Making and Evaluation of Nanopore Hydroxysodalite Zeolite Membranes for Pervaporation Applications
Mansoor Kazemimoghadam1*, Toraj Mohammadi2
2Faculty of Chemical Engineering, Iran University of Science and Technology, Narmak, Tehran, Iran
*Corresponding
author: Mansoor Kazemimoghadam,
Faculty of Chemical and Chemical Engineering, Malek Ashtar University of
Technology, Tehran Province, Tehran, Lavizan, Babaei Hwy, Shabanlou, Iran. Tel:
+98219676620; Fax: +98219676620; Email: mzkazemi@gmail.com
Citation: Kazemimoghadam M, Mohammadi T (2017) Making and Evaluation of Nanopore Hydroxysodalite Zeolite Membranes for Pervaporation Applications. J Nanomed Nanosci: JNAN-114. DOI: 10.29011/JNAN-114. 100014
1. Abstract
1. Introduction
Shows energy consumptions required by different separation methods in ethanol dehydration. In terms of energy requirement, pervaporation is an obvious choice in ethanol-water separation. Furthermore, PV has several advantages over traditional distillation: [1] reduced energy demand because only a fraction of the liquid that needs to be separated is vaporized, [2] simple equipment since only a vacuum pump is used to create a driving force and [3] lower capital cost. Thus, relatively mild operation conditions and high effectiveness make PV an appropriate technique for such separations. As a result, most PV studies have been focused on dehydration of organic mixtures [1-4].
Polymeric membranes are not generally suitable for applications involving harsh solvents like UDMH due to membrane chemical instability. However, a recent development of solvent-and-temperature resistant hydrophilic ceramic membranes made it possible to overcome the limitations of hydrophilic polymeric membranes. PV is an economical separation technique compared with conventional separation methods such as distillation especially in processes involving azeotropes, isomers and (removal or recovery of) trace substances. Due to its high separation factor and flux, PV results in energy cost saving and safe operation. In PV, feed mixture is contacted with a nonporous perm selective membrane. Separation is, in general, explained by the steps of sorption into, diffusion through and desorption from the membrane. The latter is usually considered to be fast and taking place at equilibrium, while diffusion is kinetically controlled and the slowest step of process. Permeation depends on sorption and diffusion steps. Driving force for the separation is created by maintaining a pressure lower than saturation pressure on permeate side of the membrane. The mechanism of separation is usually explained in terms of sorption-diffusion processes [8-10].
The hydrophilic membranes used in this
research were composite zeolite HS membranes. The membranes were basically made
of an active HS layer, deposited on a ceramic porous mullite support. The
active HS layer is responsible for high separation factors achieved in PV of
UDMH mixtures. The structure of zeolite HS is shown in (Figure
1).
As
shown in (Figure 1), the aluminosilicate
framework of zeolite HS is generated by placing truncated octahedrons (b-cage)
at eight corners of a cube and each edge of the cube is formed by joining two
b-cages. Each b-cage encloses a cavity with a free diameter of 0.66 nm and each
unit cell encloses a larger cavity (a-cage). There are two interconnecting,
three-dimensional channels in zeolite HS: (i) connected a-cages, separated by
0.3 nm apertures, (ii) b-cages, alternating with a-cages separated by 0.22 nm
apertures. Thus, molecules smaller than 0.3 nm in diameter can diffuse easily
through the nanopores of the zeolite. In addition, position of sodium ions in
unit cells is important since these ions act as the sites for water sorption
and transport through the membrane. For a typical zeolite, a unit cell having
the composition Na6[Al6Si6O24] (OH)2.
(1.5 H2O), eight (out of 12) sodium
ions are located inside an a-cage and four ions are located in b-cages.
Transport of solvent species (mainly water) through the zeolite matrix
comprises of three steps: (i) strong adsorption of the species into a cage from
feed side, (ii) surface diffusion of the species from cage to cage and (iii)
vaporization of the species to permeate side. Normally, any physical adsorption
process includes both Vander Waals dispersion-repulsion forces and
electrostatic forces comprising of polarization, dipole and quadrupole
interactions. However, since the zeolites have an ionic structure, the
electrostatic forces become very large in adsorption of polar molecules like H2O. This effect is manifested in the fact
that heat of adsorption of water into zeolitic adsorbents is unusually high (25-30
kcal/mole).
2)
the
porosity of body prior to leaching,
3)
the
concentration of leaching solution and
4)
Temperature.
Cylindrical
shaped (tubular) bodies (ID: 10 mm, OD: 14 mm and L: 15 cm) have been
conveniently made by extruding a mixture of about 75-67% kaolin and 25-33%
distilled water. Suitable calcinations temperatures and periods are those at
which kaolin converts to mullite and free silica. Good results have been
achieved by calcining for about 3 h at temperatures of about 1250°C [17,18].
Coating of the Support with Seeds: Adding seed crystals to this crystallization system has resulted in increased crystallization rate. The enhanced rate might be due to simply increasing the rate at which solute is integrated into the solid phase from solution due to the increased available surface area, but also might be the result of enhanced nucleation of new crystals. The secondary nucleation mechanism referred to as initial breeding results from microcrystalline dust being washed off seed crystal surfaces in a new synthesis batch. These microcrystalline fragments grow to observable sizes, and result in greatly enhanced crystallization rates due to the significantly increased crystal surface area compared to the unseeded system. Consequently, it is to be expected that addition of seed crystals to a synthesis system will introduce sub-micron sized crystallites into the system that will serve as nuclei.
Any
change of feed concentration due to permeation is negligible because the amount
of permeate is small (max 2 ml) compared to total feed volume in the system
(0.5 lit). A three-stage diaphragm vacuum pump (vacuubrand, GMBH, Germany) has
been employed to evacuated the permeate side of the membrane to a pressure of
approximately 1.5 mbara while the feed side has been kept at room pressure. The
permeate side has been connected to a liquid nitrogen trap via a hose to condense
the permeate (vapor). Permeate concentrations have been measured by a GC (TCD
detector, Varian 3400).
·
Stabilization
of porous lattices as zeolites by acting as space fillers, referred to above.
·
Through
its presence, especially at high pressures, water may be incorporated into
hydrous glasses, melts, and solids. Through chemisorptions into siliceous materials,
Si-O-Si, and Al-O-Si, bonds hydrolyze and re-form. Chemical reactivity is
enhanced and magma viscosity is lowered.
·
High
pressures of water can modify phase equilibrium temperatures.
· Water is a good solvent, a property that assists disintegration of solid components of a mixture and facilitates their transport and mixing.
Water is important as a guest molecule in zeolite structures with relatively high Al contents and consequently, aqueous media favor their formation while salts have a parallel role in the stabilization of zeolite structure. In general, the zeolitic water can be removed leaving the unchanged hydrous zeolite. In hydrothermal systems, the good solvent powers of water promote mixing, transport of materials, and facilitate nucleation and crystal growth. Water stabilizes zeolite structures by filling the cavities and forming a type of solid solution. The stabilizing effect is such that the porous aluminosilicates will not form in the absence of a guest molecule, which may be a salt molecule as well as water. However, the water concentration or the degree of dilution is important for the synthesis of HS, which can crystallize out of gels with an extremely wide range of H2O/Al2O3 ratios (from 500 to 1500).
The Na2O or alkalinity of the media plays a vital role in crystal growth, materials synthesis/preparation, and processing, on the whole. It influences the super saturation, kinetics, morphology, shape, size, and crystallinity, of the particles or materials as the OH- anions fulfill the crucial role of mineralizing agent. The Na2O is influenced by the reactants and their concentrations/ratios, followed by temperature and time. Further, with the introduction of organics, the alkalinity changes rapidly in the system, hence, alkalinity is the key parameter in determining the crystallization rate. An increase in OH concentration will generally bring about an accelerated crystal growth and a shortened induction period before viable nuclei are formed. In zeolite synthesis, pH of the alkaline solution is usually between 8 and 12. The major role of pH is to bring the Si and Al oxides or hydroxides into solution at an adequate rate.
To
study effects of gel composition on HS zeolite membrane performance, the
membranes were synthesized at different compositions (SiO2/Al2O3=1.0-5.0, Na2O/
Al2O3=15-65,
H2O/ Al2O3=500-1500) for duration 12 h and temperature
100°C. It must be also
mentioned that three samples were prepared for each condition. The results were
presented on average and the maximum deviation was less than 3%. As seen in (Table 3).
HS zeolite membranes have been successfully synthesized in ranges of SiO2/Al2O3=1.0 to SiO2/Al2O3<2.5, Na2O/ Al2O3=15-65, H2O/ Al2O3>500 to H2O/ Al2O3=1500. In H2O/ Al2O3<500 ratio, HS zeolite membranes have not been successfully synthesized, because gel composition have not enough water for synthesis a homogenous gel. Also, in SiO2/Al2O3>2.5 ratio, causes HS zeolite to transform to other zealots. It must be mentioned that 10000 is the highest measurable value using the GC at 5 wt% UDMH concentration as shown in (Table 3).
5.2. Temperature and Time
Temperature
and time have a positive influence on the zeolite formation process, which
occurs over a considerable range of temperatures. A rise in temperature will
increase both the nucleation rate and the linear growth rate; hence, the
crystallinity of the samples normally increases in time. As far as time is
concerned, zeolite synthesis is governed by the occurrence of successive phase
transformations. The thermodynamically least favorable phase will crystallize
first and will be successively replaced in time by more stable phases. The best
example is the crystallization sequence of amorphous → NaA → HS.
Shows
SEM photographs of the mullite support (a) and the HS zeolite membrane (b).
Porous structure of the support and thin layer of the membrane can be easily
observed. (Figure 6) shows morphology of the HS
zeolite membranes (surface and cross section). As seen, most of the crystals
lie disorderly on the surface. The SEM photograph of the HS zeolite membranes
(cross section) show that the mullite surface is completely covered by a zeolite
crystal layer. The HS zeolite membrane thickness was found to be about 20-30 µm
judging from the SEM observation.
effect of feed rate on permeate flux were measured at constant temperature (20°C) and constant pressure (1 bar). Increasing feed rate increases the permeate flux. As shown in (Table 4), increasing pressure increases the permeate flux. Increasing rate increases turbulence and hydrodynamic effects cause to increasing permeate flux. Temperature is known as a main parameter. Increasing temperature causes an increase in viscosity reduction. (Table 4) shows the experimental data for the flux as a function of temperature. As seen, the flux increases with temperature. According to the results, it can be said the optimum operating conditions were 60°C, 3 bar and 3 lit/min.
6. Conclusion
Zeolite
nanopore HS membranes were synthesized on the porous mullite tubes by
hydrothermal method. It was found gel compositions that Nano HS zeolite
membranes have been synthesized. It was found gel compositions, time and
temperature range that HS zeolite membranes have been synthesized. The best
range operating condition (time and temperature) for hydrothermal synthesis of
nanopore HS zeolite membrane were 12-24 h and 70-130°C respectively.
These membranes showed very good membrane performance for separation of UDMH
/water mixtures. Effect of operating condition at pervaporation process show
that increasing pressure, feed rate and temperature increases the flux
linearly.
Figure 1: Repeating Unit of Zeolite HS.
Figure
2a: pervaporation cell: 1- feed tank 2-membrane module
3- membrane 4- O-ring 5- Teflon fitting 6- stainless steel vacuum fitting 7-
vacuum hose 8- cap 9- feed tank cap.
Figure
2b: Pervaporation Setup: 1- PV cell 2- Liquid Nitrogen
Trap 3- Permeate Container 4- Three Stage Vacuum Pump.
Figure
3: PV Setup Cross Flow; 1- Feed Container and PV Cell
2- Liquid Nitrogen Trap 3- Permeate Container 4- Three Stage Vacuum Pump 5-
Centrifuge Pump 6- Tank Feed.
Figure
4: XRD of the Support.
Figure
5: XRD of the HS Zeolite Membrane.
Figure 6: SEM Micrograph of
a) The Support b) The Membrane c) Thickness of Membrane on Support.
Purification (Wt.
%) |
Energy
required (kJ/kg
EtOH) |
Process |
8.0-99.5 |
10376 |
Distillation |
95.0-99.5 |
3305 |
Azeotropic
distillation |
95.0-99.5 |
423 |
Pervaporation |
Purification (Wt. %) |
Energy required (kJ/kg EtOH) |
Process
|
8.0-99.5 |
10376 |
Distillation |
95.0-99.5 |
3305 |
Azeotropic distillation |
95.0-99.5 |
423 |
Pervaporation |
Table 1: Energy requirements for ethanol dehydration.
Component |
Percent (%) |
Phases |
Percent (%) |
SiO2 |
51.9 |
Kaolinite |
79 |
TiO2 |
0.1 |
Illite |
8 |
Al2O3 |
34.1 |
Quartz |
10 |
Fe2O3 |
1.4 |
Feldspar |
3 |
K2O |
0.8 |
Total |
100 |
Na2O |
0.1 |
||
L.O. I |
11.6 |
||
Total |
100 |
Table 2: Analysis of Kaolin Clay.
Sample |
Number of coating |
SiO2/ Al2O3 |
Na2O/ Al2O3 |
H2O/ Al2O3 |
t (h) |
T ( °C) |
UDMH (%) |
Flux kg/m2.h |
Separation factor |
1 |
1 |
1.0 |
65 |
1000 |
12 |
100 |
5 |
0.890 |
>10000 |
2 |
1 |
2.5 |
65 |
1000 |
12 |
100 |
5 |
1.340 |
176 |
3 |
1 |
5.0 |
65 |
1000 |
12 |
100 |
5 |
7.400 |
31 |
4 |
1 |
1.0 |
15 |
1000 |
12 |
100 |
5 |
0.267 |
>10000 |
5 |
1 |
1.0 |
40 |
1000 |
12 |
100 |
5 |
0.734 |
>10000 |
6 |
1 |
1.0 |
65 |
1000 |
12 |
100 |
5 |
0.890 |
>10000 |
7 |
1 |
1.0 |
65 |
500 |
12 |
100 |
5 |
3.700 |
88 |
8 |
1 |
1.0 |
65 |
1000 |
12 |
100 |
5 |
0.890 |
>10000 |
9 |
1 |
1.0 |
65 |
1500 |
12 |
100 |
5 |
1.440 |
>10000 |
10 |
1 |
1.0 |
65 |
1000 |
12 |
70 |
5 |
0.80 |
>10000 |
11 |
1 |
1.0 |
65 |
1000 |
12 |
100 |
5 |
0.89 |
>10000 |
12 |
1 |
1.0 |
65 |
1000 |
12 |
130 |
5 |
2.40 |
>10000 |
13 |
1 |
1.0 |
65 |
1000 |
6 |
100 |
5 |
1.0 |
26 |
14 |
1 |
1.0 |
65 |
1000 |
12 |
100 |
5 |
0.89 |
>10000 |
15 |
1 |
1.0 |
65 |
1000 |
24 |
100 |
5 |
0.73 |
>10000 |
Table 3: Flux and Separation Factor of HS Zeolite Membranes (dead end).
Run |
Concentration of UDMH in feed (wt %) |
P (bar) |
Q (lit/min) |
T (°C) |
Flux kg/m2.h |
1 |
5 |
1 |
0.5 |
20 |
1.112 |
2 |
5 |
1 |
1.5 |
20 |
1.447 |
3 |
5 |
1 |
3 |
20 |
1.814 |
4 |
5 |
1 |
0.5 |
20 |
1.112 |
5 |
5 |
2 |
0.5 |
20 |
1.447 |
6 |
5 |
3 |
0.5 |
20 |
1.814 |
7 |
5 |
1 |
0.5 |
20 |
1.112 |
8 |
5 |
1 |
0.5 |
40 |
2.301 |
9 |
5 |
1 |
0.5 |
60 |
2.851 |
Table 4: Cross Flow Results by Membrane Sample 1.
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