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Temperature dependence, exchangeable

Li NMR spectra show several peaks as a result of several different CIP modes arising from coordination to different sites of the anion, and (temperature-dependent) exchange between CIP and SSIP. Solvent separated lithium cation ion-pairs appear at ca +2 ppm relative to the NMR standard (LiBr in THF, 0.0 ppm)13. In the CIP solvation state the line shows a sharp deviation from the standard. Proximity to the anion shows lines at ca... [Pg.479]

EPR spectroscopy can show temperature dependent features for a number of reasons, one of which is due to a temperature dependent exchange coupling be-... [Pg.74]

UCo is a paramagnet with a weakly temperature-dependent exchange-enhanced magnetic susceptibility of 0.93 X 10 8 m3/mol at 300 K that increases by less than 2% when cooling to 1.6 K (Chen et al. 1985). The originally reported superconductivity below 1.7 K (Chandrasekhar and Hulm 1958) was recently studied in more detail by Chen et al. (1985) who found Tc = 1.22 K and a critical field Ha = 1.7 T (extrapolated to 0 K). This compound represents an example of a regular U superconductor in the sense of the Hill plot because dv v 320 pm. Also the low value of y = 7.84 mJ/mol K2 is consistent with this picture. Compared to the other U-based superconductors (Meisner et al. 1984), UCo exhibits the highest Stoner enhancement parameter, S = 7. This can be correlated with the spin-fluctuation... [Pg.341]

Fig. 5.27 Temperature dependent exchange splitting of the Gd(OOOl) surface state. Reprinted from [119], Copyright (1998), with permission from Elsevier... Fig. 5.27 Temperature dependent exchange splitting of the Gd(OOOl) surface state. Reprinted from [119], Copyright (1998), with permission from Elsevier...
Another variant of the lattice model for fluids and fluid mixtures has been developed by Lacombe and Sanchez.In their treatment the fluid lattice contains empty sites (holes), whose equilibrium concentration is temperature dependent. Exchange interaction energies are taken proportional to contact surfaces, as in Flory s theory, but hole-hole and hole-mer interactions are zero. Close-packed molecular volumes, independent of temperature and pressure, appear in place of hard-core volumes. The holes provide the free volume, and there is no need to introduce a separation of internal and external molecular degrees of freedom or a parameter c. These considerations lead to a reduced equation of state for an r-mer fluid in the form... [Pg.109]

Forbes M D E, Closs G L, Calle P and Gautam P 1993 The temperature dependence of the exchange coupling in polymethylene biradicals. Conclusions regarding the mechanism of the coupling J. Phys. Chem. 97 3384-9... [Pg.1621]

Figure B2.4.3. Proton NMR spectrum of the aldehyde proton in N-labelled fonnainide. This proton has couplings of 1.76 Hz and 13.55 Hz to the two amino protons, and a couplmg of 15.0 Hz to the nucleus. The outer lines in die spectrum remain sharp, since they represent the sum of the couplings, which is unaffected by the exchange. The iimer lines of the multiplet broaden and coalesce, as in figure B2.4.1. The other peaks in the 303 K spectrum are due to the NH2 protons, whose chemical shifts are even more temperature dependent than that of the aldehyde proton. Figure B2.4.3. Proton NMR spectrum of the aldehyde proton in N-labelled fonnainide. This proton has couplings of 1.76 Hz and 13.55 Hz to the two amino protons, and a couplmg of 15.0 Hz to the nucleus. The outer lines in die spectrum remain sharp, since they represent the sum of the couplings, which is unaffected by the exchange. The iimer lines of the multiplet broaden and coalesce, as in figure B2.4.1. The other peaks in the 303 K spectrum are due to the NH2 protons, whose chemical shifts are even more temperature dependent than that of the aldehyde proton.
For constant temperature dynamics where the constant temperature check box in the Molecular Dynamics Options dialog box is checked, the energy will not remain constant but will fluctuate as energy is exchanged with the bath. The temperature, depending on the value set for the relaxation constant, will approach con-stan cy. [Pg.321]

The exchange energy coefficient M characterizes the energy associated with the (anti)paraHel coupling of the ionic moments. It is direcdy proportional to the Curie temperature T (70). Experimental values have been derived from domain-width observations (69). Also the temperature dependence has been determined. It appears thatM is rather stable up to about 300°C. Because the Curie temperatures and the unit cell dimensions are rather similar, about the same values forM may be expected for BaM and SrM. [Pg.192]

Values of thermal conductivity are temperature-dependent and vary widely for different materials. Table 1 summarizes the thermal conductivity values of a few materials relevant to heat-exchanger analysis (1,2). [Pg.481]

A fictive sky temperature, dependent on ambient temperature, emissivity, and cloudiness, is introduced to account for the long-wave radiative heat exchange between the building envelope and the sky. [Pg.1065]

We have done our experiments with hectorite, which is a 2 1 smectite that develops negative layer charge by substitution of Li for Mg in the octahedral sheet.Samples were prepared by multiple exchange in 1.0 and 0.1 M CsCl solutions until essentially complete Cs-exchange was reached (97% of the interlayer cations). Temperature dependent data are essential to interpret the results, because there is rapid exchange of Cs among different interlayer sites at room temperature (RT). [Pg.158]

The corrosion potentials of metals and alloys are temperature dependent. The potential of a steel distillation column, heat exchanger or other item of plant varies in the temperature zones in which it is operating. Under some... [Pg.893]


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