Magnetophoresis Behaviour

7
Contribution to the Study of Ferrite Nanobeads: Synthesis, Characterization and Investigation of Horizontal Low Gradient Magnetophoresis Behaviour Maria Benelmekki a, *, Cristina Caparros a , Anna Montras b , Renao Gonçalves a , Senenxu Lanceros-Mendez a and Lluis Miquel Martinez c a Centro de Fisica, Universidade do Minho, Braga, Portugal b Sepmag Tecnologies, Parc Tecnologic del Valles, Cerdanyola del Valles (Barcelona) Spain c Sepmag Technologies, 191 Peachtree St. NE, 03030 Atlanta. GA, USA. * E-mail: [email protected] Abstract. In this work we investigate the possibilities of the use of Horizontal Low Gradient Magnetic Field (HLGMF) (<100 T/m) for filtration, control and separation of the synthesized magnetic particles, considering, the characteristics of the suspension, the size and the type of nanoparticles (NPs) and focusing on the process scale up. Reversible aggregation is considered in the different steps of magnetic nanobeads synthesis. For these purpose, we synthesized Fe 2 O 3 -silica core- shell nanobeads by co-precipitation, monodispersion and silica coating. SQUID, TEM, XRD, and Zeta potential techniques were used to characterize the synthesized nanobeads. An extensive magnetophoresis study was performed at different magnetophoretic conditions. Different reversible aggregation times were observed at different HLGMF, at each step of the synthesis route: Several orders of magnitude differences where observed when comparing citric acid (CA) suspension with silicon coated beads. Reversible aggregation times are correlated with the properties of the NPs at different steps of synthesis. Keywords: Magnetic nanoparticles, Citric Acid, magnetophoretical properties. PACS: 75.47.Lx; 75.50.Tt; 81.07.-b INTRODUCTION In recent years, substantial progress has been made in developing technologies in the field of magnetic microspheres, magnetic nanospheres and ferrofluids. Nanospheres and microspheres containing magnetic particles core inserted in a nonmagnetic matrix, are used in numerous biological applications [1]. They are used as carriers which can be targeted to a particular site by using an external magnetic field. Magnetic separation of organic compounds, proteins, nucleic acids and other biomolecules and cells, from complex reaction mixtures is becoming the most suitable solution for large production in bioindustrial purification and extraction processes. The current commercial NPs for In-Vitro application are coated with Polystyrene, copolymers, or silica [2,3,4]. Due to the low surface/volume ratio of the microspheres, and the unclear magnetic behaviour of the particles, commercial magnetic micro and nano beads have low efficiency for large volume production and potential industrial application. These limitations hinder their use as efficient and low cost carriers for bioindustrial purification and extraction processes [2,5]. In order to be effective for large scale magnetic separation processes, low cost and efficient commercial beads are necessary. The efficiency of magnetic beads may be improved by maximizing their surface/volume ratio and by a better understanding of the behaviour of the magnetic particle core, allowing better control of the separation process. In this work, the essential steps involved in the life cycle of magnetic particles, from the synthesis process to their subsequent recovery and removal using external magnetic fields (magnetophoresis) have been comprehensively studied. The aim of this study is to increase our knowledge and improve our understanding of the effect of different parameters on the behaviour of magnetic beads during their use in potential applications. 121

description

v

Transcript of Magnetophoresis Behaviour

  • Contribution to the Study of Ferrite Nanobeads: Synthesis, Characterization and Investigation of Horizontal Low

    Gradient Magnetophoresis Behaviour

    Maria Benelmekki a,*, Cristina Caparros a, Anna Montras b, Renao Gonalves a, Senenxu Lanceros-Mendez a and Lluis Miquel Martinez c

    a Centro de Fisica, Universidade do Minho, Braga, Portugal b Sepmag Tecnologies, Parc Tecnologic del Valles, Cerdanyola del Valles (Barcelona) Spain

    c Sepmag Technologies, 191 Peachtree St. NE, 03030 Atlanta. GA, USA. *E-mail: [email protected]

    Abstract. In this work we investigate the possibilities of the use of Horizontal Low Gradient Magnetic Field (HLGMF) (

  • MATERIAL AND METHODS

    Synthesis of Ferrite Nanobeads

    Nanobeads were prepared by co-precipitation of Fe3O4 from an aqueous mixture of FeSO4 and FeCl3. NH4OH was used as a precipitation agent. For these purpose, FeSO47H2O (0.5 mM) and FeCl36H2O (1 mM) were mixed and heated to 80 C. In order to precipitated the iron hydroxides, the pH value was raised and maintained to pH=3 for 30 min. The solution was rigorously stirred at a constant temperature during all the process. Then, the pH value was increased to 10.5 - 11.

    Citric acid (CA) was used to stabilize the magnetic nanoparticles, according to the method proposed by Campelj et al. [6]. Approximately 2 g of nanoparticles were mixed with 65 mL of an aqueous solution of 2% CA. The pH value of the mixture was adjusted to pH = 5 and, then, was raised to pH = 10 using concentrated ammonia. The adsorption step of the CA was maintained at 80 C and rigorously stirred for 60 min. The prepared suspension was washed with distilled water and magnetically separated several times to remove the excess of CA. Finally the NPs were dried in order to proceed to the following step.

    The CA-modified NPs were coated with silica, using tetraethyl orthosilicate (TEOS). 10 mL of NPs were mixed in a 20 mL ethanol solution (35% v/v) containing 3% (v/v) TEOS. The pH value of the solution was maintained at 11 for 90 min.

    Characterization Methods

    A LEO 906E electron microscope operating at 100 keV, was used for transmission electron microscopy. The samples were prepared by deposition of a droplet of particle solution on a copper grid coated with carbon and allowed to dry. Dynamic light scattering (DLS) and potential were performed with a Zetasizer Nano ZS (Malvern instruments), provided by a He/Ne laser of 633 nm wavelength. The Fe2O3- water dried sample was characterized by X-ray diffraction with a Bruker D8 Discover diffractometer using Cu K incident radiation. Hysteresis loop of the Fe2O3 aqueous solution at room temperature curves were measured with a superconducting quantum interference device (SQUID) magnetometer (Quantum Design MPMS5XL). The experimental results were corrected for the holder contribution.

    Magnetophoresis Experiments

    The magnetophoresis setups employed in our experiment are the SEPMAG LAB 1x25 ml 2042 and 2042 Plus systems, commercially available from SEPMAG company [7]. The system consists of a cylindrical cavity containing a high permanent magnetic field with a uniform horizontal gradient pointing toward the walls of the cylindrical vessel. All magnetic NPs are working at saturation regime. The magnetophoresis experiment is performed at Low Gradient Magnetic Field (LGMF) (

  • measurements of Fe2O3-silica core-shell sample are shown in FIGURE 2. The sample is saturated at 4 kOe with a saturation magnetization value Ms of 44 emu/g.

    FIGURE 1. Typical TEM images of clusters of Fe2O3-silica core-shell

    Magnetophoresis Behaviour

    FIGURE 3 (Left) shows magnetophoresis curves of the obtained nanobeads at different gradients, 60 T/m, 30 T/m, and 15 T/m. The total time separation depends on the magnetic force applied inside the SEPMAG system. For 15 T/m gradient, the aggregation time takes about 100s. This time decreases one order of magnitude (~10 s) when 60 T/m gradient is applied. No relevant differences between the aggregation times corresponding to 60 T/m and 30 T/m applied magnetic gradients are observed. As explained previously, magnetophoresis separation is induced by reversible aggregation of NPs [8], this reversible aggregation depends mainly on the total interaction potential between the particles: van der Waals interaction, stabilizing electrostatic energy and magnetic interaction [9].

    FIGURE 2. Magnetization curve of magnetic silica nanoclusters at room temperature

    123

  • By applying 60 T/m, at pH 10.5, the aggregation time increases from less than 1 s for non-modified NPs to 300 s for CA-modified NPs (FIGURE 3 (right)). The potential of the non-modified NPs, and the CA-modified NPs is -20 mV and -43 mV, respectively. This result suggests the important influence of the electrostatic stabilization in the magnetophoresis process. High electrostatic stabilization guarantees a very stable suspension, but induces a large separation time.

    In the case of nanobeads, the aggregation time takes 10s and the potential is -30 mV. The theoretical limit of stability in a colloidal system is |30| mV. Colloidal systems show good stability if its potential is higher than 30 mV or lower than -30 mV [10]. This result indicates that the synthesized nanobeads in the present work are at the limit of stability in colloidal systems, and will be subject to improvement in future works.

    FIGURE 3. Magnetophoresis curves. Obtained nanobeads at different gradients (Left). Reversible aggregation times on NPs

    at each step of the synthesis route (Right).

    Effect of pH on the Reversible Aggregation Process

    As shown in FIGURE 4, CA has three dissociable protons, associated with its three carboxylate groups. It has been claimed that CA act as an adsorbate tribasic acid on metal oxides (adsorbent) [11].

    FIGURE 4. Schematic representation for the synthesis of NPs, using CA to produce aqueous stable suspension

    The deprotonation of CA depends on the pH of the suspension. At pH5.5, CA appears mainly with two deprotonated species (AH2-), and then is adsorbed onto the NPs surface positively charged [6]. At pH ~ 10, CA appears at their fully deprotonated state (A3-). As reported by Hajdu and co-workers [12], the CA may be adsorbed

    124

  • on the surface of the NPs by coordinating via one or two of the carboxylate functionalities depending on the steric necessity and the curvature of the surface. When the CA affinity limit is reached, the CA adsorption increases further and a rearrangement of CA binding towards a tighter packed surface structure can occur. Only one carboxylate group of CA will be bound to the NPs surface. In these conditions, there will be at least one carboxylic acid group exposed to the solvent that should be responsible for the surface charge. Furthermore, the presence of a terminal carboxylic group provides a possible way of extending the bond formation [13]. This chemisorption process provides the electrostatic stability of the suspension.

    Different samples of CA-modified NPs, with different pH in the range 2-10 were prepared separately. Samples with pH

  • FIGURE 6. Magnetophoresis behaviour at 60 T/m of CA-modified NPs at different pH's.

    CONCLUSION

    This paper reports on the effects of the stabilizing electrostatic energy on magnetophoresis process at HLGMF (

  • Copyright of AIP Conference Proceedings is the property of American Institute of Physics and its content maynot be copied or emailed to multiple sites or posted to a listserv without the copyright holder's express writtenpermission. However, users may print, download, or email articles for individual use.

    copyright1: