265
Fluid Phase Equilibria, 29 (1986) 265-272 Elsevier Science Publishers B.V., Amsterdam - Printed in The Netherlands
EXPERIMENTAL
SOLID-LIQUID
EQUILIBRIA
OF BINARY
MIXTURES
OF
ORGANIC
COMPOUNIIS
P.C.
PROUST
Escuela
de
and
J.C.
FEHNANDEZ
Ingenieria
Valparaiso,
Quimica,
Universidad
Catllica
de
Valparaiso,
Chile.
ABSTRACT A
simple
which organic
cell
heated
or
through with
down
cooled
immersed
last
in
the
of
Systems
known is
stirred
from The
cell.
of
(
binary
a magnetic
bar,
a t.hermostated
temperature
is
jresolution:
3re
system monitored
0.01
E),
which
mixture. are
a rate
melted,
of
rise
of
include o-xylene
in
the
this
and
rate
occurs,
When which
temperature. ni trobenzene
of
p-xylene,
and
K/min.
0.06
equilibrium
mixtures and
acetone
crystallized,
partially
approximately
a sharp
determination
i-octane,
with
methanol the
at
solubility
C.
composition
Z-butanone,
n-heptane,
solid
0 p e r a t Pd
and
constructed
the
thermometer
investigated
methanol, with
35
solid-liquid
precise
been of
circulating
heated
crystal the
-
surrounding
carefully
allows
to
resistance
Solutions
has
vigorously
by
a jacket
then
cell
determination
content.s,
a platinum
the
reliable the
mixtures
The
is
and
permits
and
of
with
n-butyric
acid
2-butanone.
INTRODUCTION Solution
models
determination the
of
means
to
thermodynamic In
data
binary
measurements
if
needed of
has
parameters,
quite been
predictions
037%3612/86/$03.50
on
the
precise
which
provide
parameters
often
shown
through
which given
to
range
for set
the
the
UNIFAC
0 1986 Elsevier Science Publishers B.V.
VLE phase
results. of
et
1975)) from
other
inadequate
departs
generated
predicting al.,
obtained
parameters
(Magnussen
by
for et
mostly
a different
temperature data
are lead
that
equations
(Fredenslund
those
equilibria the
original
UNIFAC
considered apply
liquid-liquid the
depend
equilibria, model
parameters
to
situations for
use,
phase
necessary
popular
are
Similarly,when that
the
interaction
it
current of
reduction.
. Efforts
equilibrium example,
in
kinds the
coefficients the
are
obtain
particular,
activity then
which
different
al.,
For
parameters
is
1981).
substantially binary model
from
interaction do
not
always
well
compare
with
systems
(Gmehling
Thus,
if
rapid
of
many of
cited
to
be
happens
Bernini,
with
the
organic
1983). are
region,
the
equilibrium
critically
needed
to
precise
and
conditions
must
that
amount
studied,
in
information 1928;
(Washburn,
are
still
required,
binary
very
for
Land01
matrix.
to
Also,
the
measurements
old
t-
especially
parameter
some
mind,
based
(1980),
experimental
which
revised.
cell,
reasonable
data
UNIFAC contain
goals
equilibrium
of exist
more the
above
these
Collins
it
multicomponent
parameters
solid-liquid
equilibria
totality
references With
and
interaction
tabulat.ions
phase
1964),
the
Carta
and
low-temperature
the
extensive
B6rnstein,
need
of
binary
realized.
type
cover
1978; the
as
values,
many
numerous
into
determination
Al though
he
al.,
and
model
practically
this
experimental of
et
valid
this
extend he
the
equilihria
solid-liquid
can
of
have
a design
give
accurate
from
developed and
down
to
by
K.
3 cm
in
and
results
K temperature 238
simple
Marzzacco
reproducible
a 50
ambient
very
3
presented
Presently,
time.
extending
we
on
in
range
can
EXPERIMENTAL AJS?ar_at!S The glass
cell
total
of
volume
the
nitrogen
rubber and
the
with
The
cm into
a magnetic cell
is
mixtures. from
a
The
inner
in
order
magnetic
Instrulab
cell
OmniScribe Dry Figure equilibrium
allow
The
the
a perforated thermometer contents
are
the
the
is
visual
or
under
methanol
it
rate
of whole
is
accuracy can
The
joint, vacuum
and
of
the
observation
a control
empty, cell.
a ground-glass
one
cold
with
left
of
outer
passage,
regulate to
has
a
exhaust
heat
circulated of
be
0.05
filled
transfer
K. with
from
assembly
rests
the over
a
stirrer.
sensitivity
solutions,
to
methanol
cell
with to
resistance
means The
to
be
serves
inserted.
placed,by
middle
can
diameter,
tube
bar.
thermostat,
jacket
circulating An
the
The
platinum
are
vessel.
refrigerated
methanol,
cell. the
tube
insulation
Through
and
protruding
the
spin
a triple-jacketed thermal
length
which
entrance
equilibrium
provides
in
a short
through
nitrogen
inside
20 mL;
admitted
stopper,
stirred
the
is 130
of
model 0.01
4000
K is
contents.
The
digital
used;
resistance its
thermometer
probe
thermometer, is
output
in
is
direct
also
with
contact
fed
to
a with
a Houston
recorder’. nitrogen thus 1
gas
is
preventing shows
apparatus.
a
used
to
moisture schematic
flush
the
air
condensation drawing
space into
of
the
over
the
liquid.
solid-liquid
the
267
cell
The solution
known
above
space cell Typical
solution 1
mixture. increases the
When
the
last
because
only
crystal
sensible
time-temperature two
equilibrium
being
accuracy
checked
of
against
the
final
melting
of
pure
the by
t.emperature rate),
break
extrapolation
solution or
in
the
of
the
determines
the
charged
three
times to
thermometer
point
of
monitored
This
reproducible
resistance
setting
original
melting) two
is
temperature
of
the
the
repeated
consistently the
rate
the of
by that
as
supplied.
distinct;
t he
stopwatch.
double
being
after
are
K/min,
digital
air
and
appears.
the
and
the
least
temperature
measurements
results
The
very
solid
1 K above
0.06 a
The
crystalized.
heated,
melt
about
now
and
solid-liquid
solution,
to
at
is
is
(before
These
cell.
heat
the
b innry
a
Cooling
ially
carefully
disappears, (to
curve
branches
before
with
of
nitrogen,
part
methanol
of
mL
vessel.
is
then
further
sharply
dry
transfer
begins
rate
checked
rises
is
circulating
a constant and
heat
6 K occurs
phase
solid
at
recorder
increase
the
w.ith
components
mixture of
The
the
2 to
of
heterogeneous
temperature
the
of
the
50
gravimetrically.
displaced
inside
one
subcooling
The
approximately prepared
is
placed
unti
provided,
with
composition,
the
then
is
charged
is
of
in fot
within was
the each
0.02
K.
frequently
ice.
RESULTS First, acet
a comparison
ir
the
behavior
with
an
the
of
complete
1928) in
the
solubility following
n-Butyric Results
systems
are
n-butyric
shown yet
for available
It parameters
in
Figure
calculated
is
the
2-butanone,
last for
evident obtained
three the
the
n-butyric plotted
the
systems;
no
from
these VLE data
1.60
work, branch
K occur.
:
and and
p-xylene 2-butanone I
and
2,
acid-n-heptane in
Figure chap.
and
3.
equations
interaction
reduction
former
Tables
1969,
figures
that Tables
nitrobenzene-p-xylene
UNIFAC
(Prausnitz,
nitrobenzene-methanol from
in
are
with
to
acetone
2,
noted
investigated
o-xylene
and
well,
acid-rich
up
listed
are
be
the
the
verify
spanning
Critical of
then
systems
relationships
must
acetic of
were
nitrobenzene-methanol
plotted
Solubilities
differences
systems
acid-2-butanone
thermodynamic
those the
for to
solutions
It
n-heptane,i-octane,
these the
in
systems
methanol,
with
from
al.
order extremely
nine K.
et
in
International
and
where binary
with acid
respectively;
point
curve, eight
for
0.07
the
Tan
agree
, for
of in
of
1952),
results
considerably
eutectic
Nitrobenzene
*
Our
range,
data
al.,
deviation
listed
depart
the
the
et
apparatus.
composition
(Washburn,
with
(Tan
temperature
especially
*
the
determinations
The
made
system
average
earlier
of
was
acid-benzene
and 9)
usual
are
also
parameters
system. that
binary (Gmehling
interaction et
a1.,1982)
are
268 are
inadequate
binary are
predict
to
apparently
systems,
the
equilibria
solid-liquid
when
large
of
some
extrapolations
temperature
involved. Analytical-grade
greater
than
additionally
%.
dried
The
Nitrobenzene
following overall
estimated
temperature:
were
reagents 99.5
0.04
nitrogen
K
with
used, and
the
recommended accuracy
, composition:
two
certified xylene
of
the
0.0005
results
mole
we
inner
jacket
methanol
methanol
-
liquid
level
-
spin
-
in B
Solid-liquid
out
_
1 1.
probe
, .
r
Figure
are:
report
fraction.
thermometer
in
jacket-
were
procedures.
nitrogen evacuated
purities isomers
equilibrium
apparatus.
bar
out
269
TABLE 1. Solid-liquid equilibria of binary ( Nitrobenzene = component 2 )
systems
with nitrobenzene.
_______.______.__.____.____.___..____.__ ._ ._ ..._.._ ___ _-.. .._...__ -_--_-..-_-. x(l) 0.0000
0.0263 0.0512 0.0975 0.1501 0.2011 0.2499 0.3007 0.3502 0.3995 0.4520 0.4980 0.5512 0.5980 0.6274 0.6568 0.6785 0.7022 0.7267 0.7500 0.7759 0.8010 0.8257 0.8511 0.8751 0.9004 0.9195 0.9404 0.9553
T, C 5.64 4.46 3.56 2.44 1.53 0.91 0.32 - 0.11 - 0.52 - 0.90 - 1.35 - 1.69 - 2.17 - 2.51 - 2.83 - 3.14 - 3.48 - 3.80 - 4.21 - 4.69 -- 5.36 - 6.09 - 7.13 - 8.71 -10.68 -13.61 -17.08 -23.24 -29.78
SZXYkE!?
x(l) 0.0000
0.0501 0.1002 0.1546 0.2006 0.2535 0.3008 0.3500 0.4008 0.4518 0.5003 0.5510 0.5519 0.5707 0.8700 0.9000 0.9242 0.9494 1.0000
T, C 5.64 2.95 0.23 - 2.50 .- 4.96 - 7.70 -10.42 -13.15 -16.14 -19.24 -22.49 -26.02 -26.17 -27.52 -29.70 -28.66 -27.85 -27.01 -25.19
X(l) 0.0000
0.0258 0.0487 0.0505 0.1010 0.1510 0.2036 0.2513 0.3033 0.3511 0.4002 0.4512 0.4984 0.5002 0.5251 0.5505 0.5754
5.ti4 4.29 3.01 2.97 0.15 - 2.64 - 5.67 - 8.52 -11.77 -14.92 .-18.35 -22.23 -26.32 -26.44 -28.52 -30.52 -33.21
pzzylene ---x(l) T, C 5.64 0.0000 0.0508 2.96 0.1000 0.39 0.1508 - 2.15 0.2006 - 4.69 0.2507 - 7.30 -- 9.95 0.3009 0.3497 -12.57 0.3653 -13.45 -13.93 0.3762 0.3827 -13.13 0.3890 -12.75 0.3979 -12.03 0.4489 - 9.10 0.4989 - 6.53 0.5499 - 4.02 0.5994 - 1.83 0.22 0.6484 0.6978 2.23 0.7478 4.13 0.7964 5.91 0.8474 7.74 0.8978 9.35 0.9473 11.16 0.9721 12.04 1.0000 13.14
TABLE 2. Solid-liquid ( n-Butyric
xii)
equilibria of binary acid = component 2 )
n:Heptane ----
0.0060 0.0516 0.1009 0.1515 0.2023 0.2514 0.3010 0.3504 0.4017 0.4509 0.5018 0.5504 0.6004 0.6488 O.F992 0.7499 0.7805 0.7990
T. C -- 5.34 - 7.62 - 9.85 -11.72 -13.39 -14.86 -16.28 -17.53 -18.89 -20.10 -21.66 -23.00 -24.49 -26. OS -27.98 -30.33 --31.79 -32.96
El!utaer?es x(l) T, 0.0000 0.0515 0.1020 0.1497 0.2025 0.2529 0.3028 0.3512 0.4040 0.4519 0.4741 0.5022
- 5.34 - 7.90 -10.32 -12.67 -15.33 -17.94 -20.70 -23.48 -26.71 -29.88 -31.37 -33.41
C
x(l)
i-Octane .--_-----
0.0000 0.0406 0.1011 0.1517 0.2013 0.2512 0.3016 0.3506 0.4011 0.4513 0.5012 0.5516 0.607Y 0.6513 0.6995 0.7503 0.7605
systems
T. C - 5.34 - 7.35 - 9.92 -11.76 -13.42 -14.99 -16.39 -17.80 -19.11 -20.56 -21.87 -23.45 -25.31 -26.77 -28.64 -31.05 -32.69
with
n-butyric
xi11
acid.
Acetone ---..--__
o.Oobo 0.0619 0.1001 0.1544 0.2045 0.2502 0.3038 0.3500 0.4027 0.4504 0.5013 0.5185
T.
-.
C
5. 34
- 8.31 -10.10 -12.64 -15.06 -17.37 -20.14 -22.72 -25.78 -26.80 -32. 26 -33.56
271
methanol
l
-24.
-
0
p-x+na UNIFAC
.
\
\
\
_3J---,ided, ‘),, , rolyhility
0.2
0
Figure
2.
Solid-liquid
nitrobenzenr-p-xylene
equilibria
0.8
0.6 fraction
of the nitrobenzene-methanol
and
systems.
-
0
0.4 solvent mole
, , ,.
UNIFAC
0.2 solvent
0.4 mole
0.6 fraction
Figure 3. Solid-liquid equilibria of the n-butyric and n-butyric acid-2-butanone systems
acid-n-heptane
212 ACKNOWLEDGEMENTS We acknowledge de Desarrollo General
financial
Cientifico
de Investigacibn,
Calculations
organic
Fredenslund,
R.L.
by the Fondo
(Chile) Cat6lica
by Ignacio
de Valparaiso.
of solid
J. Chem. Eng. Data,
Jones
and J.M.
J.G.,T.F.
equilibria
using
Anderson UNIFAC.
Prausnitz,
and J.M. Prausnitz, tnd. Eng. Chem.
acetic
acid
in
28: 328-330.
contribution estimation of activity coefficients liquid mixtures. AIChE Journal, 21: 1086-1098. Gmehling,
National
and by the Direccibn
Olaeta.
1983. Solubility
solvents.
Aa.,
provided
Universidad
were performed
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y Tecnolbgico
1975. Groupin nonideal
1978. Solid-liquid
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Gmehling, J.G.,P. Rasmussen and A. Fredenslund, 1982. Vapor-liquid equilibria by UNIFAC group contribution. Revision & extension.2. Ind. Eng. Chem.
Process
Des. Dev.,
21: 118-127.
Landolt-BHrnstein, "7nhlenwerte 1964. ‘__________ !!!!dFuekt~onnn a&!!!Ilhyslk, Chemie_L AstEEnomie-1. Geephysjk 6th ed, Vol.11, un_d T_e&nik", Part 2c, Springer-Verlag, Berlin. Magnussen, T., P.Rasmussen and Aa. Fredenslund, 1981. UNIFAC parameter table for prediction of liquid-liquid equilibria. Ind. Eng. Chem. Process Des. Dev., 20: 331-339. Marzzacco, C. and M. Collins, 1980. Convenient freezing-point depression apparatus. J. Chem. Education, 57: 650. Prausnitz, J.M., 1969. "Molecular of ---__----__ Fluid-Phase ~ .*._ _ __.___ _ ThgEm9dyDgHicB _Eg&lililrja", Prentice-Hall, Tan,
W.,
solid Chem. Washburn,
K.A.
Krieger
Englewood
Cliffs,
NJ.
and J.G. Miller,
acetic acid in the acetic Sot., 74: 6181--6283.
1952. The polymorphism of acid-benzene system. J. Amer.
E.W. (editor), 1928. "InternBtional Critical Tables Physics Chemistry BBd Technology", Vol.IV, !%!nri9_al Da&a, -- ----L ---__--108, McGraw-Hill, New York.
pf p.