Polar molecules, dielectric absorption spectra

Many other measures of solvent polarity have been developed. One of the most useful is based on shifts in the absorption spectrum of a reference dye. The positions of absorption bands are, in general, sensitive to solvent polarity because the electronic distribution, and therefore the polarity, of the excited state is different from that of the ground state. The shift in the absorption maximum reflects the effect of solvent on the energy gap between the ground-state and excited-state molecules. An empirical solvent polarity measure called y(30) is based on this concept. Some values of this measure for common solvents are given in Table 4.12 along with the dielectric constants for the solvents. It can be seen that there is a rather different order of polarity given by these two quantities. 

A further property associated with the radial displacement of charge associated with CT electronic transitions is a change in the dipolar moment of the molecule. If the electronic transition causes, for example, an increase in the dipolar moment, the energy of the CT excited state will decrease (other factors aside) with the polarity of the solvent. Therefore, the CT absorption bands will experience solvatochromic shifts of tens of nanometers. Related solvatochromic effects will be detected in the emission spectrum of CT excited states. While the solvatochromism of absorption bands is a tool for the assignment of CT transitions in the absorption spectrum of complexes, the rationalization of such effects in terms of the solvent properties, for example, the dielectric constant, is not always possible. 

According with experimental data, the n-n band of MOx is shifted by —2,145 90 cm (—0.266 0.011 eV) when the solvent changes from iso-octane to water [16] and extrapolated as —2,410 90 cm (—0.299 0.011 eV) from gas phase to water using a linear regression in the a plot of the experimental values for the maximum absorption transition energy, Emax. of the MOx in several solvent [16] versus the normalized Reichardt solvent polarity scale, Ej [2] (see Fig. 3). In order to discuss, the absorption spectrum of solute MOx (S) in water different theoretical representations of the solvent was adopted (1) the polarizable continuum model (S -I- PCM), which provides a simplified representation of the solvent as a continuum dielectric medium (2) the average solvent electrostatic configuration (S -I- ASEC), where 250 water molecules of... 

Dielectric friction is the measure of the dynamic interaction of a charged or dipolar solute molecule with the surrounding polar solvent molecules. This concept has been applied, by Hynes et al. [339] and others [486], to solvent- and time-dependent fluorescence shifts resulting from the electronic absorption by a solute in polar solvents. If the solvent molecules are strongly coupled to the charge distribution in ground- and excited-state molecules, the relatively slow solvent reorientation can lead to an observable time evolution of the fluorescence spectrum in the nano- to picosecond range. This time-dependent fluorescence (TDF) has been theoretically analysed in terms of dynamic... 

The first process prevails at relatively low frequencies. The electric component E of radiation orients dipole moments p along the field direction, while chaotic molecular motions hinder this orientation p and E are the vectors, and the field E is assumed to vary harmonically with time t. Due to inertia of reorienting molecules the time dependence of the polarization lags behind the time dependence E(f), so that heating of the medium occurs (the heating effect is not considered in this work). The dielectric spectrum obeys the Debye relaxation, for which the absorption monotonically increases with frequency. 

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