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Author's personal copy
Chemical Physics Letters 591 (2014) 161–165
Contents lists available at ScienceDirect
Chemical Physics Letters
journal homepage: www.elsevier.com/locate/cplett
Exploiting the ion-exchange ability of titanate nanotubes in a model
water softening process
Dániel Madarász a, Imre Szenti a, András Sápi a, János Halász a, Ákos Kukovecz a,b, Zoltán Kónya a,c,⇑
a
Department of Applied and Environmental Chemistry, University of Szeged, Rerrich Béla tér 1, Szeged H-6720, Hungary
MTA-SZTE ‘Lendület’ Porous Nanocomposites Research Group, Rerrich Béla tér 1, Szeged H-6720, Hungary
c
MTA-SZTE Reaction Kinetics and Surface Chemistry Research Group, Rerrich Béla tér 1, Szeged H-6720, Hungary
b
a r t i c l e
i n f o
Article history:
Received 19 September 2013
In final form 8 November 2013
Available online 21 November 2013
a b s t r a c t
Titanate nanotubes were utilized in Ca2+ and Mg2+ removal in a continuous ion-exchange unit. Three consecutive water softening–regeneration cycles were performed. The highest measured value of the total
ion-exchange capacity was 1.2 mmol g 1 which decreased to 0.66 mmol g 1 in the third cycle. The capacity loss was due to the irreversible binding of Ca2+ ions to very strong adsorption sites, while the Mg2+/Na+
exchange was reversible. A relatively fast initial adsorption step and a subsequent slower concentration
decrease were the two processes that governed the kinetics of the ion exchange reaction.
Ó 2013 Elsevier B.V. All rights reserved.
1. Introduction
Removal of unwanted ions from drinking, industrial, waste and
other types of water is an integral part of technology planning and
design. It is also the main topic for several studies focused on
‘green’ processing. Large bodies of surface and groundwaters polluted with heavy ions and radioactive materials are still in need
of remediation and purification worldwide. For instance, the
2011 earthquake-induced nuclear disaster in Fukushima, Japan resulted in millions of tons of seawater getting polluted with radioactive materials such as 137Cs which has spread all over the world
since then.
Softened water is a basic requirement for several technological
and domestic applications. Ca2+ and Mg2+ ions cause water hardness and are directly responsible for scale and other unwanted precipitate formation as well as for the deterioration of the efficiency
of detergents (e.g. soap). Scale can plug pipelines, reduce the heat
transfer efficiency in cooling or heating applications and may lead
to furnace or boiler blasting. Several types of water softening processes such as ion exchange, evaporation, precipitation, ultrafiltration, nanofiltration and electrodeionization are used today [1–4].
Among them, ion exchange is popular due to its ease of operation
and high ‘hard’ ion removal efficiency [3].
Materials in the nanometer scale are extensively researched in
ion removal and adsorbent applications because of their large specific surface area and other potentially beneficial properties such as
special morphologies and controllable size distributions. Carbon
nanotubes have great potential in water treatment and environ⇑ Corresponding author at: Department of Applied and Environmental Chemistry,
University of Szeged, Rerrich Béla tér 1, Szeged H-6720, Hungary.
E-mail address: konya@chem.u-szeged.hu (Z. Kónya).
0009-2614/$ - see front matter Ó 2013 Elsevier B.V. All rights reserved.
http://dx.doi.org/10.1016/j.cplett.2013.11.021
mental protection [5–9] because of the many possibilities they offer for surface modification [10–14]. This resulted in the synthesis
of carbon nanotube based specific adsorbents and ion exchangers
capable of removing unwanted ions from water. Zero dimensional
metal-oxide nanoparticles provide superior adsorption kinetics for
the removal of metal ions from aqueous solutions [15,16]. By using
magnetic iron oxide nanoparticles, the effective remediation can
even be combined with a straightforward solid–liquid separation
process [17,18].
Titanate nanotubes (TiONTs) are also promising ion exchanger
material candidates. These one-dimensional nanomaterials have
a ‘rolled-up’ layered structure [19]. The layers are made of TiO6
octahedrons resulting in a negatively charged nanotube skeleton
in which the charge is compensated by cations located in ion exchange positions on the nanotube surface, at the tips and in between the layers [20]. These cations are mobile which endows
TiONTs with cation exchange properties resulting in a new type
of ionexchanger material with considerable application potential
[21,22]. Expecting a stoichiometric reaction (Na2Ti3O7 + M2+
M MTi3O7 + 2Na+), the theoretical maximum ion-exchange capacity of TiONTs is approximately 2.9 mmol g 1 for bivalent cations
(taking into account the 10 w% water content of TiONTs).
In the present study, our aim was to exploit the ion exchange
properties of titanate nanotubes in a model water softening process. Hard water containing Ca2+ and Mg2+ ions was softened in a
continuous operation fixed-bed column. Sodium chloride based
regeneration was applied between softening cycles. The concentration of ‘hard’ ions was monitored by classical analytical methods
and thus the ion exchange capacity was determined. An independent ion adsorption kinetic study was performed to facilitate the
understanding of the behavior of titanate nanotubes in the ion exchange process.
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2. Experimental
3. Results and discussion
2.1. Synthesis and characterization
3.1. Ion exchange capacity
Titanate nanotubes were synthesized by a simple alkali hydrothermal method as described previously [23–25]. Briefly, the preparation was performed by the alkaline recrystallization of anatase
TiO2. 70 g of TiO2 (Sigma–Aldrich) was mixed with 1 L 10 M aqueous NaOH (Molar) solution under intensive stirring until a white
suspension was obtained, then the suspension was aged in a
closed, cylindrical, PTFE-lined autoclave at 125 °C for 48 h. The
product was washed with 0.1 M HCl (Molar) solution and deionized water to reach neutral pH. The slurry was filtered and dried
in air at 60 °C. The obtained material was characterized by transmission electron microscopy (TEM, Philips CM10, 100 kV) and Xray diffractometry (XRD, RigakuMiniflex2, CuKa). The specific
surface area was determined from nitrogen adsorption measurements performed at 77 K in a Quantachrome Nova 3000e instrument and analyzed by the BET method. Artificial hard water was
made of analytical grade Mg(NO3)2 6H2O (Reanal) and CaCl2 2H2O (Reanal).
The elemental composition of the titanate nanotubes was analyzed by energy dispersive X-ray spectroscopy (Röntec Quantax2
EDS) built into a Hitachi S-4700 Type II cold field emission scanning electron microscope. Samples were drop-casted from alcoholic suspension onto silicon wafers and measured at 10 kV
accelerating voltage without any additional coating.
TEM images of the initial TiO2 (anatase) material show the presence of isotropic nanoparticles with a diameter of 50–130 nm (Figure 1A). In contrast, the as-synthesized titanate nanotubes
(TiONTs) are open-ended hollow tubular objects measuring 100–
150 nm in length and 6–10 nm in diameter (Figure 1B). A typical
titanate nanotube has 4 walls and approximately 0.73 nm interlayer spacing.
The synthesized white, powder-like material was identified as
sodium–hydrogen–trititanate (NaxH2 xTi3O7) by XRD (Figure 1C).
Weak and broadened reflections indicate that the material is of
lower crystallinity compared to the initial anatase material. Peaks
marked as ‘A’ and ‘T’ are characteristic of the anatase and trititanate structures, respectively. The specific surface area of titanate
nanotubes is 185 m2 g 1 because of their tubular morphology
and readily accessible inner channel surface.
The schematics of the apparatus used in the actual water softening experiments is presented in Figure 2A, whereas Figure 2B depicts the breakthrough curves of the first cycle of the TiONT based
water softening process. The total hardness (Ca2+ + Mg2+ ions) and
the individual Ca2+ and Mg2+ ion concentrations measured at the
column outlet are presented. The column was totally exhausted
after pumping 6.3 L hard water through it as described above.
The ion exchange capacity calculated from the breakthrough curve
is 1.2 mmol g 1, which is approximately 41% of the theoretical
maximum TiONT ion exchange capacity. It is interesting to note
that while the Mg2+ ion concentration in the effluent increased rapidly at the beginning of the process, the Ca2+ ion concentration was
much slower to converge to its final value. The Mg2+ breakthrough
curve features a characteristic local maximum at about 25% of total
time on stream and the magnesium concentration in the effluent at
this maximum is actually higher than in the feed. This apparent
contradiction can be explained by assuming that Mg2+ ions initially
captured by the TiONTs are eluted by the more preferred Ca2+ ions
at this stage (Nagy et al., 1998). The reason behind this is the ion
adsorption competition of the different ions with different effective nuclear charges, adherent hydrospheres and hydration energies. The ion radii of hydrated Ca2+ and Mg2+ ions are 0.30 nm
and 0.34 nm, respectively. The smaller ion radius facilitates Ca2+
migration into the layers of the trititanate structure. Moreover,
the hydrated Ca2+ and Mg2+ ions must strip their hydrate shells
in order to occupy TiONT ion exchange positions. Therefore, hydration energy affects selectivity: the lower the hydration energy, the
higher the ion exchange affinity [26]. The hydration energy of Ca2+
and Mg2+ is 1592.4 kJ mol 1 and 1922.1 kJ mol 1, respectively. In
summary, smaller ion radius and lower hydration energy of Ca2+
result in the long-term preferential adsorption of Ca2+ ions against
Mg2+ on titanate nanotubes.
The total ion exchange capacity of the TiONT column decreased
gradually during the first three consecutive softening–regeneration cycles (Figure 3A). The ion exchange capacity dropped from
1.2 mmol g 1 to 0.89 mmol g 1 in the second cycle and then further to 0.66 mmol g 1 in the third one, corresponding to 41%,
30% and 22% of the theoretical maximum ion exchange capacity,
respectively. The ion exchange capacities are smaller than that of
the reference DOWEX-50W resin (2.33 mmol g 1). The detailed
analysis of the individual ion exchange curves depicted in Figure 3B
and C revealed that the loss of total ion exchange capacity was almost exclusively due to the loss of Ca2+ sorption capacity. The Ca2+
breakthrough curves have shifted systematically to the left with
each cycle. The Ca2+ sorption capacity of the TiONT bed dropped
from 0.92 mmol g 1 to 0.64 mmol g 1 and then to 0.45 mmol g 1.
2.2. Ion exchange experiments
TiONT-based water softening experiments were performed in a
continuous flow fixed bed apparatus (Figure 2A) at room temperature. The ion exchange bed contained 12 g TiONTs. In order to
achieve a well-defined starting condition, the TiONT bed was treated with 4 L of 2.56 M NaCl solution and rinsed with 1 L 0.05 M
NaCl solution before the water softening process. In the actual
experiment, artificial hard water with a total hardness of
60 GH° (0.01 M) and a Ca2+:Mg2+ ion ratio of 1:1 was pumped
through the reactor with a feeding rate of 1.6 L h 1 until chemical
analysis indicated that the column was exhausted. The TiONT bed
was then regenerated by repeating the NaCl solution treatment described above. Three softening–regeneration cycles were performed. For comparison, the water softening process was also
carried out on a commercial DOWEX-50 W ion-exchange resin as
a reference.
The hardness of the water at the column outlet was monitored
by chelatometric titration in every 20 min. Firstly, 2 mL 10w%
aqueous NaOH solution was added to 100 mL of water sample to
mask the Mg2+ ions. The Ca2+ ion concentration was then determined using murexide (Reanal) indicator and EDTA (Reanal) solution. After reaching the equivalence point, 3 mL of 20 w% HCl
solution and 6 mL 25 w% of NH4OH solution were added to the titrated sample and the solution was titrated further using eriochrome black T (Reanal) indicator to measure the Mg2+ ion
concentration.
In the ion adsorption kinetic investigation, 3–3 g of NaCl solution pretreated TiONT was suspended in 600 mL of 60 GH° hard
water as well as in 600–600 mL 50 GH° (0.009 M) Ca2+ and
Mg2+ solution under vigorous stirring. The mixtures were sampled
at regular intervals during the course of the 164 h long experiments. The solutions was separated from the TiONTs by centrifugation and the samples were analyzed for Ca2+ and Mg2+ by
chelatometry as described above (the centrifuged titanate nanotubes were reintroduced into the mixture).
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163
Figure 1. Typical TEM images of the initial titanium-dioxide (anatase) (A), as-synthesized titanate nanotubes (B) and the corresponding XRD patterns (C).
Figure 2. Schematic view of the TiONT-based water softening apparatus (A) and breakthrough curve of the first cycle of the hardness removal process (B).
Figure 3. Total hardness (A), Ca2+ ion (B) and Mg2+ ion (C) concentration breakthrough curves measured in three consecutive softening–regeneration cycles. The cycle
number is indicated in the curve tag.
On the other hand, Mg2+ ion breakthrough curves have suffered
significantly less changes during the repetitions, corresponding to
Mg2+ sorption capacities of 0.28 mmol g 1, 0.26 mmol g 1 and
0.21 mmol g 1 in the three consecutive softening–regeneration cy-
cles, respectively. This indicates that the Mg2+ ion capacity of a
TiONT bed is almost constant but the Ca2+ ion bonding ability of
the TiONT-based ion exchanger deteriorates with time under the
used softening–regeneration parameters.
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Table 1
EDS derived alkaline element content of TiONT after subsequent softening and
regeneration cycles.
A (at.%)/Ti (at.%) 100
Softening cycles
Sodium
Magnesium
Calcium
Regeneration cycles
1
2
3
1
2
3
7.4
4.8
9.4
6.1
5.3
11.3
8.0
5.6
12.3
23.7
–
4.5
24.1
–
7.7
24.6
4.3
7.3
The energy dispersive X-ray analysis (EDS) of the TiONT water
softening cartridge after the first exhaustion revealed the presence
of adsorbed magnesium and calcium as well as sodium, titanium
and oxygen which are attributed to the pristine TiONT material
(the sign of the Si is attributed to the sample holder) (Table 1, Figure 4A). No significant change in the crystal structure of titanate
nanotubes could be observed by XRD (not shown here). The higher
amount of calcium compared to magnesium in the sample confirms the stronger Ca2+ ion bonding affinity of TiONT. The more
favorable adsorption of Ca2+ ions in the TiONT-based ion exchange
is similar to the behavior of zeotype materials and ion exchange
resins in such ion adsorption processes [27–30]. The remnant sodium content of the sample is attributed to Na+ ions bonded to
inaccessible cation positions found deep within the nanotube
walls. After regeneration, the increased sodium content can be
attributed to the elution of hard ions and their replacement by
Na+ (Figure 4B). The EDS profile of the regenerated sample reveals
the presence of calcium but the lack of magnesium. This finding
agrees well with the observed gradual loss of calcium and preservation of magnesium ion exchange capacity and indicates that calcium is more strongly bonded to the adsorption sites of TiONTs.
3.2. Ion exchange kinetics
The adsorption of both Ca2+ and Mg2+ on TiONTs was studied as
a function of time in order to gain insight into the adsorption kinetics of these ions on anisotropic titanate nanostructures. Adsorption
experiments were carried out from the individual solutions of Ca
and Mg salts and from the mixture of the hard ions as well. The
concentration of the cations was monitored after titanate nanotubes were introduced to the solutions under vigorous stirring.
The change of the concentrations during time is nearly identical
in every case (Figure 5). Bivalent ion concentration in the artificially hardened water and in the individual hard ion solutions
was reduced rapidly after introducing the TiONTs. The ‘hard’ ion
concentration was almost halved in the first 5 h of the ion exchange process. Afterwards, the ion adsorption slowed down.
These results correlate well with literature findings. Bavykin and
Walsh studied the ion exchange kinetics of the Li+/TiONT system
by monitoring the changes in pH after adding LiOH solution into
the suspension of protonated TiONT. After introducing the LiOH
solution to the suspension the pH reached a maximum value, then
dropped quickly again because of the Li+/H+ ion exchange. After the
rapid initial reaction the ion exchange process slowed down and
was completed in a few tens of minutes in the applied reaction
environment [21]. Wang et al. also report a rapid initial reaction
between Cu2+ and TiONT which slowed down and reached equilibrium after a few hours [31].
In the cases of Ca2+ and Mg2+ the alkaline ion concentrations of
the solutions decreased rapidly first and much slower afterwards
(Figure 5A). In the first 20 min the Ca2+ ion concentration in the
solution was decreasing with a rate of 2.31 mmol g 1 h 1, while
the decreasing rate of Mg2+ was smaller: 1.79 mmol g 1 h 1 (Table 2) which rates degreased further. After 48 h of TiONT exposure
the ion concentration in the Ca2+ solution became almost constant
(0.001 mmol g 1 h 1) and constant in the Mg2+ solution. In case
of artificial hard water (mixture of Ca2+ and Mg2+ solutions with
60 GH° and 1:1 M ratio of hard ions) the higher affinity of TiONT
to Ca2+ against Mg2+ was also observed (Figure 5B). The adsorption
speed of Ca2+ was much higher than that of Mg2+, 1.83 mmol g 1
h 1 and 0.79 mmol g 1 h 1, respectively, in the first 20 min. Afterward, these rates were decreased further as well as in case of individual Ca2+ and Mg2+ solutions (Table 2). In addition, the total ion
exchange capacity was calculated to 1.73 mmol g 1, which splits to
1.02 mmol g 1 Ca2+ and 0.71 mmol g 1 Mg2+ ion bonding capacities. We suggest that the first rapid ion exchange step is related
to ion binding to easily accessible sites located at the tips as well
as the inner and outer cylindrical tube surfaces of the titanate
nanotubes (Figure 6). On the other hand, the subsequent slow
ion exchange process originates from ion binding to less accessible
adsorption sites within the wall-forming layers. The high activation energy of ion migration from and into the interlayer spacing
is responsible for the slow ion exchange process.
These data confirm that the adsorption of calcium is thermodynamically preferred over magnesium because of its smaller ion radius and lower hydration energy. Therefore, Ca2+ gradually
replaces the initially adsorbed magnesium ions which are released
into the effluent. The local Mg2+ concentration maximum observed
in Figure 2B is due to the temporal overlapping of this magnesium
release from the TiONTs and the default magnesium concentration
of the feed at the column outlet.
The amount of ‘easily accessible sites’ of TiONTs was calculated
considering a typical TiONT (125 nm length, 8 nm outer diameter,
4 layers with 0.73 nm interlayer distance, hypothesized as 4 coaxial cylindrical tubes for simplification) taking into account only the
external surfaces of outer walls, the inner surfaces of the inner
Figure 4. EDS spectra of TiONT after the first softening (A) and subsequent regeneration (B) cycle.
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D. Madarász et al. / Chemical Physics Letters 591 (2014) 161–165
165
Figure 5. Kinetics of the Ca2+ and Mg2+ ion adsorption process on titanate nanotubes from Ca and Mg solution (A) and from Ca + Mg solution (B) – lines are drawn to guide the
eye.
Table 2
Speed of the ion exchange process on TiONTs as a function of time.
Period
Speed of ion exchange
(mmol g 1 h 1)
Individually
0–20 min
20–120 min
2–48 h
48–168 h
Mixed
Ca
Mg
Ca
Mg
Ca + Mg
2.313
0.133
0.008
0.001
1.794
0.153
0
0
1.831
0.129
0.005
0.001
0.792
0.110
0.002
0
2.623
0.239
0.007
0.001
experimental parameters can be attributed to the strong interaction between Ca2+ ions and calcium-selective adsorption sites.
Although more detailed studies are necessary to exactly identify
these sites in the nanotube framework, it is clear that this irreversible bonding could be exploited in e.g. radioactive (or any other unwanted) ion removal and safe storage in the future.
Acknowledgements
The financial support of the TÁMOP-4.2.2.A-11/1/KONV-20120047 and OTKA K 83889 projects is acknowledged.
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Figure 6. Simplified model of TiONT, location of easy accessible sites (green) and
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