COLLOIDAL – CHEMICAL LAWS OF INTERACTION OF MAGNETIC FLUID PAR-TICLES WITH SURFACES OF NATURAL FIBERS

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COLLOIDAL – CHEMICAL  LAWS  OF  INTERACTION

OF  MAGNETIC  FLUID  PARTICLES

WITH  SURFACES  OF  NATURAL  FIBERS

 

Lunina M. A. 1, Bayburtskiy F. S. 1, 2, Senatskaya I. I. 1,  Brusentsov N. A. 3, Razumovskiy V. A. 3

 

1.      D. I. Mendeleev University of chemical technology of Russia, Russian Federation, Moscow, 125047, Miusskaya place, 9. E – mail: Bayburt@mail.ru

2.      N. M. Emanuel Institute of biochemical physic RAS, Russian         Federation, Moscow, 119991, Kosygina street, 4. E – mail: Chembio@sky.chph.ras.ru

3.      N. N. Blokhin Oncological Research Center RAMS, Russian Federation, Moscow, 115478, Kashyrskoye shosse, 24. E – mail: Gala752@mail.ru

 

Introduction.

 

The interaction of magnetic fluids (MF) with an extraneous phase (including particles, fiber and tissue) can break the aggregation stability of a magnetic phase and cause sedimentation. Coagulation of magnetic fluid particles on a surface of an extraneous phase occurs spontaneously, that is at the expense of power resources of the system. The contact of natural fibers and tissues with magnetic fluids allows the coating of their surface with magnetic layers and gives them magnetic properties. Our investigations [1 – 3] are devoted to study this phenomenon. The preparation of metal particle films and strings from polymeric materials is possible by introducing particles of these metals in a polymeric phase during the stage of fiber formation. This method cannot be applied to fibers of natural origin, as the thermal or chemical influence on them will result in their irreversible destruction. The modification of a surface by coagulation [4, 5] allows creating biologically compatible magnetic strings and filters based on these strings.

 

Materials and methods.

 

MF were prepared by the peptization method, using various types of stabilization. MF1 contained spherical magnetite particles (Fe3O4) stabilized in aqueous medium by the anionic surfactant sodium oleate (70 g / l). MF2 contained spherical g-Fe2O3 particles stabilized in aqueous medium by the polymer dextran (200 g / l). The MF choice is based on the fact that MF1 is widely used in laboratory and industrial investigations, and that MF2 of interest in biology and medicine (Table 2). The chosen natural fibers and their properties are given in Table 2.

The basic physic and chemical parameters of the colloidal systems were analyzed as follows. The density of magnetic fluids and natural fibers was determined with a picnometer. The concentration of particles was determined gravimetrically. The size and specific surface of the magnetic particles were examined by means of line ultramicroscopic and photon-correlation spectrometer (Malvern model 4300, England). The specific surface of natural fibers was determined by adsorption of nitrogen by the BET method. The viscosity of magnetic colloids was determined with a scanning rotational rheometer Low-Shear 30. The magnetic properties were investigated with a ferrograph 1.033 (FRG). The sedimentation stability of prepared magnetic colloids was investigated in a centrifuge at 6000 rpm for 1h. The electrostatic surface properties of magnetic fluids and natural fibers were investigated by electrophoresis and electroosmosis, using a background electrolyte of 0.013 M KCl solution and correcting the pH with 0.027 M HCl and 0.0178 M KOH. The investigation of MF particle coagulation on the surface of natural fibers was carried out optically with a photocolorimeter KFK-2 after direct contact of the magnetic fluids (1.0 kg / m 3) with fibers.      

The aggregation stability of MF with positively and negatively charged particles at a pH between 6 to 8 and with or without electrolytes was investigated. The binding kinetics was investigated with or without electrolytes, using different amounts of fibers with modified or unmodified surfaces. For the surface modifiers for the fibers were anionic surfactants (sodium salt of dodecylbenzensulhonate (sulfonol), sodium salt of carboxymethylcellulose (Na-CMC)) and cationic surfactants (dodecylammonium chloride (DACl), dodecyl-dimethyl-benzen-ammonium chloride (cathamine)).

 

Results and discussion.

 

The MF – fiber interaction take place within 5 days (Figure 1 and 2) and can be explained by good particle stabilization by the surfactants and polymers. The coagulation of highly dispersed magnetic particles on a firm surface is shown in two processes: direct interaction of MF particles with points on a surface and interaction of MF particles with particles and their aggregates fixed on a surface. These processes proceed simultaneously, but at various speeds. The degree of fiber coating can be predetermined by regulating the two involved processes. The MF cooperates with all macrophases, but to different extents. The initial ratio of cooperating phase surfaces determined in parameter q is very important:

 

Q = S1S . m1 / S2S . m2                         ( 1 )

 

where S1S , S2S are the values of specific surfaces of magnetic particles and fibers (m 2 / kg), m1, m2 are the masses of the magnetic phase and fibers (kg).

The coagulation kinetics depends on the mass of the entered fiber at constant concentrations of MF (Figure 1).

 

    

 

 

Figure 1. Kinetics of particles MF1 coagulation

on a fiber (wool) at various q:

m─ without added electrolyte

─ with added electrolyte

MF1 with electrolyte in contact to a fiber

u─ q = 0.02; ─▲─ q = 0.10; ─n─ q = 0.20.

Figure 2. Kinetics of particles MF1 coagulation on a fiber (wool) at q = 0.10:

m─ without added electrolyte

─ with added electrolyte

n─ MF1 with electrolyte in contact to a fiber

s─ in contact with a fiber modified by DACl

u   in contact with a fiber modified

           by cathamine

 

The surface condition of the fiber is also very important (Figure 2). The process proceeds most effectively when cationic surfactants (DACl and cathamine) are present.

It proves to true by dependence’s of quantity fixed on fibers magnetic coagulum from equilibrium concentration of a magnetic phase in solutions MF, achieved to time of the termination of process (Figures 3 and 4). They look like curves leaving on a plateau, with the further rise upwards, that testifies to formation on a surface of fibers mono-and polylayers of magnetic particles structures.

We received similar results using catgut (data not shown).

The presented results will allow choosing the conditions to fine-tune a fiber coating with mono- or multi-layers of magnetic particles.

 

  

 

Figure 1. Amount of magnetic coagulum A from MF1 fixed on a fiber (wool) at different equilibrium concentrations Cp.

l─ pure fiber;   fiber modified with:

─ DACl;     ─ cathamine.

Figure 1. Amount of magnetic coagulum A from MF1 fixed on a fiber (wool) at different equilibrium concentrations Cp.

l─ pure fiber;   fiber modified with:

─▲─ sulfonol;     u─ Na – CMC.

 

The aggregation stability of a magnetic fluid is disturbed near a fiber. The level of this process is determined by experimental conditions such as pH. Driving forces of interaction between MF particles and a fiber are the differences of superficial forces at the borders between «particle of a magnetic phase» and «surface of a fiber – medium». The electrostatic surface properties of magnetic fluid particles and fibers depend  on the pH, as shown with zeta-potential measurements (Figures 5 and 6).

 

 

 

Figure 5. Change of zeta-potential of a natural fiber (wool) with pH.

Figure 6. Zeta-potential of a MF at different pH.

n─ MF1;   l─ MF2.

 

In the investigated range of pH 6 – 8, particles MF1 are charged negatively and MF2 are charged positively, whereas the fibers are charged negatively. To achieve higher coagulation rates for particles MF1 on fibers, it was thus necessary to reduce the negative charge. This  was achieved by preliminary modification of their surface with DACl or cathamine. Similarly, an increase of positive charge on the MF2 particles by treatment with sulfonol or Na-CMC led to increased coagulation on the fibers.

The difference between the zeta-potential of fibers and MF particles was thus increased during neutralization, as seen by the process of coagulation.

 

       

 

Figure 7. Dependence of magnetic properties of a fiber BS (wool) on the amount of magnetic coagulum A after contact with MF1.

Figure 8. Dependence of magnetic properties of a fiber BS (wool) on the amount of magnetic coagulum A after contact with MF2.

 

The magnetic properties of the fibers changed considerably depending on the way of treating the surfaces with surfactants (Figures 7 and 8). Cationic surfactant pretreated fibers (DACl or cathamine) show increased adsorption of MF1 particles stabilized with sodium oleat (Figure 7). A similar effect is seen between fibers and dextran-stabilized MF2 particles (Figure 8).

We observed a sharp increase of the magnetic fiber properties after modifying them with the anionic surfactants sulfonol and Na-CMC. The difference between the electrostatic surface forces in the system «magnetic fluid – fiber» is the basis of process coagulation. A future direction is the investigation of influence of temperature and stirring on coagulation kinetics. Our work is the basis for the coating of fiber surfaces with magnetic particles.

 

Conclusion.

 

The coagulation process depend on the fiber quantity and its surface properties. Modification of the fiber surfaces with surfactants changes their electrostatic properties, which is a precondition for the effective formation of layers of magnetic particles. The magnetic fiber coating initially us modest, but increases considerably after preliminary treatment with surfactants.

 

References.

 

1.    Lunina M. A., Bayburtskiy F. S., Nikitin L. V., Mironova L. S. // The international Conference on Colloidal Chemistry and Physical-Chemical Mechanics, Russia, Moscow, Book of Abstracts, P. 353.

2.    Brusentsov N. A., Bayburtskiy F. S., Yurchenko N. Yu., Osipov N. E. // J. Magn. Magn. Mater., 194 (1999), 83 – 89.

3.    Brusentsov N. A., Bayburtskiy F. S. // Pharm. Chem. J., 33 (1999), 57 – 61.

4.    Lunina M. A., Bayburtskiy F. S., Senatskaya I. I., Kiselyov M. R. // The 9th International Plyos Conference on Magnetic Fluids, Russia, Plyos, Book of Abstracts, P. 7 – 11.

5.    Bayburtskiy F. S., Senatskaya I. I., Brusentsov N. A., Razumovskiy V. A. // The 9th International Plyos Conference on Magnetic Fluids, Bremen, Germany, Book of Abstracts.