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. 2021 Dec 2;16(2):33–48. doi: 10.1049/nbt2.12074

Fabrication of superparamagnetic adsorbent based on layered double hydroxide as effective nanoadsorbent for removal of Sb (III) from water samples

Rokhsareh Motallebi 1, Ali Moghimi 1,, Hamidreza Shahbazi 1, Hakim Faraji 1
PMCID: PMC8918918  PMID: 34854558

Abstract

In this study, the superparamagnetic adsorbent as Fe@Mg‐Al LDH was synthesised by different methods with two steps for the removal of heavy metal ions from water samples. An easy, practical, economical, and replicable method was introduced to remove water contaminants, including heavy ions from aquatic environments. Moreover, the structure of superparamagnetic adsorbent was investigated by various methods including Fourier transform infrared spectroscopy, field emission scanning electron microscopy, energy‐dispersive X‐ray spectroscopy, and vibrating sample magnetometer. For better separation, ethylenediaminetetraacetic acid ligand was used, forming a complex with antimony ions to create suitable conditions for the removal of these ions. Cadmium and antimony ions were studied by floatation in aqueous environments with this superparamagnetic adsorbent owing to effective factors such as pH, amount of superparamagnetic adsorbent, contact time, sample temperature, volume, and ligand concentration. The model of Freundlich, Langmuir, and Temkin isotherms was studied to qualitatively evaluate the adsorption of antimony ions by the superparamagnetic adsorbent. The value of loaded antimony metal ions with Fe@Mg‐Al LDH was resulted at 160.15 mg/g. The standard deviation value in this procedure was found at 7.92%. The desorption volume of antimony metal ions by the adsorbent was found to be 25 ml. The thermodynamic parameters as well as the effect of interfering ions were investigated by graphite furnace atomic absorption spectrometry.

Keywords: graphite furnace atomic absorption, heavy metal ions, layered double hydroxide, replicable method

1. INTRODUCTION

Organic pollutants are biodegradable, whereas metal ions are non‐biodegradable. Hence, metal ions should be removed from wastewaters before discharging it to the environment [1]. Following the growing population and industrialisation of human life, extensive environmental problems have been created by carcinogenic compounds due to the presence of heavy metals. Therefore, many studies have been conducted to remove compounds from water, air, and soil. The layered double hydroxide (LDH) is one of the most popular adsorbents that has received a lot of attention today due to its ease of preparation, affordability, environmental friendliness, and non‐toxicity [2, 3, 4, 5, 6]. LDH has recently gained the attention of chemists in the use of these materials as organic and inorganic composites. LDHs have relatively weak intra‐layer bonds and thus have a high ability to capture organic and inorganic ions. LDHs have numerous applications, for example, catalysts in chemical reactions, photocatalysts, anion exchangers, sensors, plastic additives, removal of heavy metals from the soil, and wastewater heavy‐metal precipitating agents. The general formula for LDHs is shown as [MII 1−x MIII x (OH)2](A)x+ x/m nH2O. Generally, M2+ is a divalent cation such as Ni2+, Fe2+, Co2+, Mg2+ etc., and M3+ is a trivalent cation such as Fe3+, Al3+, Cr3+, and so on. The value of x in the formula for LDHs is usually chosen to be around 0.20–0.33, which is proportional to the mole fraction M3+/(M2+ + M3+). A represents an interlayer anion with a capacity of m such as NO3 , CO3 2−, Cl and SO4 2−. The values of M2+, M3+, x, and A m can vary over a wide range [7, 8, 9, 10, 11]. Wataru et al. used YVO4: Eu3+ nanoparticles that have a negative surface charge because citrate anions are adsorbed on their surface. The negative charge of YVO4: Eu3+ nanoparticles and the positive charge of LDH nanoplates are placed on the layers of quartz glass with the layer‐by‐layer (LbL) method to create multilayer films that are held together by electrostatic forces. The researchers found a relationship between the number of deposition cycles and the intensity of photoluminescence of multilayer films [12].

In general, centrifugation and filtration methods are used to separate the adsorbent material from aqueous solution [13]. These applications are time consuming and require extra cost [14]. Compared with traditional centrifugation and filtration methods, magnetic separation method is an efficient, fast and economic method for the separation of magnetic adsorbents from the medium after the adsorption treatment of pollutants is completed [15]. The separation of non‐magnetic adsorbents from sample solution after adsorption process is very difficult and also time consuming. This problem can be solved by the incorporation of magnetic nanoparticles on the surfaces of nanocomposite adsorbents and then by using a magnet [16]. Fe3O4 nanoparticles are the most widely used materials in the preparation of magnetic nanocomposite adsorbents owing to their unique properties such as chemical stability, uniform particle size, and biocompatibility [17].

One of the most important applications of superparamagnetic nanoparticles is solid‐phase extraction (SPE). In this method, superparamagnetic nanoparticles are used as a solid phase. Superparamagnetic nanoparticles can have many potential applications in ferrofluids, colour imaging, magnetic refrigeration, detoxification of biological fluids, synthesis of organic matter as a catalyst, degradative separation, controlled delivery of anticancer drugs, and magnetic cell separation. Due to their special properties, magnetic nanoparticles can be used as adsorbents in the separation, extraction, and removal of various organic and inorganic compounds, especially environmental pollutants, and separation of drugs from biological samples. These features include easy synthesis of nanoparticles, high surface area to volume due to nanometre dimensions, superparamagnetic properties that cause these particles to respond to the external magnetic field and lose their magnetic properties in the absence of an external field, the ability to easily and quickly extract different species using only an external magnetic field, no need for filtration, centrifugation during the extraction process, the ability to extract from large volumes of samples, and the ability to modify the surface of nanoparticles that enable selectivity [18, 19, 20, 21, 22, 23].

Ethylenediaminetetraacetic acid is known by the acronym EDTA. It is an amino polycarboxylic acid with the appearance of a water‐soluble crystalline white powder and the chemical formula C10H16N2O8. EDTA is known to be a widely used chelating agent in industrial and domestic purposes and can be used in a variety of fields such as agriculture, medicine, and electroplating. For example, EDTA is used in lead poisoning at a rate of 1 g every 12 h as an intravenous injection. It significantly reduces the amount of lead in the body. Regardless of the charge of other metal ions, EDTA combines with them in a ratio of 1: 1. This reaction is important not only because of the formation of the chelate with all the cations but also because most of these chelates are so stable that they have laid the foundation for volumetric methods. There is no doubt that this high stability is due to the presence of several complexing sites within the molecule, which leads to a cage‐like structure, enclosing the cation and keeping it out of the reach of solvent molecules. EDTA is very effective due to its low biodegradability in the groundwater system. EDTA has six potential sites to bond with metal ions, including 4 carboxyl groups and two amine groups [24, 25].

Atomic absorption spectroscopy (AAS) is an excellent multi‐purpose method in analytical chemistry. The concentration of toxic trace elements in well water and several other common elements such as calcium, sodium, as well as very small amounts of other metals can be measured by this method. The concentration of rare toxic elements in drinking water and some other common elements such as calcium, sodium, as well as very small concentrations of other metals can be measured by this method. Other applications include measuring lead or cadmium in a drop of blood, measuring silver in synthetic rainwater, searching for impurities in alloys, activating reagents, water analysis, direct analysis of air, direct analysis of metal ores and refined metals, and measuring alloying elements in steel such as manganese, magnesium, chromium, copper, nickel, molybdenum, vanadium, cobalt, titanium, tin, aluminium and lead [26, 27].

In aquatic environments, antimony is found in two forms, Sb (III) and Sb (V), both of which are toxic. However, Sb (III) is 10 times more toxic than Sb (V). Sb (III) is mostly found in groundwater and Sb (V), in surface water [28, 29]. A person comes in contact with antimony by breathing in antimony dust, drinking water, and eating the foods that contain it. It also enters the body through skin contact with soil, water, and materials that are soaked in it. It is dangerous to inhale antimony combined with oxygen in the gas phase. Prolonged contact with this metal at doses above 9 mg/m3 through air can cause eye, skin, and lung irritation. More serious problems, such as lung disease, heart problems, diarrhoea, vomiting, and stomach ulcers, can occur if contact continues. However, it is not entirely clear whether this element causes infertility or cancer. At a controlled dose, this element is suitable for the treatment of parasitic infections, but it causes health problems at higher doses [30].

This study was conducted with the aim of investigating the removal of antimony ions from aqueous environments modified by these magnetic nanoparticles with EDTA ligands. The conditions for achieving the goal were created, which were optimised taking into account the effective factors. The quality of adsorption, reversibility, and irreversibility was also assessed.

2. EXPERIMENTAL

Aluminium chloride hexahydrate (AlCl3·6H2O), Iron (II) chloride (FeCl2), Ferric chloride (FeCl3), ethylenediaminetetraacetic acid (EDTA), and potassium antimony (III) oxide tartrate trihydrate (C8H4K2O12Sb2·H2O) were obtained from Sigma‐Aldrich. Magnesium chloride hexahydrate (MgCl2·6H2O), methanol‐acetic anhydride, and ammonia were obtained from Merck.

2.1. Equipment

The PG990 Atomic Absorption Spectrometer was used to evaluate the amount of antimony adsorption on the synthesised adsorbent. The A1.8 Tesla magnet was used to separate the magnetic nanoadsorbent from the samples during the optimisation process. An autoclave, a vacuum oven, and an ultrasonic probe were also used to synthesise magnetic adsorbents. During the optimisation process, the incubator shaker with the refrigerator was used to adjust the temperature. The formation of functional groups was demonstrated using the PerkinElmer (spectrum two model) FTIR test. The TESCAN MIRA3 FESEM made in Czechoslovakia and energy dispersive X‐ray spectroscopy (EDS) analysis equipped with IDFix software were used to study the surface morphology of synthesised magnetic nanoparticles. In addition, the crystal structure of the sample was determined using the X‐ray diffraction (XRD) test performed by the X'pertpro device from Panalytical. The saturation magnetisation of the synthesised magnetic nanoparticles was measured using a vibrating sample magnetometer (VSM) test with LBKFB (Meghnatis Daghigh Kavir Co.). The surface zeta potential of the adsorbent was studied using a zeta potential apparatus (SZ100, Horiba Co.).

2.2. Synthesis method for Fe@Mg‐Al LDH

To fabricate the superparamagnetic nanoadsorbent, which is done in two phases, initially, 48.7 g of MgCl₂·6H₂O, 2.96 g of AlCl₂·6H₂O, 5.09 g of urea, and 12 ml of methanol‐acetic anhydride were stirred on a magnetic stirrer for 30 min. When the solution became clear, it was placed in an autoclave for 6 h at 150°C. The solid phase was then separated from the liquid using a centrifuge and washed with water and ethanol. The white product was then dried at 120°C for 12 h. In the next step, 0.12 g of the white product obtained from the previous step was added to 0.08 g of FeCl2,·0.216 g of FeCl3, and 20 ml of deionised water. Afterwards, the container containing the sample was placed on a magnetic stirrer at 50°C for 20 min. After cooling the solution of a black sample, it was homogenised by an ultrasonic device, and then 1 ml of ammonia solution was added at the same time, and it was placed on a heater at 50°C after 40 min. Finally, the black product was washed with distilled water, was separated from the liquid by a magnet, and dried at room temperature (Figure 1).

FIGURE 1.

FIGURE 1

The synthesis scheme of Fe@Mg‐Al layered double hydroxide

2.3. Adsorption parameters studies

The amount of adsorption efficiency in each phase of the optimisation was obtained from Equations (1) and (2):

R(%)=c0cec0×100 (1)
qe=c0ceM×V (2)

where C 0 is the initial concentration of a metal ion in the sample solution (mg L−1), C e is the metal ion concentration in the sample solution after finishing the contact time with the adsorbent (mg L−1), M is the adsorbent mass (g), V is the sample solution volume (L), q e is the amount of adsorbent (mg g−1) and R (%) is the percentage of the adsorption.

2.3.1. pH

Different pHs were selected from 2 to 9 to obtain the optimal pH value using a buffer solution and 0.1 mol L−1 of HCl and NaOH solution [31, 32]. The 0.04 g of Fe@Mg‐Al LDH was added to 25 ml of antimony solution with concentrations of 0.1 and 1.5 mg/L of EDTA ligand. The sample was placed on a magnetic stirrer at 20°C for 30 min. After centrifugation, the remaining ion concentration was determined by graphite furnace atomic absorption spectrometry (GFAAS).

2.3.2. Amount of nanoadsorbent

To achieve the optimal amount of nanoadsorbent, the range of 0.005–0.05 g of nanoadsorbent was added to 25 ml of 0.1 mg/L antimony solution and 1.5 mg/L of EDTA ligand, which was stabilised at pH = 8 using a buffer. It was then placed on a magnetic stirrer for 30 min. The remaining ion concentration was then determined by GFAAS.

2.3.3. Time

For the effect of time on the removal of antimony, a phosphate buffer solution with pH = 8 was used to stabilise a 0.1 mg/L of antimony solution and 1.5 mg/L of EDTA ligand. Then, 0.025 g of nanoadsorbent was added to the solution, and it was placed on a magnetic stirrer at different times for 1 to 30 min at 25°C. The remaining antimony ion concentration was then determined by GFAAS.

2.3.4. Ligand

The effect of the amount of EDTA ligand on the removal of antimony was investigated. The samples containing EDTA ligand were prepared with a concentration of 0.05, 0.25, 0.5, 0.75, 1, 1.2, and 1.5 mg/L with pH constant at 8. The samples were placed on a magnetic stirrer at an optimal time of 25 min at room temperature, adding the optimal amount of 0.025 g of adsorbent. After centrifugation, the remaining ion concentration was determined by GFAAS.

2.3.5. Solution volume

The effect of solution volume was studied on the removal of antimony for the determination of the enrichment factor and the maximum sample volume on the removal of antimony metal ions. Solutions with volumes of 25, 40, 50, 100, 250, and 200 ml of 0.1 mg/L antimony solution and the optimal amount of ligand were stabilised at pH = 8. They were then mixed with a 0.025 g of the nanoadsorbent on a magnetic stirrer at room temperature for 25 min. The remaining antimony ion concentration was determined using GFAAS.

2.3.6. Temperature

In optimal conditions, the temperatures of 10, 15, 20, 25, 30, and 35°C were studied for antimony ions extractions with the refrigerated incubator shaker apparatus. The remaining ion concentration was determined by GFAAS.

3. RESULT AND DISCUSSION

3.1. Characterisation of adsorbent

FTIR analysis was seen in Figure 2. The wavenumbers ranged from 3413.4 to 3381.31 cm−1, which were related to the stretching vibration of OH. The wavenumbers 1618.92 and 1635.40 cm−1 were created due to the vibrations of the water molecules. The appeared peaks between 500 and 800 cm−1 were related to the chemical bond between oxygen, Al‐O, and Mg‐O [7, 8]. The broad peak of about 603 cm−1 in Figure 2b corresponds to the bending vibration associated with Fe‐O, which is not present in the spectrum of Figure 2a [33, 34]. This peak indicates the magnetisation of Mg‐Al LDH.

FIGURE 2.

FIGURE 2

Fourier transform infrared spectrum of Mg‐Al layered double hydroxide (LDH) (a) and Fe@Mg‐Al LDH (b)

As can be seen in Figure 3a,b, XRD was related to the first phase of Mg‐Al LDH and the final phase of Fe@Mg‐Al LDH, respectively. In Figure 3a, the position of the (003) plane corresponds to the basal spacing of Mg‐Al LDH was appeared in 2θ = 11.26° with 7.85 Å. The peaks identified in the pattern of Figure 3a are related to the hydrotalcite structure. The two additional peaks observed in the Fe@Mg‐Al LDH pattern (Figure 3b) are due to the magnetisation of the adsorbent. Besides, due to the reduction of sharper peaks in Figure 3b, it can be seen that the crystallisation of the adsorbent decreased after the addition of Fe to Mg‐Al LDH. [7, 35].

FIGURE 3.

FIGURE 3

X‐ray diffraction (XRD) pattern of Mg‐Al layered double hydroxide (LDH) (a) and Fe@Mg‐Al LDH (b)

Figure 4a,b shows the field emission scanning electron microscopy (FESEM) images of Mg‐Al LDH and Fe@Mg‐Al LDH. Figure 4a is related to the LDH containing Mg‐Al and the particles are displayed with 35–46 nm of sizes. Figure 4b is related to LDH containing Fe@Mg‐Al and the signed points are shown with 39–151 nm and the iron element is quite clear.

FIGURE 4.

FIGURE 4

Field emission scanning electron microscopy image of Mg‐Al layered double hydroxide (LDH) (a) and Fe@Mg‐Al LDH (b) nanoparticles

Figure 5a,b is related to the EDS analysis and it shows the first phase of LDH contains Mg, Al, and O (Figure 5a), and the second phase of LDH contains Mg, Al, O, and Fe (Figure 5b).

FIGURE 5.

FIGURE 5

Energy dispersive X‐ray spectroscopy (EDS) of Mg‐Al layered double hydroxide (LDH) (a) and Fe@Mg‐Al LDH (b) nanoparticles

Figure 6a,b is related to the VSM analysis of Mg‐Al LDH and Fe@Mg‐Al LDH. The saturation magnetisation of Mg‐Al and Fe@Mg‐Al LDH are shown as 6 and 18 emv/g, respectively. This increase in magnetisation was due to the addition of iron nanoparticles to Mg‐Al LDH.

FIGURE 6.

FIGURE 6

Vibrating sample magnetometer magnetisation curve of Mg‐Al (a) and Fe@Mg‐Al (b) LDH nanoparticles

3.2. The effect of pH on the removal of antimony

The adsorption of antimony with Fe@Mg‐Al LDH depends on the pH of the nanocomposite surface. As observed in Figure 7, the pHzpc (zero point of charge) of Fe@Mg‐Al LDH was 8. With a lower pH value than 8 for Fe@Mg‐Al LDH, the hydroxyl groups of the Fe@Mg‐Al LDH surface were protonated which increased the positive change on the surface. At this time, electrostatic repulsion is created between the Fe@Mg‐Al LDH and antimony metal cations, resulting in a less removal capacity of antimony metal. At a higher pH value than 8, the hydroxyl groups of the Fe@Mg‐Al LDH surface were deprotonated which increased the negative change on the surface and the tendency to adsorb antimony metal cations increases through electrostatic attraction. However, at higher pHs and excess OH, the possibility of precipitation and formation of the hydroxylated complexes of antimony increases [36, 37]. As can be seen from the diagram (Figure 8), at acidic pHs, the Fe@Mg‐Al LDH surface has a high positive charge and the repulsive force prevents antimony metal cations from being adsorbed on it and the extraction process rate is low. As the pH increases and approaches 7, the positive charge on the surface and H+ ion in solution decreases and antimony metal cations are more easily adsorbed [7, 38, 39]. At pH = 8, the highest adsorption of antimony metal cations was observed with the nanocomposite surface.

FIGURE 7.

FIGURE 7

The Zeta potentials of Fe@Mg‐Al energy dispersive X‐ray spectroscopy (EDS) in various pH

FIGURE 8.

FIGURE 8

The effect of pH on the removal of antimony by Fe@Mg‐Al energy dispersive X‐ray spectroscopy (EDS; 0.04 g of Fe@Mg‐Al LDH, 25 ml of antimony solution with 0.1 mg/L concentration, 1.5 mg/L of ethylenediaminetetraacetic acid, 20°C for 30 min)

3.3. The effect of the amount of nanoadsorbent on the removal of antimony ions

The 0.025 g amount of nanoadsorbent was found for the maximum adsorption of antimony ions with Fe@Mg‐Al LDH (Figure 9).

FIGURE 9.

FIGURE 9

Efficiency rate by the amount of adsorbent (pH = 8, 25 ml of antimony solution with 0.1 mg/L concentration, 1.5 mg/L of ethylenediaminetetraacetic acid, 20°C for 30 min)

3.4. The effect of time on the removal of antimony

As shown in Figure 10, with the increase in time, the efficiency increased and the curve has a steep slope up to 25 min. The time of 25 min is the equilibrium time for the adsorption of Sb(III) ions by Fe@Mg‐Al LDH, which is the optimal time due to time savings and no significant difference between 25 and 30 min [40].

FIGURE 10.

FIGURE 10

Effect of time on the antimony ions removal (0.025 g of Fe@Mg‐Al LDH, pH = 8, 25 ml of antimony solution with 0.1 mg/L concentration, 1.5 mg/L of ethylenediaminetetraacetic acid, 20°C)

3.5. Effect of the amount of EDTA ligand on the removal of antimony

As shown in Figure 11, with increasing the concentration of the ligand to 1 mg/L, the efficiency increased because the ligand formed a complex with antimony. However, the lack of change in the efficiency after the concentration of 1 mg/L could be attributed to the saturation of the nanoadsorbent active surface.

FIGURE 11.

FIGURE 11

Efficiency by the ligand concentration (0.025 g of Fe@Mg‐Al layered double hydroxide, pH = 8, 25 ml of antimony solution with 0.1 mg/L concentration, 20°C for 25 min)

3.6. The effect of solution volume

As can be seen in Figure 12, with an increase in volume sample (25 ml), the recovery extraction is decreased. This is probably explained by the limitation of contact between the antimony ions and nanoadsorbent sites [41, 42].

FIGURE 12.

FIGURE 12

Effect of solution volume on the removal of antimony ions (0.025 g of Fe@Mg‐Al layered double hydroxide, pH = 8, antimony solution with 0.1 mg/L concentration, 1 mg/L of ethylenediaminetetraacetic acid, 20°C for 25 min)

3.7. Temperature effect

The purpose of measuring the temperature is to investigate the antimony ion extractions and thermodynamic parameters. As can be seen in Figure 13, the extraction efficiency increased with increasing temperature up to 30°C. As the temperature rises, the activity of the metal ions in the solution increases, and the chances of colliding with the empty sites of nanoadsorbent increase [43].

FIGURE 13.

FIGURE 13

Temperature effect on the removal of antimony ions (0.025 g of Fe@Mg‐Al LDH, pH = 8, 25 ml of antimony solution with 0.1 mg/L concentration, 1 mg/L of ethylenediaminetetraacetic acid, 25 min)

3.8. Interfering ions

Interfering cations are referred to as ions that cause a change of up to 5% in the absorbance signal of the goal ion. The effect of interfering ions was investigated on the removal of antimony. Other ions were used in addition to the antimony ions to prove the adequacy of the nanoadsorbent. For this purpose, different concentrations of interfering ions (presented in Table 1) were added to the optimal solution with the nanoadsorbent. After the extraction process and centrifugation, the remaining ion concentration was determined by GFAAS. The obtained result displayed that the addition of the cations does not have considerable interference in the determination and removal of antimony ions [44].

TABLE 1.

The effect of different concentrations of interfering ions on the adsorption efficiency of 0.1 mg/L of antimony and 1 mg/L of ethylenediaminetetraacetic acid ligand (n = 3)

Interfering ion Added (μg/L) Recovery (%)
Cr3+ 27.45 90.85
Ni2+ 30.78 89.74
Cu2+ 31.08 89.64
Pb2+ 26.04 91.32
Na+ 34.29 88.57
Ca2+ 32.28 89.24
Zn2+ 33.15 88.95
Ag+ 26.34 91.22
K+ 29.82 90.06
Co2+ 37.74 87.42
Al3+ 29.83 90.39

3.9. Elution solvent selection

The type of solvent selected for elution and desorption of antimony metal ions is one of the main factors that has a great impact on the metal removal system. In this study, various elution solvents have been used in combination and separately, and the optimal solvent for antimony metal ions removal has been selected (Figure 14). Considering the maximum antimony extraction with acidic methanol, it was selected for the desorption of antimony metal ions with the ideal balance created between the Fe@Mg‐Al LDH and this solvent. Furthermore, the volume of elution solvent was investigated with a volume range of 10–35 ml of optimum elution solvent. The result is shown in Figure 15 that the goal volume for desorption of antimony metal ions from Fe@Mg‐Al LDH was found to be 25 ml [45, 46].

FIGURE 14.

FIGURE 14

Effect of elution solvent on antimony metal ions adsorption

FIGURE 15.

FIGURE 15

Effect of elution solvent volume

3.10. Replicability

To achieve the standard deviation method as an important analytical factor, antimony metal ions were extracted and removed by nanoadsorbent five times using the method presented in this study. The remaining ions concentration was determined and a calibration curve was drawn. The standard deviation value of the method was found at 7.92%. It was acknowledged that the method was replicable.

3.11. Real samples analysis

To evaluate the accuracy of the proposed method, the standard addition method has been used for different real samples (well water, snow water, rainwater, and seawater). These samples were purified with nitric acid after passing through filtration and storage in containers. The solutions were in contact with 0.025 g of nanoadsorbent at 30°C and pH = 8 for 25 min. The adsorption ions and efficiency were investigated after the separation and signal reading by GFAAS (Table 2). The results in Table 2 show that Fe@Mg‐Al LDH is effective in preconcentration and designation of antimony ions in a complex matrix, for example, various aqueous samples.

TABLE 2.

Recovery of antimony ions was added to 1000 ml of different water samples (pH = 8)

Sample Antimony added (μg) Antimony determined (μg)
Well water 0.0 2.12 (0.401) a
10.0 12.4 (0.0502)
Snow water 0.0 N.D. b
10.0 12.1 (0.710)
Rain water 0.0 0.890 (2.17)
10.0 11.4 (0.171)
Sea water 0.0 8.74 (0.243)
10.0 18.9 (2.67)
a

Values in parentheses are RSDs based on five individual replicate analyses.

b

Not Detection.

3.12. Reusability study of the Fe@Mg‐Al LDH

To study the Fe@Mg‐Al LDH sorbent reusability, the experiments of antimony ions sorption‐desorption were carried out 6 cycles repeatedly via mentioned processes. The 25 ml of 0.1 mg/L solutions of antimony ions and 1 mg/L of EDTA were prepared at pH = 8 and then 0.025 g of Fe@Mg‐Al LDH was added and stirred for 25 min at 30°C, then centrifuged and finally washed with 25 ml of acidic methanol, and then the concentration of antimony ions in solution was monitored by GFAAS. Then, the Fe@Mg‐Al LDH was washed with water/ethanol and dried and re‐tested for the second time according to the mentioned process. This experiment was carried out five times, and the obtained results display that it is possible to apply the Fe@Mg‐Al LDH three times.

3.13. Study of isotherms

Freundlich, Langmuir, and Temkin isotherms were used to achieve the adsorption model. The amount of adsorbed antimony ions at equilibrium q e (mg/g) was calculated by Equation 2). Adsorption isotherms are equations for describing the equilibrium state of the adsorbed component between the solid and fluid phases. At this stage, the experimental data on adsorption equilibrium with Freundlich, Langmuir, and Temkin isotherms were examined. The equations for isotherm models of Langmuir, Temkin, and Freundlich are as follows, respectively [47, 48].

Ceqe=1Q0b+CeQ0 (3)
qe=BlnkT+BLnCe (4)
logqe=logKf+1nlogCe (5)

where Q 0 is the highest antimony ions sorption capacity at Fe@Mg‐Al LDH (mg/g) and b is the constant of the Langmuir Equation (L/mg), k T (L/g) and B (J/mol) are the constants of the Temkin Equation, K f ((mg/g)·(L/mg)1/n ) and n are the constants of the Freundlich Equation, C e (mg/L) is the concentration of the adsorbate in the liquid phase after reaching equilibrium, and q e (mg/L) is the amount of the adsorbate per unit mass of Fe@Mg‐Al LDH [49].

The parameters of isotherm models are deposited in Table 3. The correlation coefficient of Langmuir isotherm for antimony ions is 0.917, while this value of the Freundlich and Temkin isotherms is 0.808 and 0.847, respectively. The results show that the Langmuir model can be considered as a monolayer adsorption mechanism of antimony metal ions on the Fe@Mg‐Al LDH. Similar results were observed in the adsorption isotherm studies of various pollutant‐adsorbent systems [50, 51, 52, 53].

TABLE 3.

Freundlich, Langmuir, and Temkin isotherms constants for the adsorption of antimony ions by Fe@Mg‐Al LDH

Freundlich isotherm Langmuir isotherm Temkin isotherm
n K f ([mg/g]·[L/mg]1/n ) R 2 Q 0 (mg/g) b (L/mg) R 2 k t (L/g) B (J/mol) R 2
1.60 0.948 0.808 160 0.102 0.917 0.245 0.0660 0.847

3.14. Determination of thermodynamic parameters

Thermodynamic parameters include changes in Gibbs free energy change (ΔG), enthalpy change (ΔH), and entropy change (ΔS), which are the most important features of an adsorption process for practical applications. Thermodynamic equations help to better understand the process of adsorption, that is, to increase the adsorption efficiency. According to Table 4, since all ΔGs were positive for antimony ions, it could be concluded that all adsorption processes by the Fe@Mg‐Al LDH were non‐spontaneous [54, 55]. Additionally, if the ΔG was between 0 and 20, the adsorption processes were chemical. The positive enthalpy change of adsorption reactions on the Fe@Mg‐Al LDH indicated that these processes were endothermic. The entropy changes in adsorption by Fe@Mg‐Al LDH were positive, indicating that the degree of freedom at the solid‐solution phase in adsorption increased.

TABLE 4.

Thermodynamic parameters

T (Kelvin) lnK G 0 (kJ/mol) H 0 (kJ/mol) S 0 (kJ/mol K)
283 −1.65 3.90 14.3 0.0370
293 −1.45 3.53
303 −1.20 3.04

The standard free energy change (ΔG 0) can be calculated from the following equation 6:

ΔG0=RTLnK (6)

where R is the universal gas constant (8.314 J/mol K), T is the temperature (K) and K is the sorption equilibrium constant. The standard entropy change (ΔS0) can be calculated according to the following equation or by plotting lnK versus 1/T lnK=ΔS0RΔH0RT [56, 57].

ΔG0=ΔH0S0 (7)

3.15. Comparison of the removal of antimony (III) by different adsorbents

Table 5 presents the removal of antimony (III) by different adsorbents, which is compared with the method provided in this study. As can be seen, the adsorbent presented in this study has advantages that contain the best adsorption time and the amount of adsorbent was much less than that of previously published adsorbents for the removal of antimony (III) [58, 59, 60]. In this study, the use of EDTA causes more stability of antimony ions in solution and can increase the adsorption efficiency. Also, in the formation of EDTA complex and metal ions, it is possible to be located between the LDH layers, which increases the adsorption efficiency [61].

TABLE 5.

Comparison of the removal of antimony (III) by different adsorbents

Adsorbent Sb oxidation State pH T (K) Adsorbent dose (g/L) Contact time (min) Removal rate (%) Ref
Haematite modified magnetic nanoparticles Sb(III) 4.1 298 0.1 120 >95.5 [58]
Fe2O3 modified carbon nanotubes Sb(III) 7 298 0.5 120 99.97 [59]
Fe2O3/Fe3O4/C prepared with bamboo template Sb(III) 7 298 2 >90 [60]
Fe@Mg‐Al LDH Sb(III) 8 303 0.025 25 >94.43 This work

Abbreviation: LDH, layered double hydroxide.

4. CONCLUSION

This study was conducted with the aim of providing a simple, effective, repeatable, and inexpensive method to remove antimony metal ions. According to the findings of the study, the Fe@Mg‐Al LDH adsorbent has a good ability to remove antimony ions from various water samples with near‐neutral pH. In this method, with the minimum amount of Fe@Mg‐Al LDH (0.025 g), good results have been obtained for the removal of antimony metal ions with high adsorption capacity (160.15 mg/g). The results of the study of adsorption isotherm models demonstrate the adaptation of Langmuir adsorption mechanism for antimony metal ion adsorption in the form of complex formation with EDTA as a monolayer on the Fe@Mg‐Al LDH. It can also be acknowledged that the presence of interfering ions does not have much effect on ions extraction. Besides, the used method was replicable and had positive results on real samples. Also, based on the study of thermodynamic parameters, the process of extraction of antimony metal ions by the Fe@Mg‐Al LDH was non‐spontaneous and endothermic.

CONFLICT OF INTEREST

The authors declare no conflict of interests.

ACKNOWLEDGEMENTS

This study was supported by the Islamic Azad University, Varamin Pishva Branch.

Motallebi, R. , et al.: Fabrication of superparamagnetic adsorbent based on layered double hydroxide as effective nanoadsorbent for removal of Sb (III) from water samples. IET Nanobiotechnol. 16(2), 33–48 (2022). 10.1049/nbt2.12074

DATA AVAILABILITY STATEMENT

Data openly available in a public repository that issues datasets with DOIs.

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Data Availability Statement

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