Introduction

Heavy metal pollution in waters is a worldwide environmental issue due to their toxicity and carcinogenicity, some toxic metals are dangerous even at trace concentration1. Among the available methods, adsorption is one of the most promising strategies for trace heavy metal retention2,3,4,5,6,7. Therefore, developing advanced functional materials for target pollutants have been actively conducted. In recent decade, numerous of nanoscale materials –nanosized zirconium oxides8,9,10, flower-like MgO11,12 and urchin-like FeOOH13- are exploited for heavy metal and environmental remediation, which exhibit superior sorption capacities and selectivity14,15,16,17. Such outstanding performances are mainly dependent on their unique morphologies, enhanced reactive activity and the strong sorption affinities18. However, the difficulties in solid-liquid separation and large hydraulic resistance might be the severe challenges, thus the development of nano-adsorbent in engineering merit is of strategic importance to heavy metal capture.

Recently, a large family of hybrid nanomaterial with excellent environmental properties has stimulated research enthusiasm. Briefly, the hybrid nanomaterials are fabricated by impregnating nanoparticles onto various porous carriers (e.g. granular activated carbon19, silica20, zeolite21,22 and macroporous polymer23,24). The obtained composite can combine the excellent flow characteristics of the porous supports and the specific affinities between nanoscale particles and heavy metal. Particularly, the template structures of matrix with nanopores can greatly improve the morphologies and reduce nanoparticle sizes25,26. Therefore, such hybrid fabrication has shed some lights on further engineering nanoparticles.

Now, most researchers always pay more attentions to the astonished morphology and controllable preparation27,28. Nevertheless, the well-defined morphology with high sorption capacities aren’t always the exhibition of satisfactory performances in application views29,30 Specifically, the serious pore blocking in the anchorage of nanoparticle always leads to poor sorption diffusion, which will bring about the low sorption efficiency in high-speed flow application31,32 Viewing the classical intraparticle-diffusion theory33,34, the sorption permeation is mainly depended on the pore channel structure and a narrow entry interspace can significantly inhibit the accessibility of target heavy metals. Therefore, how to break through the diffusion barriers of pore structures is a severe problem for resolving.

As well known, highly charged unites can achieve the efficient ion directional diffusion by external electric fields, e.g. desalination by electrodialysis methods35,36,37. Therefore, we assume that the applying suitable charged surroundings within matrix interspace possibly accelerates the ion-diffusion toward available active sites. Here, we reported a new polystyrene/nano-ZrO2 composite (denoted as NZO-PS) modified with the sulfonate (-SO3Na) groups for Cu(II) sequestrations. The immobilized negatively charged groups can attract the target metals by strong electrostatic forces, boost the ion-transport and further improve the sorption utilization of nanoparticles. The representative toxic metal Cu(II) is selected as target pollutant and series batch and column tests are performed to evaluate the possible sorption behaviors and diffusion mechanism.

Results

Characteristics of NZO-PS

The detailed structure parameters of obtained NZO-PS are shown in Table S1 and systematic characterizations are illustrated in Fig. 1. Figure 1a suggests that NZO-PS is the spherical beads with sizes of approximately 800 μm. The different SEM micrographs (Fig. 1c,d) of hemisphere profile indicate that the ZrO2 particles are well incorporated into the inner surface regions and block parts of cross-linked pores. The EDS profile scanning analysis (Fig. 1e,f) reveals the entrapped ZrO2 particles are uniformly dispersed in a ring-like region.

Figure 1
figure 1

SEM characterization of NZO-PS: (a) SEM of the spherical NZO-PS bead; (b) the hemisphere profile of NZO-PS (c) SEM of PS inner surfaces (d) SEM of of NZO-PS inner surfaces; (e) the cross-section S distribution (f) the cross-section Zr distribution of NZO-PS by SEM-EDS.

Moreover, AFM analyses (Fig. 2) further gain new observations into the different morphologies before and after nano-ZrO2 incorporation. It can be detected that the inner surfaces profile of matrix PS displays outstanding height difference with a vertical height approximate ±400 μm, indicating the broad cross-linked macroporous structures. Comparatively, for NZO-PS, the visible highlight regions and smooth surface height variations (approximate 20–100 nm) further prove the successful implantation of ZrO2 particles and the possible resulting pore blocking

Figure 2
figure 2

AFM analysis of NZO-PS; (a) AFM line profile analysis of PS; (b) AFM line profile analysis of ZrP-MPN; (a) AFM 3D analysis onto the inner surface of PS; (b) AFM 3D analysis onto the inner surface of NZO-PS; (c) surface height variations comparison before and after ZrO2 loadings.

BET results (Table S1) show that the ZrO2 incorporation results in a understandable drop in pore volume and average pore diameter. Interestingly, a slightly increase in BET surface areas from 14.8 to 18.3 m2/g is possibly ascribed to the presence of nanostructure ZrO2 particles with higher surface area. TEM image (Fig. 3a) of NZO-PS further reveals that the implanted ZrO2 particles exhibit outstanding monodispersity with sizes ranging from 8 to 14 nm. Such well-defined morphology can be partly attributed to the cross-linked nanoporous template effects as well as the highly charged surroundings from the -SO3Na+ of matrix38,39. X-ray diffraction investigation proves the amorphous or low crystalline pattern of the encapsulated nano-ZrO2 (Fig. 3b) by observing the high background noise and broad peaks. Considering the mild synthesis conditions, thus, it is readily to prepare the amorphous pattern. In facts, the amorphous ZrO2 particle is more beneficial to sequestration of Cu(II) ions and the highly crystalline forms will constrain the Cu(II) accessibility by the crystal lattice match and restraint, which has been confirmed in our previous study40.

Figure 3
figure 3

(a) The TEM characterization of NZO-PS; (b) XRD patterns of the obtained NZO-PS and matrix PS.

The effects of solution pH on adsorption

Series batch tests for adsorption performances toward toxic Cu(II) ions were conducted using conventional bottle-point method. The Cu(II) uptake is a pH-dependent process (Fig. 4) for both purified ZrO2 and composite and calcium ions are also introduced for screening the potential adsorption by SO3Na groups. Especially notice that the ZrO2 particles exhibit negligible Cu(II) uptake with solution conditions until pHs > 5.0, indicating its limited applicability to acidic surroundings. Comparatively, for NZO-PS, the encapsulated ZrO2 particles display the considerable sorption performances at broad applied pH ranges (pH > 3). Such distinct appearance can be ascribed to the unique surface properties of NZO-PS. The potential proton buffering effects from sulfonic acid groups (SO3Na) and inherent high cross-linking structures41 can lead to the acidic-basic variance of inner/outer regions. Besides, the immobilized nano-ZrO2 with large surface areas and active sites, also imparts more powerful sorption affinities toward Cu (II) removal than the bulk one14,17 and the trace zirconium release further demonstrate its stability and applicability.

Figure 4
figure 4

Effect of solution pH on the uptake of Cu(II) ions onto NZO-PS and ZrO2 at 298 K.

Common competition influences on adsorption

In general, the common cations, particularly for Ca(II) Mg(II) and Na(I), are always ubiquitous in the metal-contaminated waters, the sorption interferences may be a main adverse influence due to its high contents and the same positive-charge. Therefore, it is significant to validate the underling sorption selectivity onto the given NZO-PS. Figure 5a–c shows that both NZO-PS and PS display the decreasing sorption tendency with bivalent Ca(II)/Mg(II) except for Na(I) additions continuously. Comparatively, the composite NZO-PS still exhibits distinguished Cu(II) uptake performances. Of particular note, the Cu(II) removal is slightly influenced with above 16 times Ca(II) additions, while the Cu(II) uptake onto PS brings out a dramatic decrease (near to zero) at the same conditions. In general, the sulfonate moiety binding onto PS always presents nonspecific electrostatic forces toward Cu(II) exchange and the high level of common cations additions will result in serious sorption competition. Whereas, for NZO-PS, the encapsulated ZrO2 nanoparticles can exhibit powerful inner-sphere surface complexation42,43, i.e. the monodentate and bidentate chelation. Such specific affinities will greatly enhance the Cu(II) adsorption onto NZO-PS, which has been demonstrated by EXAFS and XPS analysis44,45. Moreover, considering the possible coexistence of other heavy metals and strong competition in wastewaters, three common heavy metals (Zn(II), Ni(II), Cd(II)) were selected to evaluate the potential sorption influences and the results were shown in Figure S2. Similar to the alkaline metals additions, NZO-PS and its matrix PS also display decreasing sorption performances, particular for Ni(II) and Cd(II). Comparatively, NZO-PS still shows preferential Cu(II) sequestrations, further indicating its strong affinities and applicability. Additionally, high contents of common anions were also involved to examine the possible sorption effects (Figure S3). As is expected, the negligible Cu(II) sorption variations in absent or present anions (NO3, Cl, SO4) also demonstrate that anions might be the weak competitors for Cu(II) uptake.

Figure 5
figure 5

Cu(II) sorption competitive comparison of NZO-PS and its host material PS (a) Ca(II) ions interfere; (b) Mg(II) ions interfere; (c) Na(I) ions interfere; (d) comparison of sorption behaviors onto NZO-PS and its corresponding binary mixture ZrO2 + PS (For (a−c) 1 g/L sorbent, initial Cu(II) = 0.25 mM, pH = 5.2−5.8; (d) adsorbent: 0.1 g NZO-PS and 0.088 g PS + 0.012 g ZrO2 sorbent, 500 mg/L background calcium ions).

Furthermore, the composite NZO-PS and its corresponding composition ZrO2 powders and PS beads mixture were also investigated for Cu(II) elimination. As depicted in Fig. 5d, NZO-PS reveals more favorable sorption behaviors than its binary mixture, which further proves the importance of hybridizing nanomaterial fabrication. The preferential sorption onto NZO-PS can be ascribed to the following aspects. (1) The negative-charged SO3Na moiety within matrix can accelerate the target Cu(II) ions diffusion and then form high concentration of Cu(II) ions enrichment within the nanopores phase of NZO-PS. Such acceleration mechanism is derived from the classical “Donnan membrane effects”46 (2) The crosslinking polymeric chains of matrix can also facilitate the formation of immobilized nano-ZrO2 particles47. Therefore, the collaborative efficient sequestration in the reactive interface is achieved though the highly charged SO3Na transport enhancement and selective Cu(II) uptake onto embedded nano-ZrO2. A colourful schematic structure and sorption mechanism of NZO-PS are shown in Fig. 6.

Figure 6
figure 6

The schematic structure and sorption mechanism of the resulting NZO-PS.

To further elucidate the sorption priority, the selective distribution constant Kd (in L/g) was determined as the following equation:

where C0 is the initial Cu(II) concentrations of the solute, Ce is the Cu(II) effluents in equilibrium, V represents the volume of the solute and m is the mass of the material. Evidently, the substantially larger Kd values of NZO-PS further prove the strong affinities and favorable selectivity (Table S2).

To gain further insight into the sorption behaviors, Fourier Transform Infrared Spectroscopy (FT-IR), X-ray Photoelectron Spectroscopy (XPS) and Zeta Potential Plus analysis were conducted to obtain the possible mechanism for selective Cu(II) uptake. The distinct IR absorption peaks at 1183 cm−1 and 1128 cm−1 indicate the presence of SO3H groups (Figure S4-a). In general, the Cu(II) uptake by SO3Na are nonspecific affinities, driven by electrostatic attraction and the strongly specific adsorption is mainly ascribed to the existence of nano-ZrO2. The sharp peaks (Figure S4-b) at approximate 502 cm−1 are assigned to Zr-O bond, while Cu(II) ion uptake induced to the apparent band shifts from 502 cm−1 to 505 cm−1, suggesting the formation of strong sorption affinities. XPS investigation further demonstrate the different sorption behaviors. Figure 7a reflects the Cu 2 p binding energy of 935.8 eV by SO3-Cu, while the distinct Cu 2 p binding energy peak at 934.6 eV is ascertained by Cu(II) loaded ZrO2 particles, the apparent shifts of 1.2 eV to a lower energy level reveal the formation of the specific affinity between Cu(II) and ZrO2 (Fig. 7b). Figure 7c displays the representative Cu 2 p binding energy state of Cu(II) uptake onto NZO-PS, the expanded full width at half maximum (FWHM) implies the presence of different Cu-complex substances. Based on the binding energy of diverse Cu(II) species or sorption sites, the Cu 2 p spectra are divided into two peaks corresponding to SO3-Cu (935.8 eV) and Zr-O-Cu(934.6 eV). As for Cu(II) loaded NZO-PS, the area fractions of SO3-Cu (935.8 eV) and Zr-O-Cu(934.6 eV) are occupied around 36.0% and 64.0% respectively. However, 50 times of Ca(II) addition brings about distinguished peak areas variations with nearly 1% SO3-Cu and 99% Zr-O-Cu respectively (Fig. 7d). Such results indicates that nano-ZrO2 can endow the strong sorption selectivity toward Cu(II) removal and SO3Na can only impart negligible Cu(II) adsorption performances at electrolytic backgrounds. Moreover, the evidence of highly negatively charges onto SO3Na for diffusion enhancement is also proved by Zeta Potentials analysis. Figure S5 depicts the zeta potential variations at wide pH conditions onto NZO-PS and purified ZrO2 particles. Interestingly, the composite NZO-PS exhibits negatively large zeta potentials at broad pH ranges (2.0–13.0) and the surface charges of encapsulated ZrO2 and H+ additions will be negligible as compared to the highly negative sulfonate groups of host. Therefore, the diffusion enhancement and enrichment toward Cu(II) will be available at wide pH conditions. However, Considering the pHzpc = 5.3 of ZrO2 particles, it is believed that the favorable sorption pH ranges from 5.3 to 6.2, which coincides with the solution pH effect results.

Figure 7
figure 7

High-resolution XPS spectra of NZO-PS. a) Cu 2P spectra of Cu(II) loaded PS samples; b) Cu 2P spectra of Cu(II) loaded purified ZrO2 samples; c) Cu 2P spectra of Cu(II) loaded NZO- PS samples; d) Cu 2P spectra of Cu(II) loaded NZO- PS samples in presence of high level of Ca(II) ions competition.

Sorption kinetic evaluation and sorption isotherms

Sorption kinetic experiments were conducted to further gain new insight into the ions transport enhancement. Figure 8a–c illustrates the Cu(II) sorption kinetic curves of NZO-PS/PS and 180 min minutes are satisfactory enough to approach sorption equilibrium. It is significant to note that the similar sorption equilibrium time onto both sorbents suggests the potential sorption diffusion enhancement. In general, the ion permeation is greatly dependent on the pathway of spherically porous structure. A narrow channel usually reflects the poor diffusion property, resulting in the prolonged equilibration time and low utilization of sorbent. Thus, the blocking pore structures onto NZO-PS are usually expected to show the inefficient Cu(II) ion sorption diffusion. Whereas, the similar sorption kinetic behaviors onto NZO-PS suggest that the pore diffusion will not be the principal constraints and the surface groups (-SO3Na) within matrix will grant more prominent roles by electrostatic enhancement.

Figure 8
figure 8

Adsorption kinetics of Cu(II) ions onto NZO-PS and its matrix PS at 298 K. (a) the pseudo-first-order fitting (a) the line fitting for K values; (b) the pseudo-second-order fitting (b) the line fitting for K values; (c) the intraparticle diffusion model (sorbent: 0.2 g/L, initial Cu(II) 0.5 mM pH = 5.3–6.1); (d) sorption isotherms onto NZO-PS at different temperatures by Langmuir model fitting.

To further verify this opinion, the pseudo-first/second -order kinetic and Intraparticle diffusion models are performed and the detailed formulas as follows48:

The pseudo-first-order model:

The pseudo-second-order model:

Intraparticle diffusion model:

where qt and qe represent the amount of Cu(II) ions adsorbed (mg/g) in equilibrium and time t respectively and k, kp is the kinetic rate constant. Observably, the sorption process can be well described by the pseudo-second-order modeling (Fig. 8b Table S3) with a high correlation coefficient (R2) (>0.993). Besides, the excellent intraparticle diffusion fitting further indicates the intraparticle diffusion process. The similar K values of NZO-PS and PS further demonstrate the acceleration of ion transport.

Sorption isotherms were also performed at three different temperatures to examine the possible effects on Cu(II) uptake and the results are shown in Fig. 8d. Apparently, Cu(II) adsorption onto NZO-PS displays thermodynamics dependent process. Higher temperatures are favorable for Cu(II) uptake, which suggests the possible endothermic interactions with the maximum sorption capacities of approximate 108 mg/g. Additionally, the sorption behaviors onto NZO-PS are also described, according to the classical Langmuir, Freundlich isotherms as follows:

Langmuir model

Freundlich model

where Ce represents the Cu(II) concentrations at equilibrium and Qe is the corresponding adsorption capacity, Qm is assigned to the maximum sorption capacity, kL kF and n are parameters.

The detailed fitting data are listed in Table S4. It is observed that Cu(II) uptake onto NZO-PS can be well described by Langmuir model and the maximum calculated capacity (108 mg/g) coincides with the sorption data in experiment. Besides, the sorption performances can also roughly compare with other Cu(II) adsorbents in literatures (Table S5). The large sorption capacity further verifies the significant application feasibility.

The fixed-bed column application for Cu(II) retention

High speed column tests were performed to evaluate the applicability of the given adsorbent. Figure 9a implies that NZO-PS displays efficient Cu(II) uptake performances in a superb fast fixed-bed system and the effluents can meet the drinking water standard recommended by WHO (1 mg/L) with 2000 bed volume (BV) treated capacities before significant breakthrough. Whereas, the inefficiency onto PS may be ascribed to the weak Cu(II) affinity and strong competition. Besides, the wastewater (detailed components in Table S6) from electroplating industry in Qinhuangdao, was also tested and the results of 3200 BV treated capacities further demonstrate the efficient applicability (Fig. 9b). Moreover, the exhausted NZO-PS can be readily regenerated in ten-bed volumes (efficiency: >90%) using 0.5% HCl + 10% NaCl binary solution. Batch sorption further verifies its efficient adsorption- regeneration stability with at least five recycled uses (Fig. 9c).

Figure 9
figure 9

Comparison of breakthrough curves of Cu(II) uptake in fixed-bed columns. (a) The column adsorption curves of NZO-PS and PS; (adsorption: influent Cu(II) = 3 mg/L, Ca(II) = 200 mg/L, Mg(II) = Na(I) = 100 mg/L, pH = 5.5–6.2, SLV = 0.75 m/h, EBCT = 4 min); (b) the wastewater from electroplating industry (initial Cu(II) = 0.7–0.9 mg/L, SLV = 0.75 m/h, EBCT = 4 min); (c) batch sorption-degeneration tests onto NZO-PS at 303 K. (sorbent: 2 g/L, adsorption: Cu(II) = 50 mg/L, Ca(II) = 200 mg/L, Mg(II) = Na(I) = 100 mg/L, pH = 5.5 = 6.3; regenerant: 20 mL−0.5% HCl + 10% NaCl for 5 h at 298K) (d) influences of various feeding velocities on Cu(II) removal performance onto NZO-PS and NZO-PC.

Additionally, such outstanding Cu(II) sorption behaviors are also greatly associated to its unique functional structure. i.e. Cu(II) ion diffusion enhancement though negative-charged SO3-Na groups. Note that a new composite (NZO-PC) modified with the neutral chloromethyl groups (-CH2Cl) is also involved for a reference and its detailed preparation (Figure S1), characterization (Figure S7) were shown in supporting information. Attractively, NZO-PS exhibits satisfactory Cu(II) sorption (Fig. 9d) by varying the high feeding speeds of 15 BV/h, 30 BV/h and 60 BV/h respectively. Whereas, the neutral NZO-PC displays inefficient Cu(II) uptake with the treated capacities of about 70 BV at the feeding velocity of 15 BV/h, further decreasing the feeding speed to 1 BV/h can moderately improve its sorption performances (170 BV treatments). Considering the similar nano-ZrO2 loadings and pore structures (Table S1), it is expected that the presence of negative-charged groups SO3Na can remarkably increase the contact probability of target Cu(II) ions and available active sites, boost the potential Cu(II) sorption permeation and further enhance the efficient Cu(II) sequestration onto NZO-PS.

Next, a simple box-model is assumed to further interpret the above sorption behaviors. We hypothesize that the whole sorption system is divided into two different phases by a hypothesis diffusion membrane. The left represents sorbent phase and the right is assigned to the solution.

In the case I: NZO-PC (Figure S8a), the 0.1 mM Cu(II) ions can move cross the diffusion membrane equally for equilibrium with the equation as follows:

Nevertheless, for case II, (Figure S8b), the SO3-Na moieties are fixed onto NZO-PS and it is difficult to enter the right surroundings. Consequently, in sorbent phase, the extra-large charges will greatly attract the target Cu(II) ions diffusion and the enrichment environment (202 times calculated by Donnan principle35) in the left is realized at equilibrium, the detailed formula as follows:

The above calculation suggests that the diffusion enhancement and enrichment proportion are greatly dependent on the group contents of R-SO3Na and Cu(II) concentrations, the high fixed-charges and trace feeding metallic ions can be preferential option. Such calculation results also agree with the results of column tests.

Discussion

We offer a new route to break through the pore structure-dependent sorption diffusion process. Specifically, a new nano-ZrO2/polystyrene composite modified with a specific fixed–SO3-Na groups has been successfully fabricated for Cu(II) sequestration. The presence of negative-charged SO3-Na groups will enhance Cu(II) ions transport and enrichment by strong electrostatic force. Such functional design can overcome the potential application bottleneck for the blocked diffusion and greatly promote the sorption performance of sorbent. As another point of view, such highly charged groups can increase the potential contact opportunities of nano-ZrO2 and target Cu(II) ions, which favors for trace heavy metals sequestrations.

As for the characterization of NZO-PS, the EDS analyses reflect the uniform modified S element and ring-like Zr distributions. Such phenomenon is interesting and the uniform coverage of sulfur element testifies the homogeneous sulfonation reactions for SO3Na introduction. While, the incorporation of nano-ZrO2 may be a gradual diffusion process and the pore blocking in preparation will restrain zirconium salts precursor and strongly alkaline solutions diffusion into the center areas for active ZrO2 formation. Besides, the slightly increase of BET surface areas from 14.8 to 18.3 m2/g after immobilization can be possibly ascribed to the nanoscale sizes of ZrO2 particles, which imparts sufficient surface area and abundant activated sites for target heavy metal removal.

An interesting observations are the different pH behaviors for Cu(II) captures onto NZO-PS and ZrO2 powers. The favorable Cu(II) uptake is detected at pH = 3-6 onto NZO-PS and solution pH > 5 for bulk ZrO2. Such phenomenon can be ascribed to the different H+ activities of inner pore and external solutions. Note that the strong crosslinking net structure of polymeric matrix can anchor the embedded nano-ZrO2 particles to play a significant role for the solution chemistry variations. In addition, the surface negatively charged sulfonate group (SO3Na) can further buffer the H+ accessibility by the formation of protonated SO3H. The results imply that NZO-PS can work more efficiently under weak acidic solution than the bulky ZrO2 particles, which extends the applicability of nano-ZrO2 by hybridization design.

In summary, we fabricate a new hybrid nanomaterial by impregnating nano-ZrO2 onto polymeric porous polystyrene modified with sulfonate group (SO3Na). The charge-surface functionalization route can possibly enhance the target Cu(II) diffusion and promote utilization of embedding nano-ZrO2 particles. In addition, the hybrid material also exhibit superior selectivity and fast kinetic behaviors and recycled sorption-regeneration properties. All the results demonstrate the highly charged functionalization design is a smart choice for heavy metal remediation. Meanwhile, this route can be extended to prepare other functional composite materials.

Experimental Details

Fabrication of the hybrid HZO-PS

The fabrication of the resultant material was conducted (Fig. 10) as the following procedures. The polymeric polystyrene beads - prepared by the styrene and divinylbenzene suspension polymerization- were immersed into 93% sulfuric acid solution at 353–378 K for SO3H introduction49. Then the obtained sulfonated polystyrene beads (PS) will react with the Zr(IV) salts precursor by ion-exchange mechanism and obtained the intermediate PS-Zr(IV); afterward, 5% of NaOH solution was used as precipitant for in-situ formation of Zr(OH)4 in the inner pore regions of matrix. The framework nano-template and polymeric crosslinking chains could benefit to obtain the embedded nanoparticles. Finally, thermal treatment at 333 K was performed for the encapsulated nanoparticle immobilization and the encapsulated hydrated zirconium oxide nanocomposite NZO-PS was prepared.

Figure 10
figure 10

The simple preparation procedure of NZO-PS.

Batch Cu(II) Sorption tests

Series batch sorption experiments for adsorption performance towards Cu(II) uptake were performed by the bottle-point method. The effects of solution pH: 0.025 g of NZO-PS was introduced into 100 mL flasks containing 15 mg/L Cu(II) ions and 1% NaOH/HCl was used to adjust the desired pH values, the above bottles were then transferred into an incubator shaker at the constant temperature for above 20 h to ensure sorption equilibrium. Finally, the equilibrium pH and corresponding Cu(II) concentrations were determined. Competition tests were conducted by similar ways and the common cations -Ca(II), Mg(II), Na(II) ions- were added with different levels to evaluate the sorption selectivity toward Cu(II) ions. Kinetics tests were performed by sampling 1 mL-solution at various time intervals in a 1000 mL round-bottom flask containing 30 mg/L of Cu(II) ions and 0.2 g of NZO-PS beads. Ca(II) ions as competitor were also involved, if necessary, to estimate the potential ionic strength influence on kinetic permeation. Finally, kinetic data were calculated by determining the sample Cu(II) contents and its corresponding time. More experimental data were described in the captions and figures.

The packed column experiments

The flow-adsorption column tests were performed in a small Plexiglas column (12 mm diameter and 150 mm length) equipped with water bath equipment. The peristaltic multi-channel pump was used for getting the desired liquid velocity. The water-swelling sorbent of NZO-PS/PS (5 mL) was packed in the separated columns. the known content of Cu(II) ion feedings for stimulating heavy metal contaminated waters and real electroplating wastewaters were used to validate the application feasibility of NZO-PS. The detailed hydrodynamic parameters and feeding conditions are shown in the figure captions. The regeneration were tested in the same column after adsorption, the binary 0.5%HCl + 10%NaCl mixture was used as the regenerant in a slow liquid velocity to ensure the fully stripping and the SLV and EBCT were equal to 0.05 m/h and 60 min, respectively. Next, the flow-speed test influences were then conducted to elucidate the potential kinetic diffusion mechanism and the composite material NZO-PC was involved for comparison. Note that in this tests, all the sorbents were packed with 3 mL of volumes to avoid the possible fluid resistance interference in the high-speed sorption operations.

Characterizations

The Cu(II) contents were determined by a Shimadzu AA-6800 atomic absorption spectrometer equipped with deuterium background correction. The morphology of nanocomposite NZO-PS was taken by a field emission scanning electron microscope, FESEM (Hitachi S-4800, Japan). X-ray diffraction (XRD) patterns were performed on an XTRA X-ray diffractometer (Switzerland) and Cu Kα radiation (λ = 1.5418 Å) with a scan rate of 2o s−1. AFM images were taken using multimode 8 scanning probe microscopes (Veeco Instrument Plainview, NY, USA) with silicon nitride cantilever probes. The pore structure parameters (surface areas, pore volume, average pore sizes) were determined by nitrogen sorption measurements using micrometrics ASAP 2020 (U.S.). TEM images were recorded using high-resolution transmission electron microscopy (HRTEM, JEM2010) equipped with a Gatan CCD camera working at accelerating voltage of 200 KV. The zeta potentials of adsorbents were measured in folded capillary cells using the Nano ZS90 zetasizer (Malvern Instruments, UK). XPS analysis of given samples were conducted with a spectrometer (UlVAC-PHI model 5000 Versa probe) and the results were corrected and fitted using a curve-fitting program (XPS-peak4.1), FT-IR spectral (Nexus870, USA) were examined with a pellet of powered potassium bromide and sorbent powders in 400–4000 cm−1.

Additional Information

How to cite this article: Zhang, Q. et al. Accelerated Sorption Diffusion for Cu(II) Retention by Anchorage of Nano-zirconium Dioxide onto Highly charged Polystyrene Material. Sci. Rep. 5, 10646; doi: 10.1038/srep10646 (2015).