Zoltán
Somosi
ab,
Szabolcs
Muráth
ab,
Péter
Nagy
a,
Dániel
Sebők
c,
Istvan
Szilagyi
*ab and
Grant
Douglas
*d
aMTA-SZTE Lendület Biocolloids Research Group, University of Szeged, H-6720 Szeged, Hungary. E-mail: szistvan@chem.u-szeged.hu
bInterdisciplinary Excellence Center, Department of Physical Chemistry and Materials Science, University of Szeged, H-6720 Szeged, Hungary
cInterdisciplinary Excellence Center, Department of Applied and Environmental Chemistry, University of Szeged, H-6720 Szeged, Hungary
dCentre for Environment and Life Sciences, CSIRO Land and Water, WA, 6913 Wembley, Australia. E-mail: grant.douglas@csiro.au
First published on 24th October 2019
The efficient removal of a range of anionic and cationic contaminants from acid mine waters to facilitate water reuse or for safe discharge constitutes a major environmental challenge. Recently, layered double hydroxide (LDH)-type materials have shown considerable efficacy at experimental and full-scale for acid mine water treatment. In this study, LDH-type materials were prepared in situ under different experimental conditions with a method for their separation also developed. This work demonstrated that an interlinked network of smaller LDH aggregates was formed during synthesis leading to the development of stable colloids. Different approaches were tested to separate the solid materials containing the captured contaminants from the solute. Polyelectrolytes adsorbed strongly on the particle networks causing charge neutralization and overcharging, however, destabilization of the stable dispersions was unsuccessful. Diluting the stable dispersions led to rapid sedimentation and separation of the LDH, which facilitated higher solute recoveries.
Water impactNumerous studies document LDH as an adsorbent for different contaminants present in wastewaters, but few consider the removal efficiency of the spent adsorbent. This study gives an insight into in situ formation of LDH in both model and in acidic mine water systems enhancing the understanding of adsorption, sedimentation and colloidal properties during the removal process. |
Layered double hydroxides have the general formula of (MII(1−x)MIII(x)(OH)2)An−(n/2)·H2O, with 0.20 ≤ x ≤ 0.33 and An− as the prevailing anion, thus yielding a range of primary MII to MIII ratios of often mixed metal composition between 2:1 to 4:1. In the specific case of hydrotalcite, sensu stricto, MII is Mg2+, MIII is Al3+, in a 2:1 to 3:1 molar ratio, and An− is CO32−.19 Notably, however, a variety of other alkaline earths, transition metals, rare earth elements, and some actinides20 in addition to single anionic moieties, mixtures of anions, (metallo)oxyanions and on occasion, complex oxyanions21 may be incorporated into the hydrotalcite structure to yield a mixed composition LDH. Compared to other nanoparticles used for removal of ionic contaminant,22,23 one of the main advantages of the LDHs is the simultaneous capture of cations in the metal hydroxide layers and anions that are intercalated into the lamellar structure.
When utilized in industrial or mine water treatment for the removal of contaminants,15,16,24 one of the major impediments in maximizing the recovery of treated water is the efficient separation of LDH, as small particles or aggregates may be present due to the short reaction times following addition of reagents and which form stable dispersions. Efficient removal of LDH would facilitate higher water recoveries for reuse or environmental discharge as well as to allow the reuse of a clarified effluent suitable for other treatment processes such as the removal of remaining nitrate or sulfate as commonly found in industrial and mine wastewaters via the application of microbial bioreactors.25 Ion exchange and subsequent separation of other inorganic nanoparticles were carried out by polymer-induced aggregation,26 nevertheless, no efficient removals of LDH used for decontamination of wastewater have been reported in the literature.
In this study, we have examined the colloidal stability of four types of LDH including two formed from the treatment of an acid mine water and two model hydrotalcite compositions using different Mg precursors, Mg(OH)2 and MgCl2 to (i) better elucidate the fundamental colloidal properties of these various types of LDH, and (ii) to investigate methods to induce colloidal instability to facilitate flocculation.
Further investigation of the LDH or hydrotalcite structures was obtained from Fourier-transform infrared (FT-IR) spectra of the samples, which were recorded on a JASCO FTIR-4700 spectrometer equipped with a DTGS detector in attenuated total reflectance mode. Spectral resolution was 4 cm−1 with 256 scans collected for each spectrum. The spectra were recorded in the wavenumber range of 4000–600 cm−1. The spectra were baseline-corrected and smoothed.
Electrophoretic mobility was measured with a LiteSizer 500 (Anton Paar) device equipped with a 40 mW laser source operating at 658 nm wavelength. Disposable plastic omega-shaped capillary cells (Anton Paar) were used for the measurements. During sample preparation, calculated amount of polyelectrolyte and phosphate stock solutions were mixed with appropriate amount of samples 1–4 to adjust the flocculants and particle concentrations. The pH of the dispersions used in the experiments was kept the same as in the original samples.
Dynamic light scattering (DLS) technique was used to measure the hydrodynamic size of the dispersed particles. The measurements were carried out with the same LiteSizer device as above at 175° scattering angle in disposable plastic cuvettes (VWR). The cumulant method was used to fit the correlation functions, which were collected for 20 seconds to determine the hydrodynamic radius of the particles.
The morphology of the solids was characterized by a Hitachi S-4700 scanning electron microscope (SEM). The surface of the samples was covered with gold via physical vapour deposition before the measurements, which were conducted with 10 kV accelerating voltage.
Energy dispersive X-ray analyzer (EDX, Röntec QX2 system) was coupled to the microscope to provide the occurrence of elements in the samples. For these measurements, accelerating voltage was set to 20 kV and noble metal deposition was omitted.
The turbidity of the dispersions was assessed by recording the UV-visible (UV-vis) spectra with a Genesys 10S spectrophotometer (Thermo Scientific). The wavelength range used was 190–1100 nm with 0.1 nm scaling.
Fig. 1 Powder XRD patterns of the solid materials obtained from (a) sample 1, (b) sample 2, (c) sample 3 and (d) sample 4. |
Using FT-IR analysis, a range of peaks can be identified, which give insight into the interlayer anions present (Fig. 2). In samples 2 and 3, an intense band was found at around 1090 cm−1 corresponding to the region of sulfate symmetric stretching vibrations indicating the intercalation of sulfate ions within the LDH and/or adsorption on the outer surface. In samples 1, 2 and 3, a peak at 1365 cm−1 corresponds to carbonate asymmetric stretching, which is shifted towards higher wavenumbers in sample 4. A peak around 1635 cm−1 present in all samples corresponds to the scissor vibration of water located in the LDH interlayer. In all systems, a peak occurring at 3400 cm−1 corresponds to the valence vibration of O–H groups of water molecules or of surface M–O–H functionalities within the metal hydroxide layer of the LDH or brucite.
The above findings indicate that hydrotalcite preparation to form a predominant crystalline phase was least successful in sample 1 with the possibility of sulfate and carbonate present in an LDH/hydrotalcite surface layer, while brucite-LDH composite was found in sample 3. In sample 2 and sample 4, an LDH derivative and quintinite were formed, respectively. Samples containing hydrotalcite as the predominant phase were able to remove considerable sulfate from the acid mine wastewater, intercalated between the metal hydroxide layers and also potentially present on the outer surface. This has important implications, in particular to reduce sulfate level that is discharged to the environment, or as a reduced sulfate feedwater to sulfate-reducing bioreactors.
Electrophoretic mobilities of the samples were measured to assess the surface charge properties of the LDH and hydrotalcite particles, which were predominantly in the form of stable dispersions and as a starting point to investigate destabilisation pathways. The electrophoretic mobility for samples 1–4 were 8.9 × 10−9, 5.8 × 10−9, 4.3 × 10−9, 4.8 × 10−9 m2 Vs−1, respectively (Fig. 3) indicating a small positive surface charge of the materials in the dispersions with the similarity of all measurements consistent with the formation of a LDH/hydrotalcite layer on the Mg(OH)2 used as a precursor material in sample 1. This positive charge originates from the structure in the case of LDH/hydrotalcite29 and quintinite,30 while from the high isoelectric point and subsequent presence of protonated hydroxide groups for the brucite.31,32 All measurements were carried out at an ionic strength of 80 mM corresponding to the ionic strength of the acidic mine water that was used for the experiments.
Electrophoretic mobilities as a function of polyelectrolyte and phosphate concentrations are shown in Fig. 3. The mobilities of the brucite-containing systems (samples 1 and 3) were positive at low flocculant concentrations under the conditions investigated. In contrast, mobilities close to zero were measured in the LDH and hydrotalcite (quintinite) containing systems (samples 2 and 4) at low polyelectrolyte and phosphate concentrations. Such a reduced electrophoretic mobility is most likely due to the high ionic strength of ca. 80 mM in the dispersions, since elevated salt concentrations usually lead to screening of the surface charge and decreased mobility.40 For samples 1 and 3, charge neutralization occurred due to the adsorption of the negatively charged PSS, DXS and phosphate ions. The concentrations corresponding to the charge neutralization points are shown in Table S2.† Similar charge neutralization processes often give rise to rapid particles aggregation and to destabilization of colloidal samples.35,37,41–44
With increasing flocculant dose, particle surface charge became negative due to the progressive adsorption of negatively charged species onto the LDH/hydrotalcite surface. Similar charge reversal effects have been reported previously in systems containing colloidal particles and multivalent ions or polyelectrolytes45–47 and also for LDH.35 This phenomenon originates from the entropy gain due to the release of solvent molecules and counterions upon adsorption, from the laterally heterogeneous polyelectrolyte adsorption and from the attractive hydrophobic interaction between the polyelectrolyte and the surface.37 Adsorption of PSS and DXS caused higher magnitude of charge reversal at high flocculant concentration than phosphate owing to their excess of unbound negative charge centres following surface adsorption. Previous studies33,35,37,41,48 indicate that stable dispersions can also form at high flocculant doses, while destabilization of the dispersions are expected at the isoelectric points. In the four separate samples investigated here spanning model systems (samples 1 and 4) and real-world systems derived from acid mine waters (samples 2 and 3), effective destabilisation could not be achieved despite the use of two separate polyelectrolytes or phosphate. This phenomenon is investigated further below.
An investigation of the on-going stability of the dispersions was undertaken using DLS. Hydrodynamic radii ranged from 600 nm to 3000 nm in the samples with a polydispersity factor of approximately 0.8. While these data indicated that DLS was not a suitable technique to measure particle size and study aggregation behaviour in the samples, the DLS results suggest that the dispersions are probably composed of a network of aggregates or particles forming colloidal gel-like structures, which usually occurs at high particle concentrations, where the dispersed materials interlink in a stable 3D framework occupied by interstitial water moleclues.49–52 Such structures may be further stabilized by steric forces caused by the overlap of the adsorbed polyelectrolyte chains. The presence of these types of interactions has been reported in other polyelectrolyte-particle systems.35,53
To further investigate particle or aggregate morphology, SEM images were obtained (Fig. 4). It was found that the brucite and LDH or quintinite particles formed aggregated networks of few microns in diameter that may reflect their original hydrated structure. All samples tended to contain primary particles of a few hundred nanometers in diameter. Aggregate diameters were typically 1–3 μm. The SEM study revealed particles with irregular morphology, common to hydrotalcites and related materials synthesized by co-precipitation.13,54 The mixed chemical composition of sample 3 was also apparent with distinctly different crystal/aggregate morphologies observable.
Fig. 4 SEM images of (a) sample 1, (b) sample 2, (c) sample 3 and (d) sample 4. The scale bars indicate 1 micrometer dimension. |
To explore the composition of the solid materials, EDX analysis was performed on the aggregated samples (Fig. S1 and S2†). In sample 1, Mg and Al are uniformly distributed, however, according its XRD pattern, brucite is the main component and LDH is present only in small amounts, probably as a surface reaction rind. The elemental compositions of samples 2 and 3 are similar. These materials are intercalated with sulfate ions as confirmed in the EDX spectra and also in the FT-IR results discussed earlier. Regarding sample 4, while also containing the layer forming Mg and Al metals (like in samples 2 and 3), it has high chloride content consistent with the use of MgCl2, as a precursor reagent.
Based on information from DLS, in which suggested the presence of complex aggregates, the absorbance of the samples was measured as a turbidity proxy. This approach was successfully applied to investigate aggregation and sedimentation processes in non-transparent and polydisperse samples similar to those in the present study.48,55 As the UV-vis spectra indicated that none of the samples have a specific absorption around 450 nm, this wavelength was chosen to study the dispersion stability. Absorbance values recorded with the original samples during 60 minutes are shown in Fig. S3† and confirm that all samples formed stable dispersions.
As discussed above, neutralizing the charge of colloidal particles often leads to rapid aggregation and to unstable dispersions, from which the solids may settle.35,37,41 This phenomenon may be particularly advantageous in environmental applications, where contaminant-laden LDH/hydrotalcite needs to be removed prior to wastewater reuse or environmental discharge.13 With the development of a neutral charge, it is expected that repulsive interparticle interaction will be eliminated, thus leading to the destabilization of the particle aggregates.40 Time-resolved absorbance data of the original dispersions in the presence of the flocculants discussed above, whose dose was set to the isoelectric points (Table S2†), were recorded, however, little change in settling rates irrespective of the addition of either the PSS or DXS polyelectrolytes or phosphate was observed apart from the quintinite system in sample 4 (Fig. S4†).
Since the net charge of the particles was adjusted to close to zero via polyelectrolyte or phosphate addition, it can be assumed that the interaction between the aggregates and the stabilizing force between the colloidal networks is of non-electrostatic origin. Most likely, hydrophobic forces, steric and secondary chemical interactions such as hydrogen bonds are responsible for the interlinking between the particles and subsequent evolution of the stable 3D structures.
Since the formation of such interlinked materials occurs usually at high solid concentrations,50 the effect of dilution on the stability of the samples was investigated by measuring the time-resolved absorbance. Accordingly, samples 1 to 4 were diluted 10-fold with water, in which the pH and ionic strength were adjusted as per the original samples and time-resolved absorbance values were recorded over 60 minutes (Fig. 5).
For sample 1, rapid sedimentation was observed within five minutes indicating the destruction of the gel-like 3D structure. Similar behaviour occurred in samples 2 and 3, where complete sedimentation occurred after 25 and 20 minutes, respectively. These findings confirm the presence of interlinked particles and aggregates in the raw systems, which usually evolve at high particle concentrations, but simple dilution leads to the breakdown of the 3D network. For samples 2 and 3, the absorbance increased for a short time interval (15 and 10 minutes, respectively). This is due to the in vitro sedimentation process, which results in a transiently higher solids concentration of settling samples in the laser path. The pH of the samples was measured before and after the destabilization experiments and found to be stable (i.e., the initial and final pH was the same within the experimental error) during the measurements.
In contrast to samples 1 to 3, the turbidity of sample 4 decreased only slightly after 10-fold dilution over 60 minutes. Thus, it appears that a pure quintinite system is inherently more stable than that or either brucite/LDH or a mixed composition LDH.
To further study the effect of dilution on sedimentation, similar time-resolved settling measurements were carried out at several dilution rates. Accordingly, samples 1–4 were diluted to between 1 in 5 and 1 in 20 times the original sample suspended solid concentration with the pH and the ionic strength maintained as per the original samples with the time needed for the 50% decrease in the maximum absorbance measured (Fig. 6).
Fig. 6 Half time of sedimentation as a function of the dilution factor for sample 1 (circles), sample 2 (squares) and sample 3 (triangles). |
Sedimentation was markedly different depending on the composition of the solids and the extent of dilution. No net sedimentation was observed in sample 4 despite the substantial dilution factor employed. For sample 1–3, there was an initially steep decrease in the sedimentation time with increasing dilution with the most rapid sedimentation observed for sample 1 in the range at 5- to 10-fold dilution with a minimum sedimentation time of 125 seconds. For sample 2, sedimentation rapidly increased between 10- and 15-fold dilution with a minimum sedimentation time of 235 seconds. For sample 3, sedimentation also rapidly increased between 10- and 15-fold dilution with a minimum sedimentation time of 370 seconds.
It is apparent from this study both the morphology and composition of the LDH/hydrotalcite influences the threshold to sedimentation as exemplified by the relative stability of quintinite aggregates. In more complex systems, however, dilution is a simple and effective method to induce 3D aggregate instability that will regulate the rate of and extent of recovery of contaminant-bearing LDH in wastewater or acid mine water treatment applications. Importantly, we have observed settling rates of >10 m per day for ca. 1 g L−1 polymetallic LDH formed in situ in an acidic mine pit water.13 This high settling rate is similar to that achieved in this study after dilution to reduce total solids to similar (ca. 1 g L−1 or less) concentrations (Fig. 5 and 6). This is particularly pertinent where effective solid phase contaminant removal via settling is required prior to solute reuse or environmental discharge.
Footnote |
† Electronic supplementary information (ESI) available. See DOI: 10.1039/c9ew00808j |
This journal is © The Royal Society of Chemistry 2019 |