Abstract
In order to obtain functionalized silica colloids with magnetic properties, the three-step reaction, was carried out. The aqueous suspension of iron oxide nanoparticles as magnetic core (maghemite—γ-Fe2O3) was synthesized according to the Massart’s method (Massart in IEEE Trans Magn 17:1247–1248, 1981). A silica shell was obtained onto maghemite employing a modified sol–gel method by Salgueirino (Salgueirino-Maceira et al. in Adv Mater 19:4131–4144, 2006). As-synthesized magnetic silica core/shell nanocomposites were further functionalized by the post-grafting approach, using (3-Aminopropyl)-trimethoxysilane (APTMS) (Pham et al. in Langmuir 18:4915–4920, 2002). The obtained materials were characterized by nitrogen adsorption/desorption measurements, X-ray powder diffractometry (XRD), transmission electron microscopy (TEM). Particle sizes were measured by diffraction laser (DL). In order to establish colloidal stability of the system, zeta potential were measured. The syntheses routes led to obtain both, good purity of maghemite particles (more than 90 %) and their good coverage by outer silica shell. Thanks to their nanometer size and surface properties (especially, presence of amino groups which can ensure the electrostatic interaction between surface of adsorbent and adsorbate molecules), as-prepared nanocomposites can be considered as promising adsorbents. It can be found in the literature, that such systems are used in medicine as targeted drug delivery systems (Chen et al. in J Magn Magn Mater 322:2439–2445, 2010; Bele et al. in J Chromatogr B 867:160–164, 2008) or in environment protection as magnetically removable adsorbents (Giakisikli and Anthemidis in Anal Chim Acta 789:1–16, 2013; Tural et al. in J Phys Chem Solids 72:968–973, 2011).
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1 Introduction
In the last two decades, an increased development in the field of meso- and nanoscience has been achieved. Especially, in the field of colloidal science, in which materials have at least one characteristic dimension in the range of 1 nm to 1 µm (Xia et al. 2000). Inorganic colloidal particles are small objects which are dispersed in solvent. Nowadays, so-called core/shell structures are of great interest among researchers in many scientific groups. Such objects can deliver many interesting properties, which cannot be ensured by singular particles. Core/shell hybrid materials can be composed of different core materials, which are characterized by many interesting properties, such as: magnetic (Hyeon 2002; Deng et al. 2008; Kim et al. 2008), fluorescence (Tovmachenko et al. 2006; Reiss et al. 2009), luminescent (Mahmoudi et al. 2011) etc. Especially, superparamagnetic iron oxide nanoparticles (SPIONs) (Salgueirino-Maceira and Correa-Duarte 2007) are promising materials for many biomedical applications, such as hyperthermia treatment (Laurent et al. 2011), magnetic resonance imaging (MRI) (Schlorf et al. 2011), targeted drug delivery systems, especially in cancer treatment (Laurent and Mahmoudi 2011; Rosena et al. 2012; Wahajuddin and Arora 2012), magnetically removable catalysts (Lee and Lee 2008) and, more recently, as magnetically removable adsorbents (Tang and Lo 2013; Zhang et al. 2008). Nevertheless, there is a need to modify their surface in order to improve their biocompatibility and biodegradability. Thus, the above-mentioned magnetic cores can be modified with a broad range of outer shells, e.g. silica (Yi et al. 2005; Guerrero-Martinez et al. 2010) or polymers (Gupta and Gupta 2005; Rudzka et al. 2012; Guo et al. 2005). The surface modification of magnetic nanoparticles is crucial for the control of their chemical and physical properties, and colloidal stability, which is very important in their further applications. As mentioned above, SPIONs are very attractive in many biological applications due to the fact that they are highly biocompatible and biodegradable, as well as suitable for surface modification in order to improve those properties. What is more, the surface functionalization by outer shells provides them with a steric barrier against agglomeration.
A form of matter arrangement called the double electrical layer is created at the solid/electrolyte interface. There are some literature reports about α-Fe2O3. The novelty of the paper is characterization of the core/sell structures/electrolyte interface (Chibowski and Janusz 2002).
In this work, we present synthesis, surface characterization and zeta potential measurement of the synthesized nanoparticles composed of magnetic core and silica shell, as well as those core/shell structures functionalized with amine groups. Effects of pH and ionic strength on the zeta potential properties of the above-mentioned nanocomposites, were examined.
2 Experimental
2.1 Reagents
The following compounds were used: FeCl3·6H2O (Chempur), FeCl2·4H2O (Chempur), NH4OH (30 %, Chempur), HCl (37 %, Chempur), FeNO3·9H2O (POCH), HNO3 (65 %, POCH), tetraethoxysilane (TEOS 99 %, Sigma), ethanol (96 %, STANLAB), (3-Aminopropyl)-trimethoxysilane (APTMS 95 %, Acros). All chemicals were used as received, without further purification. For the preparation of all suspensions and solutions, deionized water (Millipore, USA), was used.
The Fig. 1 presents schematic synthesis route of functionalized core/shell nanocomposites, in respect to their surface nature.
2.2 Synthesis of γ-Fe2O3
The maghemite nanoparticles were obtained by co-precipitation of iron(II) and (III) salts in a basic medium, reported by Massart (1981). Briefly, 20 mL of a 1 M solution of FeCl3 and 5 mL of a 2 M solution of FeCl2 (in 2 M HCl), were added at room temperature to 250 mL of a 0.7 M ammonia solution. The black magnetite precipitate was produced in a few seconds and kept under mechanical stirring during 5 min. After this time, the magnetic nanoparticles were decanted by using the permanent magnet. The supernatant was removed, and moist precipitate was heated up to about 90 °C, while stirring on a hot plate. After about 5 min, magnetite nanoparticles were oxidized by adding 20 mL of 2 M HNO3 and 30 mL of 0.33 M FeNO3 to the solution. After about 1 h at 90 °C, under mechanical stirring, the oxidation step was terminated. The dispersed maghemite nanoparticles was centrifuged and redispersed in water. The cleaning process was repeated several times. The clean naoparticles were redispersed in distilled water, to obtain the final concentration 4.72 mg/mL.
2.3 Synthesis of γ-Fe2O3/SiO2
A silica shell was produced on maghemite cores using the modified well-known Stober method proposed by Salgueirino (Salgueirino-Maceira et al. 2006). Briefly, 12.44 mL of a maghemite suspension was added to the previously prepared solution containing 57.6 mL of H2O, 55 mL of EtOH and 9.7 mL of NH4OH (28 %). Finally, a solution containing 4 mL of TEOS in 60 mL of ethanol, was added to the maghemite solution. The condensation of silica shell onto magnetic nanoparticles was terminated after 4 h. In order to minimize particle aggregation, the synthesis was carried out under mechanical stirring in an ultrasonic bath. In order to remove unreacted compounds and impurities, the magnetic-core/silica-shell structures were cleaned by repeated cycles of centrifugation, and redispersion in distilled water, to obtain the final concentration 9.9 mg/mL.
2.4 Synthesis of γ-Fe2O3/SiO2/N
In order to modify their surface, the magnetic silica nanoparticles were treated with (3-aminopropyl) trimethoxysilane (APTMS) (Pham et al. 2002). Briefly, 60 mL of silica-coated maghemite nanoparticles solution was mechanically stirred in an ultrasound bath during 10 min. Afterwards, 0.03 mL of APTMS was added, and the resulting solution was stirred and sonicated for 3 h. After this time, the nanoparticles solution was cleaned three times by cycles of centrifugation, and redispersion in water. In the final cycle, ethanol was used as a suspending liquid.
2.5 Characterization of the obtained nanoparticles
In order to characterize surface of the obtained nanoparticles, several analytical techniques were employed. The nitrogen adsorption/desorption isotherms were measured at −196 °C using Nova 1200e Quantachrome Instruments analyzer. All samples were degassed at 120 °C for at least 2.5 h in a vacuum, prior to each measurement. The specific surface area (SBET) was evaluated in the 0.03–0.35 range of relative pressures. The average pore diameter (d) was calculated using the DFT method (Landers et al. 2013). The total pore volume (Vp) was calculated by converting the amount adsorbed at a relative pressure about 0.99 to the volume of liquid adsorbate. The powder X-ray diffraction (XRD) patterns were recorded using a XRPD diffractometer (Empyrean, PANalytical). The parameters chosen for the measurement were 2θ steps of 0.013°, 8 s of counting per step, and 2θ range from 5° to 90° at room temperature.
In order to measure the size of the obtained nanoparticles both, the microscopic observations and the diffraction laser technique (DL), were used. Transmission electron micrographs were obtained by transmission electron microscope (ZEISS Libra 120) at 80 keV electron beam energy.
Zeta potential were measured in ZetaSizer Nano ZS (Malvern Instruments, U.K.). All measurements were performed in diluted suspensions (at concentration 100 ppm) in two types of media: water and electrolyte (with the fixed ionic strength—0.001 M NaCl and 0.01 M NaCl) at different pH values. NaOH and HCl were employed to adjust the pH values of the suspensions. All measurements were performed at room temperature.
Depending on the particle size, which was measured before, three following equations were used in order to measure the zeta potential: Smoluchowski’s, Henry’s and Huckel’s. In apparatus (NanoZetaSizer) in which the measurements of zeta potential were carried out, there is a possibility of choice the proper equation, depending on particle radius (a) and Debye–Huckel coefficient (κ). In our studies, we used, as follows:
-
1.
Huckel’s equation (when \(\kappa a < 0.1\))
$$\mu_{\text{e}} = \frac{{2\varepsilon_{0} \varepsilon \xi }}{3\eta }$$ -
2.
Henry’s equation (when \(0.1 < \kappa a < 100\))
$$\mu_{\text{e}} = \frac{{2\varepsilon_{0} \varepsilon \xi }}{3\eta }f_{1} (\kappa a)$$ -
3.
Smoluchowski’s equation (when \(\kappa a > 100\))
$$\mu_{\text{e}} = \frac{{\varepsilon_{0} \varepsilon \xi }}{\eta }$$where ε—relative permittivity, ε0—relative permittivity in vacuum, η—viscosity of liquid, surrounding the particle; \(\kappa = \left( {\frac{{2000{\text{F}}^{2} \left( {\frac{1}{2}\sum {{\text{c}}_{\text{i}} {\text{z}}_{\text{i}}^{2} } } \right)}}{{\varepsilon \varepsilon_{0} {\text{RT}}}}} \right)^{{\frac{1}{2}}}\)
Sizes of particles were measured using the device Mastersizer 2000, produced by the Malvern Instruments, U.K. Monodispersity of the examined systems is confirmed by particles size measurements determined on Mastersizer. Particle sizing was determined based on the results obtained from the diffraction laser (DL) measurements.
3 Results and discussion
3.1 N2 adsorption/desorption measurements
The nitrogen adsorption/desorption isotherms of the iron oxides are shown in Fig. 2. Shape of isotherm of the synthesized iron(III) oxide exhibits type IV according to IUPAC (Sing et al. 1985), which characterized mesoporous materials. Moreover, the obtained surface parameters confirm such structure (Table 1). In order to compare the surface parameters of synthesized-maghemite, commercial iron(III) oxide was also determined by nitrogen adsorption/desorption measurements. Shape of this isotherm cannot be classified to any types of isotherm according to IUPAC. The commercial maghemite is characterized by less-developed porous structure (Table 1), when compared with the synthesized-one. The obtained results clearly show that the better material for further using is synthesized maghemite.
The nitrogen adsorption/desorption measurements were made only for synthesized and commercial iron oxides, because the obtained amounts of magnetic-core/silica-shell nanocomposites, as well as their amine-functionalized counterparts, were so small that it was impossible to carried out such experiments (even if the initial reactants were taken in several times more quantities). However, it can be supposed, that surface parameters after these two steps, are worse when compared with pure maghemite nanoparticles. It can be seen from TEM micrographs, that the surface of silica layer is smooth, without any apparent porosity. Thus, it can be conclude that the specific surface area of the obtained core/shell composites, decreased.
3.2 XRD analysis
The X-ray diffraction patterns of all nanomaterials are shown in the Fig. 3. In order to compare the crystallographic structure of the synthesized maghemite, the XRD patterns of commercial maghemite, were also investigated. All XRD reflexes are typical of the iron oxide spinel structure (Fe3O4 and γ-Fe2O3). The majority of reflexes match that of standard maghemite, although some of the exhibited reflexes correspond to both, maghemite and magnetite. This is due to the fact that maghemite was formed by oxidation of magnetite and that is why the crystallographic properties of both iron oxides are very similar. Thus, it is very difficult to distinguish between magnetite and magnetite/maghemite phases, because the X-ray powder diffraction patterns are not different enough in that respect. It can be seen that the presence of seven diffraction reflexes at 2θ = 30.20°, 35.45°, 43.32°, 53.81°, 57.22°, 62.98°, 74.54°, corresponds to: (220), (311), (400), (422), (511), (440), (533) (in both XRD patterns), respectively. Their presence indicates that the obtained results correspond to those of reference data for γ-Fe2O3 and Fe3O4 (Sui et al. 2013) (according to the JCPDS cards No. 00-025-1402 and 04-009-8435, respectively). Based on those results, the maghemite phase is probably the most abundant, even up to 90 % (Fig. 4).
The Fig. 3 also presents the XRD patterns of core/shell structure and functionalized core/shell structures. As before, the reflexes of maghemite are noticeable but their intensities are not as high as in the case of pure maghemite. In those two patterns, the broad diffraction peak at 2θ = 20–30° belonging to the amorphous phase of silica (Meng et al. 2015) (according to the JCPDS card No. 00-029-0085), can be observed.
3.3 TEM and size analyses
Microscopic observations and diffraction laser technique, were employed to determine the size of the obtained nanoparticles. Transmission electron microphotographs have been taken in order to obtain pictures of the synthesized samples. The TEM photos (Fig. 5) display the morphology of maghemite nanoparticles and magnetic silica structures. It can be seen, that the obtained magnetic nanoparticles and core/shell nanostructures, are almost spherical and monodispersed.
The size histograms for the synthesized materials obtained from diffraction laser are presented in the Fig. 6. The average size of particles obtained for γ-Fe2O3 using the DL method is 56 nm and is smaller compared to γ-Fe2O3/SiO2, where the average size of particles is 62, and γ-Fe2O3/SiO2/N where the average size of particles is 100 nm. The polydispersity index (PDI) is very important in the practical point of view and is used as a measure of the breadth of the particle size distribution. PDI can be explained as a number calculated from a simple two parameter fit to the correlation data called a cumulants analysis. The PDI is dimensionless and if its value is too big, sample cannot be measured by a proper apparatus or cannot be used in a proper measuring method. It is supposed that if value of PDI is lower than 0.25, the system is monodisperse. The polydispersity indexes are: 0.186 (γ-Fe2O3), 0.19 (γ-Fe2O3/SiO2) and 0.23 (γ-Fe2O3/SiO2/N), and this confirm that the examined systems are monodispersives, and it is well correlated to TEM microscopy results.
In order to isolate maghemite nanoparticles from the surroundings, as well as improve their biocompatibility, the silica coating procedure was applied. Although, the maghemite surface is characterized by the affinity for silica, the coating process can be difficult due to aggregation of maghemite nanoparticles. Thus, more than one maghemite nanoparticle constitute the magnetic core. This effect can be observed in the Fig. 5 (right).
3.4 Electrokinetic properties
From the practical point of view, there is a need to control stability of magnetic nanoparticles and core/shell nanostructures. This can be tested by means of electrophoresis, which may be considered a very useful tool in the investigations of the effectiveness of the surface modification. In the Fig. 7 zeta potential as a function of pH of the magnetic particles, and their nanocomposites, are shown. Zeta potential allowed to determine the values of isoelectric point (IEP) of the synthesized nanomaterials. It can be seen from the attached graphs, that IEP for pure maghemite is equal to 7.5, which is in agreement with the previous results (Kosmulski 2001). This confirms that ferrofluids are only stable under strong acidic and mild basic conditions. The presence of the outer silica shell dramatically changed this value to 3.5, which is also in agreement with the previous results (Rudzka et al. 2012) for pure silica, and pH > 9 for γ-Fe2O3/SiO2/N. Magnetic-core/silica-shell nanocomposites are stable in a broad range of pH which corresponds to those for typical biological fluids. Both, the silica coating and its functionalization with amine groups result in an increased chemical stability of these colloids. Such treatments allow to obtain compatible materials, especially when they are used for biomedical applications.
For the all studied samples: γ-Fe2O3, γ-Fe2O3/SiO2, γ-Fe2O3/SiO2/N the zeta potential is changing with the increasing pH. For the pure γ-Fe2O3 sample the zeta potential values are from +40 mV to −10 mV in the studied pH range 2–9. The values of γ-Fe2O3/SiO2 sample in the same pH range are from 5 mV to −55 mV, but for γ-Fe2O3/SiO2/N from 0 to 40 mV. As follows from the zeta potential values, modification of the surface has a significant effect on both, zeta potential. The differences in the zeta potential values can also result from the changes in the surface chemistry of the studied samples which undergoes modification as a result of the synthesis. All studied systems have the pH range in which they are colloidally stable (Prathna et al. 2011; Eastman 2005), and thus for γ-Fe2O3 pH 2-6 for water, γ-Fe2O3/SiO2 pH 4-8 for all studied electrolytes and γ-Fe2O3/SiO2/N for pH 3-9 for water and 0.001 M NaCl. The values of pH for the studied samples ensure their colloidal stability, and electrostatic repulsion forces increase, so aggregation and sedimentation rates are much lower. The zeta potential values at the γ-Fe2O3/NaCl interface are mainly affected by H+ ions from the solution and Na+ ions from the electrolyte. For the system γ-Fe2O3/SiO2 these are the Cl− groups from the electrolyte and OH− for the system γ-Fe2O3/SiO2/N mainly surface modifying organic groups. For such pH range values, where absolute zeta potential values are high, small average particle sizes are observed, which is in conformance with particles size determination Fig. 6. On the other hand, middle sized particles have great tendency to aggregation, which causes instability near the isoelectric point.
4 Conclusions
Amine functionalized magnetic-core/silica-shell nanocomposites have been synthesized and investigated using a broad range of analytical techniques. Maghemite nanoparticles were synthesized and coated with silica shell in order to improve their biocompatibility, and prevent aggregation. The obtained results of nitrogen adsorption/desorption measurements and X-ray diffraction indicate that synthesized maghemite is characterized by better developed porous structure with good purity of γ-Fe2O3, when compared to the commercial one. The obtained TEM micrographs show that the final materials have a core/shell structure. For the all tested materials, the values of zeta potential decrease with the increasing pH values. Zeta potential permitted to confirm the pH range for the isoelectric point (IEP): 7.5 for the γ-Fe2O3, 3.5 for the γ-Fe2O3/SiO2 and pH > 9 for the γ-Fe2O3/SiO2/N. For every of the examined systems, exists quite wide pH range where this systems are colloidally stable.
The existence of the silica layer changes the pH tendency in an important manner. PHIEP of the silica-coated maghemite nanoparticles is approximately 3.5, very distant from that of maghemite and actually closer to that of pure silica. The silica shell onto the maghemite nanoparticles causes an increase in their chemical stability, thus affecting their performance for bioapplications. It can be seen that the cationic polyelectrolyte APTMS may be employed to functionalize the magnetic silica nanoparticles, making them positive in a broad pH range. The presence of amine layer onto the magnetic silica surface stabilizes this colloidal nanocomposite. Ionic strength affects significantly on both, the zeta potential for pristine and amine-functionalized core/shell nanocomposites.
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Acknowledgments
The research leading to these results has received funding from two grants: People Programme (Marie Curie Actions) of the European Union’s Seventh Framework Programme FP7/2007-2013/under REA Grant Agreement n° PIRSES-GA-2013-612484 and designated subsidy of the Ministry of Science and Higher Education for scientific research or development work and related tasks, contributing to the development of young scientists and Ph.D. students, at the Faculty of Chemistry, UMCS.
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Gdula, K., Dąbrowski, A. & Skwarek, E. Synthesis, surface characterization and electrokinetic properties of colloidal silica nanoparticles with magnetic core. Adsorption 22, 681–688 (2016). https://doi.org/10.1007/s10450-015-9755-8
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DOI: https://doi.org/10.1007/s10450-015-9755-8