1. Introduction
The development of polymeric sorption materials, in which the natural polysaccharide chitosan is used as a matrix, is a rapidly developing field in the adsorption science. One of the attractive features of chitosan is that it can be used in adsorption processes in various physical forms, such as flakes, powders, nanoparticles, granules, membranes, and fibers/hollow fibers. To improve the mechanical properties and adsorption capacity, or even to prevent dissolution in acid medium of chitosan, numerous studies have been devoted to the chemical modification of chitosan by cross-linking or grafting with different polyfunctional agents [
1,
2,
3]. Besides this, chitosan is used as a component of composite or hybrid materials with various inorganic substances or compounds [
4]. In such composites, chitosan can be deposited on the surface of a porous material to provide high specific surface area and allow for better availability of active amino groups, improve mechanical properties, and thus optimize the efficiency of the target component uptake from the solution. In another approach, the inorganic component can be introduced into the chitosan solution, and a sorption material can then be obtained from the resulting mixture by known methods [
5,
6]. The most attractive method of composite fabrication is based on in situ formation of an inorganic component during chitosan precipitation [
7]. In this case, a more homogeneous distribution of the inorganic ion exchanger in the polymer matrix is observed. In addition, chitosan can be used as a template for the fabrication of uniformly sized nanoparticles of metal oxides (for example, iron) for a broad range of applications, including sorption [
8,
9]. The use of oxide powders without a polymer matrix is associated with a number of problems, such as low mechanical strength and small particle size, which complicates subsequent separation of the sorbent from the solution, as well as high hydrodynamic resistance when used under dynamic conditions in sorption columns. However, the fabrication of mechanically strong composite materials offers a good solution to these problems.
Chitosan-based hybrid materials are becoming a promising alternative to conventional adsorbents and are used in water treatment and purification processes to remove such toxic pollutants as heavy metals, arsenic, radioactive contaminants, and organic impurities [
3,
5,
6]. Natural clays, zeolites, perlite [
5], and various metal oxides, which are traditional inorganic adsorbents for many pollutants, are used as inorganic components for composite fabrication. Miller and colleagues proposed a TiO
2-impregnated chitosan as a sorbent for arsenic removal, which was obtained by adding anatase nanoparticles into chitosan solution followed by precipitation of sorbent granules in NaOH solution [
10,
11]. The composite sorbent Al
2O
3/chitosan for arsenic uptake was fabricated by mixing a gel of chitosan and aluminum oxide with subsequent treatment of the paste with alkali [
12]. Composite sorbents for As(III) and As(V) obtained by depositing iron oxides on chitosan flakes or in the form of chitosan granules containing oxide were reported in [
13].
Iron oxides are universal sorbents for many pollutants, including radionuclides. The most attractive type of such sorbents comprises magnetic sorbents, including magnetic chitosan-containing composites [
6,
7]. The use of such sorbents for metal ion uptake allows combining the purification process with that of the sorbent magnetic separation.
The uptake of uranium using chitosan and chitosan-based materials is known to be considered as one of the most important applications of chitosan [
14]. This also includes the fabrication of a variety of magnetic chitosan resins for uranium sorption [
15,
16,
17,
18,
19]. In magnetic sorbents, chitosan plays a special role. Magnetic nanoparticles are highly chemically active and easily oxidized in air, which leads to a loss of magnetic properties and a decrease in the degree of dispersity. When magnetic particles are coated with chitosan, not only does their susceptibility to oxidation decrease (increasing the shelf-life of the sorbents), but also their tendency to aggregation [
7]. Interestingly, magnetic chitosan-based sorbents can be further modified via the introduction of specific functional groups to enhance the selectivity or via polymer cross-linking to improve the mechanical properties or prevent solubility in acidic media [
15,
16,
17,
18,
19].
In order to remove hazardous cesium and strontium radionuclides, in addition to uranium, composite chitosan-based sorbents can be obtained. Chitosan poorly adsorbs alkali and alkali earth metals [
14]; therefore, chitosan loaded with transition metal ferrocyanides selective to cesium is used to remove cesium radionuclides [
20,
21]. Sorbents containing iron oxide [
22], including those embedded in the chitosan matrix [
23], are considered as sorbents for strontium.
The present work was aimed at the development of methods of fabrication of composite sorbents based on iron oxides homogeneously distributed in a chitosan matrix and the investigation of their sorption performance for the removal of strontium ions from highly diluted solutions.
2. Materials and Methods
Chitosan was purchased from JSC “Vostok-Bor” (Dalnegorsk, Russia); the degree of acetylation was 0.25, and the viscosity-averaged molecular weight was 250 kDa. Iron(III) chloride (FeCl3 × 6H2O), iron(II) sulphate (FeSO4 × 7H2O), ammonium hydroxide (NH4OH), hydrochloric acid (HCl), strontium (stable) chloride (SrCl2 × 6H2O), and sodium hydroxide (NaOH) were purchased from Nevareaktiv (Saint Petersburg, Russia). All chemicals were of analytical grade and were used as received without further purification.
Nonmagnetic sorbents were obtained via addition of the solutions of Fe(III) salt into a 1% solution of chitosan (in 0.1 M HCl) at the Fe/chitosan ratios 1:1, 2:1, and 4:1 (g/g)—amorphous sorbents 1A, 2A, and 3A, respectively. The NH4OH solution was added to the obtained mixture until neutral reaction. Magnetic sorbents were obtained via addition of the mixture of solutions of Fe(III) and Fe(II) salts (molar ratio 1:2) into a 1% solution of chitosan (in 0.1 M HCl) at the Fe/chitosan ratio 1:1 (g/g). The NH4OH solution was added to the obtained mixture until weakly alkaline reaction, pH 8–9 (sorbent 2M), or neutral reaction, pH 7.0 ± 0.5 (sorbent 3M). A magnetic powder of iron oxide (Fe3O4) (sorbent 1M) without chitosan was obtained via addition of NH4OH solution to the mixture of the solutions of Fe(II) and Fe(III) salts (ratio 2:1 mol/mol) until neutral reaction. Precipitates were washed with distilled water, dried, and calcined at 105 °C for 1 h.
The morphology of the composite materials and distribution of the inorganic component in the bulk were investigated using a Lyra3 XMH (Tescan, Brno, Czech Republic) scanning electron microscope equipped with an AZtecEnergy energy dispersive X-ray (EDX) microanalyzer automated with an X-Max80 detector (Oxford Instruments, Abingdon, UK). X-ray diffraction (XRD) analysis was carried out using a SmartLab diffractometer (Rigaku, Tokyo, Japan) with Cu Kα radiation in the 2θ range from 2° to 80°.
The efficacy of
90Sr uptake was studied in tap water at a sorbent/liquid ratio of 1:1000 g/mL. Air-dried sorbent with a bead size of 0.1–0.2 mm was added to tap water (pH 6.5) spiked with
90Sr radionuclide with an initial activity of 800 Bq/mL. After 7 days, the solution was separated from the sorbent and filtered through blue ribbon filter paper with a pore size of 3 µm, and the equilibrium activity was measured using a Tri-Carb 2910TR liquid scintillation alfa, beta-spectrometer (Perkin Elmer, Waltham, MA, USA). Isotherms of Sr
2+ sorption on virgin Fe
3O
4 and magnetic sorbent 3M without spiking with
90Sr at a sorbent/liquid ratio of 1:1000 (g/mL) were determined. The equilibrium strontium concentration was determined after 7 days by atomic absorption spectrometry (AAS) using a Solaar M6 spectrometer (Thermo, Waltham, MA, USA). The sorption isotherms were fitted with Freundlich (Equation (1)) and Langmuir (Equation (2)) models using SciDAVis software (version 1.23; [
24]):
where
Gmax is the maximum sorption capacity (mg/g),
C is the equilibrium concentration of Sr (mg/L),
Kf is the Freundlich constant,
Kl is the Langmuir constant, and
n is the coefficient related to the heterogeneity of the sorption centers.
The efficiency of the
90Sr uptake with different sorption materials was estimated via distribution coefficients calculated using Equation (3):
where
Kd is the distribution coefficient of
90Sr (mL/g);
A0 and
A1 are the initial and equilibrium activities of the spiked tap water (Bq/mL), respectively;
V is the volume of spiked tap water; and
m is the weight of the sorbent (g).
90Sr kinetic curves were obtained using tap water spiked with a radionuclide at a V/m ratio of 1000 mL/g. The sorption value was calculated according to Equation (4):
where
A0 and
A1 are the initial and equilibrium activities of the spiked tap water (Bq/mL), respectively.
The zero charge point (pH
PZC) of the sorbent was determined by a static method as follows: a quantity of 0.2 g of the sorbent was immersed into 0.1 M NaCl solutions with different pH values. The initial pH value was maintained by the addition of 0.05 M NaOH and HCl solutions. Sorbents were equilibrated under constant stirring for 36 h, then separated by filtration, and the equilibrium pH value was measured. The pH
PZC was assigned to the pH value corresponding to the horizontal inflection on the curve showing dependence of equilibrium pH on initial pH values [
25]. The mechanical strength of sorbents was studied under dynamic conditions when passing 5 L of tap water at a flow rate of 75 mL/h through a column diameter of 10 mm, with sorbent volume of 1 mL and granulation of 0.1–0.2 mm. After water passing, the material was dried until constant weight at 105 °C and sieved again, and the weight of sorbent particles of sizes less than 0.1 mm was estimated.
The specific surface area was measured by low-temperature N2 sorption at 77 K using an Autosorb iQ automated sorption analyzer (Quantachrome Instruments, Boynton Beach, FL, USA). Prior to the experiment, samples were degassed at 105 °C for 6 h. The specific surface area was calculated via the Brunauer–Emmett–Teller (BET) method.
4. Discussion
Investigations of the composite sorbents’ morphology revealed that beads of the 3M sorbent calcined at 105 °C have denser monolithic structure compared to the 2M sorbent (
Figure 1b,c). The layers observed in the SEM image of the 2M sorbent determine a more porous structure of this composite. To confirm this fact, the specific surface area of the composites was measured and was found to be 39.7, 58.9, and 14.8 m
2/g for samples 1A, 2M, and 3M, respectively. In terms of texture and morphology, the amorphous 1A composite is more similar to the 3M sorbent (
Figure 1a). According to the SEM–EDX mapping (
Figure 1), the proposed method of composite sorbent fabrication, in which precipitation of iron oxides occurs simultaneously with the precipitation of chitosan, yields hybrid materials with an active inorganic phase homogeneously distributed in the polymer matrix.
According to the XRD data, precipitation of iron oxides with ammonia solutions from the mixture of Fe(III) and Fe(II) salts yields precipitates which after calcination at 105 °C have nearly the same composition, regardless of the chitosan presence (
Figure 2a). Goethite, hematite, maghemite, and possibly magnetite were found in the composition of sorbents. During the precipitation of the Fe(III) salt with a solution of NH
4OH, amorphous Fe(III) oxide/hydroxide was formed. As a result, the 3M composite presented the best magnetization and was therefore easier to separate from the solution by magnetic separation compared to the 2M composite. Noteworthy, heating of chitosan up to 110 °C did not lead to changes in its crystalline structure. Instead, when precipitated together with iron oxides, amorphization of the polymer occured in the composite.
Investigations of the
90Sr uptake from tap water by magnetic and nonmagnetic amorphous composites in comparison with Fe
3O
4 powder showed that virgin Fe
3O
4 and amorphous composite 1A are the most effective sorbents (
Table 1). The high sorption efficiency of these materials can be explained by the sorbent gradual dispergation during the adsorption tests with stirring, which increased the sorbent specific surface area and simplified the access to the sorption centers. In the case of Fe
3O
4, the sorbent degradation showed a mechanical character and was accompanied by the formation of smaller particles which, however, could be separated from the solution on a cellulose filter with a pore size of 3 μm. The destruction of the composite sorbent 1A presented a different nature and was associated with the hydrolysis and formation of small flakes of brown or orange color and poorly filterable colloidal particles, probably of Fe(OH)
3, leading to visually detectable opalescence of the solution. The destruction of the sorbent 1A occured at pH 6.17 and above (
Figure 5) which limited the application of this material despite the highest value of the distribution coefficient (
Table 1). The surface of iron oxide showed a pH
PZC in the region close to neutral pH, suggesting that hydrolysis in alkaline solutions contributes to a negative surface charge. Therefore, more efficient sorption of Sr
2+ ions is observed in alkaline solutions [
22]. An increase of inorganic phase content in the nonmagnetic composite sorbents (2A, 3A) (
Table 1) lead to a noticeable intensification of the destruction process due to hydrolysis and release of
90Sr in the pseudocolloid state (sorbed on unfilterable colloidal particles of the partially degraded composite). This resulted in a poor sorption performance of composites with the increase of the inorganic phase content in a series from 1A to 3A (
Table 1). In the process of testing the strength of the sorbents, it was found that 6.6% of the magnetic powder (1M) is destroyed under experimental conditions compared to the destruction of 2.4% of composite sorbent 3M and 0.5% of 2M.
Based on the kinetics of the process of sorption during the removal of microconcentrations of
90Sr, the time of attainment of the sorption equilibrium under static conditions was 5 h for the sorbents 1A and 3M. For the sorbent 1M, this time was 15 h (
Figure 5).
Although the distribution coefficient for
90Sr on the magnetic 3M composite is somewhat lower compared to the best of nonmagnetic amorphous composite 1A (
Table 1), it showed significantly high sorption capacity toward Sr
2+ ions (
Figure 3). The parameters of the Langmuir model, which provides the most accurate fit to the experimental data of Sr
2+ sorption isotherms, showed that the 3M sorbent has high affinity toward Sr
2+ ions as well (
Table 2). A comparison of the Langmuir constants and the maximum sorption capacities of the virgin Fe
3O
4 and the 3M composite (
Table 2), taking into account the content of the inorganic phase in the 3M sorbent, allows for the conclusion that the fabrication method of the 3M composite preserves the sorption characteristics of iron oxide but provides a material with better stability in solution.