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Energy enthalpy form

Typical values of the energy to form vacancies are for silver, lOSkJmol and for aluminium, 65.5kJmol These values should be compared with the values for the activation enthalpy for diffusion which are given in Table 6.2. It can also be seen from the Table 6.2 that die activation enthalpy for selfdiffusion which is related to the energy to break metal-metal bonds and form a vacant site is related semi-quantitatively to the energy of sublimation of the metal, in which process all of the metal atom bonds are broken. [Pg.174]

Bond forming potential energy (enthalpy) of bond is decreased bond distance is decreased weak bonds —> strong bonds AH < 0. [Pg.61]

Free energies, enthalpies, and entropies of ionization for a number of reducing sugars have been determined by Christensen and co-workers (13). Their data, however, are for equilibrium mixtures of anomers rather than for individual anomeric forms. [Pg.69]

Reference data on total energies of forms 19-23 optimized by means of different theoretical methods in the gas phase are given in Table 2. Various energetic characteristics of tetrazoles can be successfully estimated. The vertical adiabatic ionization potentials of both neutral tautomers 20 and 21 were calculated for a- and Tt-radical cations <2000CPL(330)212>. The standard molar thermodynamic functions (enthalpies, heat capacities, and entropies) of... [Pg.264]

The difference will depend on the amount of dissociation existing in the chamber, the pressure and the temperature level. However the enthalpy of the equilibrium exhaust state will always be less than that of the corresponding frozen situation. This fact is true because the total enthalpy is the parameter of concern and as species recombine they release energy which can be converted to kinetic energy and form products with heats of formation lower than chamber species. [Pg.67]

The sum of the heats of hydration of the cation and the anion which form an ionic salt MX may be derived from the lattice energy (enthalpy) U and the total heat of solution (infinite dilution) q of the salt by means of the thermochemical equation... [Pg.69]

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 macroscopic state of any one-component fluid system in equilibrium can be described by just three properties, of which at least one is extensive. All other properties of the state of the same system are necessarily specified by the chosen three properties. For instance, if for a single component gas in equilibrium, pressure, temperature, and volume are known, all other properties which describe the state of that gas (such as number of moles, internal energy, enthalpy, entropy, and Gibbs energy) must have a specific single value. Since the state of a system can be described exactly by specific properties, it is not necessary to know how the state was formed or what reaction pathway brought a state into being. Such properties that describe the state of a system are called slate functions. Properties that do not describe the state of a system, but depend upon the pathway used to achieve any state, are called path functions. Work and heat are examples of path functions. [Pg.46]

Correspondingly each of the other quantities of state Z, such as internal energy, enthalpy, and entropy among others, can be formed by integration of the associated specific state quantity. For the specific quantity of state z it holds that... [Pg.258]

Equation (3.90) is the mass balance or continuity equation, (3.91) the momentum balance or Cauchy s equation of motion and (3.92) is the energy balance. As a momentum balance exists for each of the three coordinate directions, j = 1, 2, 3, there are five balance equations in total. The enthalpy form (3.83) is equivalent to the energy balance (3.92). [Pg.285]

With the boundary layer simplifications from section 3.5, the enthalpy form of the energy equation (3.83) becomes... [Pg.389]


See other pages where Energy enthalpy form is mentioned: [Pg.173]    [Pg.140]    [Pg.239]    [Pg.16]    [Pg.83]    [Pg.173]    [Pg.84]    [Pg.471]    [Pg.329]    [Pg.154]    [Pg.205]    [Pg.27]    [Pg.153]    [Pg.246]    [Pg.982]    [Pg.1033]    [Pg.137]    [Pg.202]    [Pg.437]    [Pg.621]    [Pg.137]    [Pg.332]    [Pg.80]    [Pg.312]    [Pg.39]    [Pg.140]    [Pg.123]    [Pg.63]    [Pg.71]    [Pg.251]    [Pg.2359]    [Pg.439]    [Pg.283]    [Pg.119]    [Pg.297]   
See also in sourсe #XX -- [ Pg.282 , Pg.283 , Pg.390 ]




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Energy enthalpy

Energy forms 78

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