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External interaction transitions

Under special conditions still further transitions can be observed as (1) metal-to-metal (MMCT) or intervalence (IT) charge transfers characteristic for polynuclear complexes and (2) charge transfer to solvent (CTTS) or ion-pair-charge-transfer (IPCT) detectable in cases of fairly strong external interactions [3]. [Pg.25]

Boltzmann If the external interaction with the gas model is infinitely slow, we may calculate as if the molecules had at each time a Maxwell-Boltzmann distribution corresponding to the instantaneous values of Ei, r , , rm. With this assumption we get for the sum of the energy increase and the work performed for an infinitesimal transition, i.e., for the supplied heat, ... [Pg.60]

The possibility of an entropy-enthalpy relationship for the reaction was examined and found to give a correlation coefficient of only 0.727 which was however improved to 0.971 if only the external contributions to these parameters were used, i.e. these contributions arising from solvent interactions only. If compounds with substituents ortho to the amino group were excluded, this further improved to 0.996 and is likely therefore to be real [cf. the comments on p. 9). It was argued that the different amounts of desolvation of the aromatic on going to the transition state would depend upon the substituent, and that the resultant greater freedom for solvent molecules would mean decreased interaction energy or increased enthalpy so that the linear relationship follows. [Pg.226]

In our previous works the fact of AR-DNA interactions, resulting in modifications of physicochemical properties of this biopolymer with formation of supramolecular complexes has been described [Davydova et al., 2005]. The AR-DNA interactions also leads to B —> A transition of DNA, increase the thermostability of these complexes and improving the resistance of DNA to some external influences [Davydova et al., 2006, 2007]. [Pg.185]

Frosch(84,133) have explained the external heavy-atom effect in intersystem crossing by postulating that the singlet and triplet states of the solute, which cannot interact directly, couple with the solvent singlet and triplet states, which themselves are strongly coupled through spin-orbit interaction. Thus the transition integral becomes<134)... [Pg.134]

In Equation (6) ge is the electronic g tensor, yn is the nuclear g factor (dimensionless), fln is the nuclear magneton in erg/G (or J/T), In is the nuclear spin angular momentum operator, An is the electron-nuclear hyperfine tensor in Hz, and Qn (non-zero for fn > 1) is the quadrupole interaction tensor in Hz. The first two terms in the Hamiltonian are the electron and nuclear Zeeman interactions, respectively the third term is the electron-nuclear hyperfine interaction and the last term is the nuclear quadrupole interaction. For the usual systems with an odd number of unpaired electrons, the transition moment is finite only for a magnetic dipole moment operator oriented perpendicular to the static magnetic field direction. In an ESR resonator in which the sample is placed, the microwave magnetic field must be therefore perpendicular to the external static magnetic field. The selection rules for the electron spin transitions are given in Equation (7)... [Pg.505]

Phase behavior in complex fluids such as polymer blends and block copolymers has been a rich area of the chemical sciences. Near-critical and other transitional phenomena are frequently prominent. Since molecular movement in viscous systems such as these is comparatively slow, phase transitions can be studied more easily in time, and manipulated by quenching and other external influences. Processes for controlled growth of ordered materials are often readily influenced by diffusion, a variety of external fields, and the influence of interacting boundaries, or flow. [Pg.50]


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See also in sourсe #XX -- [ Pg.206 ]




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