Journal of Molecular Liquids, 33 (1987) 203-211 Elsevier Science Publishers B.V., Amsterdam - Printed in The Netherlands
MOLECULAR DILUTE
RELAXATION
BEHAVIOUR
OF SOM
SIMPLE
LIQUIDS
203
AND THEIR MIXTURES
IN
SOLUTIONS
M.P. MADAN Department Prince
of Physics,
Edward
(Received
University
Island, Canada
8 September
of Prince
Edward
Island, Charlottetown,
ClA 4P3
1986)
ABSTRACT
The dielectric mixtures region
absorption
has been examlned
over
are consistent
by us prevlously
other polar mixtures
In
The results
two proposed
acetone,
benzene
solutions
and their
In the microwave
parameters.
The relaxation
wlth those of some other rigid molecules
and also wlth the relaxatlon non-polar
solvents
are also compared
new relatlons
of two Debye-type
benzophenone
The data has been used to determine
times and the thermodynamic
times for mixtures
workers.
In dllute
a range of temperatures.
the relaxation
studled
of thlophene,
the relaxation
In a non-polar
of some
by several other
with the computed
to represent
polar components
reported
behavlour
values employing
process
of a system
solvent.
INTRODUCTION
Recently,
we (l-3) examined
molecules
and thelr mixtures
the relaxation In dllute
and over a range of temperatures. relaxation
of many
solvents,
solutions
the general
ses, In the present thlophene,
factors
was also mentioned
benzophenone
OXI-7322/87/$03.50
bearlng
paper we report
and the mixtures In benzene
at microwave
or thelr mixtures,
In order to gain more fnformatlon
more fully
of some rlgld polar
The lack of adequate
simple llqulds
state and In non-polar papers.
behavlour
at several
both In pure liquid and discussed
in these
In thls area and to appreciate
on molecular
the dlelectrlc
of thlophene
frequencies
data on molecular
reorientation relaxation
+ benzophenone
temperatures.
proces-
times of
and acetone
+
A few data on benzophenone
0 1987 Elsevier Science Publishers B.V.
and acetone previous
have been included
studies
data has been analyzed
to estimate
Flnally,
parameters. the relaxation
for comparison
(3,4) on these molecules
the varlous
two proposed
relations
times of polar mixtures
with the experimentally
and Interpretation
in dilute
determined
benzene
from our
solutions.
molar activation
energy
have been employed
in non-polar
solvents
The
to predict
for comparison
values.
EXPERIMNTAL
The apparatus
and procedures
used to determine
the dielectric
losses in the 3 cm microwave
region
have been described
(4-6).
errors
for the dielectric
The maximum
possible
were estimated
at ?0.5%
was determined
uslng the concentration
described Several
previously
solutions
and +5X, respectively.
The estimated
(5).
which did not, in general, dlpolar
mlxtures,
exceed
the concentration
kept the same, but the degree Relatively
was varled. thiophene
temperature
constancy
were obtained
RESULTS
a range For
estimate
were employed
of absorption
circulating
for
losses.
The chemicals
Scientific
purified
was
benzene
bath with the
of ?O.Ol"C.
and Fisher
They were further
solvent
Company
in
by fractional
The data was processed
with the
AN0 DISCUSSION
investigated
benzophenone included. sparse.
wlthln
were employed.
computer.
The values of the relaxation systems
solutlons
and uniformity Aldrich
and then used immediately.
aid of a VAX-II
in T is +10x.
in the non-polar
using a Neslab
of +O.O05'C
as pure a form as possible. distillation
an accurate
from BDH Chemicals,
time, T,
ratio of the two polar components
high concentration
was controlled
error
fraction
and loss
and has also been
concentrations
0.06 welght
of dilution
in order to obtain
The temperature
method
possible
and
by us previously constant
The relaxation
variation
for each system of varying
constants
and acetone Relaxation
Holland
time, T, in dilute
are presented
in Table 1.
which were measured
data on thiophene,
and Smyth
benzene
solutions
The relaxation
previously
in general,
(7) and Garg and Smyth
for the
times
for
(3,4) are also
seem to be rather
(8) determined
the
205 Table
1.
Relaxation
Times
and their
mixtures
temperatures
of
single in
(in
polar
benzene
components
at
different
psi)
Relaxation
Times
for
T =
20%
3o”c
4o”c
5o”c
60°C
18.6
16.0
14.1
12.1
10.6
2.6
2.4
2.2
2.1
1.9
3.1
2.9
2.7
Thiophene t benzophenone
15.8
13.6
11.9
10.4
9.1
Acetone + benzophenone
7.4
6.9
6.4
8enzophenonea Thiophene
2.8b 3.2b 2.1C Acetonea
a From our b Reference ’
previous 9,
Reference
Both
thiophene
by Crossley,
Hassell
at
solution
thiophene is
the
ring, It
firmed plotted
by Garg In
(TT)
tetrachloride
have
contributes
(9)
of
low
in
25’C
respectively.
for
and Kilp
reported
viscosities ring
(8)
for
l/T for
the
and
in
has
in
been
carbon
and Kilp
Table
and short compound
1 for
(10) dilute
acetone
in
cyclohexane liquid.
containing
times.
a sulfur
atom
polarfzability
to
a much smaller
(u = 2.9D). was found
pure
systems
but
relaxation
having
larger
volume
thlophene (10)
p-xylene
data
temperatures.
molar to
whereas
and by Hufnagel
a significantly
a,
and Smyth
state
The values of
larger
as compared
against
liquid
five-membered
has a slightly
by Hufnagel
pure
and Walker
20°C.
and acetone an aromatic which
in
a number
parameter,
zero
and carbon
temperature at
cover
moment u (u = 0.550) distribution
1 and 4.
cyclohexane.
a single
solutions
system.
from
p-xylene
of
Thiophene in
in
times
cyclohexane
benzene
25°C
in
tetrachloride in
at
References
10,
relaxation reported
study,
to which
the
dipole
The Cole-Cole be fndistinguishable was later
Furthermore, thfophene,
con-
when we a good
linear
206 relationship assumptlon
within
differing
loss peaks.
interpretation
assume
In this situatlon
(11,lZ).
that these molecules
relax following
It is seen from Table 1 that thiophene relaxation compare slightly
molecule,
having
the presence
benzene
solutions
moment
molecules
in dllute
molecules.
time of 3.2 ps in carbon cyclohexane definite
(lo), which
solute-solvent
of cyclohexane. ly, furan,
thiophene
tetrachloride
This behaviour
Is only
The dielectric
negligible
moment
slightly
data on polar mixtures
In benzene
was analyzed
The results
consistent
on some monosubstituted
(13) and some rigid polar molecules
them, were indicative
process
which
value for (7).
in a similar
on these mlxbenzenes
and
(l-3), along with those
(14-17) on some of the mixtures
of a molecular
structure,
polarizability
tures,
other workers
Interesting-
less than the corresponding smaller
of a
other than that
identical
solutions.
of several
T of 2.1 ps in
to that of acetone.
as for the single component with our results
of the sur-
is indicative
manner
their mixtures
dipole-dlpole
longer relaxation
in solutions
and an almost
of the comparatively
the
in T,
rearrangement
Inert solvent,
is similar
by
such that the solute
a significantly
interaction
this
affected
times and the small
(9) and a shorter
is a relatlvely molecular
(9,lO) because
barrier
significant
In contrast,
is hardly
The decrease
due to almcst
without
also with a low dipole
has a T value which
These values
which have approximately
viscosity.
The short relaxation
point to a low potential
are able to rotate solvent
has a
at 25°C (9), but are only
(=0.550),
molecules,
usually
roundlng
solution
in pure llquld of 2.8 and 2.3 ps at 20
and similar
is not notfceable.
to
a Debye behaviour.
a very small dipole moment
observed
wfth our
(8)., This shows that the dipole rotatlon.of
of non-polar
of
a significant
consistent
in dllute benzene
same order of molar volume
interaction,
measurements
of analysis
time, T, of 2.6 ps at 20°C and 2.2 ps at 4O'C.
less than the T value found
to
(l-3), it is reasonable
well with the value of 2.6 ps in p-xylene
and 40°C respectively
dipole
to our previous
Therefore,
processes
them into two
times does not provide
on some rigid molecules
the
it is difficult
or resolve
Is similar
relaxatlon
of the results
measurements
confirming
or relaxation
In such cases the method
(3,4).
the data into two separate
process
distribution
This behaviour
and acetone
was observed,
relaxation
them from a Cole-Cole
on benzophene
previous
errors
little from one another.
distlnguish dlstfnct
experimental
of a single molecular
investigated
gave the relaxation
by of
207 the mixture which
as the resultant
is, of course,
environments
of the relaxations
strongly
encountered
in rotation
the size, shape, viscosity, solvent
general,
polar
solvent,
workers
(20-22) have attempted
to analyze
the data on mixtures
C1 and C2,
experimental
of two partially by adjusting the
measurements.
an analysis
generally,
region
two or
into
many situations, (l-3,
13)
regions fit more, its
In
more
is
spite
the
the
times
ual
dispersion
regions
solutions,
that
in
dilute
a relaxing
unit
The observed time
with
This
is
t
In dilute
benzene
which is
falls
noticed
ation
at
behavfour
of
which
of
in
in
the
at
t
2O”C,
temperatures. is
of
It
true
presented
more
seems that
may it
seems
than
one
leads
to
region. relaxation
Table
of
1 for
the the
mixtures.
has to
dilute
decays
dispersion
of
fndfvid-
peaks
behaviour
in
benzophenone
by the
in
loss
type
terms
the
as an apparent
IS added
masked
if
Therefore,
the
retains
in
that
more.
the
best
relaxation
separate
of
the
component the
distinguish
benzophenone
ps when thiophene
thfophene
shape
< 6 Oebye
gives
likely
two Oebye
be termed
results
and acetone
quite
to of
the
then
out
100 or
difficult
overlap
can
is
amplitude,
as a characteristic
solution
other
is
change time
reflected
17.1
in
increased
benzophenone
to
broad,
is
interpretation
points
In
(11). Further-
polar
between
physical (18)
by a factor
little
Ta and considered
system.
their
when it
the
relaxation
thiophene
quite
differ
solutions
process,
of
TI/T
which
each
such
own merits.
be meaningful
that
of
charactertstic
resolution
differences
considerably
when T’S
relaxation
large
use
a dispersion
ratio
two
of polar
the
of
on its
the
seem to
behaviour
of
are
and differ only
attempted not
against
when the of
non-
some
regions of amplfthe best fit to the
analysis
be assessed
(18,19).Davidson
relaxation
appear
plausfble
sfgnfffcance
two
caution
example,
does
On the other hand,
Oebye obtain
each
overlap
the
absence
reduces
for
data
(23) that
must
significant
solutions,
of
al.
out
processes
experimental
individuality,
times
et
among others,
dilute
the
Hill
superimposed parameters to
and point
and there
in
to
(l-3, 15-171,
times.
terms
in
liquid state and In dilute
relaxation
in
observed
that
solutions,
60s (14) and others
in pure
solute-
assumption
on the dilute
single
compounds tudes
in nature.
bfnary polar mixtures
such as
and/or
with the customary
from measurements
tend to be molecular
investigating
molecules
of molecular
field and solute-solute
is in accord
time obtained
of the indlvidual
by the varlety
as well as by other factors
internal
This
interactions.
the relaxation
influenced
a T value
ft. in
of
A similar this
comparatively
mixture larger
18.6
ps
behavfour the
relax-
dipole
208
moment
and molar volume
molecule
of only slightly
comparable solution, mixture
dipole moment a considerably
the To values generally because
greater
freedom
volume
weights
consistent,
with the results
equation
entropy,
before,
variation
of the transition
(3).
of activation
the relaxing
units
Table 2.
rotational
In both cases, values
average
and are
values
and the respective however,
values
are
(l-3) as well as
(14-17).
of the relaxation
state theory,
*S+ , of activation
the usual manner
greater unit.
values,
with our previous
the free energy,
but of
The T for this
component
environment
The measured
of many other workers
reorientation,
a considerably
of the relaxing
in the molecular
times,
using the rate
the thermodynamic
AGf, the enthalpy,
for the relaxation
process,
parameters
for
AH', and the _
were determined
in
These are given in Table 2. It is seen that the free # differences, AG , between two equilibrium positions of
in dilute
solutions
Thermodynamic
of benzophenone
parameters
components
and mixtures
in benzene
solutions
and its mixtures
of polar components
AG+
AH+
(kcal/mol)a
(kcal/mol)
AS+ (cal mol-l
2.6
2.1
-2.2
AcetoneC
1.7
0.60
-3.6
Thioohene
1.7
0.66
-2.6
Thiophene + benzophenone
2.7
2.0
-2.4
Acetone + benzophenone
2.3
0.72
-5.4
b Reference
1.
are
for single polar
Benzophenoneb
a At 25'C.
a
is added to benzophenone
from the corresponding
of the molecules.
From the temperature
than that of thiophene
those of the individual
as expected,
as mentioned
when acetone,
drop in T is noticed.
of motion
lie between
different,
of the change
relaxing
energy
less molar
In contrast,
to that of benzophenone,
is 7.7 ps at 20°C and reflects
and translational
dipole
of benzophenone.
deg-I)
' Reference
4.
209 of
the
order
slightly
of
2 to
less.
temperature
3 kcal/mol
The values
dependence
indicate
of
the
AS+, are found
to
be negative,
tions
in
the
possible
activated
state
is
whereas
activated
state
that only state
out, of
it
is
desirable
mixtures.
to
behaviour
solvent.
studies
relations
barrier
and only of
are
to
of
Debye-type one has
a slight
activation, configura-
configurations
on mixtures have
predict
two
system,
fewer
are
the
state.
solutions
proposed
a system
a binary
a few
they
The entropies
these
normal
dilute
and acetone
there
the
in
we (2,24) of
For
or
develop
Recently,
relaxation polar
liquid
that and for
than
In view of the situation pure
energy time.
indicating
more ordered
thiophene
a small
relaxation
molecules
in
for
the
polar
dipolar carried
relaxation
relations
the
of been
to
componets
form
times
represent in
the
a non-
(2),
Cl1
where to
C = C:/C’ 2,
dipole
Another
Ci
moments
relation
are
u’i
parameters
and have
has
the
been
general
involving
effects
discussed
previously
form
other
than
those
due
(2).
(24),
121 nhere
Cl
and C2 are
solutions where can be taken to of
the
is
a function
degree
dipole
of
the
respective
the relaxation a first order
moments. of
the
overlap
of
f 12 is
the
statistical the
the
the
third
in
c21 corresponds
individual
f ~2 can,
'cl > T
, f
value
close
very
progressively
T
concentrations, to the square
magnitude
turn,
depends
The negative
> T , as
is
of
which
and the
the
upon
value case
for
of the
iy
j/T 2
shows
in
times. > T
- T 1
the
dilute
environments
which,
be r:pre&ed
= (T
1
departures
from
a zero
value
as the
12
- T ) increases. ti
regions
to
12
For
in
term,
molecular
relaxation
thus,
f
difference’(.r
of
dispersion
in
term
interference set
difference
mixtures.
which,
times are independent of the approximation as proportional
the
present
amplitudes
unity.
Furthermore,
L-&ten TV and ~~ differ
widely,
the
molecule
if
C
1
>> Cp,
f will
has
a
a relax-
atlon time T1 and amplitude
CL imposes
its relaxation
The ratio CI/CZ for thiophene-benzophenone
mixture
and, as such, the weight of the second dispersion yield more than a single relaxation suggestions
of Forest
fering moments benzophenone moments 0.17.
and Smyth
time.
mixture,
even though
the individual
for this mixture
value,
which would
> T
mixture.
is about 30 small
to
This is in accord with the with largely
Is undetectable.
little from each other,
Therefore,
from an average
wfth T
is negligfbli
(20) that in mixtures
a weak second dispersion
differing
on the whole
dlf-
For acetone-
components
have dipole
f,, is close to 0.83, TZ/TI
being
one would expect ~~~ to be different have resulted
if T, and TV were close
together.
Table 3.
Comparison
of observed
with those calculated
relaxation using
time ~~ (in ps),
Cl3 and C23.
Thlophene t benzophenone
Acetone t benzophone
T ("C)
Obs.
Calc.Cll
Calc.C23
Obs.
Calc.Cll
Calc.C21
20
15.8
17.1
17.1
7.4
7.7
8.3
30
13.6
14.8
14.7
6.9
7.1
7.2
40
11.9
13.1
13.0
6.4
6.5
6.4
50
10.4
11.3
11.1
60
9.1
9.9
9.7
The values
of T
dipole moments
have been compared
parameters,
tory for dilute
volumes
(25), are given
with the experimentally
agree well with each other the different
Cl1 and C21 and using the data for
, computed by employing (26) and molar
obtained
in Table 3 where
values.
and, in view of the uncertainties this agreement
can be considered
they
The values in estimating very satisfac-
solutions.
ACKNOW-EDGEMENTS
The author would assistance
like to express
in making
experimental
his sincere measurements
thanks
to Mr. Andrew
and to the Natural
Wtch
for
Sciences
211 and Engfneerfng Research
Research
Commfttee
Councfl
for their
of Canada
and the Unfversfty
Senate
support.
REFERENCES
1.
M.P. Madan,
J. Mol. Lfqufds,
2.
M.P. Madan,
Can. J. Phys.,
3.
M.P. Madan,
J. Mol. Lfqufds,
29 (1984) 161.
58 (1980) 20. 25 (1983) 25.
4.
M.P. Madan,
Can. J. Phys.,
55 (1977) 297.
5.
M.P. Madan,
Can. J. Phys.,
53 (1975) 23.
6.
M.P. Madan,
Can. J. Phys.,
54 (1976)
7.
R.S. Holland
and C.P.
Smyth,
794.
J. Phys. Chem.,
8.
S.K. Garg and C.P. Smyth,
J. Chem.
9.
J. Crossley,
and S. Walker,
W.F. Hassell
59 (1955) 1088.
Phys., 42 (1965) 1397. Can. J. Chem., 46 (1968)
2181. 10.
F. Hufnagel
and H. Kflp,
11.
A. Mansfngh
and 0.8. &Lay,
2. Naturforsch.,
12.
C.P. Smyth,
'Molecular
Publfcatfon
No. 20 (1966).
13.
M.P. Madan,
Can. J. Phys.,
14.
F.F. 605, Ph.D. dfssertatfon,
15.
T.J. Bhattacharya,
18a (1963) 769.
Can. J. Phys.,
Relaxation
46 (1968) 2745.
Processes';
Chemical
Society
51 (1973) 1815. Lefden,
M.S. Mathur,
The Netherlands
T.V. Gopalan
(1958).
and P.K. Kadaba,
Mater.
Sci. Eng., 1 (1966) 183. 16.
R.L. Ohar and M.C.
17.
R.L. Ohar and J.P. Shukla,
Saxana,
18.
D.N. Davidson,
19.
C.P. Smyth, Advan.
20.
E. Forest
2. Phys. Chem.
Can. J. Chem., Mol.
Processes,
H. Kflp, S.K. Garg and C.P. Smyth,
22.
J.K. Eloranta
N.E. Hill, W.E. Vaughan,
A.H.
behavfour',
24. 25.
J. Timnermans, Elsevier
To be publfshed
A.L. McClellan, Freeman.
Price
Sot., 66 (1970) 817.
and M. Davies,
'Dfelectric
Van Nostrand-Reinhold,
constants
Co., New York, N.Y.
'Tables of experimental
San Francisco
1.
London
(1986).
'Physico-Chemfcal
Publishing
1 (1967-68)
J. Chem. Phys., 45 (1966) 2799.
Trans. Faraday
properties (1969). M.P. Madan,
26.
and P.K. Kadaba,
and molecular
84 (1973) 25.
J. Phys. Chem. 69 (1965) 1302.
21.
23.
81 (1972) 169.
39 (1961) 571.
Relaxation
and C.P. Smyth,
Neue Folge.,
Z. Phys. Chem. Neue Folge.,
(1963).
of pure organfc
compounds'.
(1965). dipole
moments'.
W.H.