C. Yaoa,
F. Wanga,
Z. Cai*b and
X. Wang*a
aDepartment of Materials Science and Engineering, University of Wisconsin – Madison, Madison, WI 53705-2275, USA. E-mail: xudong.wang@wisc.edu
bForest Products Laboratory, USDA Forest Service, Madison WI53726, USA. E-mail: zcai@fs.fed.us
First published on 21st September 2016
Nanoscale sorption is a promising strategy for catalyst and purification system design. In this paper, cellulose nanofibrils (CNFs) were densely attached with aldehyde functional groups on the surface via a mild periodate oxidation process, and then applied as mesoporous sorbents to remove Cu(II) and Pb(II) from aqueous solutions. In the studied concentration range (0.6–1.0 mmol L−1), a removal capacity of 0.75 mmol g−1 for Pb(II) and 0.58 mmol g−1 for Cu(II) was obtained. It is higher than most reported results over a much broader concentration range. Furthermore, the physical chemistry of the sorption process was studied in terms of sorption kinetics, sorption isotherm study and thermodynamic study. The results showed that the sorption process is under the combined influences of reaction kinetics, film diffusion and intraparticle diffusion, and follows the Langmuir model of monolayer adsorption. The sorption is spontaneous and endothermic. This development demonstrates an ecofriendly and cost-effective method with high level effectiveness of metal ion removal.
Recently, researchers disintegrated nanoscale cellulose from cellulose-containing materials and obtained cellulose nanofibrils (CNFs) and cellulose nanocrystals (CNCs).7–10 These high-purity nanocelluloses are readily to form homogeneous colloidal dispersions in water as hydrogel due to their surface charges and nanoscopic dimensions. Nanocellulose is characterized by easy processing and high surface area, and thus can be advantageous in metal ions removal. Several pioneer works have successfully demonstrated the application of functionalized CNFs for removal of many different metal ions including Ag(I), Cd(II), Cu(II), Zn(II), Co(II), and Ni(II), Pb(II), Cr(III) and Au(III).11–17 At low metal ions concentrations (≤1.01 mmol L−1), the metal ion sorption efficiencies were in the range of 27–100%. However, in order to reach high sorption efficiency, complex and multi-step chemical treatments were typically employed to functionalize CNF surfaces. It will be desirable, however, for the functionalization process to be simple and cost-effective while still maintaining high level effectiveness of metal ion removal. In the area of cellulose chemistry, selective oxidation of cellulose by periodate is a simple and effective oxidation process. This reaction proceeds under mild aqueous conditions, and is characterized by selective cleavage of the cellulose C2 and C3 bonds with vicinal hydroxyl groups, without simultaneous occurrence of side reactions to any extent.18–21 The resulting product has 2,3-dialdehyde units along the polymer chain. Aldehydes are very active reducing groups with a standard oxidation potential of +0.58 V, which are able to reduce metal ions including Hg(I), Pb(II), Cd(II), Ni(II), Cu(II), Pt(II), Ag(I), and Au(III) to their zero-valent forms.22,23 In this work, we successfully implemented this simple one-step periodate oxidation process to introduce aldehyde groups onto CNFs. The dialdehyde CNFs (termed as DACs) were found very effective in removing two common heavy metal pollutants, Pb(II) and Cu(II), from water. Under the same metal ion concentration range (0.6–1.0 mmol L−1), we achieved a removal capacity of 0.75 mmol g−1 for Pb(II) and 0.58 mmol g−1 for Cu(II) that was higher than most reported results.11–16,21,24,25 Compared to existing fabrication techniques, our approach is very effective for introducing functional groups to the surface of CNFs. Taking the advantage of the ultrasmall size of CNFs, the functional groups can reach an extremely high volume density, which would significantly enhance the functionality. Therefore, this cellulose processing technique is simple, cost-effective, and possesses high level effectiveness of metal ion removal, and holds great promises in ecofriendly nanomanufacture.
:
TEMPO
:
NaClO
:
NaClO2 = 1
:
0.016
:
0.07
:
1.13, and 0.05 M sodium phosphate buffer was added to form the final solution with the NaClO concentration being 0.1 M. The oxidation was carried out at 60 °C for 48 h. Oxidized pulps were then washed in distilled water and refined in a disk refiner. The refined fibers were subsequently subjected to centrifuge treatment to remove the supernatant fraction, and concentrated to 1 wt% using ultrafiltration. Finally, this suspension underwent high pressure mechanical homogenization by three pass-through of 200 and 87 μm microfluidizer chambers, mounted in series (M-110EH-30 Microfluidizer, Microfluidics, Newton, MA, USA). The resulting mixture of nanofibrils and water formed a transparent, stable aqueous colloid system (with a cellulose solid weight of 0.61%), termed as CNFs hydrogel. The CNFs hydrogel was stored at 4 °C for subsequent use. Carboxylate content of the as-processed CNFs hydrogel was determined to be ∼0.65 mmol g−1 using the electric conductivity titration method.26 Degree of polymerization (DP) of the CNFs hydrogel was estimated to be ∼600, based on the intrinsic viscosity method.27
Sodium periodate (NaIO4) oxidation was performed on the isolated CNFs hydrogel to introduce aldehyde functionalities. Specifically, solid NaIO4 was dissolved in water to form a 0.05 mol L−1 solution. CNF hydrogels were immersed in the NaIO4 solution for 20–300 hours in darkness, at room temperature. For each immersion, 20–30 g CNFs hydrogel was added into 18–27 mL NaIO4 solution, and the dose ratio of NaIO4 solution to CNFs hydrogel was fixed at 1.5 mole NaIO4 per mole of cellulose glucopyranose unit. After the designed duration of oxidation, the hydrogels were taken out of solution and repeatedly rinsed to attain a neutral pH. Thereafter, the DACs hydrogels (as well as the pristine CNFs control sample) were freeze-dried to obtain porous DACs aerogels. Freezing was completed in several minutes by plunging the hydrogels into liquid nitrogen, and the frozen samples were then dried in a freeze-dryer (4.5 Liter FreeZone Freeze Dry System, Labconco, Kansas City, MO, US) of 35 mTorr chamber pressure, 15 °C chamber temperature, and −104 °C collector temperature. Under these conditions, ice within the samples directly sublimated and was then purged from the system.
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Morphology and elemental composition of the cellulose aerogels were characterized by LEO 1530 Gemini field emission scanning electron microscope (SEM) coupled with energy dispersive spectroscopy (EDS). The crystallinity characteristics of the CNFs and DACs aerogels were analyzed using a Bruker D8 Discover X-ray diffractometer with CuKα radiation (λ = 0.154 nm) generated at 50 kV and 1 mA. The specific surface areas of the CNFs and DAC aerogels were measured using the Brunauer–Emmett–Teller (BET) method on a Quantachrome Autosorb-1 nitrogen gas sorption analyzer.
Two identical sorption experiments were performed for each condition. The resultant solutions were filtered through nylon syringe filters (pore size of 0.45 μm). Blank experiments showed that the nylon filters adsorbed neither Cu(II) nor Pb(II). Solutions were diluted to 0.5–2 mg L−1 in 4% HNO3 for determination of residual metal concentration by inductively coupled plasma optical emission spectrometry (Vista-MPX ICP-OES, Varian Inc., Palo Alto, USA). Cu was analyzed at a wavelength of 324.754 nm, and Pb was analyzed at 220.353 nm. Concentrations were analyzed based on intensity of the spectra at these wavelengths. Spectral interference of the sodium element, which possibly exists in our sample solutions, was insignificant at the chosen wavelengths. Standard solutions covering the probable concentration range of Cu and Pb in solutions were prepared by diluting commercial 1000 ppm standards with 4% HNO3 to make a working curve. Standard solutions and the HNO3 blank were re-analyzed after running every 40 samples to check for instrument drift. Three aliquots were analyzed for each sample solution. Relative standard deviation (RSD) was less than 3% for all the analyses.
Nitrogen gas BET surface area measurements were conducted to determine the surface areas of the aerogels. Nitrogen adsorption–desorption isotherms and pore size distributions were shown in Fig. 1c and d, and the specific area for CNFs and DACs aerogels was 185.1 m2 g−1 and 134.4 m2 g−1, respectively. Both of these surface area values are high, and the reduction in surface area after the oxidation treatment is possibly due to the buckling effects and the decreased hydrophilicity of dialdehyde groups as mentioned earlier.
SEM confirmed that 180 h oxidation treatment exerted insignificant influence on the cellulose porous structure. A typical CNFs aerogel presented sheet-like aggregated morphology (inset of Fig. 2a). Zoom-in SEM image showed aggregates were composed of interconnecting fibrous networks (Fig. 2a). Microstructure after oxidation is shown in Fig. 2b. The same sheet-like aggregates (inset of Fig. 2b) and mesoscale fiber network can be clearly observed. This evidenced the periodate oxidation process did not impose significant morphology change to the cellulose microstructure.
Tollen's reagent was then employed to visualize the presence and distribution of aldehyde groups on DACs, because the diamminesilver [Ag(NH3)2]+ in the reagent can easily oxidize aldehyde groups and form zero-valence Ag (inset of Fig. 2c). In our study, both CNFs and DACs hydrogels were immersed into Tollen's reagent separately. After 1 hour immersion, transparent CNFs hydrogel showed no obvious coloration while transparent DACs hydrogel turned black. SEM imaging showed only a few particles were generated on CNFs surfaces (Fig. 2c), while a large number of nanoparticles were observed on DACs. These nanoparticles were uniformly distributed on the surface of and within the DACs sheets (Fig. 2d). This comparison revealed DACs hydrogel carried a large amount of aldehyde groups from the periodate oxidation.
Porous DACs aerogels were then used to remove Cu(II) and Pb(II) from aqueous solutions. As shown in Fig. 3a, sorption amount increased rapidly in the beginning when DACs sorbents were immersed in Cu(II) and Pb(II) solutions, and then gradually reached an equilibrium value. The initial large sorption rate was attributed to large amounts of available functionality sites when first placed in solution. Both Cu(II) and Pb(II) sorption systems reached equilibrium after 5 h, where ∼58.60% Cu(II) and ∼75.09% Pb(II) were removed from the solution. Given the amount of CNF material being used, the removal capacity was found to be 0.75 mmol g−1 for Pb(II) and 0.58 mmol g−1 for Cu(II). Compared to previous reports, our porous DACs aerogels was fabricated through a simple step of oxidation under mild conditions and yielded generally higher removal efficiency. Examples includes advanced nanocellulose-derived sorbents with functional groups of sulfite ions16 (0.54 mmol g−1 Au(III)), carboxyl groups12 (0.004 mmol g−1 Cu(II)), or poly(acrylic acid) and poly(acrylic acid)/sodium humate35 (0.12 mmol g−1 Cu(II)), as well as more complexly treated cellulose by multi-step reactions (e.g. 0.41 mmol g−1 Pb(II) and 1.02 mmol g−1 Cu(II);24 1.3 mmol g−1 Hg(II);21 0.06 mmol g−1 Pb(II) and 0.25 mmol g−1 Cu(II)25).
Numerical analyses were performed to gain insights into physical chemistry of the sorption process and to reveal if they were controlled by reaction kinetics, and/or film diffusion, and/or intraparticle diffusion. The Weber and Morris method36–39 was first used to analyze the diffusion process. According to this method, the sorption amount qt (mg g−1) of both Cu(II) and Pb(II) is plotted against the square root of time t0.5 (min0.5), as shown in Fig. 3b. A linear relation was obtained from both metals, and linear fitting curves did not pass the origin, indicating there was a certain degree of film diffusion control, in addition to intraparticle diffusion in both cases. Additionally, both curves showed two linear regions where the initial segment had a relatively large slope but the latter segment was nearly flat. The presence of two slopes suggests two steps were involved in the sorption process. The sloped segment could correspond to a film diffusion dominated case; while the flat segment represents the intraparticle diffusion controlled process.
To further confirm the sorption mechanism of the initial sloped region, the first 5 h data were fitted to the film diffusion rate model,37,40 where ln(1 − qt/qe) was plotted against time t (qe and qt are the amount of ions sorbed at equilibrium and at time t, respectively). Fractional attainment of the equilibrium (qt/qe) term is related to the concentration gradient in liquid film surrounding the sorbent, which is more specific to film diffusion controlled processes. As shown in Fig. 3c, the fitting gave high correlation coefficients (R2 > 0.97) for both Cu(II) and Pb(II), suggesting that the initial sorption was controlled by film diffusion. It should be pointed out that pseudo-first order model can also fit the data for first-hours sorption. However, it is more of an empirical equation, and not able to provide very insightful mechanisms for the sorption process. Therefore, our discussion here only focuses on the diffusion model.
From above, it is reasonable to conclude, the sorption of Cu(II) and Pb(II) on DACs sorbents are initially controlled by film diffusion and later by intraparticle diffusion. In the first few hours, metal ions may only occupy the aldehyde sites near the external surface of the sorbent. In this process, transfer of metal ions within the pores could be very fast, hence, the sorption rate was determined by diffusion across boundary layers of the fluids surrounding external surfaces of the sorbent, i.e. film diffusion. As the sorption proceeded, all available surface sites became occupied and metal ions penetrated deeply within the sorbent through mesoscopic channels. This process could be much slower and the intraparticle diffusion now became the rate-limiting mechanism.
Upon sorption, the removal of metal ions by DACs was mainly attributed to chemical interactions between the aldehyde functional groups and metal ions. In this regard, pseudo-second-order model37,41–43 was used to describe the metal ion removal processes. A pseudo-second-order model has the linear form of
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The effects of ion concentration on sorption amounts were shown in Fig. 4a at different temperatures. Each of the sorption amounts was obtained under equilibrium condition. The equilibrium was confirmed by the fact that the sorption amount showed no further increase after extended immersion hours in solutions. As the concentration increased from 0.3 to 6.0 mmol L−1 at 25 °C, the sorption amount of Cu(II) and Pb(II) increased from 15.60 to 24.64 mg g−1 and from 64.86 to 160.65 mg g−1, respectively (Fig. 4a and b). Monotonic increase of the sorption amount with solution concentration was a result of the high sorption capacity of mesoporous DACs sorbents.
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| Fig. 4 Sorption isotherm of Cu (a) and Pb (b) at different temperatures, and Langmuir fitting of the isotherm data of Cu (c) and Pb (d). | ||
The sorption isotherm was then analyzed using the Langmuir model44 and Freundlich model45,46 to understand how adsorbents were distributed between the solution and sorbent solids at equilibrium. The Langmuir isotherm is based on monolayer adsorption occurring at energetically equivalent sites of the sorbent (i.e., constant heat of adsorption for all sites). It has a mathematical form of
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qe versus lg
Ce) were nonlinear and gave very low correlation coefficients (less than 0.5). On the other hand, the fittings with Langmuir model (Ce/qe versus Ce) at all temperatures were of high correlation coefficients for both Cu(II) and Pb(II) (Fig. 4c and d, and values for Langmuir parameter kL and qmax were listed in Table 1), suggesting the sorption process was monolayer and all sorption sites (i.e. the aldehyde functional groups) were equivalent, and the distribution of aldehydes was homogeneous and uniform. Uniform distribution of aldehydes could be attributed to the complete conversion of secondary hydroxyl groups that are evenly distributed on each anhydroglucopyranose unit of cellulose molecules. Homogeneity and uniformity of aldehydes were also supported by the uniform coverage and narrow size distribution of Ag nanoparticles that were produced by DACs aerogel reduction (Fig. 2d).
| Heavy metal | T (K) | kL | Langmuir qmax | kd | ln kd |
ΔG° (kJ mol−1) | ΔH° (kJ mol−1) | ΔS° (kJ mol−1) |
|---|---|---|---|---|---|---|---|---|
| Cu(II) | 298 | 0.05315 | 25.6 | 4.09 | 1.41 | −3.49 | 9.80 | 0.045 |
| 308 | 0.06176 | 26.4 | 4.61 | 1.53 | −3.92 | |||
| 318 | 0.06639 | 27.0 | 5.41 | 1.69 | −4.47 | |||
| 328 | 0.06792 | 27.4 | 5.79 | 1.76 | −4.79 | |||
| Pb(II) | 298 | 0.00713 | 172.7 | 1.47 | 0.39 | −0.95 | 2.23 | 0.011 |
| 308 | 0.00739 | 181.2 | 1.51 | 0.41 | −1.06 | |||
| 318 | 0.00701 | 195.3 | 1.54 | 0.43 | −1.14 | |||
| 328 | 0.00701 | 204.5 | 1.60 | 0.47 | −1.28 |
Fig. 4 also revealed that at the four testing temperatures, isotherms showed the same trend for both Cu(II) and Pb(II) sorption, suggesting that the sorption mechanism of DACs was independent of temperature within the study range. However, the sorption amount of both Cu(II) and Pb(II) increased slightly as temperature increased. This could be a result of enhanced metal ions mobility at higher temperature and endothermic nature of the sorption process. To better understand the temperature influences, thermodynamics parameters were calculated based on equilibrium data and the thermodynamic equilibrium constants.
According to Khan and Singh's method,47,48 the thermodynamic equilibrium constant kd can be obtained from the intercept of plots ln(qe/Ce) against qe (Fig. 5a and b, value of kd were listed in Table 1). By plotting ln
kd versus 1/T (Fig. 5c), enthalpy change ΔH°, and entropy change ΔS° in the sorption process can be determined according to following equation:
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Fig. 5 Plots of ln(qe/Ce) versus qe for Cu (a) and Pb (b); plots of ln kd versus 1/T (c) for the determination of thermodynamic parameters. | ||
Obtained values for all thermodynamics related parameters were listed in Table 1. The results showed that ΔG° was negative for all testing temperatures, and became increasingly negative when temperatures increased. This discovery suggests that the sorption processes of Cu(II) and Pb(II) on DACs were spontaneous. ΔH° for both Cu(II) and Pb(II) were found positive, indicative of the endothermic nature of sorption processes. This also supported the earlier finding that the equilibrium sorption amount increased with increasing temperature. ΔS° for both metal ions were positive, which agrees with a previously reported work49 on the adsorption of Cu(II) by wood sawdust. According to that work, the positive change of entropy might be a result of redistribution of energy between the adsorbate and the adsorbent.
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