pg.289]

The experimental results obtained by measuring ions activity after equilibration with pectins are plotted as binding isotherms [Me +Jb/Cp vs [Me +Jt/Cp where [Me2+]b is the bound cation concentration at equilibrium (equiv.l-i) calculated from measured activity using previously calculated activity coefficients. [Pg.537]

Activation energies for chain termination are smaller than for chain propagation, but they are significantly greater than zero. This might not have been anticipated inasmuch as methyl radicals seem to combine in the gas phase without measurable activation energy. ... [Pg.160]

Fig. 113.—Comparison of observed entropies of dilution (points and solid lines with results calculated for ASi according to Eq. (28) (broken line). Data for polydimethyl-siloxane, M =3850, in benzene, A (Newing ), obtained from measured activities and calorimetric heats of dilution. Entropies for polystyrene (Bawn et in methyl ethyl ketone,, and in toluene, O, were calculated from the temperature coefficient of the activity. The smoothed results for benzene solutions of rubber, represented by the solid curve without points, were obtained similarly. Fig. 113.—Comparison of observed entropies of dilution (points and solid lines with results calculated for ASi according to Eq. (28) (broken line). Data for polydimethyl-siloxane, M =3850, in benzene, A (Newing ), obtained from measured activities and calorimetric heats of dilution. Entropies for polystyrene (Bawn et in methyl ethyl ketone,, and in toluene, O, were calculated from the temperature coefficient of the activity. The smoothed results for benzene solutions of rubber, represented by the solid curve without points, were obtained similarly.
This book appears at a moment when one of the major developments of the last century in analytical chemistry, measurement science, is coming to its full maturity. The past hundred years have shown an enormous expansion in measurement activities what is measured, the purpose of the measurements, the use of measured data, and the demands placed upon these data. From the initial, almost exclusive, use of chemical reactions to make measurement the field became wider. Introducing physical and biological reactions and sensors has enormously extended the scope of analytical chemistry. [Pg.302]

A protease-specific model has also been reported in which a replication-defective adenovirus encoding an NS3 protease-SEAP fusion protein is injected into mouse tail veins, resulting in expression of the fusion protein in the liver [82, 83]. Protease activity can be detected both by measuring activity of liberated SEAP or by protease-induced liver damage. Protease activity was found to be reduced by administration of protease inhibitors. This model can be used to show that candidate inhibitors have adequate pharmacokinetic properties in mice to function in the intended target organ, but it is not a true disease model. [Pg.77]

The highly fractionated nature of the and Th series nuclides is illustrated by the measured activities in some representative waters in Figure 1. The highest activities are typically observed for Rn, reflecting the lack of reactivity of this noble gas. Groundwater Rn activities are controlled only by rapid in situ decay (Table 1) and supply from host rocks, without the complications of removal by adsorption or precipitation. The actinide U, which is soluble in oxidizing waters, is present in intermediate activities that are moderated by removal onto aquifer rocks. The long-lived... [Pg.317]

As a noble gas, Rn in groundwater does not react with host aquifer surfaces and is present as uncharged single atoms. The radionuclide Rn typically has the highest activities in groundwater (Fig. 1). Krishnaswami et al. (1982) argued that Rn and all of the other isotopes produced by a decay are supplied at similar rates by recoil, so that the differences in concentrations are related to the more reactive nature of the other nuclides. Therefore, the concentration of Rn could be used to calculate the recoil rate for all U-series nuclides produced by a recoil. The only output of Rn is by decay, and with a 3.8 day half-life it is expected to readily reach steady state concentrations at each location. Each measured activity (i.e., the decay or removal rate) can therefore be equated with the input rate. In this case, the fraction released, or emanation efficiency, can be calculated from the bulk rock Ra activity per unit mass ... [Pg.331]

Half-lives have typically been determined by measuring the activity (rate of decay) of a sample containing a known number of atoms of the nuclide in question and calculating the decay constant via the equation NX= a, where a is the measured activity. The half-lives of all of the nuclides pertinent to °Th and Pa dating have been determined in this fashion. Among those that are known most precisely are those of... [Pg.387]

Whether interfering ions are present or not, there is still the problem of how to obtain the concentration from an actually measured activity value. In order to achieve this we can choose either a standard calibration method or an incremental (or decremental) method37. [Pg.69]


See other pages where Measuring active is mentioned: [Pg.578]    [Pg.172]    [Pg.522]    [Pg.74]    [Pg.629]    [Pg.970]    [Pg.519]    [Pg.477]    [Pg.655]    [Pg.657]    [Pg.664]    [Pg.187]    [Pg.104]    [Pg.432]    [Pg.434]    [Pg.37]    [Pg.84]    [Pg.189]    [Pg.554]    [Pg.44]    [Pg.395]    [Pg.104]    [Pg.275]    [Pg.86]    [Pg.177]    [Pg.213]    [Pg.184]    [Pg.195]   
See also in sourсe #XX -- [ Pg.130 ]




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