R. Chandra et al., MICROWAVE AND INFRARED DIELECTRIC-RELAXATION OF ALKYL CARBONATES, CHLOROFORM, AND THEIR MIXTURES AT 25-DEGREES-C, Journal of physical chemistry, 97(47), 1993, pp. 12127-12133
Microwave data yielding the complex permittivity epsilon' - epsilon' -
Jepsilon'', infrared and visible refractive indices, and infrared att
enuation coefficients for liquid dimethyl carbonate [(CH3O)2CO; abbrev
:DMC], chloroform, and their mixtures have been recorded at 25-degrees
-C. For pure DMC the real part of the complex permittivity epsilon' ve
rsus frequency shows two domains: the microwave frequency range previo
usly studied and interpreted as the rotational relaxation of the metho
xy groups, -OCH3, around the carbonyl moiety, > C = 0, and a new domai
n at infrared frequencies. This latter domain showing a decay of n2 is
probably attributable to intramolecular vibrations. The profile of n(
IR2) (the squared refractive index) versus frequency for pure CHCl3 re
veals a dielectric phenomenon hinted at by literature data obtained at
far-IR frequencies. This phenomenon can be explained qualitatively as
due to weakly damped resonance absorptions. Mixtures of CHCl3 and DMC
are more interesting in the microwave frequency range than mixtures o
f CCl4 and DMC because of interactions in the former pair arising from
H bonding. Mixtures of DMC and CHCl3 have a microwave dielectric spec
trum that differs markedly from that which would be expected for mole
fraction X(DMC) = 0.50, if the two components did not interact strongl
y with each other. The dielectric relaxation frequencies of pure DMC a
nd pure CHCl3 are f(r) = 22 and 27 GHz, respectively. When they are mi
xed at a composition X(DMC) = 0.50, a dielectric relaxation spectrum i
s produced that can be interpreted by a Cole-Cole distribution with an
average relaxation frequency f(r) = 17 GHz and a distribution relaxat
ion parameter alpha = 0.08 (0 < alpha < 1 with alpha = 0 for a single
Debye relaxation process). This microwave dielectric relaxation is asc
ribed to the formation of H-bonded complexes arising from interactions
of the proton of CHC13 and the carbonyl moiety of DMC. A similar X(DM
C) = 0.50 mixture of DMC and CCl4 does not produce the same microwave
dielectric relaxation thus supporting the attribution of the phenomeno
n to the formation of a hydrogen-bonded CHCl3-DMC complex. Mixtures of
ethylene carbonate [EC] and CHCl3 UP to CEC congruent-to 3 M produce
a microwave dielectric spectrum that can also be interpreted as arisin
g from hydrogen bonding between EC and CHCl3.