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Kinetic , generally energy

Master equation methods are not tire only option for calculating tire kinetics of energy transfer and analytic approaches in general have certain drawbacks in not reflecting, for example, certain statistical aspects of coupled systems. Alternative approaches to tire calculation of energy migration dynamics in molecular ensembles are Monte Carlo calculations [18,19 and 20] and probability matrix iteration [21, 22], amongst otliers. [Pg.3021]

Adsorption. This step depends on the possible interaction between molecules and the catalyst surface. When the reactants reach the active sites, they chemisorb on adjacent active sites. The chemisorption may be dissociative and the adjacent active sites may be of the same or different origin. The chemisorbed species react and the kinetics generally follow an exponential dependence on temperature, exp( EfRT), where E3 is the activation energy of chemisorption. [Pg.199]

Assuming a steady state process (AE = 0), no kinetic (KE) or potential energy (PE) changes and mechanical work done (W) by the system on the surroundings are zero, that is KE, PE, and W = 0, the general energy balance... [Pg.78]

In most equilibrium stage processes, the general energy balance can be simplified by neglecting potential energy and kinetic energy. If, in addition, the process is workless and adiabatic, a simple enthalpy balance applies ... [Pg.152]

The techniques that have been developed to probe the kinetics of energy transfer processes In materials on a picosecond time scale can be divided into three general categories. They are the optical Kerr gate, the excite and probe technique, and the streak camera technique. [Pg.184]

In this case, as shown in Figure 4, the subsystems are stoichiometry, material balance, energy balance, chemical kinetics, and interphase mass transfer. The mass transfer phenomena can be subdivided into (1) phase equilibrium which defines the driving force and (2) the transport model. In a general problem, chemical kinetics may be subdivided into (1) the rate process and (2) the chemical equilibrium. The next step is to develop models to describe the subsystems. Except for chemical kinetics, generally applicable mathematical equations based on fundamental principles of physics and chemistry are available for describing the subsystems. [Pg.401]

The kinetic and potential energy effects can be neglected ( = 0). There is no exchange of heat with the surroundings (Q = 0). The general energy balance reduces to AH = W Note that the value of W is positive (work done on the system). ... [Pg.135]

Finally, the molecule can be translationally, vibrationally, and rota-tionally excited by the distribution of the kinetic recoil energy of the daughter nucleus among the available degrees of freedom. It is apparent from these considerations that the general theoretical treatment of the molecular excitation and fragmentation caused by the /8 decay is quite difficult, even in the case of very simple molecules. Among several theoretical treatments, we will illustrate the time-dependent perturbation theory applied by Cantwell (1956) to the decay of molecular tritium. [Pg.86]

A similar slow evolution from energy to entropy with a final synthesis of both concepts can also be observed in the historical development of chemical kinetics. The energy factor was first pointed out by Arrhenius (1889) when he explained the temperature effect on reaction rates. But in spite of the early work of Kohnstamm and Scheffer (1911) who introduced the idea of activation entropy, the importance of entropy was generally recognized only after Eyring (1935) formulated clearly the thermodynamic treatment of the transition state method. [Pg.410]

Suppose sys(f) is the total energy (internal + kinetic + potential) of a system, and ihm and /hout are the mass flow rates of the system input and output streams. (If the system is closed, these quantities each equal zero.) Proceeding as in the development of the transient mass balance equation, we apply the general energy balance equation (11.3-1) to the system in a small time interval from t to t + 1st, during which time the properties of the input and output streams remain approximately constant. The terms of the equation are as follows (see Section 7,4) ... [Pg.554]

Consider the heat of reaction of a substance obtained in a bomb calorimeter, sucti as in a bomb in which the volume is constant but not the pressure. For such a process (the system is the material in the bomb), the general energy balance, Eq. (4.2 a), reduces to (with no work, mass flow, nor kinetic or potential energy effects)... [Pg.449]

Let us first demonstrate how to calculate the heat of reaction at a temperature other than 25 C. By this we mean that stoichiometric quantities of the reactants enter and the products leave at the same temperature—a temperature different from the standard state of 25°C in stoichiometric quantities. Figure 4.18 illustrates the information flow for the calculations corresponding to those associated with Eq. (4.33) assuming a steady-state process (AH = 0), no kinetic or potential energy changes, and W = 0. The general energy balance [Eq. (4.24)] reduces to... [Pg.456]

When the gas velocity approaches the sound velocity, the kinetic energy and viscous work terms in the energy balance equation are not negligible (as assumed in Chapter 5). For these cases, we write the general energy balance equation for a differential plug-flow reactor with length dL (see Eq. 5.2.44),... [Pg.297]

More related to general photochemistry are the papers which have appeared on wholly or partly diffusion-controlled reactions. The effect of a very short lifetime of the donor on the calculation of fluorescence quantum yields and lifetimes has been analysed by Viriot et al. Andre et al. analyse the kinetics of energy transfer to an acceptor when there are two different excited states capable of acting as donors and when interaction between these states is possible. The exchange interaction contribution to energy transfer between ions in the rapid diffusion limit... [Pg.80]

Fluorocarbon and Related Chemistry Foreign Compound Metabolism in Mammals, Gas Kinetics and Energy Transfer F General and Synthetic Methods Haterocydc Chemistry Inorganic Biochemistry... [Pg.639]

Bernoulli equation = a form of the general energy equation = law of conservation of energy, applied to thermal and fluid flow situations. Particularly, illustrating the interconversion of kinetic (velocity) energy and pressure energy. Also see Venturi, betw = between, billet = See bar, billet, bloom. [Pg.427]

This scheme for an inclusion mechanism can explain why a-cyclodextrin forms complexes with such a diversity of substrate molecules The driving force is independent of the nature of the substrate. The only requirement is that the substrate molecule should be small enough to fit into the a-cyclodextrin cavity. Of course the other a-cyclodextrin-substrate interactions mentioned above will also play a role, depending on the nature of the substrate. The main and general energy contribution, however, will come from the a-cyclodextrin itself. In agreement with this statement are also the kinetic data presented in Table VIII [21]. [Pg.297]


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Kinetic , generally

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