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at
Thermochimica
Acta
j o u r n a
l
h
o
m e
p a g e :
w w w . e l s e v i e r . c o m / l o c a t e / t c a
Determination
of
the
glass
transition
temperature
of
ionic
liquids:
A
molecular
approach
Seyyed
Alireza
Mirkhani
,
Farhad
Gharagheizi
,
Poorandokht
Ilani-Kashkouli
,
Nasrin
Farahani
a
Department
of
Chemical
Engineering,
Buinzahra
Branch,
Islamic
Azad
University,
Buinzahra,
Iran
b
Department
of
Chemistry,
Buinzahra
Branch,
Islamic
Azad
University,
Buinzahra,
Iran
a
r
t
i
c
l
e
i
n
f
o
Article
history:
Received
27
October
2011
Received
in
revised
form
11
May
2012
Accepted
11
May
2012
Available online 22 May 2012
Keywords:
Glass
transition
temperature
Ionic
liquids
Quantitative
structure–property
relationship
Genetic
Function
Approximation
a
b
s
t
r
a
c
t
Following
our
recent
QSPR
models
for
the
glass
transition
temperatures
of
ammonium
1,3-dialkyl
imidazolium-based
ionic
liquids
similar
model
is
reported
in
this
work
for
remaining
classes
of
ionic
liquids.
The
roles
of
cations
and
anions
are
considered
separately.
The
Genetic
Function
Approxi-
mation
is
applied
to
select
suitable
variables
(molecular
descriptors)
and
to
develop
a
linear
QSPR
model.
Consequently,
a
simple
predictive
model
is
obtained.
Its
performance
is
quantified
by
the
following
sta-
tistical
parameters:
absolute
average
deviation
(AAD):
3.84%,
determination
coefficient:
0.8897,
and
root
mean
square
error
(RMSE):
10.594
K.
© 2012 Elsevier B.V. All rights reserved.
1.
Introduction
Historically,
the
luminous
age
of
ionic
liquids
(ILs)
has
begun
with
the
investigation
of
German
chemist
Paul
van
Walden
on
alkyl
ammonium
nitrates
for
their
low
melting
points
in
1914.
Today,
ionic
liquids
become
the
source
of
innovation
and
the
cornerstone
of
many
industrial
breakthroughs
for
their
unique
properties
such
as
high
thermal
stability,
large
liquidus
range,
high
ionic
conductivity,
high
solvating
capacity,
and
negligible
vapor
pressure.
Generally,
the
term
ionic
liquid
or
more
technically
Room
Temperature
Ionic
Liquids
(RTILs),
refers
to
the
class
of
salts
having
melting
points
close
or
below
100
◦
C
liquids
also
possess
very
negligible
vapor
pressures
owing
to
their
ionic
natures
Besides
anions,
ionic
liquids
are
typically
made
of
cations
exhibiting
bulky
rings
containing
either
nitrogen
or
phosphorus
One
of
the
potential
application
of
ILs
is
to
employ
them
as
elec-
trolytes
in
electrochemical
applications
have
intrinsic
ion
conductivity
owing
to
their
ionic
nature.
In
addition,
thermal
stabil-
ity,
non-toxicity
and
non-volatility
of
ILs
are
requisite
features
for
their
future
application
as
electrolytes.
However,
ILs
possess
lower
ionic
conductivity
in
comparison
with
the
common
electrolytes
owing
to
their
higher
viscosity.
The
strong
electrostatic
interactions
of
ionic
counterparts
in
ILs
account
for
their
higher
viscosity.
∗ Corresponding
author.
Fax:
+98
21
88
48
10
87.
addresses:
(F.
Gharagheizi).
One
of
the
important
features
of
electrolytes
is
to
possess
low
glass
transition
temperature.
The
glass
transition
temperature
refers
to
conspicuous
changes
of
thermodynamic
derivative
prop-
erties,
such
as
heat
capacity
and
thermal
expansivity
that
usually
accompany
the
solidification
of
a
viscous
liquid
during
cooling
(or
sometimes
compression)
Ionic
liquids
with
desired
glass
transition
temperature
could
be
tailored
by
selecting
the
proper
combination
of
anions
and
cations.
However,
selecting
right
combination
of
ionic
parts
of
ILs
from
experiment
is
a
challenging
task,
owing
to
enormous
numbers
of
possible
ionic
liquids
So,
predictive
models
are
essential
to
rationally
estimate
the
desired
property
before
the
synthesis
of
ionic
liquids.
In
this
com-
munication
a
model
based
on
Quantitative
Structure–Property
Relationship
(QSPR)
approach
developed
to
estimate
the
glass
transition
temperature
of
several
ionic
liquids.
2.
Methodology
2.1.
Data
preparation
The
experimental
data
for
glass
transition
temperature
of
139
diverse
ionic
liquids
were
collected
from
literatures
measurement
protocols
available
to
determine
the
glass
transition
temperature
are
Differential
Scanning
Calorimetry
(DSC),
cold-
stage
polarizing
microscopy,
NMR,
and
X-ray
scattering.
Since,
the
values
of
glass
transition
temperatures
strongly
depend
on
the
measurement
protocols,
it
is
essential
that
all
collected
data
0040-6031/$
–
see
front
matter ©
2012 Elsevier B.V. All rights reserved.
S.A.
Mirkhani
et
al.
/
Thermochimica
Acta
543 (2012) 88–
95
89
Table
1
List
of
ionic
liquids
and
their
corresponding
frequency
in
this
study.
No.
Class
AARD%
T
exp
g
range
(K)
T
pred
g
range
(K)
N
1
1-Alkyl
imidazolium
7.5
174.15–211.15
189.92–213.85
6
2
Amino
acids
2.2
238.15–250.15
228.39–256.6
11
3
Guanidinium
2.6
192.49–215.45
181.73–214.91
12
4
Isoquinolinium
4.2
193.75–253.15
200.03–267.92
9
5
Morpholinium
5.0
195.15–285.15
200.98–250.11
15
6
Oxazolidinium
1.7
185.15–203.15
183.34–203.38
8
7
Phosphonium
2.9
197.66–433.15
195.13–409.44
15
8
Piperidinium
3.6
181.15–207.15
176.41–212.55
11
9
Pyrrolidinium
5.5
157.15–235.35
159.91–196.52
16
10
Tri-alkyl
imidazolium
3.9
191.15–215.15
201.26–210.65
8
11
Triazolium
3.8
203.15–261.15
198.93–253.59
28
for
model
development
are
measured
with
one
specific
protocol.
Our
database
includes
mostly
data
measured
using
DSC,
since
the
majority
of
data
reported
in
literature
was
obtained
by
this
tech-
nique.
The
investigated
ionic
liquids
and
their
corresponding
range
of
glass
transition
temperatures
of
each
group
are
presented
in
37
anions
and
86
cations
are
present
in
the
in
the
structures
of
the
studied
ionic
liquids.
The
anion
and
cation
abbreviations
as
well
as
their
structures
are
enlisted
in
tively,
as
supporting
information
.
2.2.
Calculation
of
descriptors
The
aim
of
this
study
is
to
correlate
ILs’
glass
transition
tem-
peratures
with
their
chemical
structures,
namely,
their
anion-
and
cation-based
descriptors.
For
this
purpose,
anion
and
cation
descriptors
are
separately
calculated
for
each
ionic
liquid.
This
approach
is
successful
to
correlate
the
studied
physical
property
with
the
structure
of
both
anion
and
cation.
However,
it
fails
to
account
for
anion–cation
interactions.
SMILES
(Simplified
Molecular
Input
Line
Entry
Specification)
structures
of
all
cations
and
anions
were
imported
to
Dragon
soft-
ware
for
the
sake
of
descriptor
calculation.
About
2000
descriptors
from
15
diverse
classes
of
descriptors
are
calculated
by
Dragon
soft-
ware.
These
15
classes
of
descriptors
are:
constitutional
descriptors,
topological
indices,
walk
and
path
counts,
connectivity
indices,
information
indices,
2D
autocorrelations,
Burden
Eigen
values,
edge-adjacency
indices,
functional
group
counts,
atom-centered
fragments,
molecular
properties,
topological
charge
indices,
Eigen
value-based
indices,
2D
binary
finger
print,
2D
frequency
finger
print.
After
the
completion
of
descriptors
calculation,
only
descrip-
tors
that
could
be
calculated
for
all
anions
or
cations
are
retained.
Next,
the
pair
correlations
for
each
binary
group
of
descriptors
(all
anions
and
cations
descriptors)
are
calculated.
For
binary
groups
with
the
pair
correlation
greater
than
0.9,
one
of
descriptors
is
omitted
randomly.
2.3.
Selection
of
training
and
test
sets
In
this
study,
k-mean
clustering
is
used
to
define
training
and
test
sets.
This
approach
is
based
on
performing
a
partition
of
col-
lected
ionic
liquids
in
four
statistically
representative
clusters
of
ionic
liquids,
in
which
each
ionic
liquid
belongs
to
the
one
with
the
nearest
mean.
This
procedure
ensures
that
any
ionic
liquid
classes
(as
determined
by
the
clusters
derived
from
k-mean
clustering)
will
be
represented
in
both
compounds
series
(training
and
test).
It
per-
mits
the
designing
of
both
training
and
predicting
series,
which
are
representative
of
the
entire
“experimental
universe”.
Selection
of
the
training
and
prediction
set
was
carried
out
by
taking,
in
a
ran-
dom
way,
compounds
belonging
to
any
IL
class.
112
ionic
liquids
are
selected
for
model
derivation
as
“training
set”.
The
ability
of
the
model
to
learn
from
“training
set”
and
reproduce
the
correct
prediction
is
tested
by
introducing
a
test
set
containing
27
ILs.
3.
Sub-set
variable
selection
In
this
study
Genetic
Function
Approximation
(GFA)
is
employed
for
sub
set
variable
selection.
GFA
as
a
genetic
based
variable
selec-
combination
of
multivariate
adaptive
regression
splines
(MARS)
with
genetic
algorithm
evolve
series
of
equations
instead
of
one
that
best
fit
the
training
set
data.
The
approach
was
originally
proposed
by
the
pioneering
work
of
Rogers
and
Hopfinger
In
most
cases,
QSPR
models
are
presented
as
a
sum
of
linear
terms:
F(X)
=
a
0
+
M
k
=1
a
k
X
k
(1)
where
a
0
is
the
intercept,
a
k
is
the
model
coefficient
and
X
k
s
are
molecular
descriptors.
The
initial
QSPR
models
are
constructed
by
random
selection
of
the
number
of
molecular
descriptors.
In
the
next
step,
the
qualities
of
the
derived
models
are
evaluated
by
Friedman’s
lack
of
fit
(LOF)
scoring
function,
which
is
a
penalized
least-squares
error
measures:
LOF
(model)
=
1
N
LSE(model)
(1
−
(c
+
1
+
(d
×
p))/N)
2
(2)
In
this
LOF
function,
c
is
the
number
of
non-constant
basis
func-
tions,
N
is
the
number
of
samples
in
the
data
set,
d
is
a
smoothing
factor
to
be
set
by
the
user,
and
p
is
the
total
number
of
parame-
ters
in
the
model
and
the
LSE
is
the
least
square
error
of
the
model.
Employment
of
LOF
leads
to
the
models
with
the
better
prediction
without
over
fitting.
At
this
point,
we
repeatedly
perform
the
genetic
recombination
or
crossover
operation:
• Two
good
models
in
terms
of
their
fitness
are
selected
as
‘parents’.
• Each
is
randomly
‘cut’
into
two
sections.
A
new
model
is
created
using
the
basis
functions
taken
from
a
section
of
each
parent.
• The
model
with
the
worst
fitness
is
replaced
by
this
new
model.
• The
overall
process
is
ended
when
the
average
fitness
of
the
mod-
els
in
the
population
stops
improving.
In
this
study,
population
and
the
number
of
maximum
genera-
tions
are
set
to
100
and
5000,
respectively.
The
value
of
Mutation
probability
is
considered
to
be
1.5
in
this
study.
4.
Results
and
discussion
The
procedure
of
model
development
with
optimal
number
of
descriptors
is
described
as
follows.
90
S.A.
Mirkhani
et
al.
/
Thermochimica
Acta
543 (2012) 88–
95
The
process
initiates
by
developing
the
model
with
one
descrip-
tor.
Then,
the
accuracy
of
model
is
calculated
in
terms
of
R
2
.The
process
continued
by
incremental
addition
of
descriptors
and
cal-
culation
related
R
2
values.
The
process
continued
until
the
addition
of
one
more
descriptor
does
not
improve
the
model
accuracy
sig-
nificantly.
In
our
study,
the
best
model
with
optimum
number
of
descriptors
contains
11
descriptors:
T
g
=
intercept
+
T
g,anion
+
T
g,cation
intercept
=
368.72472(
±35.00858)
T
g,anion
=
−Mor17p
anion
×
69.247(
±11.22717)
+
HATS2v
anion
×
45.39043(
±8.67212)+R1p
anion
×
16.76226(
±4.1989)
T
g,cation
=
−MWC05
cation
×48.48417(±7.56097)
+
ATS3m
cation
×41.25879(±4.89045)−Mor30v
cation
×
83.46733(
±18.02321)
+
G2m
cation
×
69.82063(
±34.33122)
+
G2p
cation
×
48.36684(
±36.46551)
−
nCrs
cation
×
7.06894(
±1.11807)
+
nCbH
cation
×
4.9144(
±0.73748)
−
F02[N–O]
cation
×
14.91919(
±4.21278)
(3)
R
2
=
0.8897;
n
Training
=
112;
n
Test
=
27;
AAD
=
3.84%,
RMSE
=
10.594
K
In
Eq.
• Mor17p
and
Mor30v
belong
to
MoRSE
Representa-
tion
of
Structures
based
on
Electron
diffraction)
descriptors.
They
are
derived
from
infra-red
spectra
simulation
using
a
generalized
scattering
function.
These
descriptors
are
defined
as
follows:
Mor(s,
w)
=
n
i
=2
i
−1
j
=1
w
i
w
j
sin(s
·
r
ij
)
(s
·
r
ij
)
(4)
where
w
and
r
ij
are
weight
(p
=
polarizability
and
v
=
Van
der
Waals
volume)
and
Euclidian
distance
between
i,
j
atoms,
respectively.
Morse
descriptors
also
referred
as
a
transformation
of
3D
struc-
tures,
in
which
atomic
3D
structures
could
be
transformed
into
the
molecular
descriptors.
• ATS3m
belongs
to
Broto-Moreau
Autocorrelation
Descriptors
reveals
the
distribution
of
the
relative
atomic
mass
along
the
topological
distance
of
3.
• G2m
and
G2p
are
2nd
component
of
symmetry
directional
WHIM
index
weighted
respectively
by
mass
and
polarizability
belong
to
WHIM
(weighted
holistic
invariant
molecular)
descrip-
tors
which
represent
holistic
view
of
the
molecule.
They
are
calculated
on
the
projection
of
atoms
along
principal
axes.
They
encode
information
about
shape,
molecular
size,
and
symmetry
and
atom
distribution
with
respect
to
invariant
frames.
• HATS2v
is
leverage-weighted
autocorrelation
of
lag
2/weighted
by
atomic
van
der
Waals
volumes
belong
to
HATS
descrip-
tors
which
itself
belong
to
the
larger
category
called
GETAWAY
(GEometry,
Topology
and
Atom-Weights
AssemblY)
descriptors
• R1p
is
R
autocorrelation
of
lag
1
weighted
by
atomic
polarizabil-
ities
• MWC05
is
a
molecular
walk
count
of
order
5
which
belongs
to
atomic
path/walk
topological
descriptors.
The
molecular
walk
count
is
related
to
the
molecular
branching
and
size
and
in
general
to
the
molecular
complexity
of
the
graph
• nCrs
refers
to
number
of
secondary
carbons
present
in
the
ring
structures.
• nCbH
refers
to
the
number
of
un-substituted
carbon
of
the
ben-
zene
ring.
• F02[N
O]
refers
to
frequency
of
N
O
at
the
topological
distance
of
2.
The
statistical
parameters
for
the
obtained
linear
model
are
pre-
sented
below
Eq.
n
trainiing
and
n
test
are
the
numbers
of
compounds
available
in
training
set
and
test
set,
respectively,
and
R
2
is
the
squared
correlation
coefficients
of
the
model.
SDE
is
stan-
dard
deviation
error
comparing
model
results
with
experimental
glass
transition
temperature
values.
One
of
the
important
outputs
of
the
derived
model
is
to
reveal
the
contribution
of
present
anions
and
cations
to
the
glass
tran-
sition
temperatures
in
terms
of
T
g,anion
and
T
g,cation
,
respectively.
All
T
g,cation
values
are
negative
and
vary
in
the
range
of
−221
to
−136
except
for
tetraphenylphosphonium
[P(ph)
4
]
+
which
has
the
positive
value
of
33.04.
It
is
not
surprising
that
the
ionic
liquid
associated
with
this
cation
has
highest
glass
transition
tempera-
ture
(T
g
=
433.15
K)
among
all
studied
ionic
liquids.
The
smallest
cation
contribution
belongs
to
pyrrolidinium-based
cations
with
the
average
value
of
−213.95.
It
is
not
surprising
that
all
pyrrolidinium-based
cations
have
the
lowest
negative
value
among
all
other
groups.
On
the
other
hand,
amino-acid
based
cations
with
the
average
of
−146.06
have
the
highest
negative
values
of
T
g,cation
.
Since,
ionic
liquids
with
low
glass
transition
temperature
is
highly
desirable,
the
Pyrrolidinium-
based
cations
would
be
preferred
to
the
others.
Unlike
T
g,cation
,
all
T
g,anion
values
are
positive.
(heptafluoro-n-propyl)
trifluorob-
orate
and
tetrakis
(3,5-bis(trifluoromethyl)phenyl)borate
anions
have
the
lowest
and
highest
values
of
T
g,anion
,
respectively.
To
tai-
lor
the
ionic
liquid
with
low
desired
glass
transition
temperature,
the
(heptafluoro-n-propyl)
trifluoroborate
([C
3
F
7
BF
3
]
−
)
anion
is
the
best
option
for
the
anion
part,
based
on
our
model.
Another
inter-
esting
output
of
our
model
is
to
determine
which
combination
of
cation
and
anion
present
in
our
study,
lead
to
the
ionic
liquid
with
lowest
glass
transition
temperature.
The
proposed
model
sug-
gests
that
the
combination
of
N-methylpyrrolidinium
([Hmpy]
+
)
cation
with
(heptafluoro-n-propyl)trifluoroborate
([C
3
F
7
BF
3
]
−
)
has
the
lowest
glass
transition
temperature
(T
g
=
156.2
K)
among
all
3182
possible
ionic
liquids
formed
by
the
combination
of
37
anions
and
86
cations
present
in
this
study.
5.
Validation
Validation
process
is
the
crucial
stage
for
the
assessment
of
the
model
stability
and
its
predictive
capability.
If
the
developed
model
stands
up
to
the
validation
scrutiny,
it
is
dubbed
as
“verified”
model
and
could
be
safely
employed
to
estimate
the
particular
properties.
The
various
validation
techniques
applied
in
this
study
described
as
follows:
5.1.
F-Test
F
is
the
F-ratio
which
is
defined
as
the
ratio
between
the
model
summation
of
squares
(MSS)
and
the
residual
summation
of
squares
(RSS)
F
=
MSS/df
M
RSS/df
E
(5)
where
df
M
and
df
E
denote
the
degree
of
freedom
of
the
obtained
model
and
the
overall
error
respectively.
It
is
a
comparison
between
the
model
explained
variance
and
the
residual
variance.
It
should
be
noted
that
high
values
of
the
F-ratio
test
indicate
the
reliability
of
models.
The
calculated
F-value
is
equal
to
73.31.
S.A.
Mirkhani
et
al.
/
Thermochimica
Acta
543 (2012) 88–
95
91
150
200
250
300
350
400
450
150
200
250
300
350
400
450
T
g
exp
(K)
T g
rep/pred
(K)
Training set
Test set
Fig.
1.
Experimental
glass
transition
values
versus
predicted
ones.
5.2.
LOO
(leave
one
out)
validation
technique
Leave-one-out
belong
the
most
common
and
extensively
used
validation
techniques
known
as
internal
validation.
Internal
or
cross-over
validation
techniques
based
on
partitioning
of
the
sam-
ple
data
into
two
different
subsets
one
serves
as
training
set
and
the
other
as
a
validation
set.
The
modified
training
set
was
generated
by
deleting
one
object
from
the
original
data
set.
For
each
reduced
data
set,
the
model
is
calculated
and
responses
for
the
deleted
object
were
calculated
from
the
model.
The
evaluated
leave-
one-out
cross
validation
parameter
of
the
obtained
linear
model
is
0.8559.
5.3.
Adjusted
R-squared
(R
2
adj
)
In
a
multiple
linear
regression
model,
adjusted
R
2
measures
the
proportion
of
the
variation
in
the
dependent
variable
accounted
for
by
the
explanatory
variables.
Unlike
R
2
,
adjusted
R
2
allows
for
the
degrees
of
freedom
associated
with
the
sums
of
the
squares.
Therefore,
even
though
the
residual
sum
of
squares
decreases
or
remains
the
same
as
new
explanatory
variables
are
added,
the
residual
variance
does
not.
For
this
reason,
adjusted
R
2
is
gen-
erally
considered
to
be
a
more
accurate
goodness-of-fit
measure
than
R
2
.
R
2
adj
=
1
−
(1
−
R
2
)
n
−
1
n
−
p
(6)
where
n
and
p
are
the
numbers
of
experimental
values
and
the
model
parameters,
respectively.
The
less
difference
between
this
value
and
the
R
2
parameter,
the
more
validity
of
the
model
would
be
expected.
The
evaluated
adjusted-R
2
parameter
of
the
obtained
linear
model
is
0.8775.
5.4.
RQK
validation
technique
In
lieu
of
avoiding
chance
correlations
in
the
model
and
improved
its
prediction,
Todeschini
et
al.
4
RQK
con-
straints
which
must
be
completely
satisfied
1.
K
=
K
XY
−
K
X
>
0
(quick
rule)
2.
Q
=
Q
2
LOO
−
Q
2
ASYM
>
0
(asymptotic
Q
2
rule)
150
200
250
300
350
400
450
−20
−15
−10
−5
0
5
10
15
T
g
exp
(K)
Relative Deviation %
Training set
Test set
Fig.
2.
Relative
deviation
of
the
model
prediction
versus
experimental
values
of
glass
transition
temperatures.
3.
R
P
>
0
(redundancy
RP
rule)
4.
R
N
>
0
(over-fitting
PN
rule)
The
calculated
values
of
RQK
test
are
presented
as
follows:
K
x
=
0.4264,
K
xy
=
0.4633,
K
=
0.037,
Q
=
0.006,
R
P
=
0.007
and
R
N
=
0.
These
values,
calculated
according
to
standard
procedures
are
non-negative,
which
supports
the
validity
of
the
model
and
the
lack
of
chance
correlation.
5.5.
Bootstrap
validation
technique
The
bootstrap
approach
was
applied
to
verify
robustness
and
internal
prediction
power
of
the
model.
In
this
method,
K
n-
dimensional
groups
are
generated
by
a
repeated
random
selection
of
n-chemicals
from
the
original
data
set
(K
=
300
and
n
=
139).
The
model
obtained
on
the
first
selected
chemicals
is
used
to
predict
the
values
for
the
excluded
compounds
and
then
Q
2
is
calculated
for
each
model.
The
bootstrapping
was
repeated
5000
times,
in
this
study.
Consequently,
the
value
Q
2
boot
parameter
of
the
obtained
model
has
been
evaluated
to
be
0.7992.
5.6.
y-Scrambling
validation
technique
The
objective
of
this
approach
is
to
assure
the
developed
model
is
not
to
be
a
chance
correlation.
For
this
purpose,
all
responses
variable
are
shuffled
randomly
without
any
changes
in
the
pre-
dictors
set.
If
the
prediction
power
of
the
model
in
terms
of
R
2
or
Q
2
does
not
change
significantly,
then
the
validity
of
the
model
is
disputable.
The
y-scrambling
parameter
is
the
intercept
of
the
following
equation:
Q
2
k
=
a
+
br
k
(y, ˜y
k
)
(7)
where
Q
2
k
k
is
the
explained
variance
of
the
model
obtained
using
the
same
predictors
but
the
kth
y-scrambled
vector;
r
k
is
the
cor-
relation
between
the
true
response
vector
and
the
kth
y-scrambled
vector.
The
numerical
value
of
the
intercept
a
is
a
criteria
for
assess-
ing
of
the
model
if
it
is
a
chance
correlation
or
not.
The
numerical
92
S.A.
Mirkhani
et
al.
/
Thermochimica
Acta
543 (2012) 88–
95
Table
2
Experimental
and
predicted
values
of
glass
transition
temperature
of
the
studied
ionic
liquids.
No.
Group
Abbreviation
Error,
T
g
(K)
T
g
T
pred
g
ARD%
Status
Reference
1
Phosphonium
[P666,2][Ace]
200.15
197.68
1.234074
Training
2
Phosphonium
[P666,3][Ace]
201.15
199.66
0.740741
Test
3
Tri-alkyl
imidazolium
[hmmim][TFSI]
199
208.06
4.552764
Training
4
Phosphonium
[P666,14][C(CN)3]
208.15
210.44
1.100168
Training
5
Phosphonium
[P444,14][TFSI]
213.15
203.75
4.41004
Test
6
Phosphonium
[P(ph)4][TFSI]
433.15
409.44
5.473854
Training
7
Pyrrolidinium
[P14][NfO]
194.15
185.96
4.218388
Test
8
Triazolium
[Bt14][dca]
208.15
218.38
4.914725
Training
9
Triazolium
[Bt14][mesy]
235.15
226.52
3.669998
Test
10
Triazolium
[Bt1Bn][TFSI]
246.15
253.59
3.022547
Training
11
Triazolium
[Bt1Bn][dca]
239.15
242.93
1.580598
Training
12
Triazolium
[Bt1Bn][mesy]
261.15
247.93
5.062225
Training
13
Tri-alkyl
imidazolium
[P1M2,3IM][TFSI]
191.15
208.86
9.264975
Training
14
Tri-alkyl
imidazolium
[BDMIM][BF4]
205.15
210.11
2.417743
Training
15
Tri-alkyl
imidazolium
[BDMIM][PF6]
215.15
210.65
2.091564
Training
16
Guanidinium
[(MeBu)N
(Me2Taz)][NO3]
204.15
210.39
3.056576
Test
17
Guanidinium
[(MeBu)N
(Me2Taz)][N(NO2)2]
207.15
211.83
2.259232
Test
18
Pyrrolidinium
[P12][mesy]
2
167.15
184.98
10.66707
Training
19
Pyrrolidinium
[P13][mesy]
2
201.15
183.77
8.640318
Training
20
Pyrrolidinium
[P14][mesy]
2
205.15
183.71
10.45089
Training
21
Morpholinium
[MO][(CF3CO)CH(COCH3)]
285.15
233.92
17.96598
Training
22
Morpholinium
[MO][(CF3CO)2CH]
211.15
240.02
13.67274
Test
23
Morpholinium
[MO][(Me3CCO)CH(CO(CF2)2CF3)]
235.15
250.11
6.361897
Training
24
Morpholinium
[MO][(CF3CO)CH(COfuran)]
225.15
247.4
9.882301
Test
25
Morpholinium
[MO1,2O2][NTf2]
220.15
216.18
1.803316
Training
26
Morpholinium
[MO1,2O5][NTf2]
219.15
217.36
0.816792
Training
27
Guanidinium
[C27guan][TFSI],
[((C6H13)2N)2C
NMe2][TFSI]
201.04
202.2
0.577
Test
28
Guanidinium
[((C6H13)2N)2C
NMe2][dca]
195.97
192.27
1.888044
Training
29
Guanidinium
[((C6H13)2N)2C
NMe2][TfO]
194.44
201.64
3.702942
Training
30
Guanidinium
[((C6H13)2N)2C
NMe2][Tos]
203.25
197.09
3.03075
Test
31
Guanidinium
[((C6H13)2N)2C
NMe2][CF3CO2]
192.49
196.68
2.176736
Training
32
Guanidinium
Dimethyl-ammonium
thiocyanate
200.72
181.73
9.460941
Training
33
Pyrrolidinium
[P14][dca]
2
167.15
176.49
5.587795
Training
34
Pyrrolidinium
[P16][dca]
2
173.15
174.39
0.716142
Training
35
Pyrrolidinium
[P13][TFSI]
2
183.15
185.85
1.474201
Training
36
Pyrrolidinium
[P12][TFSI]
171.15
185.87
8.600643
Training
37
1-Alkyl
imidazolium
[C1Im][OAc]
175.15
196.52
12.20097
Test
38
1-Alkyl
imidazolium
[C1Im][HCO2]
174.15
189.92
9.055412
Training
39
Pyrrolidinium
[Hmpy][OAc]
165.15
169.17
2.434151
Training
40
Pyrrolidinium
[Hmpy][HCO2]
157.15
159.91
1.756284
Training
41
Piperidinium
[PP13][TSAC]
190.15
195.57
2.850381
Training
42
Piperidinium
[PP1.1O1][TFSI]
188.15
185.61
1.349987
Training
43
Piperidinium
[PP1.1O2][TFSI]
182.15
197.15
8.234971
Training
44
Piperidinium
[PP1.1O2O2][TFSI]
191.15
212.55
11.1954
Training
45
Triazolium
1-Methyl-4-(3,3,3-trifluoropropyl)-
215.15
212.36
1.29677
Training
46
Triazolium
[C4(CH2)2CF3Taz][NTf2]
206.15
205.07
0.52389
Training
47
Triazolium
[C7(CH2)2CF3Taz][NTf2]
206.15
210.85
2.279893
Training
48
Triazolium
[C10(CH2)2CF3Taz][NTf2]
205.15
206.53
0.672679
Training
49
Triazolium
[C7C2FTaz][NTf2]
203.15
212.35
4.528673
Training
50
Triazolium
[C10C2FTaz][NTf2]
211.15
210.96
0.089983
Training
51
Triazolium
[C7CF3CH(OH)CH2Taz][NTf2]
221.45
211.49
4.497629
Training
52
Triazolium
[C10CF3CH(OH)CH2Taz][NTf2]
225.95
208.12
7.891126
Training
53
Triazolium
[C4(CH2)2CF
CF2Taz][NTf2]
250.75
219.99
12.2672
Test
54
Triazolium
[C7(CH2)2CF
CF2Taz][NTf2]
216.75
217.35
0.276817
Training
55
Triazolium
[C4CO(CF2)3COOH][TfO]
205.45
209.39
1.917742
Training
56
Tri-alkyl
imidazolium
[Em2Im][ba]
207.77
201.26
3.133272
Training
57
Tri-alkyl
imidazolium
[BM2Im][ba]
202.69
203.6
0.448961
Training
58
Tri-alkyl
imidazolium
[DMPIM][TFSI]
191.15
209.55
9.625948
Training
59
Isoquinolinium
[C12isoq][TFPB]
253.15
243.55
3.792218
Training
60
Isoquinolinium
[C18isoq][TFPB]
248.15
267.92
7.966955
Training
61
Tri-alkyl
imidazolium
[AcrylateC6MEIm][NTf2]
205.15
207.29
1.043139
Training
62
Pyrrolidinium
[PY2,AcrylateC6][TFSI]
196.15
190.66
2.798878
Training
63
Piperidinium
[AcylateC6MPiPer][NTf2]
207.15
194.94
5.89428
Training
64
1-Alkyl
imidazolium
[C2Im][ClO4]
192.15
213.85
11.29326
Test
65
1-Alkyl
imidazolium
[C2Im][BF4]
186.15
208.87
12.20521
Training
66
1-Alkyl
imidazolium
[C2Im][BETI]
187.15
194
3.660166
Training
67
1-Alkyl
imidazolium
[C2Im][PF6]
211.15
208.26
1.368695
Training
68
Phosphonium
[P666,4][Ace]
202.15
201.22
0.460054
Test
69
Phosphonium
[P6666][Ace]
207.15
203.4
1.810282
Training
70
Phosphonium
[P666,7][Ace]
204.15
201.12
1.484203
Training
71
Phosphonium
[P666,8][Ace]
203.15
205.17
0.994339
Training
72
Phosphonium
[P666,10][Ace]
203.15
199.91
1.594881
Test
73
Phosphonium
[P666,12][Ace]
201.15
197.99
1.570967
Training
74
Phosphonium
[P666,16][Ace]
203.15
195.13
3.947822
Training
S.A.
Mirkhani
et
al.
/
Thermochimica
Acta
543 (2012) 88–
95
93
Table
2
(Continued)
No.
Group
Abbreviation
Error,
T
g
(K)
T
g
T
pred
g
ARD%
Status
Reference
75
Pyrrolidinium
[P1,8][NTf2]
192.15
186.47
2.956024
Training
76
Piperidinium
[PP14][TFSI]
200.15
194.73
2.707969
Test
77
Piperidinium
[PP1,8][NTf2]
197.15
193.82
1.689069
Training
78
Triazolium
[EtOHNH2Taz][N3]
223.15
209.37
6.175218
Training
79
Triazolium
[AllylNH2Taz][N3]
216.15
211.75
2.035623
Training
80
Triazolium
[NH2AllylTaz][N3]
211.15
208.92
1.056121
Training
81
Pyrrolidinium
[P13][TFSI]
2
182.15
185.71
1.954433
Test
82
Amino
acids
[GlyC1][NO3]
247.15
249.12
0.797087
Test
83
Amino
acids
[AlaC1][NO3]
239.15
240.7
0.648129
Training
84
Amino
acids
[AlaC1][Ace]
250.15
248.13
0.807515
Test
85
Amino
acids
[AlaC1][PF6]
238.15
256.6
7.747218
Training
86
Amino
acids
[AlaC1][L-lactate]
249.15
247.06
0.838852
Training
87
Amino
acids
[AlaC1][SCN]
241.15
235.95
2.156334
Test
88
Amino
acids
[SerC1][NO3]
243.15
241.86
0.530537
Training
89
Amino
acids
[AlaC2][L-lactate]
244.15
240.85
1.351628
Training
90
Amino
acids
[ValC1][NO3]
240.15
233.11
2.931501
Training
91
Amino
acids
[Leu][NO3]
242.15
228.39
5.682428
Training
92
Amino
acids
[PheC1][NO3]
241.15
242.26
0.460294
Training
93
Isoquinolinium
[C8isoq][BETI]
193.75
204.85
5.729032
Training
94
Isoquinolinium
[C10isoq][BETI]
195.35
201.23
3.009982
Test
95
Isoquinolinium
[C12isoq][BETI]
197.15
200.03
1.460817
Training
96
Isoquinolinium
[C14isoq][BETI]
206.45
200.8
2.73674
Training
97
Isoquinolinium
[C16isoq][BETI]
211.35
202.56
4.158978
Test
98
Isoquinolinium
[C18isoq][BETI]
213.85
209.47
2.048165
Training
99
Isoquinolinium
[C8isoq][BETI]
218.15
202.87
7.004355
Training
100
Pyrrolidinium
[P14][BOB]
235.35
196.52
16.49883
Training
101
Triazolium
[MeNH2Taz][NO3]
213.15
198.93
6.671358
Training
102
Triazolium
[HN3Taz][Ntet]
238.15
234.05
1.721604
Training
103
Triazolium
[Me2Taz][ClO4]
239.15
209.9
12.23082
Training
104
Triazolium
[(CH2)2N3C1Taz][ClO4]
221.15
228.35
3.255709
Training
105
Triazolium
[(CH2)2N3C1Taz][NO3]
216.15
208.7
3.446681
Training
106
Triazolium
[N3(CH2)2Taz][ClO4]
217.15
226.78
4.434723
Training
107
Triazolium
[N3(CH2)2N3Taz][NO3]
219.15
210.44
3.974447
Training
108
Triazolium
[N3(CH2)2NH2Taz][ClO4]
227.15
228.16
0.44464
Training
109
Morpholinium
[HEMMor][BF4]
2
214.15
219.36
2.432874
Training
110
Morpholinium
[HEMMor][TFSI]
2
223.15
221.18
0.882814
Training
111
Phosphonium
[(C4H9)4P][Gly]
198.33
202.89
2.299198
Training
112
Phosphonium
[(C4H9)4P][Ala]
197.66
214.36
8.448852
Training
113
Phosphonium
[(C4H9)4P][Lys]
208.01
224.73
8.038075
Training
114
Triazolium
[Bt24][BF4]
218.15
221.69
1.622737
Training
115
Pyrrolidinium
[PY1,1O2][BF4]
180.15
184.85
2.608937
Test
116
Pyrrolidinium
[PY1,1O2][TFSI]
182.15
187.31
2.83283
Training
117
Piperidinium
[PP1.1O2][BF4]
196.15
193.21
1.498853
Training
118
Piperidinium
[PP1.1O2][TFSI]
191.15
196.25
2.668062
Training
119
Piperidinium
[PP1.1O2][C3F7BF3]
181.15
176.41
2.616616
Training
120
Piperidinium
[PP14][TFSI]
196.15
194.73
0.723936
Test
121
Morpholinium
[MO1,4][TFSI]
213.15
217.66
2.115881
Test
122
Morpholinium
[MO1,4][CF3BF3]
199.15
204.6
2.736631
Training
123
Morpholinium
[MO1,4][C2F5BF3]
200.15
204.41
2.128404
Test
124
Morpholinium
[MO1,1O2][BF4]
215.15
217.51
1.096909
Training
125
Morpholinium
bis((trifluoromethyl)sulfonyl)imide
207.15
220.18
6.290128
Training
126
Morpholinium
[MO1,1O2][C2F5BF3]
195.15
206.9
6.021009
Training
127
Morpholinium
[MO1,1O2][C3F7BF3]
198.15
200.98
1.428211
Training
128
Oxazolidinium
[OX14][BF4]
198.15
196.87
0.645975
Training
129
Oxazolidinium
[OX14][TFSI]
197.15
199.57
1.227492
Training
130
Oxazolidinium
[OX1,1O2][BF4]
203.15
200.36
1.373369
Training
131
Oxazolidinium
[OX1,1O2][TFSI]
200.15
203.38
1.61379
Training
132
Oxazolidinium
[OX1,1O2][CF3BF3]
187.15
189.67
1.346513
Test
133
Oxazolidinium
[OX1,1O2][C2F5BF3]
185.15
190.36
2.813935
Training
134
Oxazolidinium
[OX1,1O2][C3F7BF3]
189.15
183.34
3.071636
Training
135
Oxazolidinium
[OX1,1O2][C4F9BF3]
191.15
188.68
1.292179
Training
136
Guanidinium
[C19guan][BF4],
[((C4H9)2N)2C NMe2][BF4]
215.45
214.91
0.250638
Training
137
Guanidinium
[C27guan][BF4],
[((C6H13)2N)2C
NMe2][BF4]
197.55
200.21
1.346495
Training
138
Guanidinium
[C27guan][TFSI],
[((C6H13)2N)2C
NMe2][TFSI]
201.75
202.22
0.232962
Training
139
Guanidinium
[C35guan][BF4],
[((C8H17)2N)2C
NMe2][BF4]
197.85
192.12
2.896133
Training
values
close
to
zero
verify
that
the
model
is
not
a
chance
correla-
tion.
In
other
hand,
the
large
values
cast
doubt
on
the
validity
of
model
and
interpret
the
model
as
unstable,
chance
correlation.
The
y-scrambling
should
be
repeated
hundreds
of
times
(in
this
work
300
times).
The
value
of
intercept
a
has
been
calculated
as
0.061
for
the
developed
linear
model.
5.7.
External
validation
technique
External
validation
technique
is
conducted
by
testing
addi-
tional
compound
for
validation
set
in
order
to
assess
the
prediction
capability
of
the
model.
The
Q
2
ext
demonstrated
as
follows
94
S.A.
Mirkhani
et
al.
/
Thermochimica
Acta
543 (2012) 88–
95
Q
2
ext
=
1
−
n
test
i
=1
(
y
i/i
−
y
i
)
2
n
test
i
=1
(y
i
− ¯y
training
)
2
(8)
where ¯y
training
is
the
average
value
of
the
glass
transition
temper-
ature
of
the
compounds
present
in
training
set, ˆy
i/i
is
response
of
ith
object
predicted
by
the
obtained
model
ignoring
the
value
of
the
related
object
(ith
experimental
glass
transition
temperature).
The
less
difference
between
this
value
and
the
R
2
parameter,
the
more
validity
of
the
model
would
be
expected.
The
evaluated
Q
2
ext
parameter
of
the
obtained
linear
model
is
0.8449.
Ultimately,
all
the
validation
techniques
demonstrate
the
final
model
as
valid,
stable,
non-chance
correlation
with
high
predictive
power.
the
predicted
glass
transition
temperature
val-
ues
versus
the
experimental
ones.
As
it
is
obvious
in
this
figure
the
majority
of
points
are
located
in
the
vicinity
of
bisection.
This
indicates
the
acceptable
accuracy
of
the
prediction.
Relative
errors
of
the
predicted
glass
transition
temperature
val-
ues
in
comparison
with
experimental
ones
are
portrayed
in
it
is
shown
in
this
figure,
the
relative
errors
of
the
majority
of
points
lie
in
0–3%
interval
which
indicated
acceptable
prediction
error.
The
ionic
liquids
abbreviations,
predicted
glass
transition
values
and
the
prediction
are
tabulated
in
More
complete
table
including
data
of
the
calcu-
lated
model
descriptors
for
all
ionic
liquids
is
available
through
The
highest
error
of
prediction
belongs
to
morpholinium
1,1,1-trifluoro-2,4-pentanedionate
with
17.96%.
The
lowest
error
reported
in
our
study
is
0.089%
for
1-decyl-4-(1-fluoroethyl)-1,2,4-
triazolium
bis((trifluoromethyl)sulfonyl)imide.
The
groups
of
1-alkyl
imidazolium
and
oxazolidinium
ionic
liq-
uids
have
the
highest
and
lowest
prediction
error
with
8.29%
and
1.67%
respectively.
6.
Conclusion
In
this
study,
a
QSPR
model
was
presented
for
prediction
of
the
glass
transition
temperature
of
several
ionic
liquids.
The
pro-
posed
model
is
a
multivariate
linear
one
involving
eleven
variables
(molecular
descriptors),
which
has
been
developed
based
on
the
experimental
data
of
139
ionic
liquids.
The
molecular
descriptors
were
selected
using
GFA
technique
and
are
calculated
based
on
the
SMILE
structure
of
ionic
liquids.
The
obtained
results
show
that
the
presented
model
is
simple,
and
accurate.
Appendix
A.
Supplementary
data
Supplementary
data
associated
with
this
article
can
be
found,
in
the
online
version,
at
http://dx.doi.org/10.1016/j.tca.2012.05.009
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