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International Journal of Modern Research in Engineering and Technology (IJMRET)
www.ijmret.org Volume 2 Issue 4 ǁ August 2017.
w w w . i j m r e t . o r g I S S N : 2 4 5 6 - 5 6 2 8 Page 1
Studying the Effect of Counter Ions on the Gas Selectivity and
Volatile Organic Compounds Separation
Fatimah Edhaim1
andAlexander Rothenberger1
1
Physical Science and Engineering Division, King Abdullah University of Science and Technology, Thuwal,
Kingdom of Saudi Arabia
ABSTRACT:The synthesis and characterization of three new metal chalcogenide aerogels, Chalcogels,
AFe3Zn3S17 (A= Na, K, or Rb) is described. Alkali metal polychalcogenides (Na2S5, K2S5, or Rb2S5)
reactwith metal acetate like Fe(OAc)2 and Zn(OAc)2in formamide solutionforming extended polymeric
frameworks by gelation. Chalcogels obtained aftersupercritical drying have BET surface areas of
430, 444, and 435 m2
/g for NaFe3Zn3S17, KFe3Zn3S17, and RbFe3Zn3S17, respectively. The effect of the
counter ions (K, Na, and Rb) wasstudied by examined the adsorption capacities of the resulting
chalcogels toward different gases and volatile organic compounds. The measurements showed that
CO2 and toluene adsorption capacities increase with the polarizability of the surface atoms in the
following order: Rb chalcogel> K chalcogel> Na chalcogel.This finding reveals a trend based on
cation size and acid–base surface properties that might have a significant impact on altering
adsorptive properties of chalcogels by using more polarizable counter ions.
KEYWORDS –Adsorption, Chalcogel, Gas and hydrocarbon selectivity, Mesoporous, Separation
I. INTRODUCTION
Volatile organic compounds (VOCs) term
represent a broad range of chemical substances that
are frequently used and emitted from chemical and
petrochemical industries. These materials are
considered to be one of the major air pollutants as
they contribute to the depletion of the ozone layer,
and increase the global warming. Moreover, some of
them are harmful to humans, plants, and animals.
Owing to their volatile nature, they rapidly combine
with the atmospheric air forming fog. Therefore, it is
important to innovate systems to reduce the emission
of VOCs into the atmosphere in an efficient and
economical manner.
Several techniques have been developed to lessen
the emission of such toxic materials such as
filtration, distillation, and absorption separation. Of
these technologies, adsorption-using membranes like
zeolite, polymeric resins, and silica gel has been
known as an effective, relatively inexpensive and
high selective method for the efficient removal of
VOCs.[1]
Recently, metal chalcogenide aerogels or chalcogels
have been described as adsorbents for selective
separations of VOCs.[2]
Chalcogels are amorphous
porous materials in which chalcogenide building
blocks are connected to transition metal ions
forming polymeric frameworks.[3]
Unlike most
porous materials, which have surfaces covered
with carbon or oxygen,[3]
Chalcogels have
surfaces coated with more polarizable and softer
chalcogen ions, [Qx]2-
(Q= S, Se, and Te; x= 1-
5),[3-4]
which provide an opportunity to explore
interactions with different molecules.
Chalcogels are usually synthesized using thesol-
gel metathesis route, which allows the usage of
various molecular chalcogenide units to form a
wide range of novel porous materials.
Recently, ithas been demonstrated that the
metathesis reaction between mixture salts and K2S5
in formamide gives rise to amorphous and high
surface area chalcogels. These chalcogels have
negatively charged networks, which are balanced by
K+
cations.[5]
Therefore, these cations are part of the
chalcogels and located within the pores to balance
the framework charge.
Incorporation of these cations within the chalcogels
causes high electrical field gradients inside the
pores. Also, the presence of soft and heavy
chalcogen atoms like sulfur on the chalcogel
surfaces results in basicity of the chalcogel
frameworks. Thus, these chalcogels show high
selectivity and large adsorption capacities toward
acidic gas like CO2 and volatile hydrocarbon vapor
like toluene.
It is well known that polar or polarizable molecules
prefer to interact with the cation sites (alkali metal
species) within porous materials and get adsorbed on
their surfaces. However, the preferential adsorptions
of the molecules vary based on the cation types,
which induce an electric field inside the pores.
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Accessible pore volume and pore size also
significantly affect the adsorptive properties of
porous materials.
Barthomeuf[6]
noticed that the adsorption capacity of
faujasites containing larger alkali metals, as charge
compensating, toward payroll (acid probe
molecules) is greater than those with a smaller cation
size. The low electronegativity of large alkali metal
ions enhances the negative charge on the pore
frameworks, and hence, increases the basicity of the
porous materials. Therefore, it is reasonable to
expect porous adsorbents containing large cations
like Cs, Rb or K could have higher adsorption
capacities for acidic adsorbates than those with
smaller size such as Li or Na.
Talu and coworkers[7]
studied the influence of ion
exchange of alkaline earth metals in Y and Z zeolites
on the methane adsorption. He observed
improvement of zeolite capacity toward methane
with increasing cation size. Talu proposed that the
small alkaline earth cations were shielded by some
cavities' molecules and limited from the interactions
with adsorbates. The shielding effect, however, does
not exist with the large cations, and hence more
adsorbate molecules would be affected and got
adsorbed.
The effect of counter-ions on the adsorption
properties has frequently been studied in zeolites.
However, up to date, there are no studies reported
about the counter-ion effects onto metal chalcogels.
Therefore, we have been motivated to investigate the
influence of different alkali metals on the adsorption
capacity of chalcogels. Chalcogels containing K+
have been investigated for gas and volatile
hydrocarbon separation, but the effect of the
presence of different alkali metals (K, Na, or Rb) on
the adsorption properties of chalcogels has not been
studied and hence is worth to be further investigated.
In this work, we synthesized three amorphous and
high surface area chalcogels AFe3Zn3S17 (A= Na, K,
or Rb) and examined the effect of present different
counter-ion size on the VOCs separation and
selective gas adsorption. The higher adsorption
capacity of CO2 and toluene vapor was found in the
following order: RbFe3Zn3S17> KFe3Zn3S17>
NaFe3Zn3S17. Our measurements revealed that the
adsorption capacity of Rb forms, where the
polarizability (cation size) and acid–base surface
properties are dominant, is the greatest.
II. EXPERIMENTAL
2.1 Synthesis
Zinc acetate (Alfa, anhydrous 99.98%), Iron(II)
acetate (Strem Chemicals, 97% anhydrous),
formamide (acros, 99.5%), absolute ethanol
(Aldrich, 99.8%), toluene (Fisher Scientific, 99.9%)
and cyclohexane (Roth Chemicals, 99.5%) were
used as received. Na2S5, K2S5, and Rb2S5 were
freshly prepared according to the literature
procedure(Fig.S1, Supporting Information)[8]
The
solvents were degased for around 12 h by bubbling
N2 gas, then placed inside a nitrogen-filled glovebox
(c(O2) < 0.1 ppm, c(H2O) < 0.1 ppm). Synthesis of
the chalcogels and solvent exchange were achieved
inside a glovebox under nitrogen.
2.2 Synthesis of NaFe3Zn3S17, KFe3Zn3S17and
RbFe3Zn3S17 Chalcogels
An amount of 17.39mg (0.1mmol) Fe(OAc)2and
18.34mg (0.1mmol) Zn(OAc)2were dissolved in 1.5
ml of formamide and mixed with another 1.5 ml of
formamide solution containing 41.26 mg, 47.70mg
or 66.25mg (0.2 mmol) of Na2S5, K2S5or Rb2S5,
respectively. Upon mixing the two solutions, a clear
dark black solution was obtained. The viscosity of
these solutions significantly increased, and the
solutions solidified into black monolithic wet gels in
a minimum one-week. The residual formamide was
poured, and the wet gels were subsequently washed
with absolute ethanol from 8 to 10 times to remove
all unreacted precursors and counter ions. The wet
gels then were dried using supercritical drying with
CO2 at 35o
C to obtain superfine black chalcogels.
III. RESULTS AND DISCUSSION
In this study, polychalcogenide clusters (Na2S5,
K2S5,or Rb2S5) and metal ion linkers (Fe2+
and Zn2+
)
were separately dissolved in formamide and mixed
at room temperature. During aging period, the
mixtures were left undisturbed for a week to allow
the viscosity of the solution to increase gradually
and form a rigid gel, Fig.1; the color also became
darker indicating gradual polymerization. The
resulting wet gels then undergo solvent exchange
followed by supercritical CO2 drying processes to
produce aerogels. The final metal chalcogenide
aerogels are brittle with black and very lightweight
particles.
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Figure1Visual representation of the sol–gel process in formamide
solutions (FM) at room temperature (RT), before the solvent
exchange, showing the completed metathesis reaction of wet gels.
3.1 Characterization
The porous morphology, spongy nature and smooth
surface structures of the chalcogels have been
detected by the scanning electron microscopy (SEM)
technique. The absence of dark areas in micro scale
demonstrated single-phase chalcogels. The
aggregation of the primary particles of nanometer
size forms the secondary (large) particles of
micrometer size (Fig. 2 A (a) B (a) and C (a)).
Transmission electron microscope (TEM) results
confirm the random porosities within the framework
(Fig. 2 A (b), B (b) and C (b)). Electron diffraction
studies of multiple regions of the samples prove the
absence of any crystalline phases, inset of Fig. 2 (A,
B, C).
Energy dispersive spectroscopy analysis (EDS)
approve that not only transition metals and the
polysulfide species are present, but alkali metals
(Na, K, Rb) also incorporate as a part of the
chalcogels. The average percentage of each element
is summarized in Fig. S2, Supporting Information.
FTIR analyses have been recorded to reveal any
residual species of organic materials after drying
processes. Some vibration bands that are assigned to
the residual amount of formamide species have been
observed; indicating a trace amount of formamide is
incorporating within the chalcogel frameworks (Fig.
S3, Supporting Information).
Figure 2Characterization and properties of the (A) NaFe3Zn3S17,
(B) KFe3Zn3S17, and (C) RbFe3Zn3S17gels. (a) Scanning electron
microscope (SEM) showing fluffy features throughout the micron
sized specimens and porous nature of these materials. (b) Low
and high magnification transition electron microscope (TEM)
images showing a nano-scale porous structure of chalcogel.
Multiple diffraction rings (inset) confirms the absence of
crystalline structure within the chalcogel network. (c) Nitrogen
adsorption–desorption isotherm. (d) Pore-size distribution plot
calculated from the adsorption isotherm by the BJH method.
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Thermogravimetric (TGA) results of the super-
critically dried chalcogel materials show small
weight loss up to 150°C (4, 7 and 3 %) for
NaFe3Zn3S17, KFe3Zn3S17and RbFe3Zn3S17,
respectively, which can be attributed to evaporation
of chemisorbed or physisorbed solvent (Fig. S4,
Supporting Information). The weight loss from
200°C to 400°C attributed to the loss of sulfur from
the inorganic frameworks, as approved by EDS after
TGA(Fig. S5, Supporting Information). The total
weight loss up to 600°C is 45%, 85% and 40% for
NaFe3Zn3S17, KFe3Zn3S17,and RbFe3Zn3S17,
respectively.
The powder XRD patterns for the tested chalcogels
indicated in the Fig. S6, Supporting Information.
Recorded patterns support the electron diffraction
data and confirm the absence of any crystalline
phase.
3.2 Adsorption Studies
Nitrogen physisorption isotherms of the resulting
samples at 77 K, total pore volume and BET
(Brunauer Emmett Teller) surface area were
determined using ASAP 2020, Micromeritics
Instruments. The resulting chalcogels possess similar
adsorption isotherms to the reported
chalcogels[9]
(Fig.2 A (c), B(c) and C (c)). The
contribution of micropores (d < 2 nm) indicated by
the minor adsorption at very low pressures (P/Po <
0.05). The most adsorption occurred at high
pressures (0.7 < P/Po < 1.0) where the macropores
(d > 50 nm) and mesopores (2 < d < 50 nm) are the
most contribute. The small hysteresis loop
demonstrated the slower desorption rate of nitrogen
comparing to the adsorption rate due to the
percolation effect of variable pore size.
The high BET surface areas (430, 444 and 435 m2
/g)
of NaFe3Zn3S17, KFe3Zn3S17and RbFe3Zn3S17
chalcogels, respectively, confirm the pore structures
of the chalcogels. The broad pore size distribution of
the chalcogels was established from BJH pore size
isotherms (Fig.2 A (d), B(d) and C (d)). The average
pore diameter of the resulting materials ranges from
24nm (NaFe3Zn3S17)to 20 nm (KFe3Zn3S17 and
RbFe3Zn3S17), as calculated from the total pore
volume and surface area with a rough approximation
of the pore shape as cylindrical and slit.
The skeletal density of the chalcogels was 2.37 g cm-
3
for NaFe3Zn3S17, 2.39 g cm-3
for KFe3Zn3S17 and
2.43 g cm-3
for RbFe3Zn3S17 chalcogel.
To evaluate the effect of alkali metals on the
adsorption properties of the chalcogels, we tested the
adsorption capacity of the targeted calcogels with
various volatile hydrocarbons (e.g., toluene and
cyclohexane) at room temperature. Based on the
recorded isotherms(Fig.3), the toluene uptake of
both chalcogels is much higher than cyclohexane
uptake, which suggests a strong interaction between
chalcogel surface and polarizable molecules of
toluene (polarity index is 2.4). Enhancement of the
adsorption capacity of toluene is also possible
through π-complexation interaction.[10]
Figure 3Adsorption isotherms of toluene and cyclohexane at
room temperature in (a) NaFe3Zn3S17, (b) KFe3Zn3S17, and (c)
RbFe3Zn3S17 chalcogels
The quantity adsorbed of toluene on the
NaFe3Zn3S17, KFe3Zn3S17and RbFe3Zn3S17
chalcogels is 2.7, 6.4, and 7.3 mmol/g, respectively,
as indicated in the toluene isotherms(Fig.3). These
results indicate that chalcogels containing larger
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cations have higher capacities for hydrocarbon
vapor. The presence of large cations within the
chalcogels induces larger electrical field than the
small cations, leading to higher adsorption capacity.
Also, it has been reported that small cations can
create week π–cation interactions,[11]
and hence lower
toluene vapor adsorption occurred on NaFe3Zn3S17
than KFe3Zn3S17 and RbFe3Zn3S17 chalcogels, Table
1.
Table 1Comparison of toluene adsorption capacity at 298 K.
Adsorbent Surface
Area (m2
/g)
Toluene adsorption
(mmol/g)
NaFe3Zn3S17 430 2.7
KFe3Zn3S17 444 6.4
RbFe3Zn3S17 435 7.3
The chalcogels were also investigated for CO2, CH4
and H2 separation at different temperatures. The
isotherms reveal that the adsorption capacity of the
chalcogels increased with increasing the cation size.
All of the chalcogels demonstrated higher adsorption
of CO2 than CH4 and H2 over the chalcogels (Fig. 4,
and Fig. S7, Supporting Information). These results
can be explained by polarization. As CO2 is more
polarizable than CH4 and H2, more interactions with
the polarizable surface of the chalcogels through
dispersion force could occur (polarizability α in units
of 10–24
cm3
: α (CO2) = 2.9 > α (CH4) = 2.6 > α (H2)
= 0.8).[4]
We also observed that the adsorption
capacity of the chalcogels toward CO2 increased in
the following order: RbFe3Zn3S17> KFe3Zn3S17 >
NaFe3Zn3S17. The adsorption capacity of the
chalcogels and the strength of the adsorption can be
controlled by the interactions between the electric
field, produced by the cations on the adsorbent
surfaces, and the adsorbate molecules. As the Rb
ions are larger and more polarizable than the Na or
K ions, more electrostatic interactions can be
induced on the RbFe3Zn3S17, and hence more
adsorption occurred. The acid–base features of the
chalcogel frameworks also contributed in improving
adsorption properties. The cations are acid species,
and the sulfidic surfaces next to the cations act as
basic sites. As the cation size increases, the basicity
sulfidic surfaces increases because the lower
electronegativity of the alkali metal cations induced
the negative charge on the sulfur atoms in the
frameworks. Thus, it is logical to expect chalcogels
with larger cations like Rb would have more
adsorption capacity for acidic adsorbates like CO2.
Figure 4Gas adsorption isotherms of CO2, CH4, and H2
observed (a) NaFe3Zn3S17, (b) KFe3Zn3S17, and (c) RbFe3Zn3S17
at 0 °C.
The presence of large rubidium atoms renders pore
surface of the sulfidic chalcogels more polarizable,
and this is reflected in its selectivity toward gases.
Prediction of gas selectivity using the ideal adsorbed
solution theory (IAST) from single component
isotherms showed almost double selectivity values
(CO2/H2: 180 and CO2/CH4: 60) for RbFe3Zn3S17
compared to KFe3Zn3S17 chalcogels with selectivity
values (CO2/H2: 120 and CO2/CH4: 35).
RbFe3Zn3S17 also reveal around four times higher
selectivity than NaFe3Zn3S17 chalcogel (CO2/H2: 11
and CO2/CH4: 5) (Fig. 5, Table 2). This again
revealed the reactivity of acidic CO2 toward the
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basic characteristic of the chalcogels containing
large cations. This finding indicates that adsorption
property of the chalcogel depends on the chemical
composition of the chalcogels and the cations
present within the pore frameworks.
Figure 5Selectivity of CO2 over H2 and CO2 over CH4in (a)
NaFe3Zn3S17, (b) KFe3Zn3S17, and (c) RbFe3Zn3S17as predicted by
IAST for equimolar mixtures of CO2/H2 and CO2/CH4 at 273 K
(Ptotal is the total pressure of the gas mixture).
Table 2Ionic radii of alkali metals and Selectivity of the
corresponding calcogels
Cation Radius
(A˚)
Corresponding
Chalcogel
Selectivity
CO2/CH4,
CO2/CH4
Na+
0.97 NaFe3Zn3S17 11, 5
K+
1.33 KFe3Zn3S17 120, 35
Rb+
1.47 RbFe3Zn3S17 180, 74
IV. CONCLUSIONS
Three chalcogels (NaFe3Zn3S17, KFe3Zn3S17and
RbFe3Zn3S17) have been synthesized using the sol-
gel metathesis reaction. The resulting chalcogels
possess high BET surface areas and are capable of
separation of different hydrocarbons and gases. The
results demonstrated that the largest capacities
toward toluene and CO2 vapor were achieved by
chacogels containing the large Rb cations because
they have larger polarizability, and can induce more
electrostatic interaction than smaller cations. These
results indicate that adsorption properties of the
chalcogels could be improved by altering the
composition of the materials.
V. Acknowledgements
This work was supported by King Abdullah University of Science
and Technology, KAUST. We thank Dr. Rachid
Sougrat(Advanced Nanofabrication, Imaging, and
Characterization Core Lab) for TEM analysis.
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Supplementary Figures:
Figure S1a) Experimental procedure of starting material A2S5 (A= Na, K, and Rb), (b, c and
d) Powder XRD patterns of the starting materials A2S5 (A= Na, K, and Rb), respectively,
confirming their purity.
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Figure S2EDS result of the resultingchalcogels after drying. Inset the table of the elements
showing the average composition.
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Figure S3 FTIR spectra showing some vibration peaks belong to the formamide species.
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Figure S4TGA of the resulting chalcogels showing gradual weight loss of (a) NaFe3Zn3S17,
(b) KFe3Zn3S17 and (c) RbFe3Zn3S17 chalcogels, under 20 ml min−1
of nitrogen flow and 10 K
min−1
of heating rate.
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Figure S5EDS analysis after TGA of the resulting chalcogelsshowing the residual of the
chalcogel.
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Figure S6 Powder XRD resultsshow the amorphous nature of the prepared chalcogenide
aerogels.
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www.ijmret.org Volume 2 Issue 4 ǁ August 2017.
w w w . i j m r e t . o r g I S S N : 2 4 5 6 - 5 6 2 8 Page 13
Figure S7Gas adsorption isotherms of CO2, CH4, and H2 observed (a) NaFe3Zn3S17, (b)
KFe3Zn3S17 and (c) RbFe3Zn3S17 at -10 °C.

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Studying the Effect of Counter Ions on the Gas Selectivity and Volatile Organic Compounds Separation

  • 1. International Journal of Modern Research in Engineering and Technology (IJMRET) www.ijmret.org Volume 2 Issue 4 ǁ August 2017. w w w . i j m r e t . o r g I S S N : 2 4 5 6 - 5 6 2 8 Page 1 Studying the Effect of Counter Ions on the Gas Selectivity and Volatile Organic Compounds Separation Fatimah Edhaim1 andAlexander Rothenberger1 1 Physical Science and Engineering Division, King Abdullah University of Science and Technology, Thuwal, Kingdom of Saudi Arabia ABSTRACT:The synthesis and characterization of three new metal chalcogenide aerogels, Chalcogels, AFe3Zn3S17 (A= Na, K, or Rb) is described. Alkali metal polychalcogenides (Na2S5, K2S5, or Rb2S5) reactwith metal acetate like Fe(OAc)2 and Zn(OAc)2in formamide solutionforming extended polymeric frameworks by gelation. Chalcogels obtained aftersupercritical drying have BET surface areas of 430, 444, and 435 m2 /g for NaFe3Zn3S17, KFe3Zn3S17, and RbFe3Zn3S17, respectively. The effect of the counter ions (K, Na, and Rb) wasstudied by examined the adsorption capacities of the resulting chalcogels toward different gases and volatile organic compounds. The measurements showed that CO2 and toluene adsorption capacities increase with the polarizability of the surface atoms in the following order: Rb chalcogel> K chalcogel> Na chalcogel.This finding reveals a trend based on cation size and acid–base surface properties that might have a significant impact on altering adsorptive properties of chalcogels by using more polarizable counter ions. KEYWORDS –Adsorption, Chalcogel, Gas and hydrocarbon selectivity, Mesoporous, Separation I. INTRODUCTION Volatile organic compounds (VOCs) term represent a broad range of chemical substances that are frequently used and emitted from chemical and petrochemical industries. These materials are considered to be one of the major air pollutants as they contribute to the depletion of the ozone layer, and increase the global warming. Moreover, some of them are harmful to humans, plants, and animals. Owing to their volatile nature, they rapidly combine with the atmospheric air forming fog. Therefore, it is important to innovate systems to reduce the emission of VOCs into the atmosphere in an efficient and economical manner. Several techniques have been developed to lessen the emission of such toxic materials such as filtration, distillation, and absorption separation. Of these technologies, adsorption-using membranes like zeolite, polymeric resins, and silica gel has been known as an effective, relatively inexpensive and high selective method for the efficient removal of VOCs.[1] Recently, metal chalcogenide aerogels or chalcogels have been described as adsorbents for selective separations of VOCs.[2] Chalcogels are amorphous porous materials in which chalcogenide building blocks are connected to transition metal ions forming polymeric frameworks.[3] Unlike most porous materials, which have surfaces covered with carbon or oxygen,[3] Chalcogels have surfaces coated with more polarizable and softer chalcogen ions, [Qx]2- (Q= S, Se, and Te; x= 1- 5),[3-4] which provide an opportunity to explore interactions with different molecules. Chalcogels are usually synthesized using thesol- gel metathesis route, which allows the usage of various molecular chalcogenide units to form a wide range of novel porous materials. Recently, ithas been demonstrated that the metathesis reaction between mixture salts and K2S5 in formamide gives rise to amorphous and high surface area chalcogels. These chalcogels have negatively charged networks, which are balanced by K+ cations.[5] Therefore, these cations are part of the chalcogels and located within the pores to balance the framework charge. Incorporation of these cations within the chalcogels causes high electrical field gradients inside the pores. Also, the presence of soft and heavy chalcogen atoms like sulfur on the chalcogel surfaces results in basicity of the chalcogel frameworks. Thus, these chalcogels show high selectivity and large adsorption capacities toward acidic gas like CO2 and volatile hydrocarbon vapor like toluene. It is well known that polar or polarizable molecules prefer to interact with the cation sites (alkali metal species) within porous materials and get adsorbed on their surfaces. However, the preferential adsorptions of the molecules vary based on the cation types, which induce an electric field inside the pores.
  • 2. International Journal of Modern Research in Engineering and Technology (IJMRET) www.ijmret.org Volume 2 Issue 4 ǁ August 2017. w w w . i j m r e t . o r g I S S N : 2 4 5 6 - 5 6 2 8 Page 2 Accessible pore volume and pore size also significantly affect the adsorptive properties of porous materials. Barthomeuf[6] noticed that the adsorption capacity of faujasites containing larger alkali metals, as charge compensating, toward payroll (acid probe molecules) is greater than those with a smaller cation size. The low electronegativity of large alkali metal ions enhances the negative charge on the pore frameworks, and hence, increases the basicity of the porous materials. Therefore, it is reasonable to expect porous adsorbents containing large cations like Cs, Rb or K could have higher adsorption capacities for acidic adsorbates than those with smaller size such as Li or Na. Talu and coworkers[7] studied the influence of ion exchange of alkaline earth metals in Y and Z zeolites on the methane adsorption. He observed improvement of zeolite capacity toward methane with increasing cation size. Talu proposed that the small alkaline earth cations were shielded by some cavities' molecules and limited from the interactions with adsorbates. The shielding effect, however, does not exist with the large cations, and hence more adsorbate molecules would be affected and got adsorbed. The effect of counter-ions on the adsorption properties has frequently been studied in zeolites. However, up to date, there are no studies reported about the counter-ion effects onto metal chalcogels. Therefore, we have been motivated to investigate the influence of different alkali metals on the adsorption capacity of chalcogels. Chalcogels containing K+ have been investigated for gas and volatile hydrocarbon separation, but the effect of the presence of different alkali metals (K, Na, or Rb) on the adsorption properties of chalcogels has not been studied and hence is worth to be further investigated. In this work, we synthesized three amorphous and high surface area chalcogels AFe3Zn3S17 (A= Na, K, or Rb) and examined the effect of present different counter-ion size on the VOCs separation and selective gas adsorption. The higher adsorption capacity of CO2 and toluene vapor was found in the following order: RbFe3Zn3S17> KFe3Zn3S17> NaFe3Zn3S17. Our measurements revealed that the adsorption capacity of Rb forms, where the polarizability (cation size) and acid–base surface properties are dominant, is the greatest. II. EXPERIMENTAL 2.1 Synthesis Zinc acetate (Alfa, anhydrous 99.98%), Iron(II) acetate (Strem Chemicals, 97% anhydrous), formamide (acros, 99.5%), absolute ethanol (Aldrich, 99.8%), toluene (Fisher Scientific, 99.9%) and cyclohexane (Roth Chemicals, 99.5%) were used as received. Na2S5, K2S5, and Rb2S5 were freshly prepared according to the literature procedure(Fig.S1, Supporting Information)[8] The solvents were degased for around 12 h by bubbling N2 gas, then placed inside a nitrogen-filled glovebox (c(O2) < 0.1 ppm, c(H2O) < 0.1 ppm). Synthesis of the chalcogels and solvent exchange were achieved inside a glovebox under nitrogen. 2.2 Synthesis of NaFe3Zn3S17, KFe3Zn3S17and RbFe3Zn3S17 Chalcogels An amount of 17.39mg (0.1mmol) Fe(OAc)2and 18.34mg (0.1mmol) Zn(OAc)2were dissolved in 1.5 ml of formamide and mixed with another 1.5 ml of formamide solution containing 41.26 mg, 47.70mg or 66.25mg (0.2 mmol) of Na2S5, K2S5or Rb2S5, respectively. Upon mixing the two solutions, a clear dark black solution was obtained. The viscosity of these solutions significantly increased, and the solutions solidified into black monolithic wet gels in a minimum one-week. The residual formamide was poured, and the wet gels were subsequently washed with absolute ethanol from 8 to 10 times to remove all unreacted precursors and counter ions. The wet gels then were dried using supercritical drying with CO2 at 35o C to obtain superfine black chalcogels. III. RESULTS AND DISCUSSION In this study, polychalcogenide clusters (Na2S5, K2S5,or Rb2S5) and metal ion linkers (Fe2+ and Zn2+ ) were separately dissolved in formamide and mixed at room temperature. During aging period, the mixtures were left undisturbed for a week to allow the viscosity of the solution to increase gradually and form a rigid gel, Fig.1; the color also became darker indicating gradual polymerization. The resulting wet gels then undergo solvent exchange followed by supercritical CO2 drying processes to produce aerogels. The final metal chalcogenide aerogels are brittle with black and very lightweight particles.
  • 3. International Journal of Modern Research in Engineering and Technology (IJMRET) www.ijmret.org Volume 2 Issue 4 ǁ August 2017. w w w . i j m r e t . o r g I S S N : 2 4 5 6 - 5 6 2 8 Page 3 Figure1Visual representation of the sol–gel process in formamide solutions (FM) at room temperature (RT), before the solvent exchange, showing the completed metathesis reaction of wet gels. 3.1 Characterization The porous morphology, spongy nature and smooth surface structures of the chalcogels have been detected by the scanning electron microscopy (SEM) technique. The absence of dark areas in micro scale demonstrated single-phase chalcogels. The aggregation of the primary particles of nanometer size forms the secondary (large) particles of micrometer size (Fig. 2 A (a) B (a) and C (a)). Transmission electron microscope (TEM) results confirm the random porosities within the framework (Fig. 2 A (b), B (b) and C (b)). Electron diffraction studies of multiple regions of the samples prove the absence of any crystalline phases, inset of Fig. 2 (A, B, C). Energy dispersive spectroscopy analysis (EDS) approve that not only transition metals and the polysulfide species are present, but alkali metals (Na, K, Rb) also incorporate as a part of the chalcogels. The average percentage of each element is summarized in Fig. S2, Supporting Information. FTIR analyses have been recorded to reveal any residual species of organic materials after drying processes. Some vibration bands that are assigned to the residual amount of formamide species have been observed; indicating a trace amount of formamide is incorporating within the chalcogel frameworks (Fig. S3, Supporting Information). Figure 2Characterization and properties of the (A) NaFe3Zn3S17, (B) KFe3Zn3S17, and (C) RbFe3Zn3S17gels. (a) Scanning electron microscope (SEM) showing fluffy features throughout the micron sized specimens and porous nature of these materials. (b) Low and high magnification transition electron microscope (TEM) images showing a nano-scale porous structure of chalcogel. Multiple diffraction rings (inset) confirms the absence of crystalline structure within the chalcogel network. (c) Nitrogen adsorption–desorption isotherm. (d) Pore-size distribution plot calculated from the adsorption isotherm by the BJH method.
  • 4. International Journal of Modern Research in Engineering and Technology (IJMRET) www.ijmret.org Volume 2 Issue 4 ǁ August 2017. w w w . i j m r e t . o r g I S S N : 2 4 5 6 - 5 6 2 8 Page 4 Thermogravimetric (TGA) results of the super- critically dried chalcogel materials show small weight loss up to 150°C (4, 7 and 3 %) for NaFe3Zn3S17, KFe3Zn3S17and RbFe3Zn3S17, respectively, which can be attributed to evaporation of chemisorbed or physisorbed solvent (Fig. S4, Supporting Information). The weight loss from 200°C to 400°C attributed to the loss of sulfur from the inorganic frameworks, as approved by EDS after TGA(Fig. S5, Supporting Information). The total weight loss up to 600°C is 45%, 85% and 40% for NaFe3Zn3S17, KFe3Zn3S17,and RbFe3Zn3S17, respectively. The powder XRD patterns for the tested chalcogels indicated in the Fig. S6, Supporting Information. Recorded patterns support the electron diffraction data and confirm the absence of any crystalline phase. 3.2 Adsorption Studies Nitrogen physisorption isotherms of the resulting samples at 77 K, total pore volume and BET (Brunauer Emmett Teller) surface area were determined using ASAP 2020, Micromeritics Instruments. The resulting chalcogels possess similar adsorption isotherms to the reported chalcogels[9] (Fig.2 A (c), B(c) and C (c)). The contribution of micropores (d < 2 nm) indicated by the minor adsorption at very low pressures (P/Po < 0.05). The most adsorption occurred at high pressures (0.7 < P/Po < 1.0) where the macropores (d > 50 nm) and mesopores (2 < d < 50 nm) are the most contribute. The small hysteresis loop demonstrated the slower desorption rate of nitrogen comparing to the adsorption rate due to the percolation effect of variable pore size. The high BET surface areas (430, 444 and 435 m2 /g) of NaFe3Zn3S17, KFe3Zn3S17and RbFe3Zn3S17 chalcogels, respectively, confirm the pore structures of the chalcogels. The broad pore size distribution of the chalcogels was established from BJH pore size isotherms (Fig.2 A (d), B(d) and C (d)). The average pore diameter of the resulting materials ranges from 24nm (NaFe3Zn3S17)to 20 nm (KFe3Zn3S17 and RbFe3Zn3S17), as calculated from the total pore volume and surface area with a rough approximation of the pore shape as cylindrical and slit. The skeletal density of the chalcogels was 2.37 g cm- 3 for NaFe3Zn3S17, 2.39 g cm-3 for KFe3Zn3S17 and 2.43 g cm-3 for RbFe3Zn3S17 chalcogel. To evaluate the effect of alkali metals on the adsorption properties of the chalcogels, we tested the adsorption capacity of the targeted calcogels with various volatile hydrocarbons (e.g., toluene and cyclohexane) at room temperature. Based on the recorded isotherms(Fig.3), the toluene uptake of both chalcogels is much higher than cyclohexane uptake, which suggests a strong interaction between chalcogel surface and polarizable molecules of toluene (polarity index is 2.4). Enhancement of the adsorption capacity of toluene is also possible through π-complexation interaction.[10] Figure 3Adsorption isotherms of toluene and cyclohexane at room temperature in (a) NaFe3Zn3S17, (b) KFe3Zn3S17, and (c) RbFe3Zn3S17 chalcogels The quantity adsorbed of toluene on the NaFe3Zn3S17, KFe3Zn3S17and RbFe3Zn3S17 chalcogels is 2.7, 6.4, and 7.3 mmol/g, respectively, as indicated in the toluene isotherms(Fig.3). These results indicate that chalcogels containing larger
  • 5. International Journal of Modern Research in Engineering and Technology (IJMRET) www.ijmret.org Volume 2 Issue 4 ǁ August 2017. w w w . i j m r e t . o r g I S S N : 2 4 5 6 - 5 6 2 8 Page 5 cations have higher capacities for hydrocarbon vapor. The presence of large cations within the chalcogels induces larger electrical field than the small cations, leading to higher adsorption capacity. Also, it has been reported that small cations can create week π–cation interactions,[11] and hence lower toluene vapor adsorption occurred on NaFe3Zn3S17 than KFe3Zn3S17 and RbFe3Zn3S17 chalcogels, Table 1. Table 1Comparison of toluene adsorption capacity at 298 K. Adsorbent Surface Area (m2 /g) Toluene adsorption (mmol/g) NaFe3Zn3S17 430 2.7 KFe3Zn3S17 444 6.4 RbFe3Zn3S17 435 7.3 The chalcogels were also investigated for CO2, CH4 and H2 separation at different temperatures. The isotherms reveal that the adsorption capacity of the chalcogels increased with increasing the cation size. All of the chalcogels demonstrated higher adsorption of CO2 than CH4 and H2 over the chalcogels (Fig. 4, and Fig. S7, Supporting Information). These results can be explained by polarization. As CO2 is more polarizable than CH4 and H2, more interactions with the polarizable surface of the chalcogels through dispersion force could occur (polarizability α in units of 10–24 cm3 : α (CO2) = 2.9 > α (CH4) = 2.6 > α (H2) = 0.8).[4] We also observed that the adsorption capacity of the chalcogels toward CO2 increased in the following order: RbFe3Zn3S17> KFe3Zn3S17 > NaFe3Zn3S17. The adsorption capacity of the chalcogels and the strength of the adsorption can be controlled by the interactions between the electric field, produced by the cations on the adsorbent surfaces, and the adsorbate molecules. As the Rb ions are larger and more polarizable than the Na or K ions, more electrostatic interactions can be induced on the RbFe3Zn3S17, and hence more adsorption occurred. The acid–base features of the chalcogel frameworks also contributed in improving adsorption properties. The cations are acid species, and the sulfidic surfaces next to the cations act as basic sites. As the cation size increases, the basicity sulfidic surfaces increases because the lower electronegativity of the alkali metal cations induced the negative charge on the sulfur atoms in the frameworks. Thus, it is logical to expect chalcogels with larger cations like Rb would have more adsorption capacity for acidic adsorbates like CO2. Figure 4Gas adsorption isotherms of CO2, CH4, and H2 observed (a) NaFe3Zn3S17, (b) KFe3Zn3S17, and (c) RbFe3Zn3S17 at 0 °C. The presence of large rubidium atoms renders pore surface of the sulfidic chalcogels more polarizable, and this is reflected in its selectivity toward gases. Prediction of gas selectivity using the ideal adsorbed solution theory (IAST) from single component isotherms showed almost double selectivity values (CO2/H2: 180 and CO2/CH4: 60) for RbFe3Zn3S17 compared to KFe3Zn3S17 chalcogels with selectivity values (CO2/H2: 120 and CO2/CH4: 35). RbFe3Zn3S17 also reveal around four times higher selectivity than NaFe3Zn3S17 chalcogel (CO2/H2: 11 and CO2/CH4: 5) (Fig. 5, Table 2). This again revealed the reactivity of acidic CO2 toward the
  • 6. International Journal of Modern Research in Engineering and Technology (IJMRET) www.ijmret.org Volume 2 Issue 4 ǁ August 2017. w w w . i j m r e t . o r g I S S N : 2 4 5 6 - 5 6 2 8 Page 6 basic characteristic of the chalcogels containing large cations. This finding indicates that adsorption property of the chalcogel depends on the chemical composition of the chalcogels and the cations present within the pore frameworks. Figure 5Selectivity of CO2 over H2 and CO2 over CH4in (a) NaFe3Zn3S17, (b) KFe3Zn3S17, and (c) RbFe3Zn3S17as predicted by IAST for equimolar mixtures of CO2/H2 and CO2/CH4 at 273 K (Ptotal is the total pressure of the gas mixture). Table 2Ionic radii of alkali metals and Selectivity of the corresponding calcogels Cation Radius (A˚) Corresponding Chalcogel Selectivity CO2/CH4, CO2/CH4 Na+ 0.97 NaFe3Zn3S17 11, 5 K+ 1.33 KFe3Zn3S17 120, 35 Rb+ 1.47 RbFe3Zn3S17 180, 74 IV. CONCLUSIONS Three chalcogels (NaFe3Zn3S17, KFe3Zn3S17and RbFe3Zn3S17) have been synthesized using the sol- gel metathesis reaction. The resulting chalcogels possess high BET surface areas and are capable of separation of different hydrocarbons and gases. The results demonstrated that the largest capacities toward toluene and CO2 vapor were achieved by chacogels containing the large Rb cations because they have larger polarizability, and can induce more electrostatic interaction than smaller cations. These results indicate that adsorption properties of the chalcogels could be improved by altering the composition of the materials. V. Acknowledgements This work was supported by King Abdullah University of Science and Technology, KAUST. We thank Dr. Rachid Sougrat(Advanced Nanofabrication, Imaging, and Characterization Core Lab) for TEM analysis. REFERENCES [1] a) D. Romero, D. Chlala, M. Labaki, S. Royer, J.-P. Bellat, I. Bezverkhyy, J.-M. Giraudon, J.-F. Lamonier, Removal of Toluene over NaX Zeolite Exchanged with Cu2+, Catalysts, 3(5), 2015, 1479-1497; b) S. Calero, P. Gomez-Alvarez, On the performance of FAU and MFI zeolites for the adsorptive removal of a series of volatile organic compounds from air using molecular simulation, PCCP, 17(39), 2015, 26451- 26455; c) Y. Yu, L. Zheng, J. Wang, Adsorption Behavior of Toluene on Modified 1X Molecular Sieves, J. Air Waste Manage. Assoc., 62(10), 2012, 1227-1232; d) K. Wormeyer, I. Smirnova, Adsorption of CO2, moisture and ethanol at low partial pressure using aminofunctionalised silica aerogels, Chem. Eng. J., 225(2013, 350-357; e) H. Wang, M. Tang, K. Zhang, D. Cai, W. Huang, R. Chen, C. Yu, Functionalized hollow siliceous spheres for VOCs removal with high efficiency and stability, J. Hazard. Mater., 268(2014, 115-123; f) C. Long, W. Yu, A. Li, Adsorption of n-hexane vapor by macroporous and hypercrosslinked polymeric resins: Equilibrium and breakthrough analysis, Chem. Eng. J., 221(2013, 105- 110; g) E. J. Simpson, R. K. Abukhadra, W. J. Koros, R. S. Schechter, Sorption equilibrium isotherms for volatile organics in aqueous solution. Comparison of head-space gas chromatography and on-line UV stirred cell results, Ind. Eng. Chem. Res., 32(10), 1993, 2269-2276. [2] a) F. Edhaim, A. Rothenberger, Rare Earth Chalcogels NaLnSnS4 (Ln = Y, Gd, Tb) for Selective Adsorption of Volatile Hydrocarbons and Gases, Z. Anorg. Allg. Chem., 2017; b) E. Ahmed, J. Khanderi, D. H. Anjum, A. Rothenberger, Selective Adsorption of Volatile Hydrocarbons and Gases in High Surface Area
  • 7. International Journal of Modern Research in Engineering and Technology (IJMRET) www.ijmret.org Volume 2 Issue 4 ǁ August 2017. w w w . i j m r e t . o r g I S S N : 2 4 5 6 - 5 6 2 8 Page 7 Chalcogels Containing [ES3]3– Anions (E = As, Sb), Chem. Mater., 26(22), 2014, 6454-6460. [3] Y. Oh, S. Bag, C. D. Malliakas, M. G. Kanatzidis, Selective Surfaces: High-Surface-Area Zinc Tin Sulfide Chalcogels, Chem. Mater., 23(9), 2011, 2447- 2456. [4] M. Shafaei-Fallah, A. Rothenberger, A. P. Katsoulidis, J. He, C. D. Malliakas, M. G. Kanatzidis, Extraordinary Selectivity of CoMo3S13 Chalcogel for C2H6 and CO2 Adsorption, Adv. Mater., 23(42), 2011, 4857-4860. [5] M. Shafaei-Fallah, J. Q. He, A. Rothenberger, M. G. Kanatzidis, Ion-Exchangeable Cobalt Polysulfide Chalcogel, JACS, 133(5), 2011, 1200-1202. [6] D. Barthomeuf, Conjugate acid-base pairs in zeolites, J. Phys. Chem., 88(1), 1984, 42-45. [7] a) S. Y. Zhang, O. Talu, D. T. Hayhurst, High-pressure adsorption of methane in zeolites NaX, MgX, CaX, SrX and BaX, J. Phys. Chem., 95(4), 1991, 1722- 1726; b) O. Talu, S. Y. Zhang, D. T. Hayhurst, Effect of cations on methane adsorption by NaY, MgY, CaY, SrY, and BaY zeolites, J. Phys. Chem., 97(49), 1993, 12894-12898. [8] Y. Oh, C. D. Morris, M. G. Kanatzidis, Polysulfide Chalcogels with Ion-Exchange Properties and Highly Efficient Mercury Vapor Sorption, JACS, 134(35), 2012, 14604-14608. [9] a) S. Bag, A. F. Gaudette, M. E. Bussell, M. G. Kanatzidis, Spongy chalcogels of non-platinum metals act as effective hydrodesulfurization catalysts, Nature. Chem., 1(3), 2009, 217-224; b) S. Bag, P. N. Trikalitis, P. J. Chupas, G. S. Armatas, M. G. Kanatzidis, Porous Semiconducting Gels and Aerogels from Chalcogenide Clusters, Science, 317(5837), 2007, 490. [10] X. Lin, A. J. Blake, C. Wilson, X. Z. Sun, N. R. Champness, M. W. George, P. Hubberstey, R. Mokaya, M. Schröder, A Porous Framework Polymer Based on a Zinc(II) 4,4„-Bipyridine-2,6,2„,6„- tetracarboxylate:  Synthesis, Structure, and “Zeolite- Like” Behaviors, JACS, 128(33), 2006, 10745-10753. [11] D. A. Dougherty, The Cation−π Interaction, Acc. Chem. Res., 46(4), 2013, 885-893. Supplementary Figures: Figure S1a) Experimental procedure of starting material A2S5 (A= Na, K, and Rb), (b, c and d) Powder XRD patterns of the starting materials A2S5 (A= Na, K, and Rb), respectively, confirming their purity.
  • 8. International Journal of Modern Research in Engineering and Technology (IJMRET) www.ijmret.org Volume 2 Issue 4 ǁ August 2017. w w w . i j m r e t . o r g I S S N : 2 4 5 6 - 5 6 2 8 Page 8 Figure S2EDS result of the resultingchalcogels after drying. Inset the table of the elements showing the average composition.
  • 9. International Journal of Modern Research in Engineering and Technology (IJMRET) www.ijmret.org Volume 2 Issue 4 ǁ August 2017. w w w . i j m r e t . o r g I S S N : 2 4 5 6 - 5 6 2 8 Page 9 Figure S3 FTIR spectra showing some vibration peaks belong to the formamide species.
  • 10. International Journal of Modern Research in Engineering and Technology (IJMRET) www.ijmret.org Volume 2 Issue 4 ǁ August 2017. w w w . i j m r e t . o r g I S S N : 2 4 5 6 - 5 6 2 8 Page 10 Figure S4TGA of the resulting chalcogels showing gradual weight loss of (a) NaFe3Zn3S17, (b) KFe3Zn3S17 and (c) RbFe3Zn3S17 chalcogels, under 20 ml min−1 of nitrogen flow and 10 K min−1 of heating rate.
  • 11. International Journal of Modern Research in Engineering and Technology (IJMRET) www.ijmret.org Volume 2 Issue 4 ǁ August 2017. w w w . i j m r e t . o r g I S S N : 2 4 5 6 - 5 6 2 8 Page 11 Figure S5EDS analysis after TGA of the resulting chalcogelsshowing the residual of the chalcogel.
  • 12. International Journal of Modern Research in Engineering and Technology (IJMRET) www.ijmret.org Volume 2 Issue 4 ǁ August 2017. w w w . i j m r e t . o r g I S S N : 2 4 5 6 - 5 6 2 8 Page 12 Figure S6 Powder XRD resultsshow the amorphous nature of the prepared chalcogenide aerogels.
  • 13. International Journal of Modern Research in Engineering and Technology (IJMRET) www.ijmret.org Volume 2 Issue 4 ǁ August 2017. w w w . i j m r e t . o r g I S S N : 2 4 5 6 - 5 6 2 8 Page 13 Figure S7Gas adsorption isotherms of CO2, CH4, and H2 observed (a) NaFe3Zn3S17, (b) KFe3Zn3S17 and (c) RbFe3Zn3S17 at -10 °C.