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Original article
11 2022
:15;
104209
doi:
10.1016/j.arabjc.2022.104209

Efficiency of a novel nitrogen-doped Fe3O4 impregnated biochar (N/Fe3O4@BC) for arsenic (III and V) removal from aqueous solution: Insight into mechanistic understanding and reusability potential

Multiscale Computational Materials Facility, Key Laboratory of Eco-Materials Advanced Technology, College of Materials Science and Engineering, Fuzhou University, Fuzhou 350100, China
Department of Chemistry, University of Chakwal, Pakistan
National Higher School of Chemistry (NHSC), University Ibn Tofail, BP. 133-14000, Kenitra, Morocco
Laboratory of Advanced Materials and Process Engineering (LAMPE), Faculty of Science, Ibn Tofail University, BP 133, 14000, Kenitra, Morocco
College of Agricultural and Environmental Sciences, Makerere University, Uganda
Laboratoire Matériaux et Environnement LME, Faculté des Sciences, Université Ibn Zohr, BP 8106, Cité Dakhla, Agadir, Morocco
Department of Chemical Engineering, Universitat Rovira i Virgili, 43007, Tarragona, Spain
Department of Ocean Science and Engineering, Southern University of Science and Technology, Shenzhen, China
Institute for Advanced Study, Shenzhen University, Shenzhen, Guangdong 518060, China
School of Chemistry and Chemical Engineering, Beijing Institute of Technology, Beijing 100081, China
Department of Chemical Engineering, Khwaja Fareed University of Engineering and Information Technology, Rahim Yar Khan 64200, Pakistan
Shaanxi Key Laboratory of Earth Surface System and Environmental Carrying Capacity, College of Urban and Environmental Sciences, Northwest University, Xian, Shaanxi 710127, China
School of Material Science and Engineering, Northwestern Polytechnical University, 71002, Xian, China
Department of Agronomy, University of Agriculture, Faisalabad 38000, Pakistan
Department of Environmental Sciences & Engineering, Government College University Faisalabad, Pakistan
College of Economics and Management, Jilin Agricultural University Changchun, Jilin, China
College of Chemistry and Life Sciences, Zhejiang Normal University, Jinhua 321004, Zhejiang, China
College of Geography and Environmental Sciences, Zhejiang Normal University, Jinhua 321004, China
Materials Design and Manufacture Simulation Facility, School of Advance Manufacturing, Fuzhou University, Jinjiang 362200, China
National Engineering Laboratory for Lake Pollution Control and Ecological Restoration, Chinese Research Academy of Environmental Sciences, 10012, Beijing, China
School of Chemistry and Chemical Engineering, Northwestern Polytechnical University, Xian, China

⁎Corresponding authors. wubo@fzu.edu.cn (Bo. Wu), Dr.AQ.Geographer@gmail.com (Abdul Qadeer), zeeshan@nwpu.edu.cn (Zeeshan Ajmal)

Disclaimer:
This article was originally published by Elsevier and was migrated to Scientific Scholar after the change of Publisher.

Peer review under responsibility of King Saud University.

Abstract

Abstract

Worldwide, arsenic contamination has become a matter of extreme importance owing to its potential toxic, carcinogenic and mutagenic impact on human health and the environment. The magnetite-loaded biochar has received increasing attention for the removal of arsenic (As) in contaminated water and soil. The present study reports a facile synthesis, characterization and adsorption characteristics of a novel magnetite impregnated nitrogen-doped hybrid biochar (N/Fe3O4@BC) for efficient arsenate, As(V) and arsenite, As(III) removal from aqueous environment. The as-synthesized material (N/Fe3O4@BC) characterization via XRD, BET, FTIR, SEM/EDS clearly revealed magnetite (Fe3O4) impregnation onto biochar matrix. Furthermore, the adsorbent (N/Fe3O4@BC) selectivity results showed that such a combination plays an important role in targeted molecule removal from aqueous environments and compensates for the reduced surface area. The maximum monolayer adsorption (Qmax) of developed adsorbent (N/Fe3O4@BC) (18.15 mg/g and 9.87 mg/g) was significantly higher than that of pristine biochar (BC) (9.89 & 8.12 mg/g) and magnetite nano-particles (MNPs) [7.38 & 8.56 mg/g] for both As(III) and As(V), respectively. Isotherm and kinetic data were well fitted by Langmuir (R2 = 0.993) and Pseudo first order model (R2 = 0.992) thereby indicating physico-chemical sorption as a rate-limiting step. The co-anions (PO43-) effect was more significant for both As(III) and As (V) removal owing to similar outer electronic structure. Mechanistic insights (pH and FTIR spectra) further demonstrated the remarkable contribution of surface groups (OH, –NH2 and –COOH), electrostatic attraction (via H- bonds), surface complexation and ion exchange followed by external mass transfer diffusion and As(III) oxidation into As(V) by (N/Fe3O4@BC) reactive oxygen species. Moreover, successful desorption was achieved at varying rates up to 7th regeneration cycle thereby showing (N/Fe3O4@BC) potential practical application. Thus, this work provides a novel insight for the fabrication of novel magnetic biochar for As removal from contaminated water in natural, engineering and environmental settings.

Keywords

Adsorption
Arsenic
Engineered adsorbents
Biochar
Desorption
Water contamination
1

1 Introduction

Toxic compounds such as heavy metal (loids) especially, arsenic (As) adversely affect to the human health and the natural environment mainly associated with its high toxicity, mutagenic and carcinogenic characteristics (Chakraborti et al., 2016; Qadeer et al., 2020; Essekri et al., 2022). Mineral weathering, geochemical reactions, mining, erosion, oil exploitation and As-bearing pesticides application have been reported as major source of groundwater As contamination (Gong et al., 2011). Depending upon pH and the redox potential, As contamination in water and soil can exist in different inorganic species such as; arsenite, As(III) and arsenate, As(V) and in organic form as; methylated As arsenocholine, and/or arsenobetaine (Urík et al., 2009; Zhang et al., 2017). In oxygen-rich environment (250–750 mV), the As (V) can exist in the form of H2AsO4-, H3AsO4, HAsO42- and AsO43-. Whereas, under oxygen-deficient environments (-250 to +250 mV), As(III) species are mainly dominant in the form of Arsenious acid (H3AsO3) at pH 1–9, which is in turn transformed into H2AsO3- as the solution pH approaches 12 at − 250 to − 500 mV redox (Kumarathilaka et al., 2018). To minimize its threshold level in an aquatic environment, many regulation authorities set an optimum threshold contaminant level of about 10 μg L−1 in drinking water (Fisher et al., 2015; Qadeer et al., 2022; Qadeer et al., 2022). In order to achieve low contamination level in water, several treatment strategies are employed including; coagulation, flocculation, photodegradation, ion exchange, chemical precipitation membrane filtration, and solvent extraction and adsorption (Yn et al., n.d.; Ff and Qi, 2011; Chen et al., 2019; Zhang and Jiang, 2019; Meng et al., 2020; Zhang et al., 2021; Ajmal et al., 2021; Hayat et al., 2022). These techniques are, however, associated with low adsorption/desorption capacities with high operational costs (Ajmal et al., 2020; Hayat et al., 2022; Brini et al., 2021). Notably, a positive bias towards adsorption technique is gaining more attention due to its high flexibility in design, ease in operation, and no sludge production and cost-effectiveness (Usman et al., 2018; He et al., 2016). To this end, various adsorbents including magnetite nano-particles (Wang et al., 2010), surface modified biochar’s (Ali et al., 2020; Ying et al., 2013), and granular activated carbon (Adeo et al., 2011) have been tested for the treatment of As contaminated water. Although the application of adsorption is somehow efficient, but the associated high cost most often limits their large-scale application (Ahmed et al., 2018; Khorram et al., 2016; Malik et al., 2021; Li et al., 2022). To minimize their high operational costs, the search for low cost, but highly efficient alternative sorbents is ongoing (Kizito et al., 2017; Wu et al., 2017; Ahmed et al., 2021; Hayat et al., 2022). The use of engineered surface adsorbents from agricultural-biomass has occupied a center stage by providing a low-cost alternative. Biochar (BC) is regarded as a potent raw material for making engineered adsorbent for aqueous separation processes (Hao et al., 2000; Kosik et al., 2020; Qadeer et al., 175 (2021)). In pristine form, the use of BC in aqueous separation is limited to its surface area, low contaminant specificity, and low end-process recovery (Naiya et al., 2009). After sorption, filtration and centrifugation steps are required for its efficient separation and irreversible sorption means that there are limited sorption sites to affect the second cycle contaminant removal. This phenomenon in turn limits the industrial scale BC application. However, to improve BC separation and species specificity during adsorption and regeneration (free of active sites) process, it’s a prerequisite to modify and activate BC before being used as an effective adsorbent material (Bakouri et al., 2010; Pan et al., 2022).

For the case of As sorption, BC pretreatment or modification is an important step to increase sorption effectiveness and efficiency. In particular As(III) and As(V) adsorption capacities on pristine BC is generally known to be low owing to its more negative charge on its surface (Mudhoo et al., 2011). In literature, various BC modification techniques have already been employed to improve its porosity, functional groups, surface area and point of zero charge (pHpzc) (Jin et al., 2014). These strategies include, activation by alkaline/acidic solutions, impregnation with nanoparticles of iron (Fe) and nano zero valent metals and conjugation with functional groups such as amides and thiols (Tan et al., 2015). Most recently, modification of biochar with Magnetite (Fe3O4) is receiving incredible research attention owing to its structural FeII presence, high stability, more reactive surface sites, and good surface chemistry (Usman et al., 2013; Duan et al., 2018; Xi et al., 2021; Zhang et al., 2021). Furthermore, magnetic surface modification has been envisaged to offer a promising solution in terms of fast pollutant recovery associated with its high separation characteristics by applying external magnetic field. The use of magnetic biochar was encouraged to recover metal ions from contaminated water (Baokang et al., 2018). Moreover, for enhanced metal (loids) adsorption, nitrogen (N) doping has also been considered as a valuable aspect in sorption studies, mainly due to attracting anionic species (arsenic), but depending upon solution pH. The analysis of N doping could provide a highly positive charged sorption sites and ultimately enhance material adsorption characteristics towards anionic species (Yoo et al., 2018). For instance, the N-doped aquatic animal waste BC has already been reported for enhanced nickel (Ni) ions removal from contaminated water (Yin et al., 2019). The N-doping effect on corn straw derived BC for the adsorption of copper (Cu) and cadmium (Cd) was observed to be more significant (Usman et al., 2012). To the best of our knowledge, there exist enormous studies on N-doped BC to evaluate its effectiveness for the elimination of metal (loids) for aqueous solution (Chen et al., 2022; Wan et al., 2019; Wang et al., 2021).

However, there is no information available in order to draw a solid conclusion towards As(III) and As(V) removal from aqueous solution by using a Fe3O4 impregnated N-doped biochar. Thus, the main objective of the present study is: (i) to carry out the facile synthesis and characterization of magnetic (N/Fe3O4@BC) in order, (ii) to evaluate the sorption capacity (including the underlying mechanisms) for As(III) and As(V) from aqueous solutions, (iii) and evaluate its separation, regeneration and reuse in continuous sorption process. Furthermore, the mechanistic evaluation was also investigated by using different models and integration techniques. It is expected that this study would prove a milestone for the ongoing research efforts for water purification from both engineering aspect and scientific approach under natural and environmental settings.

2

2 Experimental section

2.1

2.1 Material preparation and characterization

The preparation of magnetite nano-particles (MNPs) was carried out according to the procedure reported previously (Usman et al., 2012). The biochar preparation was carried out via slightly modified the method described earlier (Harikishore Kumar Reddy and Lee, 2014). Briefly, the wood pellets were cut into small pieces, and then transformed into powder form followed by washing and drying at 105 °C for 24 h. The magnetic biochar synthesis was carried out by immersing the as-obtained wood powder about 50 g by vigorous stirred (30 min) 500 mL solution of 9.25 g Ferric sulfate (Fe2(SO4)3⋅9H2O) and 10 g of Iron(II) sulfate (FeSO4). The solution pH was maintained in the range of (10–11) using 10 M sodium hydroxide (NaOH). Thereafter, the resultant mixture was dried at 65 °C followed by calcination at 550 °C for 150 min under nitrogen environment (Harikishore Kumar Reddy and Lee, 2014). A range of characterization techniques were used to determine the physico-chemical characteristics of the developed adsorbent. The Brunauer–Emmett–Teller (BET) surface area properties were investigated by using BELSORP MAX (BEL, Japan. Inc). The X-ray spectra by using Cu Kα radiation source were recorded on X-ray diffractometer (SHIMADZU XRD-6000). The scanning electron microscopic images were captured over (SEM, ZEISS SUPRA 55). The Fourier-transform infrared spectroscopy (FTIR) spectra were recorded within an intensity range of (400–4000 cm−1) on FTIR measure equipment (FT-IR, Bruker Vector 22).

2.2

2.2 Batch experiments

Adsorption of As(III) and As(V) was evaluated by batch adsorption trials. Synthetic As(V) and As(III) stock solutions (1000 mg/L) were prepared through disodium hydrogen arsenate (Na2HAsO4·7H2O Fluka, > 98 %) and sodium arsenite (Na3AsO4 Fluka, > 98 %). From the stock concentration, several dilutions (1–50 mg/L) were made. The solution pH was adjusted between 2 and 11 by using 0.1 M NaOH or HCl. The effect of different parameters on As(III & V) sorption was investigated by varying several parameters such as; reaction time was varied from 5 min to 24 h, the initial As concentration was varied from (1–35 mg/L), the phosphate concentration was varied from (1–6 mg/L), pH (2–11), and temperature (15–55 °C). The sorption vials were placed in water bath shaker at a constant agitation speed 150 rpm. At the end of each reaction time, about 5 mL of supernatant was collected and filtered through 0.45 µm syringe filter. The optimum adsorption capacity (mg/g) and removal (%) of As(V) was calculated after measuring residual adsorbate concentration of filtrate sample via molybdenum blue method as described by (Spectro molybdate method) at 880 nm (Dhar et al., 2004), via UV–vis spectrophotometer, and then, adsorption capacity on the basis of residual concentration was calculated through Eqs.1 and 2... C o - C e C o × 100

(1)
R e m o v a l % = C o - C e C o × 100 C o - C e C o × 100
(2)
q e = C o - C e M × V
where Ce and Co are the final and initial metal ions concentrations (mg/L) in aqueous medium, qe (mg/g) is the adsorbed amount per (g) of tested adsorbent, M represent the total adsorbent mass (g), while V is solution volume (L).

2.3

2.3 Desorption and regeneration tests

To investigate saturated particle regeneration potential for the developed adsorbent, the recovered particles were subject to several desorption/re-sorption trials using same pollutant concentrations and under similar conditions as those used with fresh particles. Desorption experiments were carried out by using deionized water and alkaline solutions. The adsorbate-loaded samples were centrifuged and the supernatant was decanted and discarded. Desorption was initiated by adding 10 mL of 0.1 M NaOH solution and agitated for 24 h. After agitation, the supernatant was filtered through 0.45-µm propylene syringe. Total desorbed concentration was measured through previously described adsorption estimation method. Prior to next adsorption experiments, the material was separated out, and oven dried (at 105 °C for 24 h). The dried particles were then used for subsequent adsorption/desorption/regeneration analysis. The percentage (%) desorption performance was calculated through Eq. (3):

(3)
D e s o r p t i o n % = C V X m × 100 C o - C e C o × 100

Where; C denotes desorbed metal ions concentration (mg/L), x is adsorbed capacity of metal ions prior to desorption (mg/g), m represents the total mass of particle, which is used in desorption analysis (g), while V denotes the desorption solution volume (L).

3

3 Results and discussion

3.1

3.1 Materials characterization

Characterization results showed that the surface area properties, like pristine BC surface area characteristics were found to be superior than magnetite modified biochar Fe3O4@N/BC as shown in Table 1. Conversely, the lower porosity characteristics after magnetic modification are closely associated with the blockage of fine pores from iron species, which in turn led to the loss of micro-porosity (Kumar et al., 2014). Moreover, the decrease in surface area properties are due to the presence of higher proportion of iron layer over pristine BC surface sites, and ultimately led to decline in surface area (Chen et al., 2011).

Table 1 The physico-chemical properties of tested materials used in this study.
Adsorbent Sample BET SSA (m2/g) Pore volume cm3/g Pore diameter (nm) PZC
Magnetic biochar (N/Fe3O4@BC) 109.40 0.447 16.3 8.2
Biochar (BC) 123.07 0.442 38.8 7.7
Magnetite nano-particles (MNPS) 72.20 0.411 23.0 7.1

SSA; specific surface area, PZC; point of zero charge.

The variations in BC and (N/Fe3O4@BC) crystallographic structure were characterized by X-ray Powder Diffraction (XRD) Fig. 1a. A clear difference in XRD diffractograms of pristine BC and (N/Fe3O4@BC) was observed. A clear peak, especially at 30.19 Ao was observed for (N/Fe3O4@BC). According to Wang et al., (Wang et al., 2015), these new peaks onto N/Fe3O4@BC were closely associated with the presence of Fe3O4. Moreover, the peaks at 42.13 Ao are an indication of cubic iron oxides particles over (N/Fe3O4@BC). The corresponding peaks at 57.43 Ao for (N/Fe3O4@BC), further indicates the occurrence of Fe3O4 (di-iron oxide, magnetite). The FTIR spectra were also recorded for MNPs, BC and Fig. 1b–d. Some new additional bands specifically at 501–585 cm−1 were observed for MNPs and BC, thereby indicating the presence of Fe–O surface functional group (Baig et al., 2014). Moreover, the basic proportion of K and Ca content, and Mg were considerably higher in pristine BC as compared to MNPs and (N/Fe3O4@BC). However, according to EDS spectra the contents of Fe were found higher in MNPs followed by (N/Fe3O4@BC) and BC.

(a) XRD diffractogram and, (b-d) FTIR spectrum of all tested magnetite (N/Fe3O4@BC, BC, MNPs) before and after arsenic As(II) and As(V) adsorption.
Fig. 1
(a) XRD diffractogram and, (b-d) FTIR spectrum of all tested magnetite (N/Fe3O4@BC, BC, MNPs) before and after arsenic As(II) and As(V) adsorption.

The EDS spectra of N/Fe3O4@BC also indicated a sharp line showing the existence of Fe impregnation into N/Fe3O4@BC matrix shown in Fig. 2. Overall, all tested adsorbent surface sites were uniform in content, and containing a lot of irregular shaped material, as well as a wide range of undesirable particle aggregation Figure. 1Sƚ. In comparison, (N/Fe3O4@BC)exhibited lower carbon content, which obviously indicated that magnetic modification process results into the loss of organic matter contents Fig. 2 (Perlman et al., 267 (1992)).

EDS spectra of all tested adsorbent before and after As(III & V) adsorption.
Fig. 2
EDS spectra of all tested adsorbent before and after As(III & V) adsorption.

3.2

3.2 Adsorption characteristics

3.2.1

3.2.1 Effect of as initial concentration

Optimum adsorption performance of tested materials is utterly associated with initial solution concentration since, it drives mass transfer rate underneath elevated concentration ranges between bulk liquid to solid interfaces (Auta and Hameed, 2013). The results of Fig. 3a & b, show the variation in solution concentration for As adsorption towards tested material surface sites within examined concentrations ranges (1–5 mg/L). The adsorption capacity (mg/g) and adsorption efficiency (%) indicated an entirely reverse order against elevated As solution concentration. From the Fig. 3a & b, it is clearly apparent that As(III, V) adsorption was increased by increasing initial solution concentration (1–35 mg/L) (Co–Ce), while that of % removal was decreased. The maximum adsorption rate at highest concentration (35 mg/L) was observed to be 43.74 mg/g for As(III) and 23.69 mg/g for As(V) in (N/Fe3O4@BC)followed by 23.94 mg/g for As(III) and 12.45 mg/g for (As(V) in BC and 18.10 mg/g for As(III) and 16.30 mg/g for As(V) in MNPs. On the other hand, declining in % removal could be a better elaboration of higher ionic gradient built up against fixed low adsorbent dosage (fixed number of active surface sites) (Bellacosa et al., 1998). The increase in adsorption capacity by increasing adsorbate concentration could be better elaborated via Eq. (2). The plausible explanation could be that the N/Fe3O4@BC might have more surface interaction sites after N doping and magnetic core shell structure depending upon adsorbate species interaction and the adsorbent interstitial space, those are responsible for adsorption process (Yu et al., n.d.).

Adsoprtion of Arsenic As (III & V) as a function of (a, b) initial concentration (c, d) reaction time (e, f) Temperature (g, h) Solution pH (i) Phosphate concentration.
Fig. 3
Adsoprtion of Arsenic As (III & V) as a function of (a, b) initial concentration (c, d) reaction time (e, f) Temperature (g, h) Solution pH (i) Phosphate concentration.

3.2.2

3.2.2 Effect of contact time

Contact time is considered as an important parameter in adsorption studies for target pollutant elimination (Ajmal et al., 2018). The present study reports As(III & V) adsorption as a function of reaction time by determining the relationship between adsorption capacity and material surface characteristics. It was found that initial rapid As uptake rate was more obvious within a shorter period of time of 15, 30 and 60 min for (N/Fe3O4@BC), BC and MNPs respectively. Thereafter, a declining pattern was started, where adsorption became slower until attained equilibrium (Fig. 3c & d). It can be seen that the surface adsorption was quick towards all tested materials surface sites in the order of (N/Fe3O4@BC) > BC > MNPs), respectively. All these characteristics clearly indicate the availability of more surface-active sites by producing external adsorption phenomenon towards nano-porous surface sites of tested adsorbents at the early stages of reaction, while in case of equilibrium point, porous and highly active surface adsorption site comparatively required more time to reach at equilibrium. This trend could be attributed to higher surface area and well porosity characteristics of the developed adsorbents, which should be further explored for potential realistic implication of tested materials. Conversely, a rapid uptake rate could be better explained in terms of larger driving forces existence at initial phases and therefore, initial rapid and highest adsorption capacity was more obvious (vertical curve established) for all tested material onto their porous surface sites (Nassar, 2010). The observed highest uptake capacity for As(III) and As(V) were (18.14, 9.87 mg/g) for (N/Fe3O4@BC), (9.89, 8.12) for BC and (7.38, 8.56 mg/g) for MNPs. Therefore, it is clearly understood that the magnetic modification of (N/Fe3O4@BC) was effectively involved in As sorption from bulk liquid to solid interface during adsorption process.

3.2.3

3.2.3 Effect of reaction temperature

The adsorption of arsenic species as a function of temperature was evaluated within a temperature range from 288 to 328 K. The results Fig. 3e & f, demonstrated that adsorption capacity and % adsorption was enhanced with increasing temperature ranges from 288.15 K to 318.15 K, by a maximum adsorption capacity of 17.34 & 9.37 mg/g, for As(III) and (8.49 & 9.04) for As(V) onto (N/Fe3O4@BC), and MNPs, while for BC, the maximum adsorption of As(III) and As(V) was 10.16 ± 0.35 mg/g and 7.0 ± 0.14 mg/g) at 318.18 K and 328.15 K. The findings suggest that As removal is an endothermic process, and thereby temperature above ambient would be relatively suitable approach for higher adsorption for all tested adsorbents. The enhance in sorption capacity with increasing temperature could be due to decrease in solution viscosity and high free energy, which in turn promotes As diffusivity from external laminar layer to adsorbent pores (Nassar, 2010). However, a slightly decreasing pattern for adsorption capacity, and % removal was observed at 318 K for (N/Fe3O4@BC)and MNPs, and at 338 K for BC. It further suggests, that exothermic process was started thereafter. Therefore, it was implied that endothermic interactions mainly govern the As adsorption process between 318.15 and 328.15 K and afterward exothermic interactions might be possible at higher temperature (338.15 K) leading decreased sorption.

3.2.4

3.2.4 Effect of solution pH

The solution pH is considered as a main influential parameter during the adsorption process (Ajmal et al., 2020). The adsorption of As(V) and As(III) by all three tested adsorbents was examined over a wide range of pH from 3 to 11 as shown in Fig. 3g & h. The maximum As(V) adsorption of 11.31 mg/g for (N/Fe3O4@BC), 7.64 mg/g for BC and 9.56 mg/g for MNPs was observed at pH 6, pH 5 and pH 7 respectively, while pH 9, pH 7 and pH 8 were found to be the optimum pH values for As(III) adsorption at a rate of 16.10 mg/g, 9.04 mg/g and 8.05 mg/g for N/Fe3O4@BC, BC and MNPs respectively. It was found that alkaline conditions are unsuitable for both As(V) and As(III) adsorption onto MNPs, BC and (N/Fe3O4@BC). For example, the results of BC revealed that As adsorption increased, when pH increased from 3 to 5 for As (V) and 3 to 7 for As(III) and then declined on elevated pH, which indicated that As(III & V) adsorption onto BC surface sites was might be attributed to the Van der Waals interaction between BC surface and neutral H3AsO3 and H2AsO4 species. It is reported that dominant As(V) species are present as H2AsO-4, HAsO42- and AsO43- within the pH range between 2 and 14 respectively (Wei et al., 2016). Therefore, ability of tested adsorbent to adsorb metal ions decreases significantly by increasing pH. As we know that, lower pH is responsible for adsorbent surfaces sites protonation thus, higher adsorption is closely associated with higher electrostatic attraction as a result of increased protonation of material surface sites, which in turn enhanced aqueous arsenate anions, thereby boosting As(V) adsorption. With the rise of initial solution pH, the positively charged tested adsorbent surface sites gradually decreases, thus resulted an increase in electrostatic repulsion between liquid and solid interface hence, decreasing adsorption. Similar finding has been reported for As(V) adsorption onto iron oxides and iron-containing oxides and biochar surfaces (Min et al., 2006).

On the other hand, As(III) species such as H3AsO3- and H2AsO3- are mainly found at pH lower than 9.2, while that of AsO2 exists at pH higher than 9.2 (Zhang et al., 2016). Adsorption primarily occurred through the electrostatic attractions between negative As species and positively charged tested adsorbent surface sites. It means that the solution pH not only have significant impact onto material surface charge but also greatly influenced the speciation of As species in solution. More obviously, the MNPs could also play an important role to oxidize As(III) into As(V) based on solution pH. Therefore, higher adsorption of As(III) under near neutral pH (8) conditions could be due to higher As(III) oxidation into As(V), mainly, because of dissolved oxygen as well as oxidizing intermediate at neutral pH than that of higher or lower pH condition (Zhang et al., 2016; Luo et al., 2012). Moreover, the decrease of adsorption efficiency for all tested adsorbent at alkaline pH is attributed to the more electrostatic repulsion between and negatively charged tested magnetite surface sites and anionic As species (AsO2, HAsO42) (Luo et al., 2012). Because surplus OH groups exist at that stage and adsorption primarily might occurred via hydrogen bonding between adsorbate and adsorbent surface sites. Another possible reason could be higher competition between anionic (AsO2, HAsO42-) species and hydroxyl groups (OH) at higher pH condition (Shakoor et al., 2016). All tested adsorbents shown their point of zero charge about 8.2, 7.7 and 7.1. However, they can give rise to attraction below than these values or repulsion above these values depending upon adsorbate species charge and the adsorbent surface characteristics.

However, these results clearly indicate that the arsenic adsorption towards tested material surface sites was mainly controlled via two important phenomena: (i) electrostatic interaction (ii) As(III) oxidation between bulk liquid to solid interface (Shakoor et al., 2016). As(III) oxidation mainly occurred via contact with O2 and the oxic conditions that leads to Fe(III) drying. As, anoxic conditions mostly responsible for magnetite transformation into maghemite that could also drives the oxidation process (Navarathna et al., 2019). Overall, the higher (Qmax) of (N/Fe3O4@BC)compared to pristine MNPs and BC indicates As (III &V) adsorption (N/Fe3O4@BC)was due to surface complexation pathway (Luo et al., 2017).

3.2.5

3.2.5 Effect of phosphate on as adsorption

The result regarding the effect of phosphate onto As adsorption is displayed in Fig. 3i. In practical, ionic competition especially in real wastewater is more common due to multiple contaminant diversifications. It can be seen that as the concentration of phosphate was increased, then a significant reduction of both As(III) and As(V) was observed in (N/Fe3O4@BC)and MNPs samples. It means that the competing ions especially the phosphate have their significant impact over As species in real wastewater. It could be better explained in terms of similar charge properties as well as structural characteristics of phosphorus (P) in the form of PO43-, which could be strongly bounded over positively charged (N/Fe3O4@BC)and MNPs surface sites than that by As species mainly depending upon solution pH and redox potential (Vatutsina et al., 2007). The previous results also corroborate our investigation, where the presence of P showed a strong binding interaction with MNPs. Tuutijarvi et al. (2012) also reported that P ions have enough capability to influence the adsorption of As(V) over iron based maghemite particles surface sites at pH 7 with an initial concentration > 3 mg/L (Tuutijärvi et al., 2012). In case of pristine BC, the P as competing ions didn’t significantly affect As adsorption. It’s because of negative BC surface sites, which in turn created an electrostatic repulsion phenomenon. Furthermore, the higher concentration ranges of both competing ions should also be investigated for their potential practical application.

3.3

3.3 Adsorption data modeling

3.3.1

3.3.1 Adsorption isotherm

In general, adsorption isotherm studies are critical to determine dominant adsorption phase existence between bulk liquid to solid interface for engineered adsorption systems designing (Safa and Bhatti, 2011). Thus, equilibrium adsorption data was evaluated by using two commonly employed Langmuir (Langmuir, 1918) and Freundlich models (Freundlich, 1906). The mathematical expressions are given below, while the graphical representation is presented in Fig. 4a & b.

(4)
q e = K Q C e 1 + K C e ( L a n g m u i r m o d e l )
(5)
q e = K f C e n ( F r e u n d l i c h m o d e l )
where, K indicates Langmuir bonding term related to bonding energies (L/mg), Kf is Freundlich affinity coefficient (Ln/mgn-1g) Ce (mg/L) stands for residual concentration, Q (mg/g) denotes optimum Langmuir adsorption capacity, β (L/mg) represent equilibrium constant, K defines the adsorbed metal ions, and n specify the adsorption intensity. The n indicates Freundlich constant. The isotherm parameters for both As(III) and As(V) are listed in Table 2. The good fit of Langmuir model with higher correlation coefficient value (R2) indicates the homogeneous phase of adsorbent surface sites. Moreover, its better description could be possible by calculating its separation factor value (dimensionless). Its mathematical form is given below.
(6)
R = 1 / 1 + b C o
The equilibrium and kinetic adsorption data modeling (a, b) As(III & V) data mdeling via Langmuir and Freundlich model (c,d) As(III & V) data interpretation via Pseudo 1st, 2nd and Elovich model (e, f) As(III & V) data interpretation via Intraparticle model.
Fig. 4
The equilibrium and kinetic adsorption data modeling (a, b) As(III & V) data mdeling via Langmuir and Freundlich model (c,d) As(III & V) data interpretation via Pseudo 1st, 2nd and Elovich model (e, f) As(III & V) data interpretation via Intraparticle model.
Table 2 The profiles parameters and calculated Langmuir and Freundlich modeled values for As(III) and As(V) adsorption from aqueous solution by using N/Fe3O4@BC, BC and MNPs.
Material Langmuir Freundlich
Q (mg.g−1) K(L/mg) RL2 KF (Ln/(mg(n-1).g) n RF2
As(III)- N/Fe3O4@BC 66.80 0.056 0.993 5.86 1.73 0.966
As(III)- BC 34.78 0.055 0.971 3.08 1.75 0.940
As(III)- MNPs 28.25 0.059 0.990 2.49 1.72 0.946
As(V)- N/Fe3O4@BC 34.54 0.061 0.987 3.30 1.78 0.962
As(V)- BC 16.56 0.091 0.978 2.27 2.04 0.905
As(V)- MNPs 23.41 0.095 0.976 3.32 1.96 0.942

It represents the adsorption process is favorable, when 0 < RL < 1, unfavorable RL > 1, linear adsorption RL = 1 and RL = 0, irreversible adsorption (Ngah et al., 2002). In the present study, the separation factor values were 0 < RL < 1, which further indicated that As adsorption as more favorable process through monolayer surface adsorption sites with optimum monolayer adsorption capacity of 66.80 mg g−1, 34.28 mg g−1 and 28.25 mg g−1 for As(III) and 34.54 mg g−1, 16.56 mg g−1 and 23.41 mg g−1 for As(V) in the order (N/Fe3O4@BC) > BC > MNPs, respectively. Conversely, the successful applicability of Freundlich model (R2 > 0.95), indicated the favourability of As adsorption onto multilayer surface adsorption sites of tested adsorbents. Multilayer adsorption phase further indicated that adsorption was more suitable onto adsorbent for maximum pollutant removal in aqueous environments. On the other hand, the higher Kf values indicates easy removal of As(III) and As(V) ions from contaminated water to adsorbent surface sites. The Freundlich R2 values for both As(III) and As(V) are presented in Table 2. In addition, adsorption intensity (1/n) is considered as important factor in adsorption process, which represents the adsorption from bulk liquid to solid interface. If the values of adsorption intensity n are < 1, then the adsorption is considered poor, while that in between 1 and 2 indicates the moderately difficult adsorption, on the other hand, if n lies in between 2 and 10, the adsorption is considered excellent. Even though, all the Freundlich R2 values were > 0.95 indicating physical adsorption up to some extent, the values of 1/n, clearly indicate that high intensity of sorption towards all tested adsorbents (Tofan et al., 2016). The calculated 1/n values are listed in Table 2, and were found higher than 1, indicating more than one mechanism involved in As adsorption towards all tested-adsorbents.

3.3.2

3.3.2 Adsorption kinetics

Adsorption kinetic data was evaluated by using Pseudo first order, pseudo second order, Elovich (Gerente et al., 2007) and intraparticle models (Choy et al., 2004). Mathematical expressions are given below, while the graphical representation is presented in Fig. 4c & d.

(7)
d q t q t = K 1 ( q e - q t ) 2 ( P s e u d o f i r s t o r d e r m o d e l )
(8)
d q t q t = K 2 ( q e - q t ) 2 ( P s e u d o s e c o n d o r d e r m o d e l )
(9)
d q t q t = α e x p ( - β q t ) ( E l o v i c h m o d e l )
(10)
q t = K d t 1 / 2 + C Intraparticle model
where; qe, and qt (mg/g) are the equilibrium metal ions adsorption capacity at time t, k1 and k2 are first and second order apparent rate constants, while that of α indicates initial adsorption coefficient mg/g/h) and β indicates desorption constant (g/mg). The experimental q (mg/g) and calculated qe, (mg/g) values for maximum adsorption of As(III) and As(V) were compared. When experimental and calculated values of specific models are closer the reference, model would be considered to fit the experimental data very well. Another parameter is the correlation coefficient (R2), if its value is ≥ 0.95, then the model would be considered most suitable for kinetic experimental data interpretation. Conversely, the intraparticle and Elovich model were interpreted based on β, Kd and R2 values. In case of intraparticle, the model was considered to be fit if Qt vs t1/2 plot is linear. All the calculated modeled values (q1, q2, β, C) and rate constant (k1, k2, α and Kd) are listed in Table 3.
Table 3 The profile parameter and calculated modeled values for As(III) and As(V) adsorption onto Fe3O4@N/BC, BC and MNPs.
Material Pseudo 1st order Pseudo 2nd order Elovich Intraparticle
Qexp qe (mg/g) K1 (1/h) R2 qe (mg/g) K1 (g/mg/h) R2 α (mg/g) β (g/mg) R2 Kd (mg/g/min−1) C (mg/g) R2
N/Fe3O4@BC 17.6 17.9 0.029 0.988 20.7 0.0017 0.951 1.52 0.23 0.897 0.20 1.1 0.739
BC 7.99 8.04 0.027 0.968 9.14 0.0043 0.943 0.87 0.55 0.914 0.39 2.5 0.765
MNPs 7.12 7.29 0.026 0.955 8.22 0.0031 0.941 0.56 0.43 0.941 0.66 2.6 0.907
As (V)
N/Fe3O4@BC 9.37 9.48 0.028 0.992 10.89 0.0037 0.953 0.86 0.55 0.909 0.37 2.0 0.93
BC 7.52 7.62 0.025 0.982 8.81 0.0033 0.958 0.60 0.54 0.920 1.93 2.2 0.94
MNPs 8.26 8.33 0.022 0.962 9.71 0.0028 0.946 0.55 0.49 0.948 0.50 2.4 0.89

The fitted curves for all models are presented in Fig. 4c & d. Firstly, the assumption was made for intraparticle model Fig. 3e & f, where R2 values were ≤ 0.95 and straight lines were not passing through the origin and bilinear trend was more obvious (C ≠ 0), then the intraparticle diffusion as rate limiting step was rejected for all the tested adsorbents and the initial linear trend always indicates the involvement of film diffusion. Hence, the larger values of intercept clearly indicate the involvement of mutually external forces via (film and intra-particle), which are in counter play for As(III, V) adsorption onto tested adsorbent surfaces sites, and intraparticle is not rate limiting step (Tofan et al., 2016). Secondly, it was noted that higher correlation coefficient values of pseudo first order (0.99–0.98) rather than that of pseudo second (0.95–0.90) and Elovich (0.88–0.79) indicate the successful suitability for both As(III) and As(V), and the calculated (qecal) and the experimental values (qecal) were also found to be closer with each other. Thus, higher pseudo first order model correlation coefficient values than pseudo second order, thus implying the physio-sorption mechanism as more effective. Thus, our results totally contradict with certain previous investigation where As(III &V) adsorption over magnetite nano-particles, biochar and magnetic biochar were primarily governed by chemisorption mechanism owing to best fitting of experimental data to pseudo second order model (Jiaming et al., 2018). On the other hand, the sorption rate constant values of N/Fe3O4@/BC particles is higher than BC particles, thus these findings further suggest that As(III, V) sorption is not solely depends upon material superior surface characteristics, because if it is the cause then BC and MNPs must have larger adsorption rate constant. It further indicates that sorption via surface functional group might be more dominant over (N/Fe3O4@BC) particle than that of other tested adsorbents. In reality, by seeing BET surface area characteristics, one would expect MNPs and BC to be evidence for superior adsorption rather than (N/Fe3O4@BC) in aqueous solution.

3.3.3

3.3.3 Adsorption thermodynamics

Adsorption thermodynamics is an important parameter in adsorption studies. Variations in temperature plays an important role to evaluate material adsorption performance. The adsorption of As(III) and As(V) to materials surface sites was performed by varying the temperature from 288.15 K to 328.15 K. Vent Hoff equation was used for data fitting as manifested in Fig. 4e & f.

(11)
K d = C o - C e C e

The Ce and Co (mg/L) stands for final and initial metal ions concentrations. The Gibb’s free energy change (ΔG°), was calculated through Kd by Eq. (11) and Eq. (12).

(12)
Δ G o = - R T l n K c
(13)
ln K d = - Δ G o R T = - Δ H o R T + Δ S o R

The R is the ideal gas constant with value 8.314 J·mol−1·K−1 and T is the temperature (K). Thus, a graph between lnKd v/s 1/T gives the values of enthalpy (ΔH) and entropy (ΔS) change through its slope and intercepts values. All the calculated modeled parameters i.e., ΔH°, ΔG°, ΔS° and Kd with R2 for all temperatures to all tested adsorbents are listed in Table 4. From the concern Table, it can be seen that Kd values were enhancing by increasing temperature from (288.15 – 328.15 K). Thus, increasing Kc and positive ΔH° values suggest that adsorption is endothermic in nature. On the other hand, negative Gibb’s free energy ΔG° values suggest adsorption is mainly physical, spontaneous and more favorable by increasing temperature from 288.15 K to 328.15 K. The entropy changes values (ΔS° values for all tested adsorbents were in positives range). These positive entropies change values, further indicates the higher randomness with quick interaction between adsorbate/adsorbent interfaces by increasing thermostat temperature. The increase of sorption with temperature could be due to rapid reaction between As(III) and As(V) ions and adsorbent surface functional groups at higher temperature due to decreasing solution viscosity and high free energy, which in turn promotes the As diffusivity from external laminar layer to adsorbent fine pores (Xiong et al., 2015). Furthermore, it has been shown in literature, that at ΔH° < 25 kJ mol−1, the acting forces during adsorbate/adsorbent interaction would be Van der Waals forces and might be ascribed to physisorption but if ΔH° values are in between 40 kJ mol−1 and 200 kJ mol−1, then the main dominant forces would be the chemical bonding, thereby indicating the chemical adsorption phenomena (Xiong et al., 2015).

Table 4 Adsorption of As(III) and As(V) as a function of temperature. Thermodynamics adsorption data interpratation through ven’t hoff equation.
Temperature (K) Kd -ΔGo (J/mol) ΔHo(kj·mol−1) ΔSo (j·mol K−1) R2
N/Fe3O4@BC As(III)
288.15 1.82 1434.1 37.4 135.3 0.9412
298.15 3.29 2950.8
308.15 5.56 4397.0
318.15 11.3 6419.9
328.15 10.4 6387.1
BC
288.15 1.38 784.6 20.9 76.1 0.968
298.15 2.24 2006.2
308.15 2.73 2577.1
318.15 3.56 3359.7
328.15 4.13 3870.8
MNPs
288.15 1.26 546.2 14.9 53.8 0.760
298.15 1.46 930.8
308.15 2.07 1864.5
318.15 2.95 2862.9
328.15 1.75 2208.0
N/Fe3O4@BC As(V)
288.15 1.46 899.5 23.3 84.5 0.796
298.15 1.90 1596.4
308.15 3.70 3349.4
318.15 5.07 4295.8
328.15 3.84 3668.2
BC
288.15 1.13 294.8 10.9 39.0 0.752
298.15 1.32 690.1
308.15 1.67 1315.4
318.15 2.16 2033.5
328.15 1.39 1521.6
MNPs
288.15 1.32 666.9 18.4 66.3 0.927
298.15 1.75 1382.5
308.15 2.25 2073.4
318.15 3.31 3162.1
328.15 3.07 3056.3

3.4

3.4 Potential adsorption mechanism

Proposed adsorption mechanism was investigated using a series of parameters and FTIR spectra. The FTIR spectra of all tested adsorbents (N/Fe3O4@BC, BC and MNPs) before and after As adsorption are provided in Fig. 1b–d. As it can be seen from the virgin spectra of BC and MNPs, that all tested materials were found to have almost five distinct bands at 581, 579, 563 and 937, 937 and 933, 1143, 1141 and 1129, 1635, 1631 and 1634, 3440, 3431 and 3435 cm− 1 frequencies. These bands indicate Fe-OH stretching and bending vibrations hydroxyl groups, which are converted from the iron oxide in transient complex species form such as Fe-OH,-Fe(OH)2, or FeO(OH) onto tested (N/Fe3O4@BC), BC and MNPs surface sites (Tang et al., 2011). The band that shifts from 711 to 790 and 810–899 cm− 1 as well as 937, 937 and 933 cm− 1 in to 909, 904 and 915 cm− 1 and 901, 922 and 917 cm− 1, indicates As adsorption is might be due to As-O stretching band vibration in a partial As3 +→ Fe substitution (Baig et al., 2014). In addition, peaks attributable to C—H alkene (801–899 cm−1), C—O aloxy (1221–1238 cm−1), –C⚌O stretch (1508–1539 cm−1), C—H stretch (2876–2980 cm−1) were also observed for (N/Fe3O4@BC), BC and MNPs. After As(III) adsorption these band were shifted to 895, 899 and 889 cm−1, for (N/Fe3O4@BC), BC and MNPs. Similarly, the shift in band with corresponding peaks 1219.4, 1222.2 and 1242.3 was also observed after As(V) adsorption over, BC and MNPs (Alam et al., 2018). Moreover, after As(III) adsorption some peaks (583, 585 and 587) were shifted to 576, 580 and 579 for (N/Fe3O4@BC), BC and MNPs. In addition, some new peaks appeared at 683, 677, 763, 644 and 681 cm−1, which indicate some inorganic As compound adsorption. Intensities of some corresponding peaks at 1635, 1631, 1634 cm−1 and ∼ 3440, 3431, 3435 cm−1 were seems to be decreased, which clearly indicates surface OH groups involvement, which might be replaced by As(III) and As(V) after adsorption to form Fe-O As(III)/As(V) complex. However, broad band at 3440, 3450, 3460 cm−1 corresponding to OH stretching model shows hydrogen bonding and physisorbed water molecules (Chen et al., 2011). The peak originally at 3440 cm−1 which is commonly associated with As(III) and As(V) was shifted to 3387 cm−1 and 3464 cm−1 suggesting involvement of N—H amino (stretch) group. At the same time, the peak at 1587 cm−1 was shifted to 1595 cm−1 indicating involvement of N—H amino (bending) group. This is a clear indication of the successful adsorption of As(III) and As(V) over (N/Fe3O4@BC), BC and MNPs nanoparticles via interaction with OH groups. Moreover, higher adsorption of As(V) than that As(III) on MNPs, could be clearly seen as the absorption peak in the range of 810–899 cm−1 is more intense than that of 711–790–792 cm−1 over MNPs surface sites (Zhu et al., 2009). Overall FTIR spectra from 2800 to 3400 cm−1 and 650–1750 cm−1 indicate As species binding with adsorbent. Hence, all FTIR peaks variation after arsenic As adsorption indicated the involvement of surface, Fe-O, carbonyl group and specifically hydroxyl groups (Shakoor et al., 2016). The results of pH analysis as earlier discussed are consistent, where hydroxyl plays an important role with FTIR assumption during adsorption process.

However, the pH results clearly indicate that the As adsorption towards tested adsorbents surface sites was mainly controlled via two important phenomenon: (i) electrostatic interaction and (ii) Oxidation of As(III) into As(V) between bulk liquid to solid interface (Shakoor et al., 2016). Moreover, another interesting phenomenon was noticed whenever initial metal concentration was increased, then the final pH was found to be decreased. This indicates that the adsorption is dominated by an ion-exchange mechanism by BC and (N/Fe3O4@BC)surface sites substantial oxygen content including hydroxyl and carboxyl groups, and could be considered as active center for ion exchange phenomenon (Klimmek et al., 2001). Data better fitted to Langmuir model clearly indicates the dominance of monolayer adsorption via surface complex pathway, as the affinity of As to Fe/BC, and As–Fe complexation on (N/Fe3O4@BC) after H+ ions exchange in aqueous solution. Thus, our finding clearly demonstrates adsorption via electrostatic attraction, ion exchange and surface complexation pathways. Therefore, ion exchange mechanism could not be ignored during whole adsorption process. All in all, the deeper insights and multiple potential adsorption pathways further required a wide range of high level various spectroscopic techniques analysis.

3.5

3.5 Desorption characteristics

Recycling process of tested material after As ions removal is an important parameter for reducing the pollutant load in the environment (Naciri et al., 2019). Many studies have evaluated the desorption and spent adsorbents regeneration to determine their potential continuous application in pollutant removal. Desorption of As loaded adsorbent was determined by using distilled water, NaOH and H2SO4 solutions (Fig. 5a & b). Distilled water resulted into low desorption, which was found to be nearly 26.3, 23.6 and 24.1 % for As(III) in the order of, BC > MNPs > (N/Fe3O4@BC). The As(V) desorption was 27.5, 24.5 and 25.1 % in distilled water in the order of (N/Fe3O4@BC), BC and MNPs Fig. 5a & b. Maximum As(III) desorption up to 87.1, 91.3 and 81.1 % was observed in alkaline environment from (N/Fe3O4@BC), BC and MNPs. On the other hand, As(V) desorption from (N/Fe3O4@BC), BC and MNPs was 96.3 %, 94.2 % and 95.1 %. Herein, also the low desorption of As(III) compared to As(V) was also observed and that might be As(III) oxidation into As(V), which clearly proved in pH investigation of As(III) into As(V). Even though, the low concentration of As(V) was also observed in As(III) desorption solution. But the surprising fact is the As(III) concentration was also observed in As(V) desorption solution in the order of MNPs > (N/Fe3O4@BC) > BC. So, the As(V) reduction phenomenon up to some extent could not be ignored during whole adsorption process. The obtained data indicates that spent adsorbents could be used up to 5th regeneration cycles without substantial loss of adsorption capacity during consecutive adsorption/desorption cycles. The (N/Fe3O4@BC) particle showed better desorption as well as higher adsorption performance after 5 regeneration cycles owing to its good magnetic properties and easy separation Fig. 5c & d. After consecutive adsorption desorption cycles the higher adsorption performance of (N/Fe3O4@BC) and MNPs particle might be due to the breakdown of large bulks into small one which resulted into exposure of new surface adsorption sites for maximum pollutant adsorption. On the other hand, a complete desorption was not achieved throughout the experimentation, which can be better explained in terms of adsorbent surface sites passivation, strong chemical binding between adsorbent and adsorbate as well as oxidation/reduction reaction during consecutive adsorption/ desorption cycles (H.J. A et al.,2015). Decrease in adsorption of all tested adsorbents with the passage of consecutive regeneration cycles is due to loss of adsorption surface sites. Similar results of decrease in adsorption have been reported in literature (Kizito et al., 2017). Therefore, these materials could be used as cost-effective alternative over other adsorbents with remarkable regeneration potential to remediate As contaminated water and side remediation system.

Desorption performance of all tested adsorbents for As(III) and As(V) (a,b) as well as subsequesnt adsorption/desorption cycles (c, d) by using distilled water, alkaline eluents.
Fig. 5
Desorption performance of all tested adsorbents for As(III) and As(V) (a,b) as well as subsequesnt adsorption/desorption cycles (c, d) by using distilled water, alkaline eluents.

4

4 Conclusions

In this study, the application of nitrogen doped magnetic biochar (N/Fe3O4@BC) as potential adsorbent for As removal from aqueous solution was evaluated. The obtained results revealed that As adsorption was strongly affected by variation in material structural characteristics and solution pH. Higher adsorption performance by (N/Fe3O4@BC) was observed compared to pristine BC and MNPs. Overall, As(III) adsorption was found to be in the order of (N/Fe3O4@BC) > BC > MNPs, while in case of As(V) the MNPs exhibited higher adsorption than BC, and a reverse order was observed (N/Fe3O4@BC) > MNPs > BC. Kinetic and isotherm data were satisfactorily tailored by Pseudo first order and Langmuir model thereby suggesting the physio-chemical process was the rate-limiting step. The kinetic results further indicated that the external mass transfer and physisorption affect arsenic adsorption more significantly. An alkaline eluent was a better desorption strategy allowing material regeneration up to 5 adsorption cycles without significant loss in adsorption capacity. Based on the monolayer sorption maximum and the potential to regenerate/recover sorption capacity the developed magnetically modified and N-doped biochar could prove an effective adsorbent for the treatment of low-to moderately As contaminated water.

Acknowledgment

This work is financially supported by the National Natural Science Foundation of China (50971043, 51171046, 21973012), Key Research and Development Program of China (2017YFB0701700), Natural Science Foundation of Fujian Province (2021 J01590, 2014 J01176, 2018 J01754, 2020 J01474), National Key Laboratory of Eco-materials Advanced Technology (Fuzhou University), Fujian Province University (STHJ-KF1708), Student Research and Training Program (SRTP) of Fuzhou University (27297), State Administration for Market Regulation (2021MK050) and Fujian Provincial Department of Science & Technology (2021H6011).

Declaration of Competing Interest

The authors declare that they have no known competing financial interests or personal relationships that could have appeared to influence the work reported in this paper.

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Appendix A

Supplementary material

Supplementary data to this article can be found online at https://doi.org/10.1016/j.arabjc.2022.104209.

Appendix A

Supplementary material

The following are the Supplementary data to this article:

Supplementary data 1

Supplementary data 1

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