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International Journal of Modern Engineering Research (IJMER)
         www.ijmer.com                 Vol.2, Issue.4, July-Aug 2012 pp-1757-1760        ISSN: 2249-6645

           Synthesis, Characterization Ac Conductivity of Ni2+ Doped In
                               Magnesium Ferrite

                    Pathan Amjadkhan Noorkhan1 and Sangshetty Kalayne2*
                     1
                      Department of Physics, Singhania University, Pacheri- Bari, JhunJunnu, Rajasthan
                    2*
                      Department of Physics, Rural Engineering College, Bhalki, Bidar, Karnataka, India.


Abstract: Magnesium nickel ferrites were synthesized by          In the present study authors, report synthesis,
employing sol gel technique at 1473 K sintering                  characterization and dielectric studies of MgNiFe2O4. A
temperature. A critical Rietveld analysis of XRD reveals         critical Rietveld analysis of XRD reveals that the presence
that the presence of a very small amount of NiO phase            of a very small amount of NiO phase along with the ferrite
along with the ferrite phase. It indicates that almost a         phase. It indicates that almost a stoichiometric (Mg,Ni)-
stoichiometric (Mg,Ni)-ferrite phase has been obtained at        ferrite phase has been obtained at 1473 K. SEM image
1473 K. SEM image shows that of (MgNi) ferrite is                shows that of (MgNi) ferrite is regular in shape have
regular in shape have granular in structure, compact and         granular in structure, compact and well connected grain to
well connected grain to each others. The ac conductivity         each others. The ac conductivity increases with increase in
increases with increase in applied frequency. The                applied frequency and dielectric constant decreases.
magnesium nickel ferrite (MnNiFe2O4) shows σac                   Therefore, this ferrites material is attracted to use in many
conductivity of 1.2 x 10-4 S/cm. This is may be attributed       science and technological applications.
to the dipole polarization i.e., the rotation of dipoles
between two equivalent equilibrium positions is involved.                      II.       Experimental
The high value of dielectric constant of the sample                       All Chemicals used were analytical grade (AR).
MnNiFe2O4 may be the structural changes associated with          The magnesium chloride, nickel chloride (purity 99.99%)
the magnesium nickel ferrite when the grain size is              and dehydrated ferric chloride were procured and were
reduced. Therefore, this ferrites material is attracted to use   used as received.
in many science and technological applications.
                                                                 1.1synthesis Of Magnesium Nickel Ferrite
Keywords: Ac conductivity, (MgNi) ferrite, dielectric                      The chloride salts of magnesium, nickel chloride
constant, Impedance spectra, X-ray diffraction.                  and ferric chloride are mixed in calculated stoichiometric
                                                                 with oxalic acid in equimolar ratio so as to form nickel
            I.           INTRODUCTION                            ferric oxalate precursor. The precursor is then filtered and
          Small ferrimagnetic oxides, technically known          dried at 323K to achieve constant weight. The precursor is
as ferrites have attracted considerable attention not only       mixed with polyethylene glycol (PEG) in the ratio 1:5 and
from a fundamental scientific interest but also from a           is ignited. The combustion propagates throughout the
practical point of view for growing applications in the          precursor. After completion of combustion nickel ferrite
magnetic, electronic and microwave fields [1-3].                 (MgNiFe2O4) is formed. The MgNi-ferrite is sonicated in
Simultaneous presence of magnetic and dielectric nature          acetone media for 20min and then calcinated at 1473 K to
of ferrites is vastly exploited in a variety of applications     remove the impurities. Finally, fine graded nanosized
at different frequencies. The special feature of these           nickel ferrite particles are formed [9, 10].
materials is that the properties can be tailored over wide       The pellets of 10 mm diameter are prepared with thickness
ranges by appropriate substitution of various ions in the        varying up to 2 mm by applying pressure of 10 Tons in a
chemical formula unit and control of processing                  UTM – 40 ( 40 Ton Universal testing machine). For
procedures. Ferrites are extensively used in magnetic            temperature dependent conductivity and sensor studies, the
recording, information storage, colour imaging, bio-             pellets are coated with silver paste on either side of the
processing, magnetic refrigeration and in magneto                surfaces to obtain better contacts.
optical devices [4, 5].
          Ferrites also have great promise for atomic            1.2 CHARACTERIZATION
engineering of materials with functional magnetic                         The X-ray diffraction (XRD) pattern of the
properties. The formation of corrosion product on the out        MgNiFe2O4 was recorded at room temperature by
of core surfaces in pressurized heavy water reactors             employing an x-ray powder diffractometer (Rigaku
(PHWRs) are major problem. Ferrite having spinal                 Miniflex) with CuK radiation (         =1.5405A0) in the
structure such as magnetic and nickel etc play a major role      2 (Bragg angles) range (2 ≤ 2 ≤100) at a scan speed
                                                                                               0

to prevent such problem. Thus attempts are being made to         of 0.50 minute-1.
study the various ferrites to evaluate the impact of                      The percentage transmittances for the entire
substitution of the divalent metal ions to modify the            sample are measured from 300 to        4000 cm−1. The SEM
properties of these oxides [6-8].                                images of MgNiFe2O4 were recorded using Philips XL-30
                                                                 (ESEM) scanning electron microscopy. The set up used
                                                                 for measuring ac conductivity is Hioki 3050 impedance
                                                                 analyzer, which is in turn interfaced to the computer.
                                                       www.ijmer.com                                          1757 | P a g e
International Journal of Modern Engineering Research (IJMER)
         www.ijmer.com                 Vol.2, Issue.4, July-Aug 2012 pp-1757-1760        ISSN: 2249-6645
                                                                average grain size was calculated by using line intercept
  III.          RESULTS AND DISCUSSION                          formula and it is found to be 0.21µm.
                                                                Figure 2 (c) shows that SEM image of (MgNi) ferrite. It is
2.1 X-RAYS DIFFRACTION                                          found that the image is regular in shape have granular in
                                                                structure, compact and well connected grain to each
                                                                others. The average grain size was calculated by using line
                                                                intercept formula and it is found to be 0.7µm.

                                                                2.3 AC CONDUCTIVITY
                                                                         The variation of σac of MnNiFe2O4 as a function
                                                                of frequency as shown in figure 3. The conductivity of
                                                                nickel ferrites is increases with increase in frequency. The
                                                                magnesium nickel ferrite (MnNiFe2O4) shows σac
                                                                conductivity of 1.2 x 10-4 S/cm.

                                                                                      -4    MnNiFe2O4
                                                                                 1.2x10
    Figure 1 shows the XRD patterns of Mg,Ni)-ferrite
                                                                                      -4
             annealed at temperature 1473 K.                                     1.0x10

                                                                                      -5
          It seems that the (Mg,Ni)-ferrite phase is formed                      8.0x10




                                                                      ac S/cm
completely after this heat-treatment. However, a critical                             -5
                                                                                 6.0x10
rietveld analysis reveals the presence of a very small
amount of NiO phase along with the ferrite phase. It                                  -5
                                                                                 4.0x10
indicates that almost a stoichiometric (Mg,Ni)-ferrite                                -5
phase has been obtained at 1473 K. This indicates that the                       2.0x10
amount of ferrite phase formation is dependent of                                    0.0
annealing time. By measuring particle size we actually
measure the coherently diffracting zone of a grain. The                                     2
                                                                                           10       10
                                                                                                        3
                                                                                                                 10
                                                                                                                   4
                                                                                                                         10
                                                                                                                             5
                                                                                                                                   10
                                                                                                                                     6


particle or crystallites re separated from each other by                                                    Frequency (Hz)
grain boundaries and the grain boundaries are nothing but
bulk crystal imperfections in a crystal [11]. The size of the     Figure 3 shows the variation of σac of MnNiFe2O4 as a
crystallite in the nanometer range. As can be seen from the                      function of frequency.
experiment, annealing the sample increases the size of the
particles. Heat energy helps to annihilate the deformations               This is may be attributed to the dipole
in the crystals. As a result of grain boundaries started to     polarization i.e., the rotation of dipoles between two
vanish during annealing and the small crystallites              equivalent equilibrium positions is involved. It is the
agglomerate together to form larger particles due to intra-     spontaneous alignment of dipoles in one of the equilibrium
grain diffusion.                                                positions that give rise to the nonlinear polarization
                                                                behavior of this composition.
2.2 SCANNING ELECTRON                MICROSCOPY                           This behaviour of MnNiFe2O4 obeys the universal
                                                                power law,    (ω)=  n (the solid line is the fit
                                                                                               (ω)
                                                                to the expression), where r0 is the dc conductivity
                                                                (frequency independent plateau in the low frequency
                                                                region), A is the pre-exponential factor, and n is the
                                                                fractional exponent between 0 and 1 [12]. On
                                                                crystallization, the conductivity spectrum remains similar
                                                                as that of the nickel ferrite except dispersion in the low
                                                                frequency region, where the deviation from  (plateau
                                                                                                                 dc
                                                                region) is more prominent. The deviation from            dc
                                                                (plateau region) value in the conductivity spectrum (in the
                                                                low frequency region) is due to the electrode polarization
                                                                effect. The values of  , A, and n were obtained by fitting
                                                                                        
                                                                the  to 
                                                                      (ω)       (ω)=  n. The overall behavior
                                                                                                (ω)
                                                                of  follows the universal dynamic response, which has
                                                                     ac
                                                                widely been observed in disordered materials like ionically
                                                                conducting glasses and also doped crystalline solids, and is
Figure 2 shows the SEM image of (a) NiO and (b) MgNi-           generally believed to be reflected in the mechanism of
ferrite at 1473 K.                                              charge transport behavior of charge carriers.

         Figure 2 (a) shows that SEM image of nickel
oxide. It is clearly observed from the image they are
agglomerated, highly branched and porous in nature. The

                                                      www.ijmer.com                                                              1758 | P a g e
International Journal of Modern Engineering Research (IJMER)
         www.ijmer.com                     Vol.2, Issue.4, July-Aug 2012 pp-1757-1760        ISSN: 2249-6645
                                                                           degree of covalency for the A site ions is higher than that
               2500
                                                     MnNiFe2O4             of the B site ions. All the above factors result in a high
                                                                           activation energy for the A sites compared to the B sites.
               2000
                                                                           Hence, in ordinary magnesium nickel ferrite with an
               1500
                                                                           inverse spinel structure the electron movement in B sites
                                                                           dominates compared to that in A sites.
          '




               1000
                                                                                              6
                                                                                         2.5x10
                                                                                                                                 MnNiFe2O4
               500
                                                                                              6
                                                                                         2.0x10

                 0
                       2    3         4          5      6                                     6
                      10   10       10      10       10                                  1.5x10
                                Frequency (Hz)




                                                                                       Z'
                                                                                              6
                                                                                         1.0x10
   Figure 4 shows the variation real permittivity ( of
                                                    ')
         nickel ferrite as a function of frequency.                                           5
                                                                                         5.0x10


                                                                                            0.0
         Figure 4 shows the variation real permittivity (')
of nickel ferrite of various composition as a function of                                          2
                                                                                                  10
                                                                                                        3
                                                                                                       10       10
                                                                                                                  4
                                                                                                                        10
                                                                                                                             5
                                                                                                                                 10
                                                                                                                                    6

logarithmic frequency. It is found that in all these nickel                                                 Frequency (Hz)
ferrite compositions, as frequency increases, dielectric
constant decreases up to the frequency range of 10 5 Hz and                      Figure 6 the variation of real part of impedance as a
after that it remains constant for further increasing in                                        function of frequency
frequency [13]. The strong frequency dispersion of
permittivity is observed in the low frequency region                                 The variation of real part of impedance of
followed by a nearly frequency independent behaviour                       MnNiFe2O4 is shown in figure 6 as a function of
above 103 Hz. It is observed that Debye type relaxation                    increasing frequency. It is observed that the real part of
mechanism is responsible for higher value of MnNiFe2O4.                    impedance decreases with increase in frequency. The
                                                                           initial decrease in impedance value due to the increase in
                                                                           conductivity at lower frequency region up to 103 Hz and
                                                                           further increases in applied frequency, the impedance
                                                                           value remains constant. This indicates that after 103 Hz the
                                                                           ferrite acts as lossless materials. Therefore, these ferrites
                                                                           can be used in many technological applications such as
                                                                           memory device, microwave, sensor, transducer, solar cell
                                                                           etc.

                                                                                        IV.           CONCLUSION
                                                                                    Sol-gel technique was employed to prepare the
  Figure 5 shows the variation of dielectric constant as a                 magnesium nickel ferrites were at 1473 K sintering
           function of frequency of MnNiFe2O4                              temperature. A critical Rietveld analysis of XRD reveals
                                                                           that the presence of a very small amount of NiO phase
         Figure 5 shows the variation of dielectric constant               along with the ferrite phase. It indicates that almost a
as a function of frequency for MnNiFe2O4. The high value                   stoichiometric (Mg,Ni)-ferrite phase has been obtained at
of dielectric constant of the sample MnNiFe2O4 may be                      1473 K. SEM image shows that of (MgNi) ferrite is
explained on the basis of the structural changes associated                regular in shape have granular in structure, compact and
with the magnesium nickel ferrite when the grain size is                   well connected grain to each others. The ac conductivity
reduced. Magnesium nickel ferrite crystallizes into a cubic                increases with increase in applied frequency. The
close-packed arrangement of oxygen ions. It belongs to the                 magnesium nickel ferrite (MnNiFe2O4) shows σac
class of ferrites with an inverse spinel structure having                  conductivity of 1.2 x 10-4 S/cm. This is may be attributed
structural formula, Fe3+[Mg2+Ni3+]O4. The metal ions                       to the dipole polarization i.e., the rotation of dipoles
given in the square bracket are called octahedral (B site)                 between two equivalent equilibrium positions is involved.
ions and that outside the square bracket are called                        The high value of dielectric constant of the sample
tetrahedral (A site) ions. The nickel ions (Ni2+) together                 MnNiFe2O4 may be the structural changes associated with
with half of the iron ions (Fe3+) occupy the B site and the                the magnesium nickel ferrite when the grain size is
Mg2+ occupy the remaining half of the iron ions reside in                  reduced. It is observed that the real part of impedance
A site. The presence of Mg2+ and Ni3+ ions gives rise to p-                decreases with increase in frequency. The initial decrease
type carriers (holes) whereas Fe2+ and Fe3+ ions produce n-                in impedance value due to the increase in conductivity at
type carriers (electrons). Therefore, both electrons and                   lower frequency region up to 103 Hz and further increases
holes that are present in the B sites are due to the presence              in applied frequency, the impedance value remains
of Mg and Ni ions. Since Mg ions are present in A sites,                   constant. Therefore, this ferrites material is attracted to use
electrons are the carriers in A sites. The distance between                in many science and technological applications.
the ions in A sites (0⋅357 nm) is larger than the distance
between the ions in B site (0⋅292 nm) [14-16]. Also, the
                                                                 www.ijmer.com                                                     1759 | P a g e
International Journal of Modern Engineering Research (IJMER)
        www.ijmer.com                   Vol.2, Issue.4, July-Aug 2012 pp-1757-1760        ISSN: 2249-6645
                      REFERENCE
[1]   I. Anton, I. D. Dabata and L. Vekas, “Application
      Orientated Researches on Magnetic         Fluids,” Journal
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[2]   R. D. McMickael, R. D. Shull, L. J. Swartzendruber, L.        [10]   P. Druska, U. Steinike and V. Sepelak,           “Surface
      H. Bennett and R. E. Watson,       “Magnetocaloric Effect            Structure of Mechanically      Activated and of Mechano-
      in Superparamagnets,” Journal of Magnetism and                       synthesized     Zinc Ferrite,” Journal of Solid State
      Magnetic       Materials, 111(1), 1992, 29-33.                       Chemistry, 146 (1), 1999, 13-21.
[3]   D. L. Leslie-Pelecky and R. D. Rieke,” Magnetic               [11]   V. Sepelak, K. Tkacova, V. V. Boldyrev and U. Steinike,
      Properties of Nanostructures Materials,” Chemistry of                “Crystal Srtucture Refinement         of the Mechanically
      Materials, 8 (8), 1996, 1770-1783.                                   Activated Spinel-Ferrite,” Materials Science Forum, 228,
[4]   T. Hirai, J. Kobayashi and I. Koasawa, “Preparation of               1996,       783-788.
      Acicular Ferrite Fine Particles Using an Emulsion Liquid      [12]   V. Sepelak, A. Yu, U. Rogachev, D. Steinike, C. Uecker,
      Membrane System,” Langmuir, 15 (19), 1999, 6291-                     S. Wibmann and K. D. Becker, “Structure of
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[5]   R. H. Kodama, “Magnetic Nanoparticles,” Journal of                   Ballmilling Method,” Acta Crystallographica A, 52,
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      “Sonochemical Preparation of Nanosized Amorphous                     State Chemistry, 135 (1), 1998, 52-58.
      NiFe2O4 Particles,” The            Journal of Physical        [14]   H. M. Rietveld, “Line Profile of Neutron Powder
      Chemistry B, 101 (33), 1996, 6409-6414.                              Diffraction Peaks for Structure Refinement,” Acta
[7]   D. Niznansky, M. Drillon and J. L. Renspinger,                       Crystallographica, 22, 1967, 151-152.
      “Preparation of Magnetic Nanoparticles (γ-Fe2O3) in the       [15]   H. M. Rietveld, “A Profile Refinement Method for
      Silica Matrix,” IEEE Transaction on Magnetics, 30 (2),               Nuclear and Magnetic Structures,” Journal of Applied
      1994, 821-823.                                                       Crystallography, 2, 1969, 65-71.
[8]   J. M. Yang, W. J. Tsuo and F. S. J. Yen, “Preparation of      [16]   L. Lutterotti, P. Scardi and P. Maistrelli, “LSI-a
      Ultrafine Nickel Ferrite Powder Using Ni and Fe                      Computer Program for Simultaneous Refinement of
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      1999, 50-57.                                                         Applied Crystallography, 25 (3), 1992, 459-462.
[9]   Y. Shi, J. Ding, X. Liu and J. Wang, “NiFe2O4 Ultrafine
      Particles Prepared by Co- Precipitation / Mechanical
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      Materials, 205 (2), 1999, 249-254.




                                                         www.ijmer.com                                             1760 | P a g e

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Ae02417571760

  • 1. International Journal of Modern Engineering Research (IJMER) www.ijmer.com Vol.2, Issue.4, July-Aug 2012 pp-1757-1760 ISSN: 2249-6645 Synthesis, Characterization Ac Conductivity of Ni2+ Doped In Magnesium Ferrite Pathan Amjadkhan Noorkhan1 and Sangshetty Kalayne2* 1 Department of Physics, Singhania University, Pacheri- Bari, JhunJunnu, Rajasthan 2* Department of Physics, Rural Engineering College, Bhalki, Bidar, Karnataka, India. Abstract: Magnesium nickel ferrites were synthesized by In the present study authors, report synthesis, employing sol gel technique at 1473 K sintering characterization and dielectric studies of MgNiFe2O4. A temperature. A critical Rietveld analysis of XRD reveals critical Rietveld analysis of XRD reveals that the presence that the presence of a very small amount of NiO phase of a very small amount of NiO phase along with the ferrite along with the ferrite phase. It indicates that almost a phase. It indicates that almost a stoichiometric (Mg,Ni)- stoichiometric (Mg,Ni)-ferrite phase has been obtained at ferrite phase has been obtained at 1473 K. SEM image 1473 K. SEM image shows that of (MgNi) ferrite is shows that of (MgNi) ferrite is regular in shape have regular in shape have granular in structure, compact and granular in structure, compact and well connected grain to well connected grain to each others. The ac conductivity each others. The ac conductivity increases with increase in increases with increase in applied frequency. The applied frequency and dielectric constant decreases. magnesium nickel ferrite (MnNiFe2O4) shows σac Therefore, this ferrites material is attracted to use in many conductivity of 1.2 x 10-4 S/cm. This is may be attributed science and technological applications. to the dipole polarization i.e., the rotation of dipoles between two equivalent equilibrium positions is involved. II. Experimental The high value of dielectric constant of the sample All Chemicals used were analytical grade (AR). MnNiFe2O4 may be the structural changes associated with The magnesium chloride, nickel chloride (purity 99.99%) the magnesium nickel ferrite when the grain size is and dehydrated ferric chloride were procured and were reduced. Therefore, this ferrites material is attracted to use used as received. in many science and technological applications. 1.1synthesis Of Magnesium Nickel Ferrite Keywords: Ac conductivity, (MgNi) ferrite, dielectric The chloride salts of magnesium, nickel chloride constant, Impedance spectra, X-ray diffraction. and ferric chloride are mixed in calculated stoichiometric with oxalic acid in equimolar ratio so as to form nickel I. INTRODUCTION ferric oxalate precursor. The precursor is then filtered and Small ferrimagnetic oxides, technically known dried at 323K to achieve constant weight. The precursor is as ferrites have attracted considerable attention not only mixed with polyethylene glycol (PEG) in the ratio 1:5 and from a fundamental scientific interest but also from a is ignited. The combustion propagates throughout the practical point of view for growing applications in the precursor. After completion of combustion nickel ferrite magnetic, electronic and microwave fields [1-3]. (MgNiFe2O4) is formed. The MgNi-ferrite is sonicated in Simultaneous presence of magnetic and dielectric nature acetone media for 20min and then calcinated at 1473 K to of ferrites is vastly exploited in a variety of applications remove the impurities. Finally, fine graded nanosized at different frequencies. The special feature of these nickel ferrite particles are formed [9, 10]. materials is that the properties can be tailored over wide The pellets of 10 mm diameter are prepared with thickness ranges by appropriate substitution of various ions in the varying up to 2 mm by applying pressure of 10 Tons in a chemical formula unit and control of processing UTM – 40 ( 40 Ton Universal testing machine). For procedures. Ferrites are extensively used in magnetic temperature dependent conductivity and sensor studies, the recording, information storage, colour imaging, bio- pellets are coated with silver paste on either side of the processing, magnetic refrigeration and in magneto surfaces to obtain better contacts. optical devices [4, 5]. Ferrites also have great promise for atomic 1.2 CHARACTERIZATION engineering of materials with functional magnetic The X-ray diffraction (XRD) pattern of the properties. The formation of corrosion product on the out MgNiFe2O4 was recorded at room temperature by of core surfaces in pressurized heavy water reactors employing an x-ray powder diffractometer (Rigaku (PHWRs) are major problem. Ferrite having spinal Miniflex) with CuK radiation ( =1.5405A0) in the structure such as magnetic and nickel etc play a major role 2 (Bragg angles) range (2 ≤ 2 ≤100) at a scan speed  0 to prevent such problem. Thus attempts are being made to of 0.50 minute-1. study the various ferrites to evaluate the impact of The percentage transmittances for the entire substitution of the divalent metal ions to modify the sample are measured from 300 to 4000 cm−1. The SEM properties of these oxides [6-8]. images of MgNiFe2O4 were recorded using Philips XL-30 (ESEM) scanning electron microscopy. The set up used for measuring ac conductivity is Hioki 3050 impedance analyzer, which is in turn interfaced to the computer. www.ijmer.com 1757 | P a g e
  • 2. International Journal of Modern Engineering Research (IJMER) www.ijmer.com Vol.2, Issue.4, July-Aug 2012 pp-1757-1760 ISSN: 2249-6645 average grain size was calculated by using line intercept III. RESULTS AND DISCUSSION formula and it is found to be 0.21µm. Figure 2 (c) shows that SEM image of (MgNi) ferrite. It is 2.1 X-RAYS DIFFRACTION found that the image is regular in shape have granular in structure, compact and well connected grain to each others. The average grain size was calculated by using line intercept formula and it is found to be 0.7µm. 2.3 AC CONDUCTIVITY The variation of σac of MnNiFe2O4 as a function of frequency as shown in figure 3. The conductivity of nickel ferrites is increases with increase in frequency. The magnesium nickel ferrite (MnNiFe2O4) shows σac conductivity of 1.2 x 10-4 S/cm. -4 MnNiFe2O4 1.2x10 Figure 1 shows the XRD patterns of Mg,Ni)-ferrite -4 annealed at temperature 1473 K. 1.0x10 -5 It seems that the (Mg,Ni)-ferrite phase is formed 8.0x10 ac S/cm completely after this heat-treatment. However, a critical -5 6.0x10 rietveld analysis reveals the presence of a very small amount of NiO phase along with the ferrite phase. It -5 4.0x10 indicates that almost a stoichiometric (Mg,Ni)-ferrite -5 phase has been obtained at 1473 K. This indicates that the 2.0x10 amount of ferrite phase formation is dependent of 0.0 annealing time. By measuring particle size we actually measure the coherently diffracting zone of a grain. The 2 10 10 3 10 4 10 5 10 6 particle or crystallites re separated from each other by Frequency (Hz) grain boundaries and the grain boundaries are nothing but bulk crystal imperfections in a crystal [11]. The size of the Figure 3 shows the variation of σac of MnNiFe2O4 as a crystallite in the nanometer range. As can be seen from the function of frequency. experiment, annealing the sample increases the size of the particles. Heat energy helps to annihilate the deformations This is may be attributed to the dipole in the crystals. As a result of grain boundaries started to polarization i.e., the rotation of dipoles between two vanish during annealing and the small crystallites equivalent equilibrium positions is involved. It is the agglomerate together to form larger particles due to intra- spontaneous alignment of dipoles in one of the equilibrium grain diffusion. positions that give rise to the nonlinear polarization behavior of this composition. 2.2 SCANNING ELECTRON MICROSCOPY This behaviour of MnNiFe2O4 obeys the universal power law,  (ω)=  n (the solid line is the fit  (ω) to the expression), where r0 is the dc conductivity (frequency independent plateau in the low frequency region), A is the pre-exponential factor, and n is the fractional exponent between 0 and 1 [12]. On crystallization, the conductivity spectrum remains similar as that of the nickel ferrite except dispersion in the low frequency region, where the deviation from  (plateau dc region) is more prominent. The deviation from  dc (plateau region) value in the conductivity spectrum (in the low frequency region) is due to the electrode polarization effect. The values of  , A, and n were obtained by fitting  the  to  (ω) (ω)=  n. The overall behavior  (ω) of  follows the universal dynamic response, which has ac widely been observed in disordered materials like ionically conducting glasses and also doped crystalline solids, and is Figure 2 shows the SEM image of (a) NiO and (b) MgNi- generally believed to be reflected in the mechanism of ferrite at 1473 K. charge transport behavior of charge carriers. Figure 2 (a) shows that SEM image of nickel oxide. It is clearly observed from the image they are agglomerated, highly branched and porous in nature. The www.ijmer.com 1758 | P a g e
  • 3. International Journal of Modern Engineering Research (IJMER) www.ijmer.com Vol.2, Issue.4, July-Aug 2012 pp-1757-1760 ISSN: 2249-6645 degree of covalency for the A site ions is higher than that 2500 MnNiFe2O4 of the B site ions. All the above factors result in a high activation energy for the A sites compared to the B sites. 2000 Hence, in ordinary magnesium nickel ferrite with an 1500 inverse spinel structure the electron movement in B sites dominates compared to that in A sites. ' 1000 6 2.5x10 MnNiFe2O4 500 6 2.0x10 0 2 3 4 5 6 6 10 10 10 10 10 1.5x10 Frequency (Hz) Z' 6 1.0x10 Figure 4 shows the variation real permittivity ( of ') nickel ferrite as a function of frequency. 5 5.0x10 0.0 Figure 4 shows the variation real permittivity (') of nickel ferrite of various composition as a function of 2 10 3 10 10 4 10 5 10 6 logarithmic frequency. It is found that in all these nickel Frequency (Hz) ferrite compositions, as frequency increases, dielectric constant decreases up to the frequency range of 10 5 Hz and Figure 6 the variation of real part of impedance as a after that it remains constant for further increasing in function of frequency frequency [13]. The strong frequency dispersion of permittivity is observed in the low frequency region The variation of real part of impedance of followed by a nearly frequency independent behaviour MnNiFe2O4 is shown in figure 6 as a function of above 103 Hz. It is observed that Debye type relaxation increasing frequency. It is observed that the real part of mechanism is responsible for higher value of MnNiFe2O4. impedance decreases with increase in frequency. The initial decrease in impedance value due to the increase in conductivity at lower frequency region up to 103 Hz and further increases in applied frequency, the impedance value remains constant. This indicates that after 103 Hz the ferrite acts as lossless materials. Therefore, these ferrites can be used in many technological applications such as memory device, microwave, sensor, transducer, solar cell etc. IV. CONCLUSION Sol-gel technique was employed to prepare the Figure 5 shows the variation of dielectric constant as a magnesium nickel ferrites were at 1473 K sintering function of frequency of MnNiFe2O4 temperature. A critical Rietveld analysis of XRD reveals that the presence of a very small amount of NiO phase Figure 5 shows the variation of dielectric constant along with the ferrite phase. It indicates that almost a as a function of frequency for MnNiFe2O4. The high value stoichiometric (Mg,Ni)-ferrite phase has been obtained at of dielectric constant of the sample MnNiFe2O4 may be 1473 K. SEM image shows that of (MgNi) ferrite is explained on the basis of the structural changes associated regular in shape have granular in structure, compact and with the magnesium nickel ferrite when the grain size is well connected grain to each others. The ac conductivity reduced. Magnesium nickel ferrite crystallizes into a cubic increases with increase in applied frequency. The close-packed arrangement of oxygen ions. It belongs to the magnesium nickel ferrite (MnNiFe2O4) shows σac class of ferrites with an inverse spinel structure having conductivity of 1.2 x 10-4 S/cm. This is may be attributed structural formula, Fe3+[Mg2+Ni3+]O4. The metal ions to the dipole polarization i.e., the rotation of dipoles given in the square bracket are called octahedral (B site) between two equivalent equilibrium positions is involved. ions and that outside the square bracket are called The high value of dielectric constant of the sample tetrahedral (A site) ions. The nickel ions (Ni2+) together MnNiFe2O4 may be the structural changes associated with with half of the iron ions (Fe3+) occupy the B site and the the magnesium nickel ferrite when the grain size is Mg2+ occupy the remaining half of the iron ions reside in reduced. It is observed that the real part of impedance A site. The presence of Mg2+ and Ni3+ ions gives rise to p- decreases with increase in frequency. The initial decrease type carriers (holes) whereas Fe2+ and Fe3+ ions produce n- in impedance value due to the increase in conductivity at type carriers (electrons). Therefore, both electrons and lower frequency region up to 103 Hz and further increases holes that are present in the B sites are due to the presence in applied frequency, the impedance value remains of Mg and Ni ions. Since Mg ions are present in A sites, constant. Therefore, this ferrites material is attracted to use electrons are the carriers in A sites. The distance between in many science and technological applications. the ions in A sites (0⋅357 nm) is larger than the distance between the ions in B site (0⋅292 nm) [14-16]. Also, the www.ijmer.com 1759 | P a g e
  • 4. International Journal of Modern Engineering Research (IJMER) www.ijmer.com Vol.2, Issue.4, July-Aug 2012 pp-1757-1760 ISSN: 2249-6645 REFERENCE [1] I. Anton, I. D. Dabata and L. Vekas, “Application Orientated Researches on Magnetic Fluids,” Journal of Magnetism and Magnetic Materials, 85 (1), 1990, 219- 226. [2] R. D. McMickael, R. D. Shull, L. J. Swartzendruber, L. [10] P. Druska, U. Steinike and V. Sepelak, “Surface H. Bennett and R. E. Watson, “Magnetocaloric Effect Structure of Mechanically Activated and of Mechano- in Superparamagnets,” Journal of Magnetism and synthesized Zinc Ferrite,” Journal of Solid State Magnetic Materials, 111(1), 1992, 29-33. Chemistry, 146 (1), 1999, 13-21. [3] D. L. Leslie-Pelecky and R. D. Rieke,” Magnetic [11] V. Sepelak, K. Tkacova, V. V. Boldyrev and U. Steinike, Properties of Nanostructures Materials,” Chemistry of “Crystal Srtucture Refinement of the Mechanically Materials, 8 (8), 1996, 1770-1783. Activated Spinel-Ferrite,” Materials Science Forum, 228, [4] T. Hirai, J. Kobayashi and I. Koasawa, “Preparation of 1996, 783-788. Acicular Ferrite Fine Particles Using an Emulsion Liquid [12] V. Sepelak, A. Yu, U. Rogachev, D. Steinike, C. Uecker, Membrane System,” Langmuir, 15 (19), 1999, 6291- S. Wibmann and K. D. Becker, “Structure of 6298. Nanocrystalline Spinel Ferrite Produced by High Energy [5] R. H. Kodama, “Magnetic Nanoparticles,” Journal of Ballmilling Method,” Acta Crystallographica A, 52, Magnetism and Magnetic Materials, 200 (1), 1999, 359- 1996, C367 372. [13] V. Sepelak, U. Steinike, D. C. Uecker, S. Wibmann and [6] K. V. P. M. Shafi, Y. Koltypin, A. Gedanken, R. K. D. Becker, “Structural Disorder in Prozorov, J. Balogh, J. Lendvai and I. Felner, Mechanosynthesized by Zinc Ferrite,” Journal of Solid “Sonochemical Preparation of Nanosized Amorphous State Chemistry, 135 (1), 1998, 52-58. NiFe2O4 Particles,” The Journal of Physical [14] H. M. Rietveld, “Line Profile of Neutron Powder Chemistry B, 101 (33), 1996, 6409-6414. Diffraction Peaks for Structure Refinement,” Acta [7] D. Niznansky, M. Drillon and J. L. Renspinger, Crystallographica, 22, 1967, 151-152. “Preparation of Magnetic Nanoparticles (γ-Fe2O3) in the [15] H. M. Rietveld, “A Profile Refinement Method for Silica Matrix,” IEEE Transaction on Magnetics, 30 (2), Nuclear and Magnetic Structures,” Journal of Applied 1994, 821-823. Crystallography, 2, 1969, 65-71. [8] J. M. Yang, W. J. Tsuo and F. S. J. Yen, “Preparation of [16] L. Lutterotti, P. Scardi and P. Maistrelli, “LSI-a Ultrafine Nickel Ferrite Powder Using Ni and Fe Computer Program for Simultaneous Refinement of Tartrates,” Journal of Solid State Chemistry, 145(1), Material Structure and Microstructure,” Journal of 1999, 50-57. Applied Crystallography, 25 (3), 1992, 459-462. [9] Y. Shi, J. Ding, X. Liu and J. Wang, “NiFe2O4 Ultrafine Particles Prepared by Co- Precipitation / Mechanical Alloying,” Journal of Magnetism and Magnetic Materials, 205 (2), 1999, 249-254. www.ijmer.com 1760 | P a g e