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Document Type : Original Article

Authors

Department of Chemical Engineering, Arak Branch, Islamic Azad University, Arak, Iran

Abstract

Recently, researchers have suggested the use of membranes to separate gases. They found that using Pebax polymer was very suitable for gas separation. This polymer has good properties and good solubility for carbon dioxide absorption. One of the challenges for researchers is how to turn this polymer into a thin layer for usage as a membrane. Therefore, several methods and solvents have been used to make this membrane. Researchers have calculated the carbon dioxide permeability of this polymer and obtained different results. One of the reasons for the non-uniform permeability results for this gas could be the difference in the method of making the thin film. The use of different methods and solvents affects the physical and chemical properties of this polymer. Perhaps the most important parameters during membrane construction are temperature and drying time. In this research, we want to investigate the effect of these two parameters on the final performance. Thus, the membranes were evaluated by XRD, FT-IR, FESEM, and mechanical strength analyses. Finally, the effect of the parameters on the permeability of carbon dioxide and methane was calculated and compared by the Taguchi method.

Graphical Abstract

Influence of Temperature and Time Parameters on Solution Mixing and Drying for Membrane Synthesis of Copolymer (Polyether-Block-Amide)

Keywords

Main Subjects

Introduction

Today, the chemical industry is trying to reduce some parts of the air pollution by complying with environmental standards. Carbon dioxide plays a major role in air pollution. Recently, the separation of gases by membranes is considered due to its economic process, especially when high purity is not concerned [1].

Researchers have recently used polyphosphates, polyamides, cellulose acetate, polyurethane, polyurethane urea, polyether-block-amide copolymers, and polyvinylidene fluoride to separate gas [2]. Lane and Freeman concluded that ethylene oxide (EO) has a high selectivity for carbon dioxide. The choice of copolymers containing ethylene oxides, such as polyether-block-amide or PEBA, is suitable to obtain this goal [3]. Polyether-block-amide is an elastomeric thermoplastic whose chemical and physical structure is as displayed in Figure 1.

PA, aliphatic polyamide, and PE polyether are this polymer’s hard and soft parts, respectively. The hard part provides mechanical strength and gas penetration through the PE phase. This polymer has good permeability and selectivity for carbon dioxide to methane [5]. Table 1 shows the composition and their melting temperature.  PEBA polymers are commercially produced and can also be converted into thin films. Due to their different chemical structure, these polymers have several types of grades, among which grade 1657 had the highest permeability [6].

Perhaps the most important parameters during membrane construction are temperature and drying time. In this research, the effect of these two parameters was investigated on the final performance of fabricated membranes. Hence, the first experimental design was performed by hMinitab software, and membranes were made based on this design and their structure was evaluated by XRD, FT-IR, FESEM, and mechanical strength analyses. Finally, the effective coefficient of the research parameters was calculated by the Taguchi method on permeability. Likewise, selectivity, diffusion coefficients, and solubility the membrane density were calculated and compared at 3 bar pressure and 35 °C.

Figure 1: Chemical arrangement of PEBA polymers [3, 4]

Table 1: Composition, structure, and physical properties of Pebax 1657 [3]

Sample

 Pebax1657

Chemical Structure

Crystallinity%

Melting point (°C)

PE

–(CH2-CH2-O)n–

10-14

14-22

PA

–((CH2)5–CO–NH)–

21-31

200-205

                                                                                                          

Materials and Methods

Experimental design

The experimental design was performed to study the variables of this study on membrane permeability and selectivity. This design was done by the Taguchi method and by Minitab software. The advantage is that the number of tests is less but effective. Orthogonal array tables and ANOVA analysis were used with this method.

In this research, the effect of four parameters mixing time, mixing temperature, drying time, and drying temperature was examined. Table 2 represents these parameters and their levels. The orthogonal array L9 consisted of four parameters and each one had three levels. Accordingly, 9 membrane samples with different variables were proposed, named, and listed in Table 3.

 

Table 2: Variables and their levels

Level 3

Level 2

Level 1

Unit

Factor

48

36

24

hr

Drying time

50

40

30

°C

Drying temp.

300

240

150

min

Mixing time

160

140

110

°C

Mixing temp.

 

Table 3: Experimental conditions and membranes IDs

Drying Temp

Drying time

Mixing Temp

Mixing time

Membrane ID

30

24

110

150

PB1

40

36

140

150

PB2

50

48

160

150

PB3

50

36

110

240

PB4

30

48

140

240

PB5

40

24

160

240

PB6

40

48

110

300

PB7

50

24

140

300

PB8

30

36

160

300

PB9

 

Materials

In this research, (polyether-block-amide) grade 1657 with a density of 1.14 g/cc made by the French company Arkema was used. DMF solvent was also purchased from the German company Sigma Aldrich. Methane and carbon dioxide gases with a purity of 99.9% were purchased and used from Khorramshahr Gas Oxygen Company.

Devices

XRD analysis with XRD Philips pw1730 device, FE-SEM analysis with TESCAN MIRA3 device, FT-IR analysis with Thermo device model AVATAR and for mechanical strength test Tensile Zwick device made in England model CAT-350-56 was used, which is equipped with a power supply is connected to two jaws. A digital thickness gauge model GT-313-A1 made in Japan was used to measure the thickness.

Making the membrane

For the membrane with a good mechanical strength, its thickness was selected to be 100 μm (source), and the radius of the casting dish is 3.5 cm. To make a membrane with the sizes mentioned above, 0.438 g of Pebax1657 granules was initially placed at 70 °C for 3 hours to be completely dried [9], and then it was poured into a laboratory balloon with 12.5 g of DMF solvent and it was placed in an oil bath and reflexes were inserted with a certain temperature and duration.

To preserve the morphology of the polymer solution, the petri dish was heated to 80 °C in an oven (Figure 2) [10]. The solution was poured into a petri dish, and then it was placed in an oven at a certain temperature and time and it was completely dried. With this method and the variables of this research, 9 membranes were made. The thickness and density of the fabricated membranes were calculated and listed in Table 4.

Permeability measurement

A gas permeability measuring system was designed and built as a fixed volume (Figure 3). This system can measure permeability at different pressures. The membrane module was made by using pure stainless steel. Both sides of the rubber ring membrane were used to prevent gas from settling. In addition, a thin metal mesh made of steel was used to prevent the membrane from tearing. The effective surface of the membrane in this system is 17.71 cm2. Trojan experiments were performed on the required gases at a temperature of 35 °C and a pressure of 3 times, each with three repetitions. Gas permeability was calculated by using the constant volume method and Equation 1 and it was also reported in the Barrer unit:

1 Barrer =10-10 cm3 (STP)·cm / (cm2. s. cmHg)

In this relation, (cm3) V is the volume of the tank after the cell, L (cm) is the thickness of the membrane, A (cm2) is the effective surface of the membrane, T (K) is the temperature, (psia) is the absolute pressure of the inlet gas and (bar/s) dP/dt pressure changes over time [11], [12]. The ideal selectivity of gases was calculated by using Equation 2 [13, 14]:

CO2 diffusion coefficient was calculated according to Equation 3 by using the calculation time method [14]:

Where, time θ was obtained by extrapolating the linear part of the pressure diagram in terms of time and its intersection with the time axis. The solubility coefficient of gases was calculated according to Equation 4 [14]:

SA = PA/DA                                                                                 (Eq. 4)

Permeability, selectivity, solubility coefficient, and diffusion coefficient of fabricated membranes are reported in Table 5 and Figure 4 and 5 [18, 19].

Figure 2: Nanocomposite membrane synthesis steps

Table 4: Mass, thickness, and density of synthesized membranes

Density (cm3/gr)

Mass (gr)

Thickness (µm)

Membrane ID

1.21

110

88

PB1

1.20

140

91

PB2

1.18

160

89

PB3

1.19

110

93

PB4

1.19

140

87

PB5

1.17

160

85

PB6

1.22

110

90

PB7

1.23

140

89

PB8

1.18

160

92

PB9

Figure 3: Permeability measurement system

Table 5: Permeability, diffusion coefficient, solubility coefficient, and selectivity

ID

PCO2

PCH4

CO2/CH4

DCO2

SCO2

PB1

49.5

3.13

15.81

46.3

1.07

PB2

53.3

3.31

16.1

47.1

1.13

PB3

54.6

3.34

16.34

47.6

1.15

PB4

51.4

3.18

16.16

46.1

1.11

PB5

59.3

3.64

16.29

49.1

1.20

PB6

52.2

3.61

14.6

46.5

1.12

PB7

55.9

3.54

15.79

48.7

1.15

PB8

51.6

3.28

15.7

46.6

1.10

PB9

52.8

3.24

16.3

46.4

1.14

Figure 4: Permeability and selectivity of CO2 and CH4

Figure 5: The diffusion coefficient, solubility coefficient of CO2

 

Results and discussion

XRD analysis results

The X-ray jump (XRD) test was used to investigate the crystal structure of the synthesized particles. This XRD analysis is from 10 degrees to 80 degrees and the device step is 0.05 degrees per second. At 5.20 and 42.4 degrees, respectively, the X-ray reflections of the crystal structure of the polymer are related [15, 16]. The weaker peaks observed at other angles are related to impurities and unknown phases (Figure 6).

Figure 6: X-ray diffraction (XRD)

 

FT-IR analysis

This analysis was performed on 600 to 4000 (cm-1) on the desired membranes. As depicted in Figure 7, the peak at 1635 cm-1 is the tensile vibrations (C=O) of carbonyl. The peak in wave number 1730 is attributed to another carbonyl group, both of which are in the hard phase. The peak in 1538 is related to the N-H flexural vibration in polyamide parts, and the peak in 3290 cm-1 is related to the tensile vibration (N-H) [17]. Peaks 2861 cm-1 and peaks 1460 cm-1 were further associated with C-H tensile and flexural vibrations, respectively. These results were in good agreement with other studies (Figure 7) [16].

Figure 7: Fourier transform infrared spectroscopy (FT-IR)

FE-SEM analysis

The penetration of gases in polymer membranes depends on their morphology. FESEM imaging was performed to examine the structure of the membranes. Figure 8 displays the images made in this study. The surface of PB-5 and PB-7 membranes is uniform but cracks were observed on PB-4 and PB-9. The accumulated polymer layers were observed in PB-1. Fine particles were also seen on the surface of PB-6 and PB-8. These cases appear to be caused by drying or dissolving the polymer.

Mechanical strength analysis

Mechanical strength analysis determines how much tensile strength material can withstand before permanent degradation. It is possible to determine how much pressure the membrane can be exposed to the duration of the gas separation process. The results of this analysis show which membrane has more strength. The band-shaped specimens were placed between the two jaws and lasted at a speed of 5 mm/min.mm/min test, the conditions, and the speed of traction are constant. Table 6 indicates the reaction of the synthesized membranes during the application of tensile force. Studies show the PB-5 membrane is more resistant. The reason for the adhesion and tensile strength of this polymer can be its complete dissolution and drying.

Figure 8: Scanning Electron Microscope (FE-SEM)

Table 6: Mechanical strength and stress-strain analysis data

Membrane ID

Tensile strength (MPa)

Elastic modulus (MPa)

Elongation at break (%)

PB1

17.3

113.1

697 ± 2

PB2

19.2

118.3

792± 5

PB3

18.95

151.3

641 ± 5

PB4

20.6

130.5

736 ± 3

PB5

21.8

148.4

791 ± 2

PB6

20.8

119.9

751± 5

PB7

17.9

99.3

741 ± 5

PB8

18.87

108.3

636 ± 3

PB9

19.3

138.3

691 ± 2

 

Analysis of variance (ANOVA)

This analysis is to examine the involvement degree of experimental factors in the outcome. If one of them has less than a 5% effect, it may be ignored. Carbon dioxide permeability is analyzed in Table 7 and the methane gas permeability is indicated in Table 8. According to these data, the drying time parameter has played a greater role in the permeability of these two gases.

Finally, according to the obtained data by the Taguchi method, the optimized value for effective factors was suggested by Minitab software and listed in Table 9.

 

Table 7: Analysis of variance for the maximum CO2 permeability

Percentage of participation

Total net squares

Variance

Sum of Squares

Degrees of Freedom

Factor

5.941

124.168

62.084

124.168

2

Mixing time

3.12

65.214

32.607

65.214

2

Mixing Temp

74.47

1556.43

778.215

1556.43

2

Drying time

16.462

344.049

172.24

344.049

2

Drying Temp

-

-

-

0

0

Error

-

-

-

2089.886

8

Sum total

Table 8: Analysis of variance for the maximum CH4 permeability

Percentage of participation

Total net squares

Variance

Sum of Squares

Degrees of Freedom

Factor

8.73

0.342

0.177

0.354

2

Mixing time

8.248

0.323

0.167

0.335

2

Mixing Temp

24.193

0.949

0.48

0.961

2

Drying time

56.283

2.208

1.11

2.22

2

Drying Temp

2.546

-

0.005

0.052

9

Error

-

-

-

10.854

17

Sum total

Table 9: Optimized amount of research factors by Minitab software

Drying temp (°C)

Drying Time (hr)

Mixing temp. (°C)

Mixing Time (min)

42

38

143

220

 

Conclusion  

In this study, the polymer membrane was produced through the molding and evaporation of solvents. Its performance in CO2/CH4 separation was investigated at feed pressure 3 times and a temperature of 35 °C. The results of the FT-IR test ruled out the formation of a new chemical bond between the zeolite and the polymer. FESEM images of the membranes revealed that the search parameters had a significant impact on their morphology. Permeability, selectivity, solubility coefficient, and diffusion coefficient of fabricated membranes have the best selectivity performance. The diffusion coefficient and the solubility coefficient obtained are in good agreement with similar research. Research variables are very important in membrane construction. If not selected correctly, they can cause the following problems:

1- Lack of perfect evaporation of solvent causes blockage of the existing pores and reduces solubility and permeability.

2- The thickness of the membrane is the most important parameter to estimate the coefficient of gas penetration into the membrane. Improper drying or incomplete dissolution of the polymer in the solvent affects the thickness. The value of this parameter mass transfer and mechanical strength at the same time.

3- Mechanical strength and membrane density are further affected by research variables. The XRD analysis shows that the amount of hard phase crystallization of the membranes is significantly different.

A small amount of solvent or impurities in the membrane can clog some pores and reduce solubility and permeability. Finally, it can be concluded that the correct choice of research variables, especially drying time, is an important factor for Pebax membrane synthesis and has a great impact on achieving the highest permeability and selectivity.

Acknowledgements

The authors would like to present their gratitude to the Department of Chemical Engineering, Arak Branch, Islamic Azad University, Arak, Iran.

Funding

This research did not receive any specific grant from fundig agencies in the public, commercial, or not-for-profit sectors.

Authors' contributions

All authors contributed to data analysis, drafting, and revising of the paper and agreed to be responsible for all the aspects of this work.

 

Conflict of Interest

There are no conflicts of interest in this study.

ORCID:

Seyed Mohammad Faghih

https://www.orcid.org/0000-0002-1552-8591

Hossein Mazaheri

https://www.orcid.org/0000-0003-4461-5018

HOW TO CITE THIS ARTICLE

Seyed Mohammad Faghih, Mahmoud Salimi, Hossein Mazaheri. Influence of temperature and time parameters on solution mixing and drying for membrane synthesis of copolymer (polyether-block-amide). Chem. Methodol., 2022, 6(10) 762-772

https://doi.org/10.22034/CHEMM.2022.348432.1562

URL: http://www.chemmethod.com/article_153728.html

[1]. Brunettia A., Scura F., Barbieria G., Driolia E., Membrane technologies for CO2 separation, Journal of Membrane Science, 2010, 359:115 [Crossref], [Google Scholar], [Publisher]
[2]. Ehsani A., Pakizeh M., Synthesis, characterization and gas permeation study of ZIF-11/Pebax® 2533 mixed matrix membranes, Journal of the Taiwan Institute of Chemical Engineers, 2016, 66:414 [Crossref], [Google Scholar], [Publisher]
[3]. Bernardo P., Jansen J.C., Bazzarelli F., Tasselli F., Fuoco A., Friess K., Izák P., Jarmarová V., Kačírková M., Clarizia G., Gas transport properties of Pebax®/room temperature ionic liquid gel membranes, Separation and Purification Technology, 2012, 97:73 [Crossref], [Google Scholar], [Publisher]
[4]. Xiang L., Pan Y., Zeng G., Jiang J., Chen J., Wang C., Preparation of poly(ether-block-amide)/attapulgite mixed matrix membranes for CO2/N2 separation, Journal of Membrane Science, 2016, 500:66 [Crossref], [Google Scholar], [Publisher]
[5]. Zanetti M., Camino G., Thomann R., Mülhaupt R., Synthesis and thermal behaviour of layered silicate–EVA nanocomposites, Polymer, 2001, 42:4501 [Crossref], [Google Scholar], [Publisher]
[6]. Budd P.M., McKeown N.B., Fritsch D., Yampolskii Y., Shantarovich V., Gas permeation parameters and other physicochemical properties of a polymer of intrinsic microporosity (PIM-1), Journal of the Taiwan Institute of Chemical Engineers, 2010, 29-42 [Crossref], [Google Scholar], [Publisher]
[7]. Kianfar E., Pirouzfar V., Sakhaeinia H., An experimental study on absorption/stripping CO2 using Mono-ethanol amine hollow fiber membrane contactor, Journal of the Taiwan Institute of Chemical Engineers, 2017, 80:954 [Crossref], [Google Scholar], [Publisher]
[8]. Raghu A.V., Gadaginamath G.S., Mathew N.T., Halligudi S.B., Aminabhavi T.M., Synthesis and characterization of novel polyurethanes based on 4,4′-[1,4-phenylenedi-diazene-2,1-diyl]bis(2-carboxyphenol) and 4,4′-[1,4-phenylenedi-diazene-2,1-diyl]bis(2-chlorophenol) hard segments, Reactive and Functional Polymers, 2007, 67:503 [Crossref], [Google Scholar], [Publisher]
[9]. Azizi N., Isanejad M., Mohammadi T., Behbahani R.M., Effect of TiO2 loading on the morphology and CO2/CH4 separation performance of PEBAX-based membranes, Frontiers of Chemical Science and Engineering, 2019, 13:517 [Crossref], [Google Scholar], [Publisher]
[10]. Hosseinzadeh Beiragh H., Omidkhah M., Abedini R., Khosravi T., Pakseresht S., Synthesis and characterization of poly (ether-block-amide) mixed matrix membranes incorporated by nanoporous ZSM-5 particles for CO2/CH4 separation, Asia-Pacific Journal of Chemical Engineering, 2016, 11:522 [Crossref], [Google Scholar], [Publisher]
[11]. Jamshidi M., Pirouzfar V., Abedini R., Pedram M.Z., The influence of nanoparticles on gas transport properties of mixed matrix membranes: An experimental investigation and modeling, Korean Journal of Chemical Engineering, 2017, 34:829 [Crossref], [Google Scholar], [Publisher]
[12]. Monteleone M., Esposito E., Fuoco A., Lanč M., Pilnáček K., Friess K., Bezzu C.G., Carta M., McKeown N.B., Jansen J.C., A Novel Time Lag Method for the Analysis of Mixed Gas Diffusion in Polymeric Membranes by On-Line Mass Spectrometry: Pressure Dependence of Transport Parameters, Membranes, 2018, 8:73 [Crossref], [Google Scholar], [Publisher]
[13]. Khoramzadeh E., Mofarahi M., Lee C.H., Equilibrium Adsorption Study of CO2 and N2 on Synthesized Zeolites 13X, 4A, 5A, and Beta, Journal of Chemical & Engineering Data, 2019, 64:5648 [Crossref], [Google Scholar], [Publisher]
[14]. Murali, R.S., Ismail A.F., Rahman M.A., Sridhar S., Mixed matrix membranes of Pebax-1657 loaded with 4A zeolite for gaseous separations, Separation and Purification Technology, 2014, 129:1 [Crossref], [Google Scholar], [Publisher]
[15]. Suhas D.P., Aminabhavi T.M., Jeong H.M., Raghu A.V., Hydrogen peroxide treated graphene as an effective nanosheet filler for separation application, Rsc Advances, 2015, 5:100984 [Crossref], [Google Scholar], [Publisher]
[16]. Habib N., Shamair Z., Tara N., Nizami A.S., Akhtar F.H., Ahmad N.M., Gilani M.A., Bilad M.R., Khan A.L., Development of highly permeable and selective mixed matrix membranes based on Pebax®1657 and NOTT-300 for CO2 capture, Separation and Purification Technology, 2020, 234:116101 [Crossref], [Google Scholar], [Publisher]
[17]. Rahman M.M., Shishatskiy S., Abetz C., Georgopanos P., Neumann S., Khan M.M., Filiz V., Abetz V., Influence of temperature upon properties of tailor-made PEBAX® MH 1657 nanocomposite membranes for post-combustion CO2 capture, Journal of Membrane Science, 2014, 469:344 [Crossref], [Google Scholar], [Publisher]
[18]. Rahman M.M., Filiz V., Shishatskiy S., Abetz C., Neumann S., Bolmer S., Khan M.M., Abetz V., PEBAX® with PEG functionalized POSS as nanocomposite membranes for CO2 separation, Journal of Membrane Science, 2013, 437:286 [Crossref], [Google Scholar], [Publisher]
[19]. Ghadimi A., Mohammadi T., Kasiri N., Gas permeation, sorption and diffusion through PEBA/SiO2 nanocomposite membranes (chemical surface modification of nanoparticles), International Journal of Hydrogen Energy, 2015, 40:9723 [Crossref], [Google Scholar], [Publisher]