Wenqiang Ma1, Shuangping Xu1, Hongge Jia1, Jingyu Xu1,2, Da Liu3, Mingyu Zhang1, Yanqing Qu1, Hailiang Zhou1, Yushu Zhang1, Xintian Wang1, Wenwen Zhao1. 1. College of Materials Science and Engineering, Heilongjiang Provinces Key Laboratory of Polymeric Composite Materials, Qiqihar University, Qiqihar 161006, China. 2. Liaoning Key Lab of Lignocellulose Chemistry and BioMaterials, Liaoning Collaborative Innovation Center for Lignocellulosic Biorefinery, College of Light Industry and Chemical Engineering, Dalian Polytechnic University, Dalian 116034, China. 3. College of Chemical Engineering, Daqing Normal University, Daqing 163712, China.
Abstract
Excessive CO2 emissions have resulted in global warming and are a serious threat to the life of people, various strategies have been implemented to cut carbon emissions, and one of them is the use of a gas separation membrane to capture CO2 effectively. In this experiment, the butadiene-bridged polymethylsiloxane (BBPMS)/ethyl cellulose (EC)/ionic liquid (IL) ternary composite membranes were prepared by EC as a substrate, BBPMS, and IL as additives in tetrahydrofuran under high-speed stirring and coated on the membrane. The membrane structure was characterized by a Fourier transform infrared spectrometer and scanning electron microscope, and the membrane properties were tested by a membrane tensile strength tester, thermal weight loss analyzer, and gas permeability meter. The results show that the surface of the ternary composite membrane is dense and flat with a uniform distribution, and the membrane formation, heat resistance, and mechanical properties are good. The permeability coefficient of the ternary composite membrane for CO2 reached 1806.03 Barrer, which is 20.00 times higher than that of the EC/IL hybrid matrix membrane. The permeability coefficient of O2 reached 321.01 Barrer, which is 19.21 times higher than that of the EC/IL membrane. When the doping amount of BBPMS is 70-80%, the O2/N2 gas permeation separation of the BBPMS/EC/IL ternary composite membrane is close to the Robertson 2008 curve. It is always known that in the gas separation process the membrane material is the most crucial factor. The success of this experiment points to a new direction for the preparation of new membrane materials.
Excessive CO2 emissions have resulted in global warming and are a serious threat to the life of people, various strategies have been implemented to cut carbon emissions, and one of them is the use of a gas separation membrane to capture CO2 effectively. In this experiment, the butadiene-bridged polymethylsiloxane (BBPMS)/ethyl cellulose (EC)/ionic liquid (IL) ternary composite membranes were prepared by EC as a substrate, BBPMS, and IL as additives in tetrahydrofuran under high-speed stirring and coated on the membrane. The membrane structure was characterized by a Fourier transform infrared spectrometer and scanning electron microscope, and the membrane properties were tested by a membrane tensile strength tester, thermal weight loss analyzer, and gas permeability meter. The results show that the surface of the ternary composite membrane is dense and flat with a uniform distribution, and the membrane formation, heat resistance, and mechanical properties are good. The permeability coefficient of the ternary composite membrane for CO2 reached 1806.03 Barrer, which is 20.00 times higher than that of the EC/IL hybrid matrix membrane. The permeability coefficient of O2 reached 321.01 Barrer, which is 19.21 times higher than that of the EC/IL membrane. When the doping amount of BBPMS is 70-80%, the O2/N2 gas permeation separation of the BBPMS/EC/IL ternary composite membrane is close to the Robertson 2008 curve. It is always known that in the gas separation process the membrane material is the most crucial factor. The success of this experiment points to a new direction for the preparation of new membrane materials.
As
a major greenhouse gas, the increasing amount of CO2 in
the atmosphere and oceans is not only contributing to global
warming and climate change but is also having a significant impact
on the growth of some plants and microorganisms.[1] On the other hand, as an abundant and readily available
non-toxic carbon resource, CO2 has been used as an important
feedstock for the production of chemicals, fuels, and polymers.[2] Therefore, effective, simple, and cost-effective
separation and capture of carbon dioxide is important for reducing
the greenhouse effect and utilizing carbon resources.[3−5]Carbon dioxide separation and capture technologies mainly
include
temperature swing adsorption technology,[6] porous solid adsorption,[7] and membrane
separation.[8−10] Among them, the membrane separation methods are widely
used for their economic, efficient, and convenient advantages.[11,12] The separation of gases, such as CO2/CH4,
CO2/N2, and O2/N2 by membrane
separation methods, has a history of being used for several decades.[13] Various polymeric materials with excellent formability
and tunable properties, such as ethyl cellulose (EC), silicone rubber,
polyolefins, polyimides, and polysulfone, have been widely used as
membrane materials for gas separation.[14−16] EC is produced using
natural cellulose and has good membrane making properties, high tensile
strength, and carbon dioxide as well as oxygen selectivity; therefore,
it occupies an important position in the field of carbon dioxide and
oxygen separation.[17] However, the carbon
dioxide permeability coefficient of the pure membrane of ethylcellulose
is not high and to improve the gas separation performance, modification
or co-blending of ethylcellulose is a good method, by adding various
carbon-based hybrid matrix materials such as zeolites,[18] silica,[19] carbon
nanotubes,[20] titanium dioxide,[21] and ionic liquids (IL).[22] Although these methods can increase the permeability or/and selectivity
of CO2, their increment is limited due to poor compatibility
and a non-uniform distribution. Therefore, it is still important to
develop high-performance polymeric gas separation membrane materials
with high gas separation performance, good stability, mechanical properties,
durability, easy preparation process, and low cost.In recent
years, research on the application of polysiloxanes in
the direction of gas separation membranes has become more and more
extensive,[23] but little research has been
reported on the use of diene-based compounds bridged with polymethylhydrosiloxanes
(BBPMS). Diene-bridged polymethylsiloxane has become an important
research direction for gas separation membrane materials due to its
many unique features, such as simple reaction conditions, high gas
permeability, low cost input, and high structural variability.[24,25]EC as an abundantly available, renewable, and low cost non-ionic
cellulose ether was used in a lot of fields, such as food, filtration,
microencapsulation, and medicine.[26] Remarkably,
EC with a large number of ethyl groups and the unsubstituted hydroxyl
groups resulted in it possessing easy film formation[27] and good gas separation performance.[28,29]In order to further broaden the research of EC as gas separation
membrane materials, this paper is based on the groups’ previous
adequate research on the blended membrane of 1-carboxymethyl-3-methylimidazolium
chloride salt (IL) and EC.[26] A series of
butadiene-bridged BBPMS/EC/1-carboxymethyl-3-methylimidazolium chloride
(IL) composite membranes with butadiene-bridged BBPMS contents of
40, 50, 60, 70, 80, and 90% were prepared by incorporating polysiloxane.
The structural, mechanical, and thermal properties were characterized
and tested, and a series of hybrid matrix membranes were focused on
O2/N2 and CO2/N2 permeation
performance and separation selection performance. It is always known
that in the gas separation process, the membrane material is the key
factor.[30] In this paper, we propose and
prepare an effective and simple EC-based gas separation membrane with
preferential permeability to carbon dioxide. Successful preparation
of new membrane materials opens up new paths for the development of
separation membranes.
Experimental Section
Materials
EC was purchased from Chembee
(Shanghai, China). The EC (M70) was 40–100 MPa·s, 95%
pure, and contained 5% toluene/isopropanol = 80:20. PMHS and Karstedt’s
catalyst were purchased from Kejunchi Technology Co. (Shenzhen, China).
1-Carboxymethyl-3-methylimidazole chloride salt (IL) was purchased
from Aulico New Material Technology Co. (Qingdao, China). Butadiene
was purchased from Inokai Technology Co. (Beijing, China). Tetrahydrofuran
(THF) was purchased from Comio Chemical Reagent Co. (Tianjin, China),
the THF is analytically pure, 98% purity.
Preparation
of Butadiene-Bridged BBPMS
According to Scheme , a three-necked flask was
evacuated for 10 min and flushed with
nitrogen. Then, 5 mL of butadiene (approximately 15% of hexane), 0.1
mL of the Karstedt’s catalyst, and 10 mL of THF were added
to a three-necked flask. The mixture was stirred at 85 °C for
1 h. Subsequently, 1 mL of PMHS was added and stirred for another
4 h to obtain a colorless and clear solution.
Scheme 1
Synthesis of Butadiene-Bridged
BBPMS
Preparation
of BBPMS/EC/IL Ternary Blended
Membrane
EC (1.80 g, 7.58 mmol) and THF (20 mL) were placed
in a flask and stirred at high speed. After the EC was completely
dissolved, a well-mixed methanol solution containing 1-carboxymethyl-3-methylimidazolium
chloride salt (IL) (8%, 156.52 mg) was added, and then the reaction
was continued for 2 h to obtain EC (IL: 8 wt %) homogeneous solution.
The reaction was carried out at room temperature.The BBPMS
synthesized in Materials section was added
to an EC (IL: 8 wt %) homogeneous solution and continued to react
for 1 h at room temperature to obtain a homogeneous cast membrane
solution; the cast membrane solution was filtered through a 200 mesh
filter and then the membrane was spread on a clean glass plate and
dried naturally at room temperature for 12 h. After 12 h of vacuum
drying at room temperature, the membrane was removed from the glass
plate to obtain a BBPMS/EC/IL ternary composite membrane. The composite
membrane composition of this study is shown in Table .
Table 1
Composition of Composite
Membranes
no.
sample
BBPMS addition
amount (mL)
BBPMS/loadinga (wt %)
composite membranes/matrixb (wt %)
1
IL/EC
0.00
0.00
100.00
2
BBPMS
30.00
100.00
0.00
3
MMM(40%)
1.30
40.00
60.00
4
MMM(50%)
1.90
50.00
50.00
5
MMM(60%)
2.80
60.00
40.00
6
MMM(70%)
4.40
70.00
30.00
7
MMM(80%)
7.50
80.00
20.00
8
MMM(90%)
16.90
90.00
10.00
Mass fraction of
BBPMS in the composite
membrane.
Mass fraction
of EC (IL: 8 wt %)
in the composite membrane.
Mass fraction of
BBPMS in the composite
membrane.Mass fraction
of EC (IL: 8 wt %)
in the composite membrane.
Measurements
A Fourier transform
infrared (FTIR) spectrometer (Spectrum Two, PE company, Waltham, Massachusetts,
USA) was used to characterize the molecular structures of the functional
groups in mixed matrix membranes. The surface structure of gas separation
membranes were studied by scanning electron microscopy (SEM, JSM-6490,
JOEL, Japan). The thickness of the membranes was measured by a thickness
gauge (CH-1-B, Liuling Instrument Factory, Shanghai, China). The graduation
value was 0.001 mm, the measurement range was 0–1 mm, and the
error was about ≤0.007 mm. Mechanical properties were analyzed
with a membrane tensile testing machine (XLW(PC)–500N, Sumspring,
Jinan, China) at 25 °C. A thermogravimetric analyzer (Q5000IRS
type, American TA Co., Ltd., USA) was used to test the thermal performance
of the membranes. During the test, the membranes were heated to 550
°C. The pure gas permeation property tests were performed using
a fixed-volume pressure increase instrument time-lag apparatus (VAC-V2
type, Labthink instrument Co., Ltd, Jinan, China) at 34 °C. The
membranes were first placed in a stainless-steel cell, and the disk
was sealed with rubber O-rings to avoid leakage. Then, both the upstream
and downstream sides of the system were degassed at ambient temperature
to ensure that the system was not disturbed. Next, pure gases (CO2, O2, and N2) were fed into the membrane
individually, and the permeability of each pure gas was measured at
a feed pressure of 2 bar. The permeability coefficients of the mixed
gas were measured by a gas chromatographic method using a differential
pressure gas transmission instrument (GTR-11MH type) at 34 °C.[31]
Results and Discussion
Infrared Analysis of Membranes
The
peaks and absorption bands of components in the obtained ternary composite
membranes were observed and assigned by FTIR spectrometry. Judging
from Figure , the
two weak spectral bands of 2954 and 2840 cm–1 belong
to the C–H bond stretching vibration of methyl and methylene
groups in EC, respectively. The Si–CH3 absorption
peak of BBPMS appears at 1261 cm–1. However, the
Si–H characteristic absorption peak of BBPMS does not appear
at 2165 cm–1, probably because the double bond in
1-carboxymethyl-3-methylimidazolium chloride (IL) reacts with the
Si–H bond, making the Si–H bond completely reacted.
The absorption peak at 1568 cm–1 originates from
the vibration of the imidazole ring skeleton. Therefore, it can be
proved that the presence of IL, EC, and BBPMS in the mixed matrix
membrane, and the gradual decrease of the methyl/methylene peak in
the IR spectrum with the gradual increase of the doping amount of
BBMPS, proves that the amount of EC gradually decreases, which is
also consistent with the doping ratio of the composite membrane.
Figure 1
FTIR spectrum
of the ternary composite membrane [(a): MMM(90%),
(b): MMM(80%), (c): MMM(70%), (d): MMM(60%), (e): MMM(50%), and (f):
MMM(40%)].
FTIR spectrum
of the ternary composite membrane [(a): MMM(90%),
(b): MMM(80%), (c): MMM(70%), (d): MMM(60%), (e): MMM(50%), and (f):
MMM(40%)].FTIR was used to verify the change
of the double bond of the EC,
IL, BBPMS, and ternary composite membrane (because the IR images of
different scales of ternary composite membranes are similar, they
are referred to by the same curve). As shown in Figure , the C=C characteristic absorption
peak of IL does appear at 1680 cm–1 and the Si–H
characteristic absorption peak of BBPMS does appear at 2165 cm–1. Both the C=C double bond and Si–H
are missing in the final ternary composite membranes, which proves
the successful reaction of IL with BBPMS.
Figure 2
FTIR spectrum of the
EC, IL, BBPMS, and ternary composite membrane.
FTIR spectrum of the
EC, IL, BBPMS, and ternary composite membrane.
SEM Analysis of Membranes
Figure gives the optical
pictures of the EC/IL membrane and the BBPMS/EC/IL ternary composite
membranes. Compared to the colorless and transparent EC/IL membrane,
the ternary composite membrane become less and less transparent as
BBPMS increases. However, the ternary composite membranes also show
the same excellent flexibility with repeated curling without deformation
or breakage as the EC/IL membrane.
Figure 3
Optical photos [(A) transparency of the
membrane varies with the
amount of BBMPS doping and (B) flexibility of the membrane] of the
EC/IL membrane (g) and BBPMS/EC/IL mixed matrix membranes [(a): MMM(90%),
(b): MMM(80%), (c): MMM(70%), (d): MMM(60%), (e): MMM(50%), and (f):
MMM(40%)].
Optical photos [(A) transparency of the
membrane varies with the
amount of BBMPS doping and (B) flexibility of the membrane] of the
EC/IL membrane (g) and BBPMS/EC/IL mixed matrix membranes [(a): MMM(90%),
(b): MMM(80%), (c): MMM(70%), (d): MMM(60%), (e): MMM(50%), and (f):
MMM(40%)].To further observe the distribution
of BBPMS in the ternary composite
membranes by SEM analysis. Figure gives the surface SEM images of the EC/IL membrane
(g), (h) pure BBPMS, and BBPMS/EC/IL ternary composite membranes [(a):
MMM(90%), (b): MMM(80%), (c): MMM(70%), (d): MMM(60%), (e): MMM(50%),
and (f): MMM(40%)]. According to Figures and S1, the surface
of EC/IL membrane is dense, flat and smooth. Compared with the EC/IL
membrane, the surface changes of the BBPMS/EC/IL ternary composite
membranes became more and more obvious with the increase of BBPMS
content.However, the surface of the membranes were still uniformly
distributed without agglomeration, indicating that homogeneous ternary
composite membranes of EC-doped BBPMS and IL were successfully prepared.
Figure 4
Surface
SEM images of the EC/IL membrane (g) and BBPMS/EC/IL mixed
matrix membranes [(a): MMM(90%), (b): MMM(80%), (c): MMM(70%), (d):
MMM(60%), (e): MMM(50%), (f): MMM(40%), and (h): BBPMS].
Surface
SEM images of the EC/IL membrane (g) and BBPMS/EC/IL mixed
matrix membranes [(a): MMM(90%), (b): MMM(80%), (c): MMM(70%), (d):
MMM(60%), (e): MMM(50%), (f): MMM(40%), and (h): BBPMS].
Mechanical Property Analysis
As the
gas separation membranes, they should have enough tensile strength
and elongation at break during use. Figure shows the test data on the tensile strength
and elongation at break of the EC/IL membrane and BBPMS/EC/IL ternary
composite membranes with membrane thicknesses between 117 and 136
μm. From Figure , it can be seen that the tensile strength and elongation at break
of the composite membranes increased when the doping amount of BBPMS
was 40 and 50% compared with the undoped membranes. The elongation
at break and tensile strength of the composite membrane reached the
maximum when the doping amount of BBPMS was 50%. When the doping amount
of BBPMS exceeded 50%, the elongation at break and tensile strength
started to decrease. In addition, with the increase of BBPMS doping,
the elongation at break of the ternary composite membranes eventually
became smaller than that of the EC/IL membrane. However, the tensile
strength was always higher than that of the EC/IL membrane. This may
be due to the increase of BBPMS doping, the silicon hydrogen bond
in the polysiloxane breaks to form a hydrogen bond, and then the broken
hydrogen bond combines with the −OH in the EC. The BBPMS/EC/IL
hybrid membranes formed a kind of structure with interpenetrating
networks.[31]
Figure 5
Mechanical properties
of the EC/IL membrane and BBPMS/EC/IL membrane.
Mechanical properties
of the EC/IL membrane and BBPMS/EC/IL membrane.
Thermal Property Analysis
The thermogravimetric
(TG) test plots of the EC/IL membrane and BBPMS/EC/IL ternary composite
membrane are given in Figure . From Figure , it can be seen that the temperature at 5% weight loss is in the
range of 260–280 °C. With the increase of BBPMS doping,
the weight loss temperature gradually increases, which is due to the
fact that BBPMS is a cross-linked polymer whose thermal stability
is better than that of EC. The residual amount of the mixed matrix
membrane at 600 °C increased with the increase of BBPMS doping.
The presence of BBPMS in a prepared hybrid matrix membrane was also
demonstrated by the TG test.
Figure 6
TG analysis of the EC/IL membrane and BBPMS/EC/IL
membrane.
TG analysis of the EC/IL membrane and BBPMS/EC/IL
membrane.
Gas Separation
Properties
The prepared
BBPMS/EC/IL ternary composite membranes were tested for the single
component gas permeability of CO2, N2, and O2, and the test data are shown in Table . According to the results in Table , the BBPMS complex membrane
shows good gas transmission performance. CO2 permeability
of the BBPMS complex membrane is up to 1417.01 Barrer, O2 permeability of the BBPMS complex membrane is up to 248.63 Barrer,
and N2 permeability of the BBPMS complex membrane is up
to 97.12 Barrer. In contrast, its separation performance is not that
good. The PCO/PN permselectivity values of the BBPMS membrane
is 14.59 and the PO/PN permselectivity values of the
BBPMS complex membrane is 2.56. Meanwhile, it can be seen that the
gas permeability of the membranes gradually increased with the increase
of the BBPMS doping amount, and the gas separability first increased
and then gradually decreased. When the doping of BBPMS reaches 90%,
the CO2 permeation of the MMM(90%) membrane was 1806.03
Barrer, which is 20.04 times higher than that of the IL/EC membrane,
which is due to the high gas permeability of the introduced BBPMS
structure itself.[32] Combining the solubility
and diffusion coefficients of CO2, O2, and N2 gases listed in Table , it can be found that the CO2 permeation was dominated
by dissolution, and its solubility has a large increase with the addition
of BBPMS, which also proved that the addition of BBPMS has shown great
improvement in the CO2 permeation. Generally, in the prepared
BBPMS/EC/IL mixed matrix membranes compared to the prepared EC/IL
membranes, the separation factor of CO2/N2 increases
significantly and the O2/N2 separation coefficients
are not very different. (The calculation formula has been placed in
the Supporting Information).
Table 2
Gas Permeability, Gas Solubility,
and Diffusivity Coefficients of BBPMS Complex Membrane, EC/IL Membrane,
and BBPMS/EC/IL Membrane Measured (Single-Component Gas Permeability)
P(Bar)a
α
Sb
Dc
no.
samples
CO2
O2
N2
CO2/N2
O2/N2
CO2
O2
N2
CO2
O2
N2
1
MMM(90%)
1806.03
321.01
103.22
17.51
3.11
48.11
5.12
2.87
3.75
6.27
3.60
2
MMM(80%)
1034.09
208.03
55.32
18.72
3.76
26.52
3.99
1.24
3.90
5.21
4.46
3
MMM(70%)
585.99
124.82
30.73
19.14
4.07
14.23
2.50
0.97
4.13
4.99
3.16
4
MMM(60%)
405.98
76.05
20.23
20.09
3.76
10.20
2.21
0.69
3.98
3.44
2.94
5
MMM(50%)
350.06
46.53
13.10
26.73
3.55
8.52
1.45
0.57
4.11
3.21
2.31
6
MMM(40%)
212.09
29.42
10.44
20.39
2.83
6.25
1.32
0.39
3.39
2.23
2.69
7
IL/EC
90.10
16.71
3.83
23.52
4.36
3.12
2.01
0.11
2.89
0.83
3.39
8
BBPMS complex membrane
1417.01
248.63
97.12
14.59
2.56
30.44
4.56
2.14
4.66
5.45
4.54
1 Barrer = 10–10 cm3(STP) cm cm–2 s–1 cmHg–1.
Ln 10–3 cm3(STP) cm–3 cmHg–1.
Ln 10–6 cm2 s–1.
1 Barrer = 10–10 cm3(STP) cm cm–2 s–1 cmHg–1.Ln 10–3 cm3(STP) cm–3 cmHg–1.Ln 10–6 cm2 s–1.The gas
permeation selectivity of the prepared ternary composite
membrane was also compared with the Robeson curve.[30] CO2/N2 permeability of the BBPMS/EC/IL
membranes were determined, and the results are shown in Figure a. When BBPMS were doped at
50, 70, 80, and 90%, the CO2/N2 capacity of
the composite membrane exceeded the Robeson line of 1991. Especially,
when the doping amount of BBPMS was 90%, the CO2/N2 capacity of the composite membrane has been closer to the
Robeson line of 2008. The O2/N2 permeability
of the BBPMS/EC/IL membranes were also determined, and the results
are shown in Figure b. When BBPMS were doped at 70 and 80%, the O2/N2 capacity of the composite membrane exceeded the Robeson line of
1991. When the doping amount of BBPMS was 90%, the O2/N2 capacity of the composite membrane has been closer to the
Robeson line of 1991. All the above data show that this ternary composite
membrane idea is successful.
Figure 7
Plot of permselectivity vs permeability for
the gas pairs (a) CO2/N2 and (b) O2/N2 (single
component gas permeability).
Plot of permselectivity vs permeability for
the gas pairs (a) CO2/N2 and (b) O2/N2 (single
component gas permeability).The prepared BBPMS/EC/IL ternary composite membranes were tested
for the mixed component gas permeability of CO2/N2 and O2/N2, and the test data are shown in Table . According to the
results shown in Table , the BBPMS complex membrane shows good gas transmission performance.
CO2 permeability of the BBPMS complex membrane is up to
1326.01 Barrer, O2 permeability of the BBPMS complex membrane
is up to 224.62 Barrer, and the transmission amounts of N2 in different gas mixtures are 87.80 (CO2/N2) and 80.24 (O2/N2), respectively. In contrast,
its separation performance is not so good. The PCO/PN permselectivity
values of BBPMS membrane is 15.12, and the PO/PN permselectivity
values of the BBPMS complex membrane is 2.80. Meanwhile, it can be
seen that the gas permeability of the membranes gradually increased
with the increase of the BBPMS doping amount, and the gas separability
first increased and then gradually decreased. When the doping of BBPMS
reached 90%, the CO2 permeation of the MMM(90%) membrane
was 1577.02 Barrer, which is 20.12 times higher than that of the IL/EC
membrane, which is due to the high gas permeability of the introduced
BBPMS structure itself.[32] Combining the
solubility and diffusion coefficients of CO2/N2 and O2/N2 gases in Table , it can be found that the CO2 permeation was dominated by dissolution, and its solubility has
a large increase with the addition of BBPMS, which also proved that
the addition of BBPMS shows great improvement in the CO2 permeation. Generally, in the prepared BBPMS/EC/IL mixed matrix
membranes compared to the prepared EC/IL membranes, the separation
factors of CO2/N2 and O2/N2 increase significantly. (The calculation formula has been placed
in the Supporting Information).
Table 3
Gas Permeability, Gas Solubility,
and Diffusivity Coefficients of the BBPMS Complex Membrane, EC/IL
Membrane and BBPMS/EC/IL Membrane Measured (Mixed Component Gas Permeability)
P(Bar)a
α
Sb
Dc
CO2/N2
O2/N2
CO2/N2
O2/N2
CO2/N2
O2/N2
CO2/N2
O2/N2
no.
samples
CO2
N2
O2
N2
CO2
N2
O2
N2
CO2
N2
O2
N2
1
MMM(90%)
1577.02
80.60
269.61
70.92
19.62
3.81
43.61
2.60
4.81
2.42
3.62
3.13
5.63
3.00
2
MMM(80%)
903.10
43.21
174.70
38.81
20.90
4.52
24.20
1.11
3.62
1.00
3.69
3.92
4.90
3.91
3
MMM(70%)
508.32
23.72
104.80
22.32
21.43
4.69
12.92
0.92
2.30
0.81
3.93
2.61
4.60
2.83
4
MMM(60%)
352.21
15.63
63.81
14.49
22.61
4.40
9.33
0.72
2.11
0.62
3.81
2.20
2.99
2.42
5
MMM(50%)
306.43
10.21
39.12
9.10
30.00
4.33
7.71
0.63
1.32
0.53
4.00
1.73
3.01
1.80
6
MMM(40%)
185.32
8.10
24.69
7.32
22.82
3.42
5.59
0.44
1.20
0.32
3.32
1.99
2.10
2.42
7
IL/EC
78.40
3.12
14.03
2.93
25.32
4.91
2.81
0.13
1.79
0.10
2.83
3.13
0.83
2.91
8
BBPMS complex membrane
1326.01
87.80
224.62
80.24
15.12
2.80
35.60
2.20
4.50
2.13
3.73
4.02
5.01
3.81
1 Barrer = 10–10 cm3(STP) cm cm–2 s–1 cmHg–1.
Ln 10–3 cm3(STP) cm–3 cmHg–1.
Ln 10–6 cm2 s–1.
1 Barrer = 10–10 cm3(STP) cm cm–2 s–1 cmHg–1.Ln 10–3 cm3(STP) cm–3 cmHg–1.Ln 10–6 cm2 s–1.The gas
permeation selectivity of the prepared ternary composite
membrane was also compared with the Robeson curve.[33] CO2/N2 permeability of the BBPMS/EC/IL
membranes were determined, and the results are shown in Figure a. When BBPMS were doped at
50, 70, 80, and 90%, the CO2/N2 capacity of
the composite membrane exceeded the Robeson line of 1991. Especially,
when the doping amount of BBPMS was 90%, the CO2/N2 capacity of the composite membrane was closer to the Robeson
line of 2008. The O2/N2 permeability of the
BBPMS/EC/IL membranes were also determined, and the results are shown
in Figure b. When
BBPMS was doped at 70, 80, and 90%, the O2/N2 capacity of the composite membrane exceeded the Robeson line of
1991. When the doping amounts of BBPMS were 70 and 80%, the O2/N2 capacity of the composite membrane was closer
to the Robeson line of 2008. All the above data show that this ternary
composite membrane idea is successful.
Figure 8
Plot of permselectivity
vs permeability for the gas pairs (a) CO2/N2 and (b) O2/N2 (mixed
component gas permeability).
Plot of permselectivity
vs permeability for the gas pairs (a) CO2/N2 and (b) O2/N2 (mixed
component gas permeability).
Conclusions
The ternary composite membranes
with different ratios of BBPMS/EC/IL
were prepared based on the previous study of EC/IL hybrid matrix membranes.
The composite membranes have good mechanical properties and can maintain
less than 5% thermal weight loss at 260 °C. The prepared composite
membranes showed great improvement in the permeability of CO2 and O2. The CO2 permeation reaches 1806.03
Barrer at 90% doping of BBPMS, which is 20.04 times higher than that
of the MMM(0%) membrane. O2 permeation reaches 321.01 Barrer,
which is 19.21 times higher than that of the MMM(0%) membrane. Moreover,
when the doping of BBPMS is 70 and 80%, the O2/N2 permeation performance of the membrane exceeded the Robertson 1991
curve and closed to the Robertson 2008 curve.In summary, the
BBPMS/EC/IL ternary composite membranes exhibited
excellent gas separation performance, thermal stability, and mechanical
property, which made it have more potential as a gas separation material.
Authors: Marcello Monteleone; Elisa Esposito; Alessio Fuoco; Marek Lanč; Kryštof Pilnáček; Karel Friess; Caterina Grazia Bezzu; Mariolino Carta; Neil Bruce McKeown; Johannes Carolus Jansen Journal: Membranes (Basel) Date: 2018-09-03