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2019

A comparative study of magnetic

chitosan (Chi@Fe3O4) and graphene oxide modified magnetic chitosan

(Chi@Fe3O4GO) nanocomposites for efficient removal of Cr(VI) from water

Subedi, N

Elsevier BV

Tieteelliset aikakauslehtiartikkelit

© Elsevier B.V.

CC BY-NC-ND https://creativecommons.org/licenses/by-nc-nd/4.0/

http://dx.doi.org/10.1016/j.ijbiomac.2019.06.151

https://erepo.uef.fi/handle/123456789/7731

Downloaded from University of Eastern Finland's eRepository

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A comparative study of magnetic chitosan (Chi@Fe3O4) and graphene oxide modified magnetic chitosan (Chi@Fe3O4GO) nanocomposites for efficient removal of Cr(VI) from water

Nabin Subedi, Anna Lähde, Emmanuel Abu-Danso, Jibran Iqbal, Amit Bhatnagar

PII: S0141-8130(19)31391-1

DOI: https://doi.org/10.1016/j.ijbiomac.2019.06.151

Reference: BIOMAC 12657

To appear in: International Journal of Biological Macromolecules Received date: 22 February 2019

Revised date: 29 May 2019 Accepted date: 20 June 2019

Please cite this article as: N. Subedi, A. Lähde, E. Abu-Danso, et al., A comparative study of magnetic chitosan (Chi@Fe3O4) and graphene oxide modified magnetic chitosan (Chi@Fe3O4GO) nanocomposites for efficient removal of Cr(VI) from water, International Journal of Biological Macromolecules, https://doi.org/10.1016/

j.ijbiomac.2019.06.151

This is a PDF file of an unedited manuscript that has been accepted for publication. As a service to our customers we are providing this early version of the manuscript. The manuscript will undergo copyediting, typesetting, and review of the resulting proof before it is published in its final form. Please note that during the production process errors may be discovered which could affect the content, and all legal disclaimers that apply to the journal pertain.

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A comparative study of magnetic chitosan (Chi@Fe3O4) and graphene oxide modified magnetic chitosan (Chi@Fe3O4GO) nanocomposites for efficient removal of Cr(VI)

from water

Nabin Subedia, Anna Lähdea, Emmanuel Abu-Dansoa, Jibran Iqbalb, Amit Bhatnagara,*

aDepartment of Environmental and Biological Sciences, University of Eastern Finland, P.O. Box 1627, FI-70211 Kuopio, Finland

bCollege of Natural and Health Sciences, Zayed University, P.O. Box 144534, Abu Dhabi, United Arab Emirates

*Corresponding author: amit.bhatnagar@uef.fi

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2 Abstract

Magnetic chitosan (Chi@Fe3O4) nanocomposite was synthesized and modified with graphene oxide (Chi@Fe3O4GO) and the potential of both materials as adsorbents was assessed for the removal of chromium (Cr(VI)) from water. The physico-chemical characteristics of magnetic nanocomposites were studied by Fourier transform infrared spectroscopy (FTIR), scanning electron microscopy (SEM), x-ray diffraction (XRD), Raman spectroscopy and Brunauer–

Emmett–Teller (BET). The synthesized adsorbents exhibited varied Cr(VI) removal efficiency at solution pH 2. The reaction kinetics correlated well with the pseudo-second- order model. The maximum adsorption capacity was found to be 142.32 and 100.51 mg g-1 for Chi@Fe3O4 and Chi@Fe3O4GO respectively. Analysis of thermodynamic parameters suggested that the reaction occurred spontaneously and was endothermic in nature.

Reusability studies showed that the adsorbents can be reused for up to 4th cycles of regeneration. Fixed bed column experiments revealed that the adsorption performance of Chi@Fe3O4 was affected by the flow rate, adsorbent loading and influent metal ion concentration. The results suggest that the prepared adsorbents have the potential to be used in removing Cr(VI) ions from contaminated water.

Keywords: Cr(VI); chitosan; graphene oxide; magnetic nanocomposite; water treatment.

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3 1. Introduction

Water resources have been facing severe stress globally due to increasing demands and pollution caused by human activities. Heavy metals are directly or indirectly being released into the aquatic environment due to several anthropogenic activities [1]. Chromium and its compounds find many industrial applications for a wide-ranging purpose in metal industry, dye preparation, leather tanneries, and aerospace etc. Chromium occurs primarily in two different forms as trivalent Cr(III) and hexavalent Cr(VI) [2]. Although trivalent chromium has not been found to pose risk to human health and the environment, hexavalent chromium is well known for its toxicities (mutagenic, genotoxic and carcinogenic capabilities) [3]. The toxicity of Cr(VI) has been attributed to its small size which allows it to pass easily through the cell membrane [4]. International Agency for Research on Cancer (IARC) has classified Cr(VI) and its compounds as group 1 chemicals referring to these compounds being carcinogenic to humans [5]. The World Health Organization recommended guideline value for total chromium in drinking water is 0.05 mg L-1 [6]. The European Union has also recommended the same value on its council directive 98/83/EC on the quality of water intended for human consumption [7]. However, United States Environmental Protection Agency has established maximum contaminant level for total chromium as 0.1 mg L-1 [8].

Adsorption technology has been adopted as one of the most promising techniques and effectiveness of various adsorbents has been shown in water treatment applications [3,9].

Recently, composite adsorbents have attracted the attention of researchers to bring together the benefits of different precursor materials into one adsorbent. Chitosan, a deacetylated chitin product, is a carbohydrate biopolymer having hydroxyl groups and highly reactive amino groups [10]. As an inexpensive biopolymer and being abundant in nature, it has been widely explored to remove heavy metals from aqueous solution. The presence of amino functional groups in chitosan increases its adsorption capacity compared to its precursor

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(chitin) [11]. Chitosan, however, can dissolve in acidic media therefore, researchers have sought to stabilize it with different nano scale materials for the removal and recovery of metal ions [2,12] and graphene oxide has been one of such stabilization agent. Graphene oxide (GO) is a monolayer planar structure of graphite containing sp2 hybridized pure carbon [13]

and has been reported to possess adsorption capacity with some drawbacks such as recovery from treated water [14]. Although the use of magnetic chitosan has been reported for water remediation, the effect of incorporating GO on the magnetic chitosan on water remediation has been less reported. This study aimed to first synthesize chitosan-based magnetic nanoparticles, followed by modification with GO to assess the effect of GO addition on the functional groups of chitosan for the removal of Cr(VI) from aqueous medium. The characterization of the composite nanomaterials was done by Fourier transform infrared spectroscopy (FTIR), scanning electron microscopy / energy dispersive spectroscopy (SEM / EDS), Raman spectroscopy, X-ray powder diffraction (XRD) and Brunauer–Emmett–Teller (BET) methods. The effects of solution pH, adsorbent dosage, initial ion concentration, ionic strength and co-existing ions on Cr(VI) removal by adsorbents were studied in batch mode.

The experimental data was applied to different kinetic and isotherm models to examine the suitability of the model. Finally, continuous fixed-bed column studies were conducted to see the practical applicability of the prepared nanocomposite.

2. Materials and methods

All the chemicals used in the experiments were analytical grade. Potassium dichromate (K2Cr2O7) (Sigma Aldrich) was used to prepare Cr(VI) stock solution. Graphite powder, hydrogen peroxide (H2O2) and ethylene glycol were purchased from Fisher scientific.

Potassium permanganate (KMnO4), sulphuric acid, iron(II) chloride and iron(III) chloride and

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chitosan (low molecular weight) were obtained from Sigma Aldrich. Milli-Q water was used as solvent for preparing the solution of synthetic contaminated water.

2.1. Preparation of graphene oxide

Graphene oxide was prepared using analytical grade KMnO4, H2SO4 and natural graphite flakes using modified Hummer’s method [15]. In short, 2 g of graphite powder was added with constant stirring in 100 mL concentrated H2SO4 in an ice bath. Afterwards, 4.025 g sodium nitrate (NaNO3) was added slowly followed by pinch by pinch addition of 10 g KMnO4. Then, the mixture was stirred for two h. Then flask was placed in an ice bath on a magnetic stirrer and diluted with 100 mL de-ionized water. Later, 20 mL H2O2 was added to terminate the reaction. The reaction mixture thus obtained was centrifuged at 7000 rpm for 5 min and the supernatant was discarded. The slurry was washed five times by replacing the supernatant with de-ionized water. Graphite oxide thus obtained was dried at 60 ℃ for 6 h in a hot air oven.

The dried graphite oxide was ground to powder and transferred to a conical flask with 100 mL de-ionized water. The mixture was ultra-sonicated for 30 min by placing it in an ice bath to control the temperature during ultra-sonication. After ultra-sonication, the mixture was centrifuged at 7000 rpm for 5 min and the supernatant liquid was discarded and the solid was transferred to a glass plate and kept in a hot air oven at 50 ℃ for drying. The obtained solid was termed as graphene oxide (GO).

2.2. Synthesis of magnetic chitosan-graphene oxide nanocomposites

Chitosan based magnetic nanocomposites were synthesized by solvothermal process adopted with some modification from literature [16,17]. Shortly, 0.2 g GO was dissolved in 75 mL ethylene glycol with the aid of ultra-sonication for 2 h. Thereafter, 0.54 g iron(III) chloride

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hexahydrate and 0.23 g iron(II) chloride tetrahydrate were added to the solution. A known amount of chitosan was added for the preparation of Chi@Fe3O4GO.The mixture was placed on a magnetic stirrer and 3.6 g of sodium acetate was added slowly while stirring the mixture.

The mixture was agitated for 30 min. Then the mixture was transferred into a Teflon walled autoclave and kept inside an oven at 200 ℃ for 12 h. The autoclave was allowed to cool down to room temperature before opening it. The mixture thus obtained was centrifuged to separate the solid mass and washed with DI-water and ethanol for three times each. Finally, the solid obtained was dried in hot air oven at 50 ℃. The exact procedure without adding GO was repeated to obtain Chi@Fe3O4. Fe3O4 nanoparticles were obtained following the same procedure without involving GO and chitosan.

2.3. Characterization of nanocomposites

The surface functional groups of the precursors and synthesized composites (before and after adsorption), were analyzed with FTIR using Thermo Nicolet iS50 model (Thermo Fisher Scientific, Madison USA). The spectra were recorded in iS-ATR mode from 400–4000 cm−1 at variable (40, 45, and 50) scans for optimum spectra. For quality control, the loaded composites were well dried and the instrument was precooled using liquid nitrogen before conducting the analysis. The particle structure and morphology were imaged with a scanning electron microscope (SEM, Carl Zeiss Sigma HD|VP) operated at a 2 kV acceleration voltage. The energy dispersive spectroscopy (EDS, Thermo Noran NS7 double-EDS 60 mm2 detectors, ThermoFisher, Waltham, USA) was carried out to analyze the elemental composition of the Composites. The crystallinity and phase composition of the Composites were analyzed with X-Ray diffraction (XRD, AXS D8 Advance with Cu Kα). Raman spectroscope (Thermo DXR2xi Raman) was used analyze the composition of the particles.

The specific surface area of the samples was determined with nitrogen adsorption isotherms

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(i.e. BET method) measured with Tristar II 3020 porosity analyzer (Micrometrics Instrument Corp., USA). The surface charge of the materials was determined by zero point of charge (pHzpc). A solution of 0.01M NaCl was adjusted to pH 2, 4, 6, 8 and 10 using aliquots of 1M and 0.1M HCl or NaOH aqueous solution. Then, 0.05 g of the material was contacted with 25 mL of pH adjusted solution and agitated for 24 h. The solution was filtered, and the final pH was recorded carefully. The pHzpc value was determined from the plot of (initial pH - final pH) versus pHi (initial pH) of the solution.

2.4. Adsorption experiments

The adsorption experiments were performed using a rotary shaker. For most of the experiments, initial chromium concentration was kept as 40 mg L-1. Cr(VI) solution was prepared by diluting appropriate volume of stock solution in DI-water. Batch adsorption experiments were carried out by adding 0.5 g L-1 of adsorbent in 15 mL centrifuge tubes containing 10 mL Cr(VI) solution. All the adsorption experiments were carried out at solution pH of 2, except for the effect of pH which was done by varying the pH from 2-10. The tubes were agitated until equilibrium was reached. The adsorbent was separated by centrifugation followed by filtration through cellulose acetate filter (pore size 0.45µm). After the adsorption experiments, the remaining concentration of Cr(VI) in the solution was measured after complexation with 1,5 diphenyl carbazide [18] in a UV-visible spectrophotometer (Simazdu corporation, Japan) at maximum wavelength of 540 nm. The removal efficiency (R%) and adsorption capacity (qe) of the composites were calculated using equation (1) and (2) respectively.

(1)

(2)

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where, and are the Cr(VI) concentrations before and after the adsorption, is the volume of each sample and is the used mass of adsorbent.

2.4.1. Batch studies

The effect of pH on Cr(VI) removal was examined in the pH range at 2 ,4, 6, 8 and 10 at room temperature. The initial pH adjustment was made using aliquots of solutions of HCl and NaOH as required. The pH was measured using a pH electrode (METTLER TOLEDO), standard buffer solutions were used to calibrate the device. The effect of adsorbent dose on adsorption was studied by using varying dosage of adsorbent in the range 0.25-1.5 g L-1 in 10 mL adsorbate solution with initial concentration of 40 mg L-1. Various molar concentrations of NaCl (0-0.5 M) were utilized to study the effect of ionic strength. The effect of contact time was analyzed by using 0.5 g L-1 of adsorbent in 10 mL adsorbate solution. Samples were collected at various time points up to 240 min. The experimental data was further utilized for kinetic modelling to gain insights into the reaction kinetics. Cr(VI) solutions of varying concentration in the range 10 – 100 mg L-1 were prepared by diluting appropriate volume of stock to study the effect of initial concentration of pollutant in the solution. The experimental data was finally used in isotherm modelling. The effect of temperature on the adsorption capacities of the Composites were studied at various temperature (279 K, 295 K and 308 K) using 40 mg L-1 Cr(VI) solution. Furthermore, the adsorption data was accounted for the calculation of thermodynamic parameters. The presence of similarly charged species in the solution may affect the adsorption of targeted pollutant onto the adsorbent. Therefore, the effect of co-existing ions on Cr(VI) adsorption was studied in the presence of similarly charged anionic species (Cl-, NO3-

, SO42-

and PO43-

) at two concentrations (25 mg L-1 and 50 mg L-1).

2.4.2. Fixed bed column experiments

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For fixed bed column studies, the columns were packed with a measured amount of the adsorbent material in a laboratory scale glass column. Then, the solution containing a known concentration of Cr(VI) was fed to the column using a peristaltic pump. Fixed bed column experiments were carried out with Chi@Fe3O4. Effluent was sampled at various time points;

final concentration of pollutant was examined until the saturation of adsorbent was observed.

The effect of the following parameters, on Cr(VI) adsorption were investigated; (i) Effect of flow rate: flow rate was differed between 1 mL min-1 and 2 mL min-1, keeping adsorbent loading and initial pollutant concentration constant at 25 mg and 20 mg L-1, respectively. (ii) Effect of adsorbent loading: two different loadings; 25 mg and 50 mg were used to examine the effect of loading while keeping flow rate and pollutant concentration constant at 1 mL min-1 and 20 mg L-1, respectively. (iii) Effect of pollutant concentration: influent Cr(VI) concentration was varied between 20 mg L-1 and 40 mg L-1 at flow rate of 1 mL min-1 and adsorbent loading of 25 mg.

The breakthrough curve shows the performance of fixed bed column. The breakthrough curve is expressed as Ct/Co as a function of time or effluent volume for given bed height. The time taken for the appearance of breakthrough and shape of the curve are of great importance for establishing the operation and dynamic response of adsorption column [19,20]. The effluent volume ( ) can be calculated using equation (3) [19]:

(3)

where (mL min-1) and (min) are volumetric flow rate and total flow time respectively.

The area under the breakthrough curve can be utilized to calculate the total mass of Cr(VI) adsorbed, (mg), as shown in equation (4)[21]:

(4)

where (mg L-1) is the adsorbed metal concentration.

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The equilibrium uptake capacity of column ( ) is defined by the total amount of metal adsorbed per unit dry mass (g) of adsorbent as shown in equation (5) [20]:

(5)

The total amount of metal ions entering the column ( ) can be calculated using equation (6)[20,21]:

(6)

And the removal capacity of Cr(VI) metal ions can be calculated by using equation (7)[20,21]:

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The unadsorbed chromium concentration at equilibrium ( ; mg L-1) in the column can be derived from equation (8)[22]:

=

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3. Results and discussion

3.1. Characterization of nanocomposites

The FT-IR spectra of Fe3O4, chitosan modified ferrites (Chi@Fe3O4), chitosan and graphene oxide modified ferrites (Chi@Fe3O4GO), and chitosan are presented in Fig 1(a). For chitosan, the broad peak stretching from ~3400 to 3280 cm-1 is assigned to polymeric OH [23]. The broad nature of the peak suggests the presence of both OH group and other H-bonded moieties as reported in other study [24]. Two peaks (~1647 and ~1555 cm-1) were recorded for the amine groups of chitosan and these peaks suggest the presence of varied forms of amines due to the degree of deacetylation as reported elsewhere [25]. The two intense peaks at ~1062 and ~1026 cm-1 are assigned to C-OH bond stretching [26]. The intensity of the C- OH bond stretching suggests that the bonds may exist as group frequencies which can include

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both saturated (C-H, C-OH), and unsaturated (CH2) bonds which is a consequence of acetylenic alkene. The chitosan modified ferrites (Chi@Fe3O4) spectra revealed a reduction in the OH, and C-OH bond stretching of chitosan suggesting an interaction with ferric oxide.

Further modification of the material with graphene oxide (Chi@Fe3O4GO) revealed marked changes in the peak assigned to amine functional groups. The peak at ~1647 cm-1 disappeared and peak at 1555 cm-1 was significantly reduced. Secondly, the C=C bond usually found in the region of ~1631 cm-1 of graphene spectra [27] was significantly suppressed. These phenomena suggest the interaction of C-C bonds of graphene oxide and amine functional groups of chitosan, which can result in the formation of new C-H or C-N bonds. The peak at

~1020 cm-1 on Chi@Fe3O4GO assigned to C-N stretch [24] is therefore attributed to the interaction of C-C bonds of graphene and amine functional groups of chitosan. One consequence of this bond formation is that adsorption processes that involve amine functional group will be negatively affected and this is further discussed in section 3.2. At the lower end of the spectra, the peak in the region of ~541 cm-1 is assigned to oxide moieties in Fe3O4, and OH of the other materials. The intensity of the peak recorded for the oxide functional group suggests the amount of oxide present in each of the material. The well-ordered and smooth form of the spectra recorded at the lower ends of the spectrum for all the materials, as seen from the inset figure (Fig 1(a)) which shows that the recorded spectra were stable.

Fig. 1

Fig. 1(b) shows the XRD patterns of the samples which are in good agreement with the elemental analysis. The peaks around 35º, 43º, 54º, 57º and 63º, the shoulder observed at 30º in the 2θ range can be assigned for Fe3O4. Based on the XRD, no crystalline carbon or chitosan is present in the samples [28].

Fig. 1(c) shows the Raman peaks of the samples that can be assigned to the carbon D- and G- bands. The intensity maxima of Chi@Fe3O4GO was observed at 1342 and 1599 cm-1 and of

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Chi@Fe3O4 at 1394 and 1586 cm-1. In both cases, the peaks are broad and strongly overlapping. The second order Raman peaks of carbon (2D) are absent. The broad, overlapping spectra indicates that the structure consists mainly sp2 amorphous carbon, which may contain additional functional groups [29,30].

The surface charge of the adsorbent is vital during the adsorption process. The pH at which the net surface charge of the adsorbent is zero is determined by pHzpc. When the solution pH is higher than the pHzpc, the adsorbent’s surface is negatively charged and attracts cationic species. On the other hand, when the solution pH is less than the pHzpc, the adsorbent’s surface becomes positive attracting anionic species [31]. The results of the pHzpc analyses of the synthesized materials are presented in Fig. 1(d). The results showed that although both synthesized materials were variably charged, Chi@Fe3O4GO was more negatively charged than Chi@Fe3O4 and this is as a result of the introduction of free electrons from the intercalation of GO. This characteristic property of the synthesized Chi@Fe3O4GO suggests it can be limited in the adsorption of Cr(VI) anions. This was subsequently confirmed in the adsorption studies which fits in the aim of this study.

The SEM images of Chi@Fe3O4 (Fig. 2 (a) and (b)) and Chi@Fe3O4GO (Fig. 2 (d) and (e))), and related EDS mapping (Fig. 2 (c)) and (Fig. 2 (f)) of Chi@Fe3O4 and Chi@Fe3O4GO, are presented in Fig. 2. The chitosan particles with smooth surface formed a porous supporting framework. However, no separate GO sheets or flakes could be observed in Chi@Fe3O4GO.

A rough textured surface consisting of small magnetic iron oxide particles deposited on the surface of chitosan was observed in both cases. The slightly higher and uniform coverage of Fe3O4 particles were detected on Chi@Fe3O4 than on Chi@Fe3O4GO. The average elemental weight percentage (wt.%) of the adsorbents was obtained via SEM/EDS analysis. The higher amount of carbon (33.9 %) was observed in Chi@Fe3O4GO as compared to 22.3 % in Chi@Fe3O4, which is most likely due to the added graphene oxide. The main source of

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carbon for Chi@Fe3O4GO is the basal plane of graphene nanosheets and chitosan whereas chitosan is the only carbon source in Chi@Fe3O4. Nitrogen detected by EDS is most likely attached to the amino groups of chitosan.

Fig. 2

According to the nitrogen adsorption measurements, the total surface area of Chi@Fe3O4GO and Chi@Fe3O4 were found to be 5.4 m2g-1 and 2.3 m2g-1, respectively. The pore volume was 0.02 cm3g-1 in both cases. The addition of graphene oxide more than doubles the surface area but have no effect on the pore volume. The results agree well with the SEM images, which shows smooth chitosan-based surfaces supporting the iron oxide particles (see Fig. 2b).

3.2. Effect of solution pH

The pH of the media affects the surface charge of the adsorbent as well as degree of ionization and the ionic forms of the adsorbate, thus selection of optimum pH is vital in adsorption studies [32]. Different species of chromium co-exists between pH 1-6, such as Cr2O72-, HCrO4-, Cr3O102-, Cr4O132- where HCrO4- being the predominating species, whereas the form shifts to CrO42-

and Cr2O72-

as the pH goes higher [33]. The solution pH showed significant impact on the adsorption of Cr(VI) by the composites as can be seen from Fig. 3 (a), which depicted maximum adsorption at pH 2. The highest adsorption capacity (84.84 mg g-1) was recorded with Chi@Fe3O4, while the lowest capacity (10.28 mg g-1) was recorded with Fe3O4, although it followed the same pH dependent trend. The higher adsorption at acidic pH could be attributed to the protonation of adsorbent’s surface due to H+ ions which in turn increases the electrostatic attraction between positively charged adsorbent’s surface and negatively charged chromate ions. The adsorption sharply dropped as the solution pH kept on increasing. Similar pH dependent results have also been reported by other authors [3,34-36]. Hence, pH 2 was taken as optimal value for further studies. The slightly reduced adsorption capacity of Chi@Fe3O4GO for Cr(VI) ions (Fig. 3 a) suggests the blockage of

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some of the functional groups of Chi@Fe3O4 (involved in adsorption) during the modification by GO to synthesize Chi@Fe3O4GO as discussed in section 3.1. Due to the diminished nature of the peak assigned to amine functional group of Chi@Fe3O4GO, it can be deduced that there was less interactions between Cr(VI) ions and the amine group on the surface of Chi@Fe3O4GO, as compared to the surface of Chi@Fe3O4. Using chitosan only as Cr(VI) adsorbent, the removal capacity was found to be 32.83 mg g-1 (Fig. S1) at pH 2, and the highest capacity of 35.59 mg g-1 was recorded at pH 4. These results justify the modification of chitosan for more efficient adsorption performance.

Fig. 3 3.3. Effect of adsorbent dosage

The effect of adsorbent dosage on Cr(VI) adsorption onto the composites was investigated with different dosage of composites ranging from 0.25 g L-1 to 1.5 g L-1. Fig. 3 (b) shows that the removal efficiency of both the materials increased with the increase in dosage although it remained unchanged when an optimum dose level was reached. Similar observation has been reported in other adsorption studies [34,37]. Such phenomenon can be attributed to the fact that the increase in adsorbent mass increases the availability of adsorption sites, thereby increasing the removal of Cr(VI). Fig. 3(b) also shows that the adsorption capacity is negatively affected by increasing the adsorbent dose. The adsorption capacity of an adsorbent is inversely proportional to its mass as suggested by equation (2). At higher dosage, fewer active adsorption sites are used resulting in decreased ratio of adsorbed ions to the adsorbent mass. Thus, lowering the adsorption capacity of the adsorbent [38].

3.4. Kinetic modeling

The time dependent characteristics of adsorption of Cr(VI) ions onto the synthesized materials was studied and the results are presented in Fig. 4. The adsorption of Cr(VI) was

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found to occur rapidly in the first hour of the experiment. To provide enough time for interaction between adsorbate ions and adsorbent, 180 min was selected as equilibrium time for the remaining experiments. To understand the mechanism of rate-controlling steps, the experimental data from equilibrium studies were modelled using various commonly used kinetics models. Pseudo-first-order kinetic equation [39] is mathematically expressed can be as in equation (9):

(9)

Pseudo-second-order kinetic equation [40] predicts chemical rate controlling step. It can be expressed mathematically as equation (10):

(10)

where, (mg g-1) and (mg g-1) are adsorption capacities at time ‘t’ and at equilibrium respectively. (min-1) and (g mg-1 min-1) are the rate constants for pseudo-first-order and pseudo-second-order kinetic models. The results from the kinetic studies are presented in Fig.

4 (a), and 4 (c). It was found that the adsorption of Cr(VI) was rapid initially, however, it became slower with time and finally attained a plateau indicating equilibrium. The parameters of the kinetic modelling and data are presented in Table 1. The R2 value for the two kinetic models suggests that adsorption data fits better with pseudo-second order model (R2 = 0.995 and 0.984 for Chi@Fe3O4, and Chi@Fe3O4GO, respectively). Diffusion mechanism was studied by applying the intra-particle diffusion model, equation (11) [41].

Intraparticle diffusion model theoretically assumes the uptake of adsorbate, differs almost proportionally with the square root of contact time ( ) and can be written as [42].

(11)

where, is the kinetic rate constant of intra-particle diffusion model and ‘C’ is the intercept. The fitting of intra-particle diffusion model as presented in Fig. S2 depicted two distinct phases of Cr(VI) adsorption onto both adsorbents. Intraparticle diffusion is

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considered to be the rate limiting if the qt vs t0.5 produces a straight line passing through the origin [43]. Thus, it can be concluded that multiple mechanisms are involved in the adsorption process. The first phase characterized by a steeper qt versus t0.5 slope was attributed to the diffusion of Cr(VI) species to the external surface of the composites. The second phase characterized by gradual adsorption stage and lower qt versus t0.5 slope suggesting intra-particle diffusion as rate limiting step in this phase [44]. The corresponding values of the model parameters, coefficient of determination (R2) and root mean square error are summarized in Table 1.

Fig. 4 Table 1 3.5. Adsorption isotherms

To evaluate the adsorption capacities of Cr(VI) onto the synthesized adsorbents, the equilibrium data was applied to non-linear form of most widely used isotherm models, namely Langmuir [45], Freundlich [46], and Dubinin-Radushkevich [47] models.

Langmuir isotherm model assumes homogenous, monolayer (thickness of adsorbed layer is in the extent of one molecule) adsorption that can occur at a finite number of localized sites [48]. The non-linear form of Langmuir isotherm equation is given as equation (12):

(12)

where, (mg g-1) and (mg g-1) are the equilibrium adsorption capacity and maximum monolayer adsorption capacity respectively. (mg L-1) is the equilibrium sorbate concentration and is the Langmuir isotherm constant.

The influence of shape of adsorption isotherm in terms of a dimensionless constant known as separation factor or equilibrium parameter ( , can be calculated using equation (13) [49].

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where, is the Langmuir isotherm constant and (mg L-1) is the initial adsorbate concentration. The value of separation factor ( indicates favorability of adsorption such that when > 1 (unfavorable), = 1 (linear), 0 < < 1 (favorable) and = 0 (irreversible). The values calculated based upon above equation are listed in Table 1. The

values falling in between 0 and 1 confirms the favorability of the isotherm [50].

Freundlich isotherm is an empirical model describing non-ideal, reversible, multilayered adsorption onto heterogeneous surface. It is widely used in heterogeneous systems. Non- linear form of Freundlich isotherm equation can be expressed as equation (14):

(14)

where, (mg g-1) (dm3 g-1)n is called Freundlich constant related to the relative adsorption capacity of the material, (mg L-1) is the equilibrium sorbate concentration and n is a dimensionless empirical parameter related to adsorption intensity.

Dubinin-Radushkevich model is generally used for studying the adsorption on microporous materials. It predicts the nature of adsorption process. The non-linear form of Dubinin- Radushkevich isotherm is expressed in equation (15):

(15)

where (mg g-1) is the maximum adsorption capacity, (mol2 (kJ2)-1) is the activity coefficient and is Polanyi potential. Polanyi potential is mathematically expressed as equation (16):

(16) where R (8.314 J mol-1 K-1) is the universal gas constant and T (K) is the absolute temperature. The mean free energy is calculated using the activity constant as given in equation (17):

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The mechanism of adsorption is predicted by the value of E. If the value is between 8 and 16 kJ mol-1, the process is controlled chemically, and if the value is < 8 kJ mol-1, the process is controlled physically.

The corresponding Langmuir, Freundlich, and Dubinin-Radushkevich parameters for Cr(VI) adsorption onto synthesized adsorbents are presented in Table 1. The values of determination coefficient (R2) and residual root mean square error (RMSE) calculated from these models were used to compare the fitting of the models. For both composites, the value of R2 from Freundlich (0.985 and 0.984) and Langmuir (0.969 and 0.968) models for Chi@Fe3O4 and Chi@Fe3O4GO respectively, showed better fit compared to Dubinin-Radushkevich. The RSME value for these two models is comparatively low for both studied adsorbents. The good fitting of Freundlich isotherm model as shown in Fig. 4 (b) and 4 (d) suggests that adsorption of Cr(VI) takes place on heterogeneous surface of the adsorbent. The value of adsorption intensity n reflects the nature of the adsorption process. The adsorption process is said to be favorable when the value of n is between 1 and 10. When the value of 1/n gets close to zero, the adsorption process becomes more heterogeneous and denotes chemisorption whereas when the value gets more than 1 indicates cooperative adsorption [51,52]. In this study, the value of n (Table 1) lies within the range of 1 – 10 indicating favorability of the adsorption process. The fitting of the isotherms data on Langmuir model also suggests the dominance of one of the composites since the model predicts a monolayer adsorption. The maximum adsorption capacity was found to be 142.32 and 100.51 mg g-1 for Chi@Fe3O4 and Chi@Fe3O4GO, respectively.

3.6. Effect of ionic strength

The effect of ionic strength on Cr(VI) adsorption onto the composites was investigated using varying concentrations between 0.0 M and 0.5 M of NaCl in the buffer solution. It is clear

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from Fig. 5 (a) that the adsorption capacity of the synthesized adsorbents is significantly affected by the presence of the salt. For both composites, the increase in salt concentration had negative effect on their adsorption capacities. One of the reasons for the reduced adsorption capability might be due to the competition between chromate and chloride species for the same adsorption sites. Similar results have been reported by other authors [53].

Fig. 5 3.7. Effect of co-existing ions

Generally, surface water, ground water or industrial wastewater contain various ions and affect the adsorption process. Therefore the influence of commonly occurring ions i.e.

chloride, nitrate, sulphate and phosphate on Cr(VI) adsorption was studied at varying concentration of co-anions at 25 mg L-1 and 50 mg L-1 having adsorbate [Cr(VI)]

concentration of 40 mg L-1 at pH 2. The results are presented in Fig. 5 (b) and (c). From the figure, it can be noted that the removal capacity of the composites is slightly hindered by the presence of anionic species like chloride (Cl-), nitrate (NO3-), sulphate (SO42-) and phosphate (PO43-

). However, the presence of SO42-

ions in higher concentration reduced the adsorption capacity by approximately 20 mg g-1 of the composites. The results suggest that there exists the competition among the negative ions and Cr(VI) species for the adsorption sites. Similar results have also been reported elsewhere [54].

3.8. Thermodynamic parameters

The analysis of thermodynamic parameters is useful to learn about the spontaneity of the reaction. These parameters i.e. change in Gibbs free energy (∆G˚), change in enthalpy (∆H˚) and change in entropy (∆S˚) can be computed from the experimental data. The change in Gibbs free energy can be calculated by using van’t Hoff equation (18):

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where, (L g-1) is the equilibrium constant, also called distribution coefficient, (8.314 J mol-1 K-1) is the universal gas constant and (K) is the absolute temperature. Fig. S3, also called van’t Hoff plot gives a straight line with slope and intercept equal to – /R and /R, respectively.

Alternately, Gibbs equation (eq. 19) can be utilized which is expressed in terms of and .

(19) The enthalpy and entropy can be estimated using equation (20):

(20) The values of thermodynamic parameters are given in Table 2. The negative value of indicates that the adsorption of Cr(VI) onto the composites is a spontaneous process. The change in enthalpy (∆H˚) was 30.58 kJ mol-1 and 41.46 kJ mol-1 which indicates the adsorption process is endothermic in nature. The positive value of signifies an increase in the randomness of Cr(VI) ions on the solid-solution interface during the adsorption process [55].

Table 2 3.9. Reusability studies

The reusability of an adsorbent is important for its use in industrial application considering cost-benefit feature besides its efficiency. The reusability of the synthesized composite was examined by adsorption-desorption experiments. The adsorption experiments were first carried out under optimum conditions using batch mode (initial chromium concentration 40 mg L-1, pH of 2, adsorbent dosage of 0.5 g L-1 and temperature 295 K). Then adsorbent mass was separated and transferred to a different flask to carry out desorption procedure.

Desorption experiments were carried out using two eluents viz. 0.1 M NaOH and 0.1 M HNO3 [56]. The efficiency of Chi@Fe3O4 upto fourth cycle of regeneration is presented in

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Fig. 6 (a). The adsorption efficiency of Chi@Fe3O4 using 0.1 M NaOH eluent remained above 75% after four successive adsorption-desorption cycles. However, when using 0.1 M HNO3 as eluent, the removal efficiency decreased consistently with each regeneration cycle.

Thus, the synthesized magnetic nanocomposite could be regenerated with 0.1 M NaOH as eluent and used effectively and economically for the removal of hexavalent chromium from aqueous solution. Fig. 6 (b) shows the adsorbent separation by magnet.

The adsorption capacities of synthesized composites were compared with other adsorbents reported in literature (Table 3). The synthesized composites used in this study were found to have better adsorption capacities than other reported adsorbents. The adsorption capacity of Chi@Fe3O4 was found to be better than that of Chi@Fe3O4GO. Hence, it was selected for fixed bed column experiments.

Fig. 6 Table 3 3.10. Fixed bed column studies

3.10.1. Effect of flow rate

The breakthrough curves at different flow rates on Cr(VI) adsorption are shown in Fig. 7(a).

The initial flow rates of 1 ml min-1 and 2 ml min-1 were maintained for a constant adsorbent loading of 25 mg and initial pollutant concentration of 20 mg L-1.It is clearly evident from Fig. 7(a) that as the flow rate increased, the appearance of breakthrough and the exhaustion time decreased. The parameters calculated using the column data are presented in Table 4 which shows that as the flow rate is doubled from 1mL min-1 to 2 mL min-1 the removal capacity (Y%) decreases from 27.62% to 15.43% and the concentration of unadsorbed chromium in the eluent solution increased from 17.26 mg L-1 to 21.02 mg L-1. This tendency can be attributed to insufficient residence time due to higher inflow of pollutant solution

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resulting in lower adsorption of Cr(VI) ions. Similar phenomenon has been reported elsewhere [20,63].

Fig. 7 Table 4 3.10.2. Effect of adsorbent loading

The effect of various adsorbent loadings is shown in Fig. 7(b). From the figure, it can be observed that the increase in adsorbent loading from 25 mg to 50 mg delays the time for occurrence of breakthrough curve. The figure also indicates the increase in effluent volume ( ) with the increase in loading. Further, calculation of column parameters, presented in Table 4, also shows that the removal capacity of the column increased from 27.62% to 41.85% as the adsorbent loading was increased from 0.025 g to 0.05 g and the concentration of unadsorbed Cr(VI) decreased from 17.26 mg L-1 to 14.14 mg L-1. This might be due to the availability of adsorption sites of the material as the adsorbent loading on the column increases. The slope of breakthrough curve decreased with increased adsorbent loading, thus resulted in broadened mass transfer zone [64].

3.10.3. Effect of pollutant concentration

For investigating the effect of different initial influent concentration, two different initial Cr(VI) concentrations viz. 20 mg L-1 and 40 mg L-1 were fed through the system Fig. 7(c) shows the effect of influent pollutant concentrations. The breakthrough time for 40 mg L-1 occurred earlier than that for 20 mg L-1 and reached exhaustion time rapidly. Analysis of column data, shown in Table 4, revealed that when the influent concentration is doubled the capacity of the column decreased from 27.62% to 10.07% and the concentration of unadsorbed Cr(VI) ions increased from 17.26 mg L-1 to 43.82 mg L-1. This might be due to early saturation of available adsorption sites by the solution with higher influent

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concentration. Similar tendency has been reported elsewhere [63,65]. The Cr(VI) removal mechanism by Chi@Fe3O4 is presented in Fig. 8.

4. Conclusions

Composite adsorbents were successfully synthesized to bring together the unique properties of different parent materials (precursors) to achieve different removal capacities of Cr(VI).

The effect of various experimental conditions (pH, dosage, ionic strength, co-existing ions) were examined. The adsorption kinetics followed the pseudo-second-order model for both composites. The maximum monolayer adsorption capacity for Chi@Fe3O4 was found to be 142.32 mg g-1 while for Chi@Fe3O4GO was 100.51 mg g-1. The Chi@Fe3O4GO removal capacity was ~29 % less than Chi@Fe3O4. The thermodynamic parameters showed the process is spontaneous and endothermic. Reusability study confirmed that the composites could be used multiple times without losing considerable capacity to adsorb Cr(VI) ions thus, making the process economically feasible. Fixed bed column studies depicted that the column performance was significantly affected by flow rate, adsorbent loading in the column and initial metal ion concentration. Overall, the synthesized magnetic nanocomposites have potential to be used as adsorbent for the removal of toxic Cr(VI) metal ions from aqueous solution.

Acknowledgment

The research was supported by the research cluster grant (R18029) from Zayed University, Abu Dhabi, United Arab Emirates. First author (N.S.) is grateful to Dr. Santhosh Chella (Postdoc) for his guidance in the preparation of the adsorbent materials and to Koen Silvius of Hogeschool van Arnhem en Nijmegen, Netherlands for the help in some lab. experiments.

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Table 1. Adsorption kinetic and isotherm parameters for Cr(VI) adsorption onto Chi@Fe3O4 and Chi@Fe3O4GO.

Model Parameters

Adsorbent

Chi@Fe3O4 Chi@Fe3O4GO

Pseudo-first-order

(mg g-1) 69.457 76.098

(min-1) 0.194 0.265

R2 0.976 0.965

RMSE 4.007 5.142

Pseudo-second-order

(mg g-1) 79.466 73.164

(g mg-1 min-1) 0.005 0.006

R2 0.995 0.985

RMSE 1.770 3.432

Intra-particle diffusion

3.474 3.252

36.541 43.969

R2 0.761 0.731

RMSE 11.987 13.902

Langmuir

(dm3 mg-1) 0.24 0.36 -1) 142.381 100.514

0.041 – 0.303 0.027 – 0.217

R2 0.969 0.968

RMSE 14.956 11.21

Freundlich

g-1) (dm3 g-1)n 53.151 40.373

4.012 4.495

R2 0.984 0.985

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RMSE 9.535 6.432

Dubinin-Radushkevich

-1) 122.673 98.097

2.036 0.792

R2 0.914 0.931

RMSE 18.806 6.788

E 0.496 0.795

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Table 2. Thermodynamic parameters for Cr(VI) adsorption onto Chi@Fe3O4 and Chi@Fe3O4GO.

Adsorbent Temperature (K) (kJ mol-1) (kJ mol-1) (J mol-1 K-1)

Chi@Fe3O4GO

279 -4.49

30.580 125.541

295 -6.36

308 -8.15

Chi@Fe3O4

279 -6.07

41.465 169.697

295 -8.12

308 -11.09

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Table 3. Comparison of adsorption capacities of synthesized MNCs and various reported adsorbents for Cr(VI) removal.

Adsorbent qe (mg g-1) References

Chitosan 22.09 [57]

Cross-linked chitosan 78 [58]

Chitosan grafted graphene oxide 104.16 [59]

Magnetic chitosan-GO nanocomposite 82.14 [60]

Magnetic chitosan nanoparticles 64.31 [32]

Ethylenediamine-modified cross-linked magnetic chitosan resin 51.81 [2]

Amino-functionalized SiO2@CoFe2O4-GO 136.4 [61]

Commercial activated carbon 153.96 [62]

Chi@Fe3O4 142.38 This study

Chi@Fe3O4GO 100.51 This study

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