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A final report on
SYNTHESIS AND PROPERTIES OF POLYMER BASED
ION EXCHANGE MEMBRANE AND ITS APPLICATION IN
ENVIRONMENTAL REMEDIATION
By
Dr. JITHA KUNHIKRISHNAN M
Submitted to
University Grants Commission
South West Region
Bangalore
20th June 2019
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Acknowledgement
I express my deep sense of gratitude to University Grants Commission for the financial assistance provided to this minor research project.
I am also thankful to Dr.Sivadasan Thirumangalath, The Principal, Sree Narayana College, Kannur for his encougement and co-operation.
I specially thank Dr. Anitha P.K., Head of the Department of Chemistry, Sree Narayana College, Kannur, and Dr.C. Reetha, The Former Head of the same, for helping me and providing the facilities.
I also thank all the faculty members of Dept. of Chemistry, Sree Narayana College, Kannur, for their kind support and co-operation.
My thanks are due to CWRDM-Calicut, Sealab-Aroor, NIT-Calicut and Nirmalagiri college -Koothuparamba for the assistance rendered for the analytical studies.
Finally, I thank my family members and all the near and dear ones for their limitless support and encouragement throughout the course of investigation.
Dr. Jitha Kunhikrishnan M
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INDEX
1. Introduction 3
2. Review 10
3. Fabrication of zirconium tugstophosphate doped polymer 18 membrane and its application
3.1 Chemicals used 18
3.2 Characterization 18
3.3 Preparation of zirconium(IV)tugstophosphate doped membrane 19
3.4 Batch adsorption studies 20
3.5. Optimization of adsorption studies 21
3.6. Kinetics of adsorption 22
3.7. Potentiometric sensing of lead ion 25
3.8. Results and discussion
4. Fabrication of titanium dioxide doped polymer-
membrane and its application 36
4.1 Chemicals used 36
4.2 Preparation of titanium dioxide doped membrane 36
4.3 Physico- chemical characterization 36
4.4. Kinetics and thermodynamics of dye adsorption 37
4.5 Treatment of textile effluent waste 38
4.6 Results and discussion 38
5. References 48
6. List of tables 53
7. List of figures 54
8. Conclusion
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1. INTRODUCTION
Ion exchange is a process in which ions of one substance are replaced by
similarly charged ions of another substance. In water softening, for example,
the hardness causing calcium and magnesium ions are replaced by hydrogen and
sodium ions by passing the hard water over an ion-exchange resin. The solid must
ofcourse contain ions of its own for the exchange to proceed rapidly and extensively
to be of practical value. The solid must have an open permeable molecular structure
so that ions and solvent molecules can move freely in and out. Many substances both
natural (e.g.: certain clay minerals) and artificial, have ion exchanging properties, but
for analytical work synthetic organic ion exchanger are chiefly of interest certain
inorganic materials e.g.: zirconyl phosphate, also possess useful ion exchange
capacities and have specialized application.
Ion exchange is one of the most important analytical techniques used widely for
separations involving closely related elements .The importance of this technique is
revealed from the large amount of literature accumulated during the last two decades.
Some of the book related on this area is those by Helfferich (1), Inczeddy (2), Marcus
and Kerts (3), Samuelson (4) and Riemann and Walton (5).
The phenomenon of ion exchange was first reported by two English agricultural
chemists in 1850.They proved that soil can remove potassium or ammonium ions
from water with the release of an equivalent amount of calcium and magnesium.
An important advance was made in 1935, when Adams and Holms (6)
published the first paper on the synthesis of ion exchange resins. This led to rapid
progress in research on the theoretical and practical aspects of ion exchange so that
1935 may said to mark the new beginning of ion exchange.
1.1 Ion exchange equilibrium
Ion exchange process may be represented by chemical equations. In general,
where A ion of valance ‘n’ and B ions of valance ‘z’ are exchanged on a cation
exchanger in contact with an electrolyte solution. The equation is as follows:
− + ⇆ − +
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Where R is the equivalent amount of the ion exchange anion. The above equation
obeys the law of mass action and the thermodynamic equilibrium constant can be
derived. Applying the law of mass action to the equilibrium set up,
= ( × )( )
Where aA and aB are the activities of A and B ions measured in the liquid phase, and
arA and arB are the mean activities measured in the solid phase, K is the
thermodynamic equilibrium constant which solely depends on the temperature and not
on the change of activities.
The two quantities which are important from the point of view of separation are the
distribution coefficient Kd and the selectivity coefficient . Both can be
experimentally determined.
1.2. Theory of Ion exchange
Even now there is no fully satisfactory general theory concerning the operation of ion
exchangers and there are many questions which cannot be answered unambiguously.
The theories proposed are,
a) The double layer theory
b) The lattice exchange theory and
c) The Donnan membrane theory
According to double layer theory, an inner fixed layer is surrounded by a
diffuse and mobile outer layer of charges which owe their existence to absorbed ions.
They may be different from ions that are already present in the inner portion of the
colloidal particles. Donnan theory deals with unequal distribution of ions on both
sides of the membrane, one side contain an electrolyte, one of whose ions cannot –
penetrate the membrane. In ion exchange equilibrium, the interface between solid and
liquid phases may be considered as membranes. These theories are almost similar
since the law of electro-neutrality governs these laws. The only difference is in the
position and origin of exchange sites.
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1.3. Types of Ion exchanger
The three important groups of ion exchanger are inorganic, natural organic base
and synthetic ion exchanger. Among inorganic ion exchangers, the aluminosilicates,
both natural and synthetic, are suitable for technical purposes. Zeolites are naturally
occurring anion exchanger .Aluminum, Iron (II) and zirconium hydroxide etc acts as
synthetic inorganic anion exchangers. Cellulose based ion exchangers containing
phosphoric, sulphonic acid and diethyl amine groups come under natural organic base
ion exchangers. Synthetic ion exchange resin consists of a large organic molecular
network to which active groups able to ionize are fixed. The active groups of cation
exchange resins can be phenolic hydroxyl(-OH),carboxyl(-COOH) or phosphoric
acid(H3PO4).While for anion exchange resins, the active groups are usually primary,
secondary, tertiary or quaternary basic groups. Ion exchanger in the liquid form is
known as liquid ion exchangers. The behavior of liquid ion exchangers is similar to
that of resin ion exchangers. In both techniques, exchange of ions of like sign occurs
between two immiscible liquid in contact with each other. Analogous to resin ion
exchangers, there are both liquid anion exchanger and liquid cation exchangers.
Liquid anion exchangers are mainly primary, secondary, tertiary amines or quaternary
ammonium salts of high molecular weight. The liquid cation exchangers are usually
phosphoric acid esters or carboxylic acids. Chelating ion exchange resins contain
various chelating groups attached to the resins matrix. Dimethylglyoxime,
iminodiacetic acid etc are the examples. An important feature of chelating ion
exchangers is greater selectivity of metal ions. The affinity of a particular metal ion
for a certain chelating resins depends mainly on the nature of the chelating groups and
the selectivity of the resin is based on the different stabilities of metal complex
formed on the resin under various pH conditions. However the exchange process in
chelating resin is slower than in the ordinary type of exchangers.
Ion exchange resins are polymers with cross-linking (connections between long
carbon chains in a polymer). The resin has active groups in the form of electrically
charged sites. At these sites, ions of opposite charge are attracted but may be replaced
by other ions depending on their relative concentrations and affinities for the sites.
Two key factors determine the effectiveness of a given ion exchange resin:
favorability of any given ion, and the number of active sites available for this
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exchange. To maximize the active sites, significant surface areas are generally
desirable. The active sites are one of a few types of functional groups that can
exchange ions with either plus or minus charge. Frequently, the resins are cast in the
form of porous beads. The size of the particles also plays a role in the utility of the
resin. Smaller particles usually are more effective because of increased surface area
but cause large head losses that drive up pump equipment and energy costs.
Temperature and pH also affect the effectiveness of ion exchange, since pH is
inherently tied to the number of ions available for exchange, and temperature governs
the kinetics of the process. The rate-limiting step is not always the same, and
temperature's role is still not thoroughly understood.
For technical purposes thin plates or membranes are produced from ion
exchange materials. The main characteristic of ion exchange membrane in contrast
with conventional semi permeable membrane is that, they are selective for one type of
ion. The use of ion exchangers as ion selective electrodes is a new field in which
works are rapidly progressing.
1.4. Ion exchange membrane
Today, separation membranes have become essential materials not only in
industries, but also in day-to-day life. Thus, innumerable membranes have been
developed for the use in reverse osmosis, nanofiltration, ultra filtration,
microfiltration, pervaporation separation, electrodialysis and in medical use such as
artificial kidney .Among these membranes, ion-exchange membranes are one of the
advanced separation membranes. Basic applications of the ion-exchange membrane
process are based on the Donnan membrane equilibrium principle and have been paid
attention to solve two important environental problems: (i) recovery and enrichment
of valuable ions, and (ii) removal of undesirable ions from wastewater, especially to
extract toxic metal ions. Basically, the ion-exchange membranes separate cations from
anions and anions from cations, so they should have a high transport number for
counter ions. Such membranes with high transport number have the potential
applications in new field’s such as separation of ionic materials, mostly used in the
solutions containing multi-components, such as electrodialytic concentration of
seawater to produce sodium chloride, demineralization of saline water, desalination of
cheese whey, demineralization of sugarcane juice, etc. In some cases, specific ions
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have been used industrially: monovalent selective ion exchange membranes and
proton selective ion-exchange membranes are important. Apart from these
applications, several trials have been carried out to be used as sensors such as
humidity sensor ,carbon monoxide sensor , drug sensor, carriers for enzymes, solid
polyelectrolyte’s, a carrier for functional materials, generation of photo voltage and
photocurrent, etc. The generation of photo voltage from anion exchange membranes is
a new phenomenon and might lead to a new application of the ion-exchange
membranes.
In the past, excellent review articles appeared on different aspects of ion-
exchange membranes. However, none of the articles was dedicated to compile the
different methods for the preparation of ion-exchange membranes. Most commercial
ion-exchange membranes can be divided, according to their structure and preparation
procedure, into two major categories, either homogeneous or heterogeneous.
According to Molau, depending on the degree of heterogeneity of the ion-exchange
membranes, they can be divided into the following types: (a) homogeneous ion-
exchange membranes, (b) inter polymer membranes, (c) micro heterogeneous graft-
and block-polymer membranes, (d) snake-in-the-cage ion-exchange membranes and
(e) heterogeneous ion-exchange membranes. All the intermediate forms are
considered as the polymer blends from the viewpoint of macromolecular chemistry
1.5. Classification of Ion exchange membranes
There are different methods of classifying ion-exchange membranes:
Classification based on function is clear; ion-exchange membranes have an electrical
charge, which is positive or negative. The function of ion-exchange membranes is
determined from the species of the charge of the ion-exchange groups fixed in the
membranes and their distribution:
1. Cation exchange membranes, in which cation exchange groups (negatively
charged) exist and cations selectively permeate through the membranes.
2. Anion exchange membranes, in which anion exchange groups (positively charged)
exist and anions selectively permeate through the membranes.
3. Amphoteric ion exchange membranes, in which both cation and anion exchange
groups exist at random throughout the membranes.
4. Bipolar ion-exchange membranes which have a cation exchange membrane layer
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and anion exchange membrane layer (bilayer membranes).
5. Mosaic ion exchange membranes, in which domains having cation exchange
groups exist over cross-sections of the membranes and domains of anion exchange
groups also exist.
Basically, three basic properties are required for ion-exchange membranes:
(1) to exist as a membrane;
(2) to be insoluble in solvents; and
(3) to have fixed charges in the membrane.
To achieve these properties, many methods have been developed: after ion exchange
groups are introduced in a polymer, the polymer is changed into an insoluble
membrane; a polymeric membrane is produced and ion-exchange groups are then
Introduced in the membrane, etc.
1.6. Ion exchange properties
1.6.1 Ion exchange capacity
Ion exchange capacity of an exchanger means the total amount of the
exchangeable ions of unit weight. Salt splitting capacity is measured when, for
instance the amount of sodium ions absorbed by the cation exchange resin in the
hydrogen form, from a sodium chloride solution, and for anion exchange it is the
amount of base from salt by unit weight or unit volume of the hydroxyl form anion
exchanger. For mono functional strongly basic or acidic exchanger, the salt splitting
capacity is identical with the total capacity.
The apparent capacity may differ from the theoretical values, when the ions
examined cannot occupy every exchange site because of their greater size. The
apparent capacity called the break through capacity is not a constant and it depends on
the condition under which it is determined.
1.6.2. Disitribution coefficients
It is the ratio of concentrations of the substance measured in the exchanger and
in the solution phase respectively. The distribution coefficient Kd is a measure of the
extent to which an ion is removed from solution and is defined as the number of
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milliequivalent of an ion absorbed per gram of the exchanger divided by the number
of milliequivalent of that ion per ml remaining in the solution at equilibrium.
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2.REVIEW
The last year or so have seen a great upsurge in the researches on synthetic
inorganic ion exchangers as they are stable towards heat and radiation. The main
emphasis has been given to the development of new materials possessing chemical
stability, reproducibility in ion exchange behavior and selectivity for certain metal
ions are important from analytical point of view. Important advances in this field have
been reviewed by a number of workers at various stages of its development.
According to Vesely and Pekarek (7) synthetic inorganic ion exchangers can be
classified in to following categories,
(1) Oxides and hydrous oxides.
(2) Heteropoly acid salts.
(3) Acid salts of polyvalent metals.
(4) Aluminosilicates synthetic zeolites and clay.
(5) Insoluble hydrated metal ferro and ferricyanide.
(6) Miscellaneous.
2.1. Oxides and Hydrous oxides
In 1972 Vesely and Pekarek (7) have given an exhaustive survey covering the
preparation, properties, uses and theory of hydrous oxides of bivalent, trivalent,
quadrivalent, quinquivalent and sexivalent ions. De and Sen (8) gave synthesis,
properties and analytical application of the hydrated oxides of metals such as Al, Si,
Sn, Zr, Ce and Tungsten oxides. Hydrous alumina sample are constantly used in
analytical separation as adsorbent and desorbent.
2.2 Acid salts of polyvalent metals
Vesely and Pekarek (7) De and Sen (8) have given details of various acidic salts
of polyvalent metals having different anionic part such as phosphate, arsenate,
antimonite, selenate, ferrocyanides, molybdate, tungstate etc. In 1980 Walton(9) has
reviewed bismuth tungstate, cobalt arsenate, and antimonates of thorium and nickel.
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Industrial application of ion exchangers, ways of increasing efficiency of ion
exchange method for mixture separation, substance purification and preparation,
characteristics and properties of group(IV) acid salt as ion exchangers have been
discussed. Ruvarac and Howe(10), Clearfield(11), Besse(12), Garicia(13),
Laginestra,(14) Alberti(15) have discussed the catalytic properties and application of
ion exchangers and super ionic conductivity in cubic potassium- antimonate(V),
zirconium phosphate and exchange of alkali metals, thermal, redox and catalytic
characterization of inorganic ion exchange membrane and recent trends in inorganic
ion exchangers.
A new exchanger thorium tellurite act as a cation exchanger in alkaline medium
and anion exchanger in acidic medium another thorium based ion exchanger thorium
iodate was synthesized and characterized by C.Janardanan and Jitha (16). It was found
to be selective towards Pb (II).
Chromatographic and proton conduction behavior of 44 metal ions on thin
layers of stannic phosphate have been described. Selectivities of alkali metals on
stannic antimonate, prediction of Ksp from Rf values and of thin layer chromatography
of 47 metal ions in H2O-HCl system in stannic pyrophosphate and poly phosphate
were synthesized and planar chromatography of 36 metal ions on tin(IV)phosphate,
tin(IV)molybdate and tin(IV)tungstate impregnated papers were carried out.
Separation follows the order tin (IV) molybdate > tin (IV) tungstate > Tin (IV)
phosphate.
Cerium (IV) tellurite was prepared and characterized as a new inorganic cation
exchanger by Nabi et al(17). Ceric phosphate was used in the separation of carrier
free Bismuth-210 from Lead-210, Yttrium-90 from Strontium-90.Thin layer
chromatography of ten previous metal ions and separation of Zn (II), Cd (II), and Co
(II) on Cerium metaphosphate were conducted. Cerium phosphate was characterized
and synthesized, by Nilchi et.al (18).Cerium (IV) selenite, cerium (IV) arsenite,
cerium (IV) vanadate etc were extensively studied as ion exchangers by Hussein(19),
C.Janardanan(20) and their coworkers. Study of selectivity of certain metal ions Cs
(I), Sr (II), Co (II) etc. and kinetic study of alkali metals on Ceric antimonate have
been reported. Cerium silicate was synthesized and used by Maragch for the sorption
studies of radinuclei on it.
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Varshney and his co-workers conducted cation exchange study, effect of
gamma-irradiation on ion exchange behavior and separations on thermally stable
phase of antimonysilicate. A new exchanger antimony(V)tungstate was synthesized
and was used to remove chromium(VI), mercury(VI), lead(II) etc. C.Janardanan(20)
and co-workers synthesized many antimony based exchangers such as
antimony(III)arsenate, antimony(III)molybdate, antimony(III)vanadate,
antimony(III)tungstate, antimony(III)selenite and explored their ion exchange
properties.
Bismuth antimonate was synthesized and its ion exchange properties were
extensively studied by Janardanan et.al (20) Bismuth tungstate was used as an
absorbent for thin layer chromatography of organic acid by Kulshrestha et.al (21)
Abou Mesalam et.al (22) studied the retention behavior of Nickel, Copper, Cadmium
and Zinc ions from aqueous solution on silicotitanate and silicoantimonite.
Silver ion selective Lithium titanium phosphate glass-ceramic cation exchanger
was synthesized and latter was applied to the bacteriostatic materials. Ion exchange
properties of Tin(IV) iodate were studied by Janardanan et.al(20) and separation of
Pb(II) and Cu(II) from industrial waste was successfully carried out on it.
Thorium phosphosilicate – a new mercury selective ion exchanger was
synthesized and the effect of gamma irradiation on its ion exchange property was
reported.
Lead selective cerium (IV) phosphomolybdate and antimony (III)
molybdotungstate were studied in detail by Janardanan et.al (20). They also made a
comparative study of the ion exchange property of antimony (III) tungstoselenite with
antimony (III) tungstate and antimony (III) tungstovanadate.
Titanium(IV)arsenophosphate,Titanium(IV)tungstoarsenate,Titanium(IV)molyb
doarsene, Titanium(IV)vanadophosphate were synthesized and characterized.
Titanium (IV) molybdoarsenate has been used for the separation of Pb (II) and Hg (II)
from lanthanum and cerium.Titanium tungstopyrophosphate, Titanium
tungstophosphate and Titanium tungstosilicates were prepared by Zhang (23) et.al and
Siddiqi et.al (24).The latter conducted the separation of methylamine from ethylamine
by GC on a column packed with Titanium (IV) tungstophosphate.
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2.3. Ion exchange membrane
Traditionally, ion exchange membranes are classified into anion exchange
membranes and cation exchange membranes depending on the type of ionic groups
attached to the membrane matrix. Cation exchange membranes contain negatively
charged groups, such as –SO3−, –COO−, –PO3
2−,–PO3H−, –C6H4O
−, etc., fixed to the
membrane backbone and allow the passage of cations but reject anions. While anion
exchange membranes contains positively charged groups, such as –NH3+, –NRH2
+, –
NR2H+, –NR3
+, –PR3+,–SR2
+, etc., fixed to the membrane backbone and allow the
passage of anions but reject cations (25,26). According to the connection way of
charge groups to the matrix or their chemical structure, ion exchange membranes can
be further classified into homogenous and heterogeneous membranes, in which the
charged groups are chemically bonded to or physically mixed with the membrane
matrix, respectively.
However, most of the practical ion exchange membranes are rather homogenous and
composed of either hydrocarbon or fluorocarbon polymer films hosting the ionic
groups (27)
The development of ion exchange membrane-based process began in 1890 with the
work of Ostwald (28) who studied the properties of semi permeable membranes and
discovered that a membrane can be impermeable for any electrolyte if it is
impermeable either for its cation or its anion. To illustrate this, the so-called
“membrane potential” at the boundary between a membrane and its surrounding
solution was postulated as a consequence of the difference in concentration. In 1911,
Donnan (29) confirmed the existence of such boundary and developed a mathematical
equation describing the concentration equilibrium, which resulted in the so-called
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“Donnan exclusion potential”. However, the actual basic studies related ion exchange
membranes were firstly begun in 1925 and carried out by Michaelis and Fujita with
the homogeneous, weak acid collodium membranes (30). In 1930s, Sollner presented
the idea of a charge-mosaic membrane or amphoteric membrane containing both
negatively and positively charged ion exchange groups and showed distinctive ion
transport phenomena (31). Around 1940, interest in industrial applications led to the
development of synthetic ion exchange membrane on the basis of phenol-
formaldehyde-polycondensation(32).Simultaneously, Meyer and Strauss proposed an
electrodialysis process in which anion exchange and cation exchange membranes
were arranged in alternating series to form many parallel solution compartments
between two electrodes (33).It was hard to go into the industrial implications because
commercial ion exchange membranes with excellent properties especially low electric
resistance were still not available at that time. With the development of stable, highly
selective ion exchange membrane of low electric resistance in1950 by Juda and
McRae of Ionics Inc. (34)and Winger et al. at Rohm in 1953 (35), electrodialysis
based on ion exchange membranes rapidly became an industrial process for
demineralizing and concentrating electrolyte solutions. Since then, both ion exchange
membranes and electrodialysis have been greatly improved and widely used in many
fields. For example, in 1960s, first salt production from sea water was realized by
Asahi Co. with monovalent ion perm selective membranes (36); in 1969, the
invention of electrodialysis reversal (EDR) realized long-term run without salt
precipitation or deposition on both membranes and electrodes (37); in 1970s, a
chemically stable cation exchange membrane based on sulfonated polytetra-
fluorethylene was first developed by Dupont as Nafion, leading to a large scale use of
this membrane in the chlor-alkali production industry and energy storage or
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conversion system (fuel cell) (38); simultaneously, a composition of cation exchange
layer and an anion exchange layer into a bipolar membrane in 1976 by Chlandaet al.
(39) brings many novelty in electro dialysis applications today (40). Also, stimulated
by the development of new ion exchange membranes with better selectivity, lower
electrical resistance and improved thermal, chemical and mechanical properties, other
applications of ion exchange membranes apart from the initial desalination of
brackish water have recently gained a broader interest in food, drug, chemical process
industry as well as biotechnology and waste water treatment nowadays (40-47).
Apart from polymeric ion exchange membranes, an ion exchange membrane can also
be prepared from inorganic material, such as zeolites, betonite or phosphate salts (48-
50).However, these membranes are rather unimportant due to their high cost and other
disadvantages, such as relative bad electrochemical properties and too large pores
though they can undergo higher temperatures than organic membranes(51). It can be
expected that ion exchange membranes prepared from polymers can possess both
chemical stability and excellent conductivity if the membranes were incorporated into
inorganic components, such as silica. So inorganic–organic ion exchange membrane
were development in late of 1990s by sol–gel for applications in severe conditions,
such as higher temperature and strongly oxidizing circumstances (51–53). Thus, till
now, various ion exchange membranes including inorganic–organic (hybrid)ion
exchange membranes, amphoteric ion exchange membranes, mosaic ion exchange
membranes, bipolar membranes(ion exchange composite membranes) are available
.Though ion exchange membranes and the related processes has received
multidiscipline attention in both theoretical investigations and industrial applications
nowadays, a more recently informative review including all the ion exchange
membrane types and synthesis or novel ion exchange membrane-based processes is
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still insufficient except some reviews on specific aspects, such as modifications of ion
exchange membranes (54,55). Electro-catalytic membrane reactors (56), radiation-
induced graft copolymerization for ion exchange membrane preparation (57,58), ion
exchange membrane applications (44) or bipolar membrane process and applications
in environmental protection (47) and in food industry (48). Furthermore, ion exchange
membrane related processes are gradually considered less important than pressure-
driven membrane processes, such as RO due to the commercial interests. But they are
actually indispensable for separation of ionic species, especially in environmental
protection and clean production and in many applications, ion exchange membrane-
related processes are in direct competition with other separation techniques, such as
distillation, ion exchange and various chromatographic procedures. Therefore, to
awaken researcher’s interest in this field and also to understand the present states ion
exchange membrane research, this review is to give a summary of what have been
accomplished in ion exchange membranes and development of novel ion exchange
membrane processes.
2.4. Membrane Adsorption Technology
Membrane separation has been increasingly used recently for the treatment of
inorganic effluent due to its convenient operation. Membrane adsorbent technology
is a membrane integration technology that was developed in the mid-1980s
.(49)Adsorption is a mass transfer process by which a substance is transferred from
the liquid phase to the surface of a solid, and becomes bound by physical and/or
chemical interactions. The heavy metal ions in the aqueous solution can be captured
by the adsorbent though the physical or chemical adsorption. Generally, chemical
adsorption is more popular for heavy metal removal because it has stronger
interactions and higher adsorption capacity towards heavy metals. The special
20
functional groups on the surface of the adsorbents provide significant interactions
with heavy metals, resulting in the adsorptive separation of heavy metals from
water.
Adsorption is a very significantly economic, convenient and easy operation
technique. It shows high metal removal efficiency and is applied as a quick method
for all types of waste water treatment. A membrane adsorbent is made by
connecting functional groups to the surface and pore wall of polymer membranes;
the target pollutants are selectively adsorbed to the functional group. The membrane
adsorbent effectively combines the filtration performance of the membrane. When
the contaminated water flows through the membrane, the functional active binding
sites will combine with the target pollutants to remove contaminants from drinking
water with a high adsorption rate and capacity because of the very short contact
distance at a submicron-scale level between the target pollutants to the adsorbed
active binding site of the membrane adsorbents ( 50).
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3. FABRICATION OF ZIRCONIUM(IV) TUNGSTOPHOSPHATE
DOPED POLYMER MEMBRANE AND ITS APPLICATION
3.1 Chemicals used :
Poly styrene sulphonic acid, poly vinyl alcohol, and maleic acid used for the
preparation of membrane were of analytical grade and was purchased from Alfa aeser.
Salts of heavy metals such as lead, copper, cadmium, mercury, cobalt etc. were from
Loba chemie. Zirconium oxy chloride, sodium tungstate, sodium phosphate etc were
from Merck.
3.2. Preparation of Zirconium(IV)tungstophosphate doped
polymer- membrane
3.2.1. Preparation of the ion exchanger.
Zirconium tunsgstophosphate (ZWP) was prepared by mixing desired
concentration of zirconium oxychloride to a mixture of solution of sodium tungstate
and sodium phosphate. The slurry obtained was kept overnight and filtered. The
exchanger was converted into H+ form by transferring it into 1.0M HCL in a 100 ml
beaker and shaken occasionally. It was filtered , washed was then dried at room
temperature.
3.2.2. Fabrication of membrane.
Membrane of different compositions were made by mixing polystyrene
sulphonic acid, poly vinyl alcohol and ZWP gel, in different proportions. Maleic acid
was added as a cross-linker.
A definite amount of poly vinyl alcohol(PVA) dissolved in hot water was
boiled with maleic acid in dil.H2SO4. To this poly styrenesulphonic acid(PSSA)
dissolved in distilled water was added carefully and heated. Zirconium
tungstophosphate suspended in distilled water was then slowly added to the above
mixture in drop wise manner and homogenized using vortex mixer.
Different composition membranes were prepared by mixing different ratios of
the components and it was spin coated on a Table - Top Spin-Coating Unit (Spektron
22
Instruments).(Fig.2)To get thick membranes mutliple layer coating was done.
Different samples were analysed for their maximum performance.
3.3. Physico-chemical Charcterisation
3.3.1. Instrumental Analysis:
Thermal stability (TGA) of PVA- PSSA-ZWP membrane was determined using
NETZSCH STA 449F5 Thermogravimetric analyzer under N2 atmosphere. Samples
were heated up to 900oC at the rate of 30oC/min. X-ray diffraction (XRD) is used to
study the crystal structure of prepared composite membrane. The structural analysis
was performed using X-ray diffractometer (Rigaku Miniflex 600) equipped with
CuKα radiation (λ= 1.54056A°) at 2θ angles between 5° and 80°. Mechanical strength
was measured using Universal testing machine.
3.3.2. Determination of Ion exchange capacity(IEC) of the ion exchanger.
The total ion exchange capacity of the exchanger was determined as follows.
1.0g of the exchanger was taken in H+ form in a 100 ml beaker. It was then
equilibrated with 20 ml 1.0 M NaCl solution for 24 hours. The solution was decanted
into conical flask, diluted to 50 ml. The hydrogen ion eluted from the exchanger was
determined titrimetrically with standard NaOH. From the titre value the ion exchange
capacity of the exchanger was determined using the following equation: IEC = (Volume of NaOH × Molarity of NaOH)(Weight of exchanger taken) 3.3.3. Determination of temperature stability
Several 1.0 g portions of the sample were heated at various temperatures in air
oven for 3h and the ion exchange capacities were determined by usual process after
cooling to the room temperature.
3.3.4. Determination of percentage water uptake and IEC of the membrane
For the water uptake measurement, a sample of the dry membranes were
weighed and immersed in distilled water for 24 hours, then excess water was removed
23
with absorbent paper and the wet sample was weighed. The water uptake was
calculated according to the following equation.
% Water uptake = (Ww − Wd)Wd × 100
Where Ww is the wet sample weight and Wd is the dry sample weight.
3.4. Batch adsorption studies of heavy metal ion on the
membrane
For adsorption studies standard solutions of Ni(II), Co(II), Cd(II), Pb(II) and
Cu(II) were prepared carefully by dissolving the desired amount of respective metal
nitrate salt.
3.4.1 Adsorption procedure
The adsorption equilibrium experiments of Ni(II), Co(II), Pb(II), Cu(II), and
Hg(II) were performed using a batch process to determine the amount of metal ion
adsorbed.
Membrane samples were equilibrated in a series of aqueous solution of
different metal ions. The solutions were kept overnight with intermediate shaking.
The membrane samples were then removed and the concentrations of metal ions in
the remaining solutions were determined using AAS (Agilent technologies). The
amount of metal ions adsorbed per unit mass of the adsorbent and the percentage of
adsorbed metal ions were obtained using equations given below.
qe =
VW
CeCo , where q is the amount of adsorbed metal ion at
equilibrium in mg/g. It is called metal adsorption capacity. V is the volume of the
adsorption medium, C0 is the initial metal ion concentration in mg/L. Ce is the
equilibrium metal ion concentration in mg/L and W is the dry weight of the
membrane in grams.
24
% adsorbed metal ion =Co
CfCo ,where, Cf is the final metal ion concentrations in
adsorption medium in mg/L.
3.5. Optimization of adsorption studies on the membrane
The studies were optimized for maximum sorption under different conditions
like effect of initial feed concentration, effect of pH, effect of membrane thickness.
Studies were also carried out to find the selectivity of membrane in presence of
different metal ions.
3.5.1. Effect of initial feed concentration on adsorption
Different initial concentration of the metal ions for which the membrane
showed higher affinity were prepared and equilibrated. The %adsorption were
determined for different initial concentrations.
3.5.2. Effect of membrane thickness on the adsorption percentage
Membrane of different weights were prepared by mixing the components in
same proportion ratios. The membrane samples of different thickness were then
equilibrated with metal ion solution and % adsorption for different samples were
calculated.
3.5.3. Effect of sorption medium pH
PH dependence of metal ion adsorption was performed by equilibrating
adsorbed samples in a series of solutions of different pH. The pH of the solution was
adjusted to a desired value by adding 1M HNO3 and 1M NaOH solution and noted
using Cole parmer pH meter(model: P200).
3.5.4. Selectivity studies
Affinity of membrane towards a particular metal ion in presence of other metals
was determined. This was done by equilibrating mixture solution of different metal
ions.
25
3.6. Kinetics of adsorption
Lagergren's pseudo first order and Ho's pseudo second order kinetic models were used
to investigate the mechanism of adsorption process.
Lagergren's equation can be expressed as
= k1(qe-qt)
where k1 is the pseudo first order adsorption rate constant.
by integrating above equation, for the condition that t=0 to t=t and qt=0 to qt = qt.
Therefore the linear form of equation obtained become,
ln(qe-qt) = lnqe - k1t ............................(1)
log(qe-qt) = logqe - . ..............................(2)
where qe and qt are the amount adsorbed at equilibrium, at time ‘t’ in minutes.
when log(qe-qt) is plotted against t, straight line is obtained. The slope gives the value
of rate constant k1.
Ho's pseudo second order equation can be expressed as
= k2(qe-qt)2 .............................(3)
where k2 is the pseudo second order rate constant.
by integrating equation (3) for the condition t=0 to t=t and qt=0 to qt = qt. therefore the
linear form of equation become,
= +
3.6.1. Adsorption isotherm
Langmuir, Freundlich, Dubinin-Radushkevich (D-R), Temkin isotherm models were
used to plot adsorption isotherms, which express the equilibrium relationship between
adsorbent and adsorbate (51).
Langmuir adsorption
26
Langmuir adsorption assumes monolayer adsorption in which the extent of adsorption
takes place on the surface of solid and is represented as,
= + (52)
Ce (mg/L) and qe (mg/L) are the equilibrium concentration and equilibrium adsorption
capacity. qm and KL are langmuir constants related to adsorption capacity (mg/g) and
energy of adsorption (L/g) respectively. Plot of Vs Ce gives straight line with slope
and intercept . The important characteristics of langmuir isotherm can be expressed in terms of RL, a
dimensionless constant, separation factor and can be written as,
= 11 + Co
where Co (mg/L) is the initial concentration of adsorbate.
According to the value of RL, four possibilities are there, RL>1.0 for Unfavourable
adsorption, RL=1.0 for Linear adsorption, 1>RL>0 for Favourable adsorption and
RL=0 for Irreversible adsorption (52,53).
Freundlich adsorption isotherm
Freundlich adsorption isotherm assumes multilayer adsorption and it is used to
describe the adsorption characteristics for the heterogeneous surface (54). The
logarithmic form of freundlich adsorption isotherm is written as
logqe = logKF + logCe (55)
Where qe is the amount of adsorbate per unit mass of adsorbant (mg/g). Ce is the
equilibrium concentration of adsorbate (mg/l). n and KF are Freundlich constants. Plot
of logqe Vs logCe gives a straight line with slope , which is ranging between 0 and 1.
It is a measure of not only surface homogeneity but also measure of adsorption
intensity. If the value of is closer to zero, it indicates the surface become more
heterogeneous. Value of below 1 indicates a normal langmuir isotherm while
above 1 indicates co-operative adsorption.
27
Dubinin-Radushkevich isotherm
It is generally used to express the adsorption behaviour on the heterogeneous surface
and their linear form is expressed as
lnqe = lnqs -Kad �2
where qe is the amount of adsorbate (mg/g), qs is the monolayer adsorption capacity
(mg/g), � is the polanyi potential, kad is the Dubinin-Radushkevich isotherm constant
(mol2/KJ2) related to mean free energy of adsorption. ie
E = 1/(√−2 )
B is the isotherm constant. If E value is in between 8 and 16 KJ/mol, adsorption
mechanism follows chemical adsorption and E<8 KJ/mol indicates that adsorption
mechanism is physical in nature [14]. Polanyi potential can be expressed as,
ℇ = 1 + 1 Where R is the gas constant (J/K/mol) and T is the absolute temperature.
The plot of lnqe Vs �2 gives a straight line with negative slope –Kad and intercept of
lnqs. The values of Kad and qs will be obtained.
Temkin isotherm
It expresses the effect of adsorbent - adsorbate interaction. By ignoring extremely low
and large value of concentration, this model assumes the heat of adsorption of
molecule decreases linearly with coverage due to adsorbate - adsorbent interaction.
Temkin isotherm can be written as,
= ( ) Here = B
Where R is the universal gas constant (8.314J/K/mol), T is the temperature at 298K, b
is the Temkin isotherm constant, A is the equilibrium binding constant (L/g). B is the
constant related to heat of adsorption (J/mol). The plot of qe against lnCe gives the line
with slope and intercept lnA.
28
3.7.Potentiometric sensing of lead ion using the membrane.
3.7.1. Preparation of ion selective electrode:
The prepared membrane was fixed to one end of a glass tube of diameter 1.5cm.
Then it was activated with 0.1M lead ion solution for 24hrs.
3.7.2. Calibration of the ion selective electrode:
SCE was used as internal reference electrode for the ion selective electrode. It
was then coupled with another SCE, the whole unit was then immersed in test
solution. EMFs were measured for varying lead ion concentration using a digital
potentiometer (Scientific Tech., model: ST DPS-01)
3.8 Result and discussions
Various samples of zirconium tungstophosphate obtained were white in
colour. The sample having higher ion exchange capacity (0.80meq/g) was used for
systematic study (Table1). The exchanger was found to be stable in 1.0 M mineral
acid and 1.0M salt solution.
Fig 1: PVA- PSSA- ZPW Membrane
29
Table 1: Preparation conditions and ion exchange capacities of various samples
The Na+ ion exchange capacity of zirconium tungstophosphate at room
temperature was found to be 0.80meq/g. The effect of heating on the ion exchange
capacity shows an abrupt decrease on ion exchange from 200° C (Table.2)
Temperature (℃) Duration (hr) Na+ I.E.C
50 3 0.77
100 3 0.70
200 3 0.60
300 3 0.25
400
3 0.15
Table 2: Effect of temperature on the ion exchange capacity of the exchanger
A stable zirconium tungstophosphate doped poly-vinyl alcohol-polystyrene
sulphonic acid membrane was obtained using spin coater (Fig.2). Sample-3 having
high IEC was used for futher studies.(Table.3). The membrane was found to be stable
in 1M HCl and NaOH.
Sample
No
Molar Ratio Volume
Ratio
pH Appearance I.E.C
(meq/g) Zr2+ WO3- PO42-
1
2
3
0.1
0.2
0.05
0.05
0.2
0.05
0.05
0.2
0.05
1:1:1
1:1:1
1:1:1
1
1
1
White
amorphous
solid
0.60
0.80
0.35
30
Fig 2: Spin coating unit with IR currer
Sample
No:
Weight % of RPM
TemperatureOC
PSSA PVA ZWP
1 50 40 10 5000 45
2 50 45 5 5000 60
3 40 50 10 10000 60
Table 3: Spin coating parameters and composition of different membrane samples
5 10 15 20 25 30 35 40 45 50
0
200
400
600
800
1000
1200
1400
Inte
ns
ity
(a
.u)
(degree)
Fig 3: XRD data Fig 4: TG curve
31
Fig 5: IR spectrum
XRD data shows a crystalline nature for the polymer membrane,this may be mainly
attributted to the presence of ZWP.(Fig.3)
The broad strong peak at 3231cm-1 in the IR data indicates the OH stretching of
structural hydroxyl group. The strong peak at 2901cm-1 can be attributed to carboxylic
hydroxyl group. The medium peak at 1644cm-1 is due to the C=O stretching of the
ester group formed as a result of esterification between polyvinyl alcohol and maleic
acid. The peak at 1416cm-1 may be due to the free carboxylic acid which did not take
part in the esterification reaction, showing lower extend of cross linking. The peaks at
1324 and 1076cm-1 can be attributed to S=O stretching of sulphonic acid group. The
weak peak at 2094cm-1 is due to aromatic C-H bending. The peaks at 912 and 823cm-1
can be assigned to C-H bending of cross linked poly vinyl alcohol.((Fig.5)
As per thermogravimetric analysis, the polymer shows three step degradation.
The first weight loss observed in the temperature range 1000C could be due to the loss
of physically bound water molecules. The second weight loss ranging from 200-
3700C may be due to the condensation of structural hydroxyl group and
desulphonation of sulphonic acid group. By 4300C, the polymer degrades.(Fig.4)
32
The affinity of membrane towards different heavy metal ions was found to be in
the order Pb>Cu>Cd>Co>Hg. Metal adsorption capacity for Pb(II) was 60mg/g. The
membrane showed least affinity towards Hg(II).(Fig.6)
Cu(II) Pb(II) Cd(II) Co(II) Hg(II)
0
20
40
60
80M
eta
l A
dso
rpti
on
%
Metal ions
Fig 6: % removal of various heavy metals
A study on effect of membrane thickness on adsorption was done by varying the dry
weight of membrane and the result showed that for initial concentration of 500mg/L
of Pb(II). The adsorption increased until a maximum value was reached at a
membrane thickness corresponding to 1.0g dry weight of membrane (Fig.7). Increase
in adsorption is attributed to the increase in the sorption sites available. But as the dry
weight increased to 1.2g the % adsorption decreased. This may be due to the non-
availability of sorption sites for the Pb(II) ions as a result of change in pore size
.
0 .2 0 .4 0 .6 0 .8 1 .0 1 .2
76
78
80
82
84
86
88
90
92
94
96
Met
al A
dso
rpti
on
%
M em brane Th ickn ess (g )
Fig 7: Effect of membrane thickness on adsorption
33
Study on the effect of initial feed concentration shows that as the
concentration increased % adsorption decreased. This may due to the saturation of
available sites (Fig.8).
500 600 700 800 90064
66
68
70
72
74
76
78
80
82
84M
etal
Ad
sorp
tio
n %
Initial metal concentration (mg)
Fig 8: Effect of initial metal ion concentration on adsorption
Study on the effect of pH on the adsorption capacity shows that the %
adsorption increased as the pH increased and a maximum was reached when the pH of
the medium was equal to 7.0 (Fig.9). The low adsorption capacity of all metal ions at
lower pH can be ascribed to competitive adsorption of H3O+ ions and metal ions for
the same active adsorption sites.
Selectivity of membrane towards Pb(II) in presence of other metal ions like Cd,
Zn, Cu, Hg, and Co were determined and the studies showed that though the
membrane was selective towards Pb(II), the % adsorption decreased. This may be
probably due to the competitive adsorption of Pb(II) and other heavy metal ion.
Optimisation studies of membrane adsorption for Pb(II) shows that an effective
adsorption can be attained by a membrane of thickness corresponding to 1.0g dry
weight of membrane at a pH of 7.0 at a lower concentration range of 200ppm.
34
3 4 5 6 750
55
60
65
70
75
80
85
Met
al A
dso
rpti
on
%
pH
Fig 9: Effect of pH on adsorption of heavy metals
Calibration plot of potentiometric sensing of lead ion using the membrane was
not satisfactory with an average linear regression coefficient 0.78. So further studies
on sensing behavior of the membrane were not carried out.
Results of kinetic study reveal that the linear regression coefficient of second order is
higher than that of first order kinetic model. In pseudo second order model, the
experimental and calculated values are more agreeable to each other(Table.4). This
indicates that second order kinetic model is best model to explain the mechanism of
adsorption of lead ions onto the membrane.(Fig.10,11)
35
Kinetic parameters
Heavy metal
Pb2+
First order kinetics (lagergren’s)
qe (exp)
(mg/l)
0.4861
qe (calc)
(mg/l)
0.1961
K1
(min-1)
0.0184
R2 0.9059
Second order kinetics (Ho’s)
qe (exp)
(mg/l)
0.4982
qe (calc)
(mg/l)
0.5859
K2
(g/mg.min)
0.3484
R2 0.9905
Table 4: Pseudo first order and second order kinetic
parameters
36
Fig 10: Lagergren’s pseudo first order
kinetic model for Pb2+ ions
Fig 11: Ho’s pseudo second order kinetic
model for Pb2+ ions
The distribution of heavy metals between solid and liquid phase was studied using
Langmuir, Freundlich, Dubinin and Temkin isotherm models( Fig: 12-15). From
linear regression coefficient values, it is clear that Langmuir isotherm model is the
better one to explain the adsorption. From the slope and intercept obtained from
graph, monolayer adsorption capacity (qm), separation factor (RL), energy of
adsorption (KL) were calculated. The negative RL values indicates that the adsorption
of heavy metals onto the membrane is a feasible one.
Freundlich isotherm constant n and Kf correspondsing to adsorption intensity
and adsorption capacity are given in (Table.5). Freundlich constant n value smaller
than 1 indicates that the adsorption is a chemical process.
Monolayer adsorption capacity (qs), mean free energy of adsorption (E),
Dubinin isotherm constant (Kd) values were obtained from D-R isotherm plot. Mean
free energy of adsorption of Pb2+ ion is 0.4454, indicates that mechanism of
adsorption is physical in nature.
37
Temkin constant related to heat of adsorption (b) obtained from graph is negative
for Pb2+ ions and reveals that the adsorption of Pb2+ onto the membrane was
endothermic in nature
Table 5: Langmuir, Freundlich, Dubinin, Temkin isotherm parameters
Isotherm parameters
Heavy metal
Pb2+
Langmuir constants
qm (mg/g) 0.3728
KL -0.3761
RL -0.0790
R2 0.9906
Freundlich constants
n -2.7670
KF 1.1863
R2 0.9678
Dubinin isotherm constants
qs 0.4385
Kad -2.5209x10-6
E (KJ/mol) 0.4454
R2 0.8378
Temkin isotherm constants
A (l/g) 6.4904x10-3
B -0.1897
b -13060.4744
R2 0.9827
38
Fig 12: Freundlich isotherm Fig 13: Langmuir isotherm
Fig 14: Dubinin isotherm Fig 15: Temkin isotherm
39
5. Fabrication of Titanium dioxide doped polymer
membrane and its application
5.1 Chemicals used:
Poly vinyl alcohol, carboxymethyl cellullose and maleic acid used for the preparation
of membrane were of analytical grade and was purchased from Alfa aeser. Malachite
green and methylene blue congo red rhodamine blue etc. were from Loba chemie.
Titanium dioxide, was from Merck.
5.2 Preparation of titanium dioxide doped polymer membrane:
Membrane of different compositions were made by mixing poly vinyl alcohol,
carboxymethyl celluose and titanium dioxide, in different proportions. Maleic acid
was added as a cross-linker.
A definite amount of poly vinyl alcohol dissolved in hot water was boiled with
maleic acid in dil.H2SO4. To this carboxymethyl cellulose dissolved in distilled water
was added carefully and heated. Titanium dioxide suspended in distilled water was
then slowly added to the above mixture in drop wise manner and homogenized using
vortex mixer.
Different composition membranes were prepared by mixing different ratios of
the components and it was spin coated on a Table - Top Spin-Coating Unit (Spektron
Instruments). To get thick membranes mutliple layer coating was done. Different
samples were analysed for their dye removing capacities.
5.3 Physico - chemical characterization:
5.3.1 Instrumental Analysis:
Thermal stability (TGA) of PVA- PSSA-ZWP membrane was determined
using NETZSCH STA 449F5 Thermogravimetric analyzer under N2 atmosphere.
Samples were heated up to 900oC at the rate of 30oC/min. IR spectrum of composite
membrane was recorded using agilent cary 630 FTIR spectrometer with KBr pellet
technique.The surface morphology of the PVA-CMC-TiO2 membrane was examined
using scanning electron microscopy.
40
4.3.2. Ion exchange capacity of TiO2 and the membrane:
Ion exchange capacity of TiO2 and PVA-CMC-TiO2 membrane was determined
by titrimetric method as described in Chapter 3.
4.3.3. Degree of swelling:
Degree of swelling of PVA-PSSA-ZPS membrane was measured by immersing
membrane in distilled water at room temperature for 24 hours. The membrane was
then removed, surface water was wiped and subsequently weighed. It was then dried
in an air oven at 55°C and weighed again. Net weight loss (degree of swelling) was
calculated using the expression,
W = x 100
Wdry and Wwet are weight of dry membrane and weight of water absorbed membrane
respectively.
4.3.4.Chemical stability of the membrane:
Chemical stability of PVA-CMC-TiO2 membrane was investigated by soaking the
membrane into different solvents and dilute acid solution for 24 hours at room
temperature.
4.3.5. Dye adsorption studies on the membrane:
Different dyes were made to adsorb on the the membrane and the result was
analysed using UV-Visible spectrophotometer. Effect of contact time, initial feed
concentration, pH and temperature on adsortion of dyes were studied. Kinetic studies
on adsorption were then carried out for the dye that was adsorbed to a greater extend..
5.4 Kinetics and thermodynamics of dye adsorption
Kinetics of membrane adsorption was done by adding the prepared membrane
in 20ml, 10ppm MB and MG dye solutions. Adsorption at different time intervals
were determined. A water bath shaker was used for the purpose. The resulting sample
after the removal of membrane was analysed on UV-Visible spectrophotometer.
Theoretical calculations were done as described in chapter 3. For thermodynamic
studies adsorptions were carried out for different temperature.
41
5.5 Treatment of textile effluent waste using the membrane
Efficiency of the membrane was tested for the treatment of textile effluent
waste collected from the nearby loom unit. The sample dye waste was analysed on
UV- Visible spectrophotometre for its intial concentration.
An effluent treatment column was made, by carefully embedding the
membranes in an ion exchange column. Effluent waste was directly poured onto the
coulmn and the flow at the outlet was maintained at 0.1ml per minute. After the
treatment the eluted waste water was analysed on UV- Visible spectrophotometer.
6. Results and discussion
Fig 16: PVA-CMC-TiO2 Membrane in wet and dry form
Polymer membranes obtained were of different compositions. One sample out
of three showed good dye adsoprtion poperty. The composition ratio for PVA, CMC
and TiO2 for this membrane was 50:20:30 by weight percentage (Fig.16). So this
membrane was used for further analysis.The SEM image of PVA-CMC-TiO2
composites is depicted in (Fig.17). Heterogeneous surface is observed which indicates
good interfacial adhesion between TiO2 and polymer matrix. Aggregation of TiO2
particle on the surface of polymer matrix was also observed.
42
Fig 17: SEM image of PVA-CMC-TiO2 membrane
IR spectrum clearly shows the presence of esteric bonds confirming
crosslinking and it also shows some structural hydroxyl grops are still present where
the exchange takes place(Fig 18). Tg curve shows that three step degradation process
and presence of TiO2 incearses thermal stability to a little extend(Fig.19).
Fig 18: IR spectrum Fig 19: TG curve
It was observed that IEC value of TiO2 was 3.2meqg-1 and that of PVA-CMC-
TiO2 membrane was found to be 6.436 meqg-1. Results show that composite
membrane has high capacity to exchange H+ ions than the inorganic counter part. It
may be due to large number of movable H+ ions as well as high water uptake of
polymer matrix.
The results show that swelling degree of membrane is less as compared to
polymer matrix without TiO2. The percentage degree of swelling of PVA-CMC
membrane was found to be 215% and the TiO2 doped membrane was found to be
186.22 ± 5% . Crosslinking decreased the swelling degree. When crosslinking agent,
maleic acid was added to PVA matrix, esterification reaction occured within the
matrix. Addition of TiO2 to the polymer matrix, reduced the free volume in the blend
and this also decreased the water uptake capacity of the membrane
43
Chemical stability of PVA-CMC-TiO2 membrane was investigated by soaking
the membrane into different solvents and dilute acid solution for 24 hours at room
temperature. Sample did not show any physical change and there was also no
noticeable weight change .
The membrane was found to adsorb malachite green(MG) and methylene blue
(MB)in a very efficient manner. The Fig.20,21 shows the dye content before and after
adsorption on the membrane. Almost complete removal can be noticed distinctly from
the UV-visible spectrum. So further studies were carried out for the adsorption of
these two dyes.
The effect of time on adsorption was investigated. The adsorption of dyes onto
the membrane at different time interval ranging from 10min to 90minute is shown in
(Fig.22) Adsorption initially increased and then reached an equilibrium. Dye
adsorption onto the membrane increased with increase in time. Observation shows
that equilibrium was reached at 90min for MB and 80min for MG by using 10ppm
dye solution. A rapid decolorisation occurred after 50 minutes for MB and after
30min for MG. Percentage of dye removal using PVA-CMC-TiO2 membrane is in the
order of MG > MB.
Fig 20: UV-Visible spectrum of MG
before and after adsorption
Fig 21: UV-Visible spectrum of MB
before and after adsorption
44
Fig 22: Effect of time on dye adsorption
The effect of temperature on dye adsorption on the membrane was conducted at
318K, 328K and 338K using 10ppm dye solutions. Adsorption capacity increased
with increase in temperature. (Fig23) The temperature dependence on adsorption was
measured using van’t Hoff plot. From the slope and intercept, spontaneous nature of
the process was confirmed.
Fig 23: Effect of temperature on dye adsorption on MG and MB
Initial concentration is an important factor in dye adsorption process.
Optimisation studies were done with initial concentration ranging 20ppm to 100ppm.
Observations show that as the initial concentration increased, the dye adsorption also
increased.(Fig 24)
45
Fig 24: Effect of initial concentration on the removal of dyes
pH dependence is also an important parameter in membrane adsorption studies.
The effect of pH on adsorption was studied at pH ranging from 3 to 10. Maximum
adsorption capacity has been observed at pH 6 for MB and pH 10 for MG. In the case
of MB, percentage of dye removal increased initially upto pH 6 and then decreased.
(Fig .25)
Fig 25: Effect of pH on dye adsorption
46
Kinetic studies of membrane adsorption were done by equilibrating the
prepared membranes in 20ml, 10ppm MB and MG dye solutions. Adsorption studies
were carried out at different time intervals. The dye solutions after adsorption were
analysed using U-Vvisible spectrophotometer.( Fig. 26,27)
Results reveal that the second order kinetics and intra-particle diffusion model
are the most fitted ones(Table.6)
Fig 26: Lagergren’s pseudo first order
kinetic model for MB and MG
Fig 27: Ho’s pseudo second order kinetic
mode for MB and MG
Kinetic parameters
MB
MG
First order kinetics
(lagergren’s)
qe (exp)
(mg/l)
1.2693 1.3097
qe (calc)
(mg/l)
0.8991 0.0594
K1
(min-1)
0.0849 0.2796
R2 0.9811 0.9435
47
Table 6: Pseudo first order and second order kinetic parameters
Langmuir, Freundlich, Dubinin and Temkin isotherm models were used to
study the adsorption properties of prepared membrane. From linear regression
coefficient values, it is observed that Langmuir isotherm was the best fitted model for
explaining adsorption of both MB and MG dyes on the surface of PVA-CMC-TiO2
membrane. From slope and intercept obtained from graph, monolayer adsorption
capacity (qm), separation factor (RL), energy of adsorption (KL) were calculated.
Malachite green showed high adsorption capacity than MB. The negative RL values
indicates that the adsorption of dyes on to the membrane is a favourable one.
Freundlich isotherm constant n and Kf corresponding to adsorption intensity
and adsorption capacity resp. are given in(Table.7 ). Freundlich constant n is less than
one and indicates that the adsorption is a chemical process.
Monolayer adsorption capacity (qs), mean free energy of adsorption (E),
Dubinin isotherm constant (Kd)etc. were obtained from D-R isotherm plot shown in .
Mean free energy of adsorption of MB is 3.92 and MG is 5.11 indicating that
mechanism of adsorption is physical in natureFig( 28-31).
Second order kinetics (Ho’s)
qe (exp)
(mg/l)
1.2693 1.3097
qe (calc)
(mg/l)
1.3978 1.3671
K2
(g/mg.min)
0.2055 0.5774
R2 0.9996 0.9999
48
Table 7: Different isotherm parameters
Temkin constant related to heat of adsorption (b) obtained from graph is
negative for MB and MG dyes and it reveals that the adsorption of MB and MG dye
on to the membrane was endothermic in nature.
Isotherm parameters
MB
MG
Langmuir constants
qm(mg/g) 1.0965 1.1578
KL -25.4743 -53.9817
RL -3.9409x10-3 -1.8559x10-3
R2 0.9960 0.9992
Freundlich constants
n -23.5849 -49.5049
KF 1.2167 1.2788
R2 0.8739 0.8732
Dubinin isotherm constants
qs 1.1118 1.1877
Kad -0.0325 -0.0191
E 3.9223 5.1164
R2 0.7966 0.6477
Temkin isotherm constants
A (l/g) 5.9774x10-8 1.7851x10-11
B -0.0716 -0.0494
b -3.4602x104 -5.0153x104
R2 0.8441 0.7716
49
Fig 28: Langmuir isotherm Fig 29: Freundlich isotherm
Fig 30: Dubinin isotherm Fig 31: Temkin isotherm
The spontaneous nature of adsorption onto the membrane was proved by
adsorption thermodynamics. Adsorption studies were carried out at different
temperatures such as 318K, 328K and 338K using 10ppm MB and MG solutions.
Temperature dependence on adsorption constant was obtained from Van’t Hoff plot,
which is given in Fig.32. Table.8 shows the thermodynamic parameters like ∆H°, ∆S°
and ∆G° for adsorption. From the results, it is clear that the positive value of ∆H°
indicates that the adsorption of dyes onto the PVA-CMC-TiO2 membrane is
endothermic. The positive value of ∆S° indicates that the dye molecules adsorbed
50
onto the membrane surface are organised. The ∆G° values were obtained by
substituting the values of ∆H° and ∆S° in Gibbs free energy equation. Here negative
value of ∆G° indicates that adsorption of MB and MG dyes onto the membrane is
spontaneous in nature(Table.8).
Fig 32: Van’t Hoff plot for adsorption of Dyes onto the membrane
DYES
∆H
(J/mol)
∆S
(J/mol.K)
∆G
(KJ/mol)
MB
37.0197
128.3416
-3.8208x104
MG
20.9829
83.8284
-2.4959x104
Table 8: Thermodynamic parameters for the
adsorption of dyes onto the membrane
51
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56
6. List of figures
Fig 1: PVA- PSSA- ZPW Membrane
Fig 2: Spin coating unit with IR currer
Fig 3: XRD data
Fig 4: TG curve
Fig 5: IR spectrum
Fig 6: % removal of various heavy metals
Fig 7: Effect of membrane thickness on adsorption
Fig 8: Effect of initial metal ion concentration on adsorption
Fig 9: Effect of pH on adsorption of heavy metals
Fig 10: Lagergren’s pseudo first order kinetic model for Pb2+ ions
Fig 11: Ho’s pseudo second order kinetic model for Pb2+ ions
Fig 12: Freundlich isotherm
Fig 13: Langmuir isotherm
Fig 14: Dubinin isotherm
Fig 15: Temkin isotherm
Fig 16: PVA-CMC-TiO2 Membrane in wet and dry form
Fig 17: Sem image of PVA-CMC-TiO2 membrane
Fig 18: IR spectrum
Fig 19: TG curve
Fig 20: UV-Visible spectrum of MG before and after adsorption
Fig 21: UV-Visible spectrum of MB before and after adsorption
Fig 22: Effect of time on dye adsorption
Fig 23: Effect of temperature on dye adsorption on MG and MB
Fig 24: Effect of initial concentration on the removal of dyes
Fig 25: Effect of pH on dye adsorption
Fig 26: Lagergren’s pseudo first order kinetic model for MB and MG
Fig 27: Ho’s pseudo second order kinetic mode for MB and MG
Fig 28: Langmuir isotherm
Fig 29: Freundlich isotherm
Fig 30: Dubinin isotherm
Fig 31: Temkin isotherm
Fig 32: Van’t Hoff plot for adsorption of Dyes onto the membrane
57
7. List of tables
Table 1: Preparation conditions and ion exchange capacities of various
samples
Table 2: Effect of temperature on the ion exchange capacity of the exchanger
Table 3: Spin coating parameters and composition of different membrane
samples
Table 4: Pseudo first order and second order kinetic parameters
Table 5: Langmuir, Freundlich, Dubinin, Temkin isotherm parameters
Table 6: Pseudo first order and second order kinetic parameters
Table 7: Different isotherm parameters
Table 8: Thermodynamic parameters for the adsorption of dyes onto the membrane
58
Conclusion
A novel cross linked polyvinyl alcohol-poly styrenesulphonic acid- zirconium
tunstophosphate(ZWP) membrane was prepared by dispersing ZWP gel into PVA-
PSSA blend by spin coating method. It was proved to be an effective adsorbent for the
removal of heavy metal Pb2+ ion from aqueous solutions. The incorporation of
Zirconium tungstophosphate gel into PVA-PSSA blended solution improved the
thermal properties, as well as selectivity of heavy metals towards the membrane.
Characterisation of membranes was done by XRD, FTIR, TGA etc. Adsorption
studies were carried out by batch adsorption process. Effect of pH, contact time,
initial concentration etc. were studied. It showed maximum selectivity towards lead
ion .Optimisation studies of membrane adsorption for Pb2+ shows that an effective
adsorption can be attained by a membrane of thickness corresponding to 1.0g dry
weight of membrane at a pH of 7.0 at a lower concentration range of 200ppm. Kinetic
studies were used to explain the mechanism of adsorption process. Pseudo second
order kinetic model and Langmuir isotherm models are more fitted. Potentiometric
lead ion sensing was tested on ion selective electrode fabricated using the membrane.
A new polymeric membrane doped with titaniun dioxide was also prepared.
Instrumental characterization like TGA, XRD, SEM etc. were done. The new polymer
matrix was polyvinyl alcohol and carboxymethyl cellulose. Ion exchange properties,
degree of swelling and dye adsorption studies were carried out. The membrane was
found to adsorb malachite green (MG) and methylene blue (MB) in a very efficient
manner. The effect of different parameters on adsorption was investigated.
Observation shows that equilibrium was reached at 90min for MB and 80min for MG
by using 10ppm dye solution. A rapid decolorisation occurred after 50 minutes for
MB and after 30min for MG. Percentage of dye removal using PVA-CMC-TiO2
membrane was found to be in the order of MG > MB. Kinetic and thermodynamic
studies were carried out. Langmuir, Freundlich, Dubinin and Temkin isotherm etc.
were the theoretical models used. The negative value of ∆G° indicates that adsorption
of MB and MG dyes onto the membrane is spontaneous in nature. Effective dye
removal was also done with textile effluent waste.
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