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Enthalpy derivatives

Using a guided ion beam instrument the translational energy dependent reaction cross sections of endothemiic fragmentation processes can be detemiined [32]. Modelling these cross sections ultimately yields their energy tln-esholds and a great deal of valuable themiochemical infomiation has been derived with this teclmique. Precision of 0.2 eV can be obtained for reaction tln-esholds. Bimolecular reactions can also be studied and reaction enthalpies derived from the analysis of the cross section data. [Pg.1346]

Calculate liquid densities, molar tray and condenser-reflux drum holdups, ana hquor and vapor enthalpies. Determine holdup and enthalpy derivatives with respect to time by forward difference approximations. [Pg.1340]

The methods summarized by Eqs. 8 and 9 have both been applied to halocarbenes. The proton affinities obtained by ICR bracketing125 (Table 6) are consistently lower than those derived from enthalpies of formation (Table 7). The case of dichlorocarbene, with a difference in AH of 15 kcal/mol), is particularly disturbing and has been analysed in some detail.134 Notably, the PA of CCl2 from an earlier bracketing experiment126 was closer to the enthalpy-derived PA. The discrepant results from similar experiments125126 indicate that HCClJ is not a good substrate for proton transfer studies. [Pg.38]

An interesting, but controversial, article on the analysis of equilibrium data has appeared (94). The establishment of true equilibrium is tested by concordance between enthalpies derived from second and third law treatments. [Pg.24]

Chapter B outlines a typical statistical-mechanical formulation of polypeptide conformations in terms of these three parameters and describes its use for the evaluation of s and tr from observed helix-coil transition curves. Then the reported values of AH and a for selected polypeptide-solvent pairs are given and their implications are briefly discussed from a molecular standpoint. Here AH denotes the transition enthalpy derived from s by a thermodynamic relation. [Pg.69]

Some of these ambiguities can be partially solved using a simple approach recently proposed by Gamier et al. [62], The sublimation pressure of a solid can be estimated using experimental fusion properties and the vaporization enthalpy derived from the equation of state. Using the Clapeyron equation P b can be approximated by ... [Pg.49]

Substituting this equation, along with heat capacities for the enthalpy derivatives, into equation (18.79) gives... [Pg.348]

Please follow this unique method of enthalpy derivation, as no other such methodology has been presented to date, per the best of my research. [Pg.30]

Sublimation enthalpies derived from Method 5, 6, and 7 are included in Table 2. [Pg.226]

In Eq. (83), all terms are either known or measurable, except the quantity of interest . Moreover, it should be noted that Eq. (83) is very interesting since it takes into account a small adsorbate, i.e., —CH2— group, whose surface area and surface free energy are slightly affected by temperature. This means that the variations in area and surface entropy of an adsorbed —CH2— group are negligible with temperature. Therefore, it is possible to determine the surface enthalpy derived from the Gibbs-Helmholtz equation... [Pg.422]

Diakonov (1998b) argues that the surface enthalpy derived from the slope of the line relating heat of solution to surface area is apparenf rather than true. This is because the number of moles of substance does not increase linearly with surface area. The true thermodynamic surface enthalpy (or other thermodynamic function) is then argued to be 1.5 times the apparent quantity. It is not clear to me whether this argument, as presented initially by Eniistiin and Turkevitch (1960) is valid, and this point needs further clarification. [Pg.79]

The slopes of these lines provide partial molar enthalpies of solution of 97.5 4.7 and 89.2 2.6 kJ mol1 for NaBr and Nal, respectively, where the thermodynamic reference state is the solid halide. The solvation enthalpies derived from these values are —265.6 9.9 and —225.0 7.9 kJ mol-1 for bromide and iodide ion, respectively. The salts are considered to dissolve in the metal as the dissociated ions, solvated by liquid metal, and the solutions show large deviations from ideal but small deviations from regular behaviour.16 The solubilities of potassium chloride in liquid potassium and in... [Pg.3]

Figure V-3 Comparison of the caleulated enthalpy, derived from integration of Eq.(V.2) with respect to T (line), with literature data. The measured data are from [50COU/KIN] ( ), [58DOUA IC] ( ), [52RED/LON] (A) and [51SKI] (T). Figure V-3 Comparison of the caleulated enthalpy, derived from integration of Eq.(V.2) with respect to T (line), with literature data. The measured data are from [50COU/KIN] ( ), [58DOUA IC] ( ), [52RED/LON] (A) and [51SKI] (T).
Comparison of the calculated enthalpy, derived from integration of Eq.(V.2) with respect to T, with literature data.89... [Pg.534]

Comparison of the calculated enthalpy, derived from integration of... [Pg.534]

The Ed terms are obtained from the calculations and Eyib includes the zero point energy and temperature corrections to the vibrational enthalpy derived by computed harmonic vibrational frequencies. The corrections due to transhition, vibration and rotation are treated classically, using the equipartition theorem. The consideration that BH" " and B rotational contributions are quite similar, that the proton has only translational degrees of freedom and that the eventually different populations of the vibrational states that originate bringing the system from zero degrees to room temperature, are practically cancelled in the calculation of PA, yield tis to consider... [Pg.98]

It is important to note that the above formulas represent fluctuations (8X=X - (X)) in the properties of the whole system, that is, bulk fluctuations. They are useful expressions but provide no information concerning fluctuations in the local vicinity of atoms or molecules. These latter quantities will prove to be most useful and informative. One can also derive expressions for partial molar quantities by taking appropriate first (to give the chemical potential) and second (to give partial molar volume and enthalpy) derivatives of the expressions presented in Equation 1.28. However, these do not typically lead to useful simple formulas that can be applied directly to theory or simulation. For instance, while it is straightforward to calculate the compressibility, thermal expansion, and heat capacity from simulation, the determination of chemical potentials is much more involved (especially for large molecules and high densities). [Pg.10]


See other pages where Enthalpy derivatives is mentioned: [Pg.90]    [Pg.205]    [Pg.206]    [Pg.17]    [Pg.243]    [Pg.1067]    [Pg.217]    [Pg.161]    [Pg.161]    [Pg.114]    [Pg.656]    [Pg.659]    [Pg.664]    [Pg.577]    [Pg.21]    [Pg.165]    [Pg.21]    [Pg.1602]    [Pg.1612]    [Pg.151]    [Pg.1067]    [Pg.306]    [Pg.594]    [Pg.1067]    [Pg.122]    [Pg.405]    [Pg.597]   
See also in sourсe #XX -- [ Pg.83 , Pg.88 ]




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