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Free enthalpy Keyes

Molar is the key point. The molar free enthalpy of reaction is also called molar energy of reaction. This is not a very important distinction because this quantity has nothing to do with enthalpy or energy The important point is not to forget the adjective molar in the naming. (We recall that it is the energy-per-entity, an effort indeed, which is an intensive state variable, whereas energy is... [Pg.162]

Key Terms enthalpy, H free energy of formation, AG standard entropy change, AS° entropy, S spontaneous process standard free energy change, AG° free energy, G... [Pg.472]

Key Concepts of Interfacial Properties in Food Chemistry Equation D3.5.12 G = U + PV - TS = yA + p,/j, i Equation D3.5.13 where H is the enthalpy, F the Helmholtz free energy, and G the Gibbs free energy. These basic equations can be used to derive explicit expressions for these quantities as they apply... [Pg.614]

Fig. 9.2. Flowchart of prilocaine hydrochloride solid state forms and melt with transformation temperatures under ambient pressure conditions (left) and semi-schematic energy/temperature diagram of the polymorphs (right). Key H, enthalpy G, Gibbs free energy AHf, heat of fusion Liq, liquid phase (melt). Reproduced from [36]... Fig. 9.2. Flowchart of prilocaine hydrochloride solid state forms and melt with transformation temperatures under ambient pressure conditions (left) and semi-schematic energy/temperature diagram of the polymorphs (right). Key H, enthalpy G, Gibbs free energy AHf, heat of fusion Liq, liquid phase (melt). Reproduced from [36]...
A spectral band is characterised by its frequency range, its intensity, and its shape and breadth. The frequency change in the XH stretching tend (Av) is often used as an approximate measure of the strength of the H-bond. Enthalpies of H-bond formation are usually determined from the temperature variation of the free-associated intensity ratio of the same bands. Of even greater interest are, however, the geometries and the potential surfaces of H-bonded species and the distribution of the electronic charge therein. For this the spectra of the isolated H-bond complexes that is, gas phase spectra are needed. The fine structure of the bands has to be examined. Key questions are how do the new vibrational motions introduced by the formation of a H-bond interact with the internal motions of the components X and Y How could this be inferred from the observed breadth and fine structure of the bands ... [Pg.43]

Key Mechanism 4-1 Free-Radical Halogenation 136 4-4 Equilibrium Constants and Free Energy 138 4-5 Enthalpy and Entropy 140 4-6 Bond-Dissociation Enthalpies 142 4-7 Enthalpy Changes in Chlorination 143 4-8 Kinetics and the Rate Equation 145... [Pg.7]

This is a very useful relationship among three state functions, free energy, enthalpy, and entropy. It is a key tool in the application of thermodynamics to chemical problems. Close examination of equation 23 reveals that, in the form AS = AH/T — AGIT, it is a different version of equation 17b that is, it reexpresses the entropy changes of the second law in terms of state functions of the system itself. [Pg.27]

The key step in the derivation by Reuter et al. of their lattice model is the use of detailed balance to determine the sticking coefficients for each species on each type of site.31 The total adsorption rate at a particular site can be expressed as Tad = SI(p, T), where S is the local sticking coefficient and I(p,T) is the impingement rate of the species of interest from a gas phase with partial pressure p and temperature T. At steady state, the total adsorption and desorption rates must satisfy the detailed balance condition TdesjTad = exp[(Fb—/j,(T, p))/kT, where Fb is the free energy of the adsorbed species and fi(T, p) is the chemical potential of the gas phase species. The adsorption free energy is well approximated by the adsorption enthalpy, which is simply the adsorption energy calculated by a DFT calculation. This approach provides a direct link between the adsorption and desorption rates and the pressure and temperature of the bulk gas phase. [Pg.112]

Chapter 11 deals with free radicals and their reactions. Fundamental structural concepts such as substituent effects on bond dissociation enthalpies (BDE) and radical stability are key to understanding the mechanisms of radical reactions. The patterns of stability and reactivity are illustrated by discussion of some of the absolute rate data that are available for free radical reactions. The reaction types that are discussed include halogenation and oxygenation, as well as addition reactions of hydrogen halides, carbon radicals, and thiols. Group transfer reactions, rearrangements, and fragmentations are also discussed. [Pg.1210]

This chapter reviews the fundamental concepts in thermodynamics that a user should master to obtain reliable results in simulation. The thermodynamic network (equations 5.39 to 5.42, and 5.68 to 5.74) links the fundamental thermodynamic properties of a fluid, as enthalpy, entropy, Gibbs free energy and fiigacity, with the primary measurable state parameters, as temperature, pressure, volumes, concentrations. The key consequence of the thermodynamic network is that a comprehensive computation of properties is possible with a convenient PVT model and only a limited number of fundamental physical properties, as critical co-ordinates and ideal gas heat capacity. [Pg.179]

JVo is a key parameter which significantly affects the physical properties of AOT reversed micelles. In the case of an AOT/oil solution, discontinuity of several physical properties of the solubilized water is observed at IVg 10 [16]. Below IV 10, the water is bound to the AOT polar head-groups and counterions, and further addition of water leads to the appearance of free water in the core of the water pools. However, the state of the water in the AOT reversed micelles, especially below Wg 2, appears unusual. We found that the solution enthalpy of the water in AOT/various organic solvents solutions indicated a great change in the state of the solubilized water [17,18]. [Pg.399]

In contrast to the 5—>8 CDD-generating route, the production of DT is not likely to be facilitated by the participation of additional monomers along the 5 10 route. None of the key species are foimd to be coordinatively stabUized by monomer complexation, which has to compete for coordination with the coordinated olefinic double bond of the Cjo chain, either on the enthalpy or on the free energy surface [11]. [Pg.208]

Table 10 Calculated Gibbs free energies of the reactions AG° (298.15 K), enthalpies of the reactions A//° (298.15 K), the sum of key barriers ( b in kcal mol ) along the reactive channels, and experimental branch ratios of the dehydrogenation products [18]... Table 10 Calculated Gibbs free energies of the reactions AG° (298.15 K), enthalpies of the reactions A//° (298.15 K), the sum of key barriers ( b in kcal mol ) along the reactive channels, and experimental branch ratios of the dehydrogenation products [18]...
We have illustrated that for a catalytic reaction in a zeolite to have a maximum rate, the adsorption free energy should be a maximum. Zeolites with medium-sized cavities are preferred over zeolites with small cavities because in the latter entropy loss dominates the gain in enthalpy. This compares with the anti-lock-and-key behavior of some enantiomeric catalytic systems discussed in the final section of Chapter 2. The catalytic systems that have an optimal misfit with their cavity perform the best, again demonstrating that the occupation is maximized while minimizing the entropy loss. [Pg.200]


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