Lianyuan Gonga and
Li Feng*ab
aKey Laboratory of Coal Processing and Efficient Utilization of Ministry of Education, School of Chemical Engineering and Technology, China University of Mining and Technology, Xuzhou 221116, Jiangsu, China. E-mail: cumthgfl@163.com; Tel: +86 13852488050
bNational Engineering Research Center of Coal Preparation and Purification, Xuzhou 221116, Jiangsu, China
First published on 21st October 2015
As an attempt to avoid the low defluoridation capacity of conventional adsorbents, this study offers a novel copolymerized hydroxyapatite–aluminum (HAP–PAC) adsorbent and evaluates its performance in fluoride removal of drinking water, and a possible fluoride removal mechanism is proposed based on the characterization results obtained by FTIR, XRD, BET, SEM and EDS. The results indicate that the copolymerization material prepared by co-crystallization with aluminum chloride is featured by the chemical combination between hydroxyapatite (HAP) and poly-aluminium chloride (PAC). A certain amount of Ca2+ and OH− in the HAP crystal lattice are partially replaced by Al3+ and Cl− doping from PAC, and the structure of the copolymerization material shows a uniform trend. In addition, mainly by chemical adsorption, the highest defluoridation capacity (DC) of the copolymerization material can reach up to 18.12 mg g−1, an increase of 14.02 mg g−1 as compared with conventional hydroxyapatites. When aluminum chloride is replaced by bauxite in the study, the highest DC is 13.72 mg g−1 due to the co-occurrence of chemical and physical combinations and relatively lower homogeneous structure caused by the co-existence of HAP and PAC while electrostatic attraction and chemical adsorption are both involved. As for the material prepared by the physical mixing method, in which the combination between HAP and PAC is mainly dominated by physical effects, its maximum DC is 13.08 mg g−1, with physical adsorption as its main form of defluoridation.
Adsorption is widely applied nowadays to remove excessive fluorine in drinking water due to its simple operation on instruments and low running cost;6,7 the kernel for this method is the choice of an appropriate adsorbent. Popular adsorbents include activated alumina,8,9 bone charcoal,10 biological macromolecule fluoride agents,11 kaolin,12 and hydroxyapatite.13,14 Of all the adsorbents, activated alumina, widely employed several years ago, is seldom used now because of its low defluoridation capacity (DC), which consequently leads to a lot of regenerations and secondary pollution by adding chemical reagents, and the need to adjust the values of pH of the water system, which increases the complexity of its normal usage. To improve the adsorption efficacy of activated alumina, researchers have tried to modify the surface of alumina. For instance, La3+-modified activated alumina (La-AA) was studied by Jiemin Cheng et al.15 The comparison of adsorption characteristics of La-AA and original alumina in the removal of fluoride concluded that the maximum DC values of AA and La-AA were 2.74 and 6.70 mg g−1 at pH = 7.0, respectively. A novel adsorbent of sulfate-doped Fe3O4/Al2O3 nanoparticles with magnetic separability was prepared, characterized and applied by Liyuan Chai et al.16 Test results showed that the adsorption by this adsorbent for fluoride by a two-site Langmuir model was 70.4 mg g−1 at pH = 7.0 with initial fluoride concentrations of 160 mg L−1. Bansiwal et al.17 examined copper oxide coated alumina (COCA) by impregnating alumina with copper sulphate solution followed by calcination at 450 °C in the presence of air. The analysis indicated that the DC of COCA obtained through the Langmuir model was 7.22 mg g−1, which was advanced by 5.0 mg g−1 as compared with unmodified AA. One disadvantage of these adsorbents is that certain amounts of aluminum dissolves in the water during the defluoridation process, which poses a potential threat to human health in the long-term drinking.
Hydroxyapatite (HAP), as a new type of fluoride removal material, is superior to activated alumina in terms of its high fluoride removal capacity and availability. However, its unfixed property can induce turbidity, water filtration difficulty and the reactivation process of HAP is also extremely complex. To solve these problems, Weihua Xu et al.18 studied a novel type of high hardness granular filter material made by hydroxyapatite with a modification with attapulgite. However, this material has lower DC because of its smaller contact area with water systems. Then, Li Feng et al.19 reported a method for heat regeneration of the hydroxyapatite/attapulgite composite beads for defluoridation of drinking water and its total DC can reach up to the level of the powdered material of HAP. Another adsorbent of alginate bioencapsulating nano-hydroxyapatite (n-HApAlg), synthesized by Pandi K et al.,20 has a higher DC (3.87 mg g−1) than the original n-Hap (1.296 mg g−1) and calcium alginate (CaAlg) composites (0.68 mg g−1). Yulun Nie et al.21 stated that aluminum modified calcium hydroxyapatite (Al-HAP) nanoparticles produced by the co-precipitation method possessed a higher DC of 32.57 mg g−1 with an initial fluoride concentration of 10 mg L−1. The adsorption capacity of nano-materials can be increased because of its huge specific surface area. However, its difficulty in interception cannot eliminate the possibility of entering the human body. In addition, its fluoride removal capacity is greatly influenced by the concentration of nano-materials in fluorine-containing water: the higher the concentration is, the larger the capacity will be.19
Poly aluminium chloride (PAC), as an inorganic polymer flocculation, is commonly applied in wastewater treatment owing to advantages such as strong coagulability, big floc, less dosage, and high water purification efficiency.
This study proposes a new sorbent of HAP–PAC copolymerization material based on the analysis of fluoride removal of HAP/active aluminum and the flocculation effects of PAC. Because of its high DC, it is capable of removing fluoride intensively and producing drinkable water without any health concerns.
The prepared water sample was transferred into a coagulation blender container until the volume reached 0.6 L. Then, 0.09 g of filtering material was added into the container followed by stirring at the speed of 200 rpm for 30 min. After maturating for 30 min, 25 mL of supernatant was pipetted into a 50 mL volumetric flask and 10 mL of TISAB solution was added. During the whole process, the volume was maintained. Finally, the electromotive force E of the solution was tested by a fluoride ion-selective-electrode, pF-1 (made in China). A standard curve could be drawn by setting the electromotive force E of the standard solution as the Y-axis vs. the logarithm of solution concentration as the X-axis. The equation obtained was y = −57.071x + 235.23 with a correlation index R2 = 0.9999. The concentration (mg L−1) of fluoride ion in the solution could be calculated based on this curve.
As Fig. 1 shows, the DC of pure HAP is 4.10 mg g−1, and its capacity shows no distinct variation as a small quantity of PAC is added to make the ratio turn into 0.022. It then rises quickly from 0.022 to 0.132 and possesses the maximum DC of 13.08 mg g−1 when the Al/Ca molar ratio is 0.132. However, the DC decreases with further increase in the Al/Ca molar ratio. The possible explanation for this phenomenon lies in the fact that a certain type of synergistic effect between HAP and PAC may be induced with the increase of Al/Ca molar ratio, thus improving the capacity of defluoridation. Moreover, the flocculation precipitation caused by the flocs from PAC and turbidity from fluor-hydroxyapatite accelerates the adsorption reaction between adsorbent and fluoride in water, which in turn mitigates the potential dangers of turbidity value decreases in water and aluminum dissolved from PAC. It can be observed that the filtering material with the best proportion exhibits the highest efficiency for the removal of fluoride. As the ratio increases beyond the optimal one, further additions of PAC means more impurities in the filtering material, which lowers its adsorption ability, and thus weakening its DC.
Fig. 2 shows the impact on DC as filtering materials prepared by chemical synthesis under different Al/Ca molar ratio. The preparation methods are divided into the crystalline aluminum chloride (AlCl3·6H2O) method and the bauxite method due to the difference in the choice of the raw materials.
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Fig. 2 The influence of different Al/Ca molar ratio on defluoridation capacity on chemical synthesis. |
It can be observed from Fig. 2 that the overall trend of the two curves displays some similarity, that is, the fluoride removal capacity will increase firstly and then decrease with increasing Al/Ca molar ratio, and the DC of the bauxite method is relatively lower. An account for this is that the two filtering materials form a stable structure when copolymerization occurs between special amounts of HAP and PAC in the preparation process and leads to their relatively higher DC. However, if Al/Ca molar ratio surpasses its optimal value, then it will finally induce physical mixture, this procedure will lead to the decrease of DC. As compared with the AlCl3·6H2O method, the effective content of the prepared product is relatively lower in view of the high content of impurities in raw bauxite, which triggers its poor copolymerization with HAP. Consequently, the adsorption capacity of the filtering material generated from the bauxite method is not as effective as that created from the AlCl3·6H2O method. The optimal Al/Ca molar ratio of filtering materials produced by the AlCl3·6H2O method and the bauxite method demonstrates an identical value of 0.22, and the corresponding DC are 18.12 mg g−1 and 13.72 mg g−1, respectively. Both methods increase the DC by 14.02 mg g−1 and 9.62 mg g−1 over conventional hydroxyapatite.
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Fig. 3 FTIR spectra of filtering materials (in Fig. 3: H1 is the copolymerization material prepared by AlCl3·6H2O; H2 is the filtering material prepared by bauxite; H3 is the filtering material prepared by physical mixing method). |
Fig. 3 indicates that HAP shows a strong P–O stretching vibration peak at 1040 cm−1 and a P–O bending vibration double peak at 605 cm−1 and 570 cm−1. In addition, HAP also presents a relatively weaker –OH stretching vibration peak at 3450 cm−1 and a relatively weaker –OH bending vibration peak at 1640 cm−1. The characteristic peaks of PAC are listed below. A relatively stronger broad peak at 3410 cm−1 and a relatively stronger sharp peak at 1640 cm−1 are ascribed to the stretching vibration and bending vibration of –OH, respectively. The characteristic peak at 598 cm−1 is assigned to the bending vibration of Al–Cl.
In comparison with the infrared spectra of pure HAP and PAC, both the spectra of H1 and H2 at near 3410 cm−1 and 1640 cm−1 show relatively stronger –OH stretching vibration and bending vibration peaks, which are similar to those of PAC. However, it is worth noting that a red shift occurs at 3410 cm−1, a blue shift occurs at 1640 cm−1, and their wavenumbers display slight differences. This result clearly suggests that the material structure is different from that of pure HAP and PAC. While a relatively higher P–O stretching vibration peak, which is similar to HAP in this respect, appears at near 1040 cm−1, the band exhibits obvious shifts to higher wavenumbers when the intensity of the absorption peak decreases significantly and the wavenumber changes slightly. This may be due to the bending vibration of the Al–OH–Al groups. In addition, the single peaks at 604 cm−1and 565 cm−1, respectively, may be attributed to the bending vibration of the OP⋯Cl groups. A part of the hydroxyl groups in HAP may be replaced by Cl in PAC. On the basis of these aforementioned results, it can be said that the chemical action plays a dominant role in the synthesis of H1 and H2 and that the degree of the action and the results display slight differences.
The spectra of H3 at 3425 cm−1 and 1640 cm−1 have the relative stronger stretching vibration and bending vibration peaks of the –OH group, which bears certain similarities to PAC at 3410 cm−1 and 1640 cm−1. The change of the wavenumber at 3425 cm−1 may be the result of the overlap of peaks between PAC and HAP. There is also a relatively higher P–O stretching vibration peak, which is also shown in HAP at 1040 cm−1, and doublets at 604 cm−1 and 565 cm−1 just like HAP. The change of wavenumbers may be attributed to the overlap of peaks at 598 cm−1. On the grounds of the aforementioned results, it can be concluded that physical action plays an important role in the formation procedure of H3 but does not change the respective structures of HAP and PAC.
The XRD patterns of Fig. 4(a) show that the crystalline peaks occur at 2θ = 25.9°, 32°, 33°, 35.5° and 40°, thus confirming the formation of a hydroxyapatite structure. Based on existing data, the characteristic peaks of PAC are 7.5°, 8.3°, 10.2°, 10.8°, 12.7°, and 13.5°.23 In comparison with Fig. 4(a) and (b), it can be found that filtering materials H1 and H2 have different characteristic diffraction peaks with pure HAP or PAC. Evidence obtained from the XRD study suggests that these synthesized filtering materials have changed the respective molecular structures of HAP and PAC. However, the formation procedure of filtering material H3 does not alter the respective structures of HAP and PAC because multiple HAP and PAC characteristic peaks are found in H3. This means that the mixing between these two materials mainly belongs to a physical measure, which conforms to the information as obtained from FTIR.
As can be observed in Fig. 4(b), the crystallization degree of H3 is the lowest with relatively more impurity peaks, whereas the crystallization degrees of H1 and H2 are relatively higher. The peak shape is extremely sharp, the peak width higher and narrower, and the background thinner. These results imply that the chemical reaction is able to enlarge the grain crystals of H1 and H2, and stimulate the decrease of crystal defects and intercrystalline disordered structures, which further demonstrates that the structures of H1 and H2 are more evenly distributed than that of H3.
Adsorbent | as,BET (m2 g−1) | Average pore diameter (nm) | Total pore volume (cm3 g−1) |
---|---|---|---|
H1 | 43.807 | 5.206 | 0.057 |
H2 | 22.783 | 4.305 | 0.025 |
H3 | 28.429 | 12.844 | 0.091 |
EDS area-scan diagrams and EDS line-scan diagrams of H1, H2, and H3 are displayed in Fig. 6(a)–(c). The EDS line-scan diagram indicates that all surfaces of H1, H2, and H3 contain elements Ca, Al, Cl, P, and O. Surface scanning energy spectrum in Fig. 6(a) and (b) suggest that the morphological structures of all elements except oxygen show identical trends and they are uniformly distributed on the surfaces of H1/H2. This proves that the elements in H1 and H2 are specified by homogeneous distribution and are in a stable combination. In view of the alternation of FTIR functional groups and the preparation process, it can be speculated that copolymerization occurs between HAP and PAC and that the possible combination form for this procedure is that a certain amount of Ca2+ and OH− in the HAP crystal structure is partially doped and replaced by Al3+ and Cl− in PAC. The elements Ca, P, Al and Cl in H3 display identical morphology and structure. However, the morphology and structure between these two groups is apparently different, which indicates Ca and Al in the filtering material are unevenly distributed. On the basis of the preparation process, the conclusion can be drawn that HAP and PAC are physically mixed with each other during the synthetic process and that there is no occurrence of a copolymerization reaction. The information reflected is consistent with FTIR and XRD.
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Fig. 7 Defluoridation capacity onto H1 (a), H2 (b) and H3 (c) at various time, and the inserted small figure indicates pseudo-second-order adsorption rate of F−. |
The pH of the medium is one important variable, which significantly affect the extent of adsorption of fluoride. Fig. 8 shows the effect of the initial solution pH on fluoride adsorption onto H1, H2 and H3 at the given conditions. Clearly, the maximum defluoridation capacity (DC) is recorded at pH = 5.69 and shows a gradual decreasing trend with increases in the solution pH. The reduction of fluoride removal in the alkaline pH range should be attributed to competition of hydroxyl ions with fluoride for adsorption sites because of the similarity in charge and ionic radii for fluoride and the hydroxyl ion.
Data from the adsorption isotherms are modeled using the Langmuir and Freundlich isotherm models with the resulting isotherm constants presented in Table 2.
Adsorbent | Adsorption model | Relevant parameter | 308 K | 318 K | 328 K |
---|---|---|---|---|---|
H1 | Langmuir | Qm (mg g−1) | 19.194 | 24.876 | 32.030 |
a | 0.181 | 0.168 | 0.144 | ||
R2 | 0.9997 | 0.9884 | 0.9772 | ||
Freundlich | n | 2.045 | 1.873 | 1.814 | |
KF | 3.973 | 4.575 | 4.974 | ||
R2 | 0.9781 | 0.9869 | 0.9772 | ||
H2 | Langmuir | Qm (mg g−1) | 17.544 | 23.866 | 29.412 |
a | 0.318 | 0.25 | 0.191 | ||
R2 | 0.9396 | 0.974 | 0.9914 | ||
Freundlich | n | 2.599 | 2.211 | 2 | |
KF | 5.562 | 6.109 | 6.142 | ||
R2 | 0.8972 | 0.9647 | 0.9704 | ||
H3 | Langmuir | Qm (mg g−1) | 12.180 | 20.202 | 24.450 |
a | 0.469 | 0.246 | 0.163 | ||
R2 | 0.9183 | 0.9526 | 0.9233 | ||
Freundlich | n | 3.293 | 2.149 | 1.985 | |
KF | 5.033 | 5.018 | 4.711 | ||
R2 | 0.9152 | 0.9572 | 0.9242 |
Langmuir model
Freundlich model
As observed in Fig. 9 and Table 2, fluoride adsorption onto H1 is well described by the Langmuir model. It indicates that homogeneous distribution of active sites on the adsorbents surface and the adsorption of fluoride occur in a monolayer adsorption manner. The Langmuir model of H2 is not as good as that of H1 on account of the participation of physical adsorption in H2. H3 is well described by both models, it indicates that H3 is dominated by physical adsorption, and it only belongs to the Langmuir model when the pores are sufficiently small. Furthermore, as the temperature increases from 35 °C to 55 °C, a positive effect is observed on the adsorption of fluoride (Table 2). This phenomenon is because of the increased tendency of fluoride attached to filtering materials, which may also indicate that the adsorption of fluoride onto filtering materials is endothermic in nature. To study the feasibility of the process, the thermodynamic parameters were obtained from the following equations.
ΔGθ = −RT![]() ![]() |
The value of Kθ can be obtained from the intercept of a plot of ln(Qe/Ce) vs. Ce, in which Ce is the equilibrium concentration (mg L−1), and Qe is the amount adsorbed at equilibrium (mg g−1). The values of ΔHθ and ΔSθ can be obtained from the slope and intercept of a plot of lnK vs. 1/T and the results are presented in Table 3. The adsorption of fluoride onto H1, H2 and H3 are endothermic in nature.
Adsorbent | Temperature | K | ΔG (kJ mol−1) | ΔH (kJ mol−1) | ΔS (J mol−1 K−1) |
---|---|---|---|---|---|
H1 | 308 K | 2.017 | −1.796 | 27.889 | 81.796 |
318 K | 2.181 | −2.061 | |||
328 K | 2.308 | −2.281 | |||
H2 | 308 K | 1.300 | −0.672 | 14.246 | 51.490 |
318 K | 1.451 | −0.954 | |||
328 K | 1.505 | −1.047 | |||
H3 | 308 K | 1.102 | −0.248 | 9.571 | 33.345 |
318 K | 1.239 | −0.548 | |||
328 K | 1.243 | −0.557 |
Al3+ + 4OH− → [Al(OH)4]− | (1) |
Ca10(PO4)6(OH)2 + [Al(OH)4]− → Ca10(PO4)6OH·Al(OH)4 + OH− | (2) |
During the defluoridation procedure, electrostatic adsorption can be encouraged as positively charged filtering material contacts with F−. Moreover, the large number of –OH functional groups in the crystal lattices are capable of conducting replacement reactions or ion exchange reactions with F− in water. In addition, [Al(OH)4]− and Ca10(PO4)6OH·Al(OH)4 are produced during the copolymerization process for this type of material, which makes it possible for the occurrence of chemical adsorption between them and fluoride ions. Moreover, the HAP–PAC copolymerization material is also accompanied by the generation of a hydrolytic condensation product [Al13O4(OH)24]7+ and gel [Al(OH)3].26 The ligand hydroxyl ions embedded in these products can exchange with fluorine ions.
Based on the comprehensive analysis of these three types of filtering materials, it can be theorized that the defluorination process of H1 is dominated by chemical adsorption and partly accompanied by physical adsorption, of which the main reaction equations are expressed as below ((7)–(12)). Both electrostatic adsorption and partial chemical adsorption will occur during the defluorination process of H2, its reaction equations being shown as below ((3)–(12)). Physical adsorption is the main reaction form on the surface of H3 when contacting with F− (moreover, unbroken ingredients of HAP may also conduct relatively weaker electrostatic adsorption and ion exchange process), its chief reaction equations are conveyed as below ((3)–(6)).
Physical adsorption process:
[AlxCa10−x(PO4)6Cly(OH)z](x+2−y−z)+ + nF− → [AlxCa10−x(PO4)6Cly(OH)z](x+2−y−z)+…nF− | (3) |
[AlxCa10−x(PO4)6Cly(OH)z](x+2−y−z)+ + (x + 2 − y − z)F− → [AlxCa10−x(PO4)6Cly(OH)z]…Fx+2−y−z | (4) |
Ca10(PO4)6(OH)2 + nF− → Ca10(PO4)6(OH)2…nF− | (5) |
[Al2(OH)nCl6−n]m + nF− → [Al2(OH)nCl6−n]m…nF− | (6) |
Chemical adsorption process:
[AlxCa10−x(PO4)6Cly(OH)z](x+2−y−z)+ + mF− → [AlxCa10−x(PO4)6Cly(OH)z−mFm](x+2−y−z)+ + mOH− | (7) |
[AlxCa10−x(PO4)6Cly(OH)z](x+2−y−z)+ + zF− → [AlxCa10−x(PO4)6ClyFz](x+2−y−z)+ + zOH− | (8) |
Ca10(PO4)6OH·Al(OH)4 + xF− → Ca10(PO4)6(OH)1−yFy·Al(OH)4−x+yFx−y + xOH−, (0 ≤ y ≤ 1, 0 ≤ x ≤ 5) | (9) |
[Al(OH)4]− + xF− → [Al(OH)4−xFx]− + xOH−, (0 ≤ x ≤ 4) | (10) |
[Al13O4(OH)24]7+ + xF− → Al13O4(OH)24−xF7+x + xOH−, (0 ≤ x ≤ 24) | (11) |
Al(OH)3 + xF− → Al(OH)3−xFx + xOH−, (0 ≤ x ≤ 3) | (12) |
The HAP–PAC copolymerization material can trap the particles in water during the procedure of defluorination. Then, these particles, treated as adsorbates, will precipitate together with the materials. Through this inner mechanism, the goal of fluoride removal in water can be thoroughly achieved. The general procedure of fluoride removal is illustrated in Fig. 10.
(2) The copolymerized HAP–PAC material prepared by means of aluminum chloride crystallization is characterized by the chemical combination between hydroxyapatite and poly aluminum chloride, and a certain amount of Ca2+ and OH− in HAP crystal lattice is partially doped and replaced by Al3+ and Cl− in PAC. The structure of the copolymerization material possesses a highly homogeneous structure. Moreover, its highest DC can reach up to 18.12 mg g−1 when the Al/Ca molar ratio is 0.22, an increase of 14.02 mg g−1 when compared with pure hydroxyapatite, and the fluoride removal process is mainly dominated by chemical adsorption process (ion exchange).
(3) As for the filtering material prepared by bauxite, a small part of Ca2+ and OH− in HAP crystal lattice are doped and replaced by Al3+ and Cl− in PAC, and both chemical combination and physical combination will occur during this procedure while the degree of uniformity is relatively weaker on account of the co-existence of HAP, PAC, and copolymerization material. The maximum DC is 13.72 mg g−1 at the optimal Al/Ca molar ratio 0.22. Electrostatic attraction and ion exchange are the two main processes for defluorination.
(4) In consideration of the filtering material prepared by physical mixing, the combination between HAP and PAC is mainly physical effects, with its highest DC reaching 13.08 mg g−1 at the best Al/Ca molar ratio 0.132. Physical adsorption is the governing form during this procedure of defluorination.
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