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K.S. Nagaraju et al.Int. Journal of Engineering Research and Application www.ijera.com
ISSN : 2248-9622, Vol. 6, Issue 9,(Parte-5) September.2016, pp.39-42
www.ijera.com 39|P a g e
Dielectric properties of Ni-Al nano ferrites synthesized by citrate
gel method
K.S. Nagaraju 1
and D. Ravinder 2*
1
Department of Physics, Vivakananda Degree College ,Malleswaram, West Post, Bangalore-
560055,Karnataka, India
2*
Department of Physics, Osmania University, Hyderabad- 500 007, Telangana, India
ABSTRACT
Ni–Al ferrite with composition of NiAlxFe2-xO4 (x=0.2, 0.4 0.6, and 0.8, ) were prepared by citrate gel method.
The Dielectric Properties for all the samples were investigated at room temperature as a function of frequency.
The Dielectric constant shows dispersion in the lower frequency region and remains almost constant at higher
frequencies. The frequency dependence of dielectric loss tangent (tanδ) is found to be abnormal, giving a peak
at certain frequency for mixed Ni-Al ferrites. A qualitative explanation is given for the composition and
frequency dependence of the dielectric loss tangent.
Keywords: Ferrites; Citrate method; lattice parameter; dielectric constant; dielectric loss
I. INTRODUCTION
Ni-Al ferrite is a well-known spinel
magnetic material. In the inverse spinel structure
of NiFe2O4, the tetrahedral sites are occupied by
ferric ions and octahedral sites by ferric and nickel
ions. Ni Al X Fe2- XO4 ferrites are ferrimagnetic
materials with a large number of technological
applications in telecommunications and
entertainment electronics. Ni Al ferrites are among
the most widely used soft magnetic materials
because of high frequency applications as they
posses high electrical resistivity and low eddy
current losses [1-3]. It is known that magnetic
properties of ferrites are sensitive to preparation
technique and their microstructures [4]. The
electrical and magnetic properties of such ferrites
depend strongly on distribution of cations at the
tetrahedral (A) and octahedral [B] sites in the
lattice [5 -7]. It is well known that zinc ions can be
used to alter the saturation magnetization. It is
believed that the addition of zinc ions also affects
the lattice parameter and it would therefore be
expected to change the Curie temperature of the
material [8]. The substitution of divalent ions in
pure ferrites leads to the modification of the
structural, electrical and magnetic properties [9].
The conventional solid-state reaction route is
widely used for the production of ferrite because of
its low cost and suitability for large scale
production. The citrate method is used to speed up
the synthesis of complex materials. It is a simple
process, which offers a significant saving in time
and energy consumption over the traditional
methods. Several researchers have reported the
synthesis of Ni-Zn ferrites using different
techniques like, refluxing process [10], ceramic
[11], hydrothermal [12], combustion [13], co-
precipitation [14], reverse micelle process [15],
spark plasma sintering [16], micro emulsion [17]
and ball milling etc.
In this work, we present the results of
systematic doping of non-magnetic Al content on
the dielectric properties of Ni ferrite synthesized
by citrate method.
II. EXPERIMENTAL
The starting materials were nickel nitrate,
zinc nitrate, iron nitrate, citric acid and ammonia all
of analytical grade. The solution of nickel nitrate
(Ni (NO3)2. 6H2O, ferric nitrate (Fe(NO3)3.9H2O)
and Aluminium nitrate(Al(NO3)2.6H2O) in their
stoichiometry were dissolved in a de ionized
water. Citric acid was then added to the prepared
aqueous solution to chelate Ni2+
, Al3+
and Fe3+
in
the solution. The molar ratio of citric acid to total
moles of nitrate ions was adjusted at 1: 3. The
mixed solution was neutralized to pH 7 by adding
ammonia (NH3) solution. The neutralized solution
was evaporated to dryness by heating at 1000
C on
a hot plate with continuous stirring, until it
becomes viscous and finally formed a very viscous
gel. Increasing the temperature up to 2000
C lead to
ignition of gel. The dried gel burnt completely in a
self propagating combustion manner to form a
loose powder. Finally the burnt powder was
calcined in air at temperature of 10000
C for one
hour to obtain spinel phase. Afterwards the powder
was pressed into pellets of thickness 3 mm and a
diameter of 10 mm with press by applying a
pressure of 2 tons/in2
.The final sintering was done
at 1000o
C, afterwards the pellets were coated with
silver paint for better electrical contact to measure
RESEARCH ARTICLE OPEN ACCESS
OPEN ACCESS
K.S. Nagaraju et al.Int. Journal of Engineering Research and Application www.ijera.com
ISSN : 2248-9622, Vol. 6, Issue 9,(Parte-5) September.2016, pp.39-42
www.ijera.com 40|P a g e
the dielectric properties.The dielectric data are
measured by Impedance Analyser at room
temperature in the frequency range 1 MHz to
13MHz.
III. RESULTS AND DISCUSSIONS
3.1Dielecric constant with frequency:
The effect of frequency on the dielectric
constant (ε') can be seen from Figs. 1to 4 and that
the value of dielectric constant decreases
continuously with increasing frequency. The
decrease in the values of dielectric constant as the
frequency increases can be due to electron
exchange interaction between Fe2+
and Fe3+
ions,
which cannot follow the alternating electric field.
The decrease of dielectric constant with increase of
frequency as observed in the case of Ni-Al ferrite.
A similar behavior was also observed in [18-21] of
various ferrite systems. The explanation for the
decrease in the values of ε' as the frequency
increases can be related to electron exchange
interaction between Fe2+
and Fe3+
ions which
cannot follow the alternation of the electric field
beyond a certain frequency.
3.2 Dielectric loss tangent (tan δ) with
frequency:
The variation of tan δ with frequency can
be seen from Figs.5 to 8, it can be seen from the
figures that in the case of Ni-Al nano ferrites. A
qualitative explanation can be given for the
occurrence of the maxima in tan δ verses frequency
curves in Ni-Al as pointed out by Iwauchi[22],
there is a strong correlation between the conduction
mechanism and the dielectric behavior of ferrites.
The conduction mechanism in n-type ferrites is
considered as due to hopping of electrons between
Fe2+
and Fe3+
situated on the octahedral sites. As
seen, when the hopping frequency is nearly equal
to that of external applied electric field a maximum
of loss tangent may be observed [23]. As such it is
possible that in the case of in Ni-Al nano ferrites
the hoping frequencies are of the approximate
magnitude to observe a loss maximum at 8 MHz
respectively
IV. CONCLUSIONS
It may be concluded that a series of Ni-Al
ferrite with compositional formula NiAlX Fe2-XO4
where =0.2, 0.4, 0.6, and 0.8, are prepared by
citrate gel method. The lattice constant was found
to be increases with zinc composition. The
variation of dielectric constant and dielectric loss
tangent was explained on the basis of electronic
exchange between The Fe2+
and Fe3+
ions
ACKNOWLEDGMENTS
One of the KSN is grateful to Prof. G.K.
Narayan Reddy, President of JES
And former Vice-Chancellor of Karnataka
University and Dr. Manchegowda, Honorary
Secretary, JES.
REFERENCES
[1]. X. He, G. Song, J. Zhu, Materials Letters.
59 (2005) 1941-1944.
[2]. Y. Matsuo, M. Inagaki, T. Tomozawa, F.
Nakao, IEEE Trans. Magn. 37 (2001)
2359-2361.
[3]. P.S. Anil Kumar, J.J. Shrotri, S.D.
Kulkarni, C.E. Deshpande, S.K.Date,
Mater. Lett. 27 (1996) 293-296.
[4]. H. Su, H. Zhang, X. Tang, Y. Jing, Y. Liu,
J. Magn. Magn. Mater. 310 (2007) 17-21.
[5]. J.L. Dormann, M. Nogues, J. Phys.:
Condens. Matter. 2 (1990) 1223-1237.
[6]. N. Rezlescu, E. Rezlescu, C. Pasnicu,
M.L. Craus, J. Phys. Condens. Matter. 6
(1994) 5707-5716.
[7]. A.E. Virden, K. O’Grady,
J.Magn.Magn.Mater. 290–291 (2005)
868-870.
[8]. A.M. El-Sayed, Ceramics. Int. 28 (2002)
363-367.
[9]. Z. Zhong , Q. Li, Y. Zhang, H. Zhong, M.
Cheng, Y. Zhang, Powder Technology.
155 (2005) 193-195.
[10]. A. Dias, R.L. Moreira, Materials Letters.
39 (1999) 69-76.
[11]. S. E. Jacobo, S. Duhalde, H.R. Bertorello,
J. Magn. Magn. Mater. 272–276 (2004)
2253-2254.
[12]. S.D. Shenoy, P.A. Joy, M.R.
Anantharaman, J. Magn. Magn. Mater.
269 (2004) 217-226.
[13]. S. A. Morrison, C. L. Cahill, E. E.
Carpenter, S. Calvin, R. Swaminathan, M.
E. McHenry, V. G. Harris, J.Appl.Phys.
95 (2004) 6392-6395.
[14]. J. Sun, J. Li, G. Sun, W. Qu, Ceramics
International. 28 (2002) 855-858.
[15]. A. Verma, T.C. Goel, R.G. Mendiratta,
M.I. Alam. Mat. Sci. Engg. B60 (1999)
156-162.
[16]. G. Pozo Lopez, S.P. Silvetti, S.E. Urreta,
E.D. Cabanillas. Physica B. 398 (2007)
241-244.
[17]. C. Upadhyay, D. Mishra, H.C. Verma, S.
Anand, R.P. Das. J. Magn. Magn. Mater.
260 (2003) 188-194.
[18]. S.Mahalakshmi , K.Srinivasa Manja
J.alloys.comp457(2008)522-525
[19]. D.Ravinder, J.Vijaya Bhasker Redddy,
Mater.Lett.57(2003)4344-4350
K.S. Nagaraju et al.Int. Journal of Engineering Research and Application www.ijera.com
ISSN : 2248-9622, Vol. 6, Issue 9,(Parte-5) September.2016, pp.39-42
www.ijera.com 41|P a g e
[20]. N.Rezlescu,E.Rezlescu, Sliod state
Commun,14(1974)69.
[21]. V.R.Murthy, J.Sobbhandari,
phys.Stat.sol(A) 36(1976)K133
[22]. K.Iwauchi
Japan.J.Appl.Phys.10(1971)1520
[23]. A.M Abdeen ,O.M Hemeda, E.E Assem,
M.M. EI-sehly,
J.Magn.Magn.Mater238(2008)75
K.S. Nagaraju et al.Int. Journal of Engineering Research and Application www.ijera.com
ISSN : 2248-9622, Vol. 6, Issue 9,(Parte-5) September.2016, pp.39-42
www.ijera.com 42|P a g e

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Dielectric properties of Ni-Al nano ferrites synthesized by citrate gel method

  • 1. K.S. Nagaraju et al.Int. Journal of Engineering Research and Application www.ijera.com ISSN : 2248-9622, Vol. 6, Issue 9,(Parte-5) September.2016, pp.39-42 www.ijera.com 39|P a g e Dielectric properties of Ni-Al nano ferrites synthesized by citrate gel method K.S. Nagaraju 1 and D. Ravinder 2* 1 Department of Physics, Vivakananda Degree College ,Malleswaram, West Post, Bangalore- 560055,Karnataka, India 2* Department of Physics, Osmania University, Hyderabad- 500 007, Telangana, India ABSTRACT Ni–Al ferrite with composition of NiAlxFe2-xO4 (x=0.2, 0.4 0.6, and 0.8, ) were prepared by citrate gel method. The Dielectric Properties for all the samples were investigated at room temperature as a function of frequency. The Dielectric constant shows dispersion in the lower frequency region and remains almost constant at higher frequencies. The frequency dependence of dielectric loss tangent (tanδ) is found to be abnormal, giving a peak at certain frequency for mixed Ni-Al ferrites. A qualitative explanation is given for the composition and frequency dependence of the dielectric loss tangent. Keywords: Ferrites; Citrate method; lattice parameter; dielectric constant; dielectric loss I. INTRODUCTION Ni-Al ferrite is a well-known spinel magnetic material. In the inverse spinel structure of NiFe2O4, the tetrahedral sites are occupied by ferric ions and octahedral sites by ferric and nickel ions. Ni Al X Fe2- XO4 ferrites are ferrimagnetic materials with a large number of technological applications in telecommunications and entertainment electronics. Ni Al ferrites are among the most widely used soft magnetic materials because of high frequency applications as they posses high electrical resistivity and low eddy current losses [1-3]. It is known that magnetic properties of ferrites are sensitive to preparation technique and their microstructures [4]. The electrical and magnetic properties of such ferrites depend strongly on distribution of cations at the tetrahedral (A) and octahedral [B] sites in the lattice [5 -7]. It is well known that zinc ions can be used to alter the saturation magnetization. It is believed that the addition of zinc ions also affects the lattice parameter and it would therefore be expected to change the Curie temperature of the material [8]. The substitution of divalent ions in pure ferrites leads to the modification of the structural, electrical and magnetic properties [9]. The conventional solid-state reaction route is widely used for the production of ferrite because of its low cost and suitability for large scale production. The citrate method is used to speed up the synthesis of complex materials. It is a simple process, which offers a significant saving in time and energy consumption over the traditional methods. Several researchers have reported the synthesis of Ni-Zn ferrites using different techniques like, refluxing process [10], ceramic [11], hydrothermal [12], combustion [13], co- precipitation [14], reverse micelle process [15], spark plasma sintering [16], micro emulsion [17] and ball milling etc. In this work, we present the results of systematic doping of non-magnetic Al content on the dielectric properties of Ni ferrite synthesized by citrate method. II. EXPERIMENTAL The starting materials were nickel nitrate, zinc nitrate, iron nitrate, citric acid and ammonia all of analytical grade. The solution of nickel nitrate (Ni (NO3)2. 6H2O, ferric nitrate (Fe(NO3)3.9H2O) and Aluminium nitrate(Al(NO3)2.6H2O) in their stoichiometry were dissolved in a de ionized water. Citric acid was then added to the prepared aqueous solution to chelate Ni2+ , Al3+ and Fe3+ in the solution. The molar ratio of citric acid to total moles of nitrate ions was adjusted at 1: 3. The mixed solution was neutralized to pH 7 by adding ammonia (NH3) solution. The neutralized solution was evaporated to dryness by heating at 1000 C on a hot plate with continuous stirring, until it becomes viscous and finally formed a very viscous gel. Increasing the temperature up to 2000 C lead to ignition of gel. The dried gel burnt completely in a self propagating combustion manner to form a loose powder. Finally the burnt powder was calcined in air at temperature of 10000 C for one hour to obtain spinel phase. Afterwards the powder was pressed into pellets of thickness 3 mm and a diameter of 10 mm with press by applying a pressure of 2 tons/in2 .The final sintering was done at 1000o C, afterwards the pellets were coated with silver paint for better electrical contact to measure RESEARCH ARTICLE OPEN ACCESS OPEN ACCESS
  • 2. K.S. Nagaraju et al.Int. Journal of Engineering Research and Application www.ijera.com ISSN : 2248-9622, Vol. 6, Issue 9,(Parte-5) September.2016, pp.39-42 www.ijera.com 40|P a g e the dielectric properties.The dielectric data are measured by Impedance Analyser at room temperature in the frequency range 1 MHz to 13MHz. III. RESULTS AND DISCUSSIONS 3.1Dielecric constant with frequency: The effect of frequency on the dielectric constant (ε') can be seen from Figs. 1to 4 and that the value of dielectric constant decreases continuously with increasing frequency. The decrease in the values of dielectric constant as the frequency increases can be due to electron exchange interaction between Fe2+ and Fe3+ ions, which cannot follow the alternating electric field. The decrease of dielectric constant with increase of frequency as observed in the case of Ni-Al ferrite. A similar behavior was also observed in [18-21] of various ferrite systems. The explanation for the decrease in the values of ε' as the frequency increases can be related to electron exchange interaction between Fe2+ and Fe3+ ions which cannot follow the alternation of the electric field beyond a certain frequency. 3.2 Dielectric loss tangent (tan δ) with frequency: The variation of tan δ with frequency can be seen from Figs.5 to 8, it can be seen from the figures that in the case of Ni-Al nano ferrites. A qualitative explanation can be given for the occurrence of the maxima in tan δ verses frequency curves in Ni-Al as pointed out by Iwauchi[22], there is a strong correlation between the conduction mechanism and the dielectric behavior of ferrites. The conduction mechanism in n-type ferrites is considered as due to hopping of electrons between Fe2+ and Fe3+ situated on the octahedral sites. As seen, when the hopping frequency is nearly equal to that of external applied electric field a maximum of loss tangent may be observed [23]. As such it is possible that in the case of in Ni-Al nano ferrites the hoping frequencies are of the approximate magnitude to observe a loss maximum at 8 MHz respectively IV. CONCLUSIONS It may be concluded that a series of Ni-Al ferrite with compositional formula NiAlX Fe2-XO4 where =0.2, 0.4, 0.6, and 0.8, are prepared by citrate gel method. The lattice constant was found to be increases with zinc composition. The variation of dielectric constant and dielectric loss tangent was explained on the basis of electronic exchange between The Fe2+ and Fe3+ ions ACKNOWLEDGMENTS One of the KSN is grateful to Prof. G.K. Narayan Reddy, President of JES And former Vice-Chancellor of Karnataka University and Dr. Manchegowda, Honorary Secretary, JES. REFERENCES [1]. X. He, G. Song, J. Zhu, Materials Letters. 59 (2005) 1941-1944. [2]. Y. Matsuo, M. Inagaki, T. Tomozawa, F. Nakao, IEEE Trans. Magn. 37 (2001) 2359-2361. [3]. P.S. Anil Kumar, J.J. Shrotri, S.D. Kulkarni, C.E. Deshpande, S.K.Date, Mater. Lett. 27 (1996) 293-296. [4]. H. Su, H. Zhang, X. Tang, Y. Jing, Y. Liu, J. Magn. Magn. Mater. 310 (2007) 17-21. [5]. J.L. Dormann, M. Nogues, J. Phys.: Condens. Matter. 2 (1990) 1223-1237. [6]. N. Rezlescu, E. Rezlescu, C. Pasnicu, M.L. Craus, J. Phys. Condens. Matter. 6 (1994) 5707-5716. [7]. A.E. Virden, K. O’Grady, J.Magn.Magn.Mater. 290–291 (2005) 868-870. [8]. A.M. El-Sayed, Ceramics. Int. 28 (2002) 363-367. [9]. Z. Zhong , Q. Li, Y. Zhang, H. Zhong, M. Cheng, Y. Zhang, Powder Technology. 155 (2005) 193-195. [10]. A. Dias, R.L. Moreira, Materials Letters. 39 (1999) 69-76. [11]. S. E. Jacobo, S. Duhalde, H.R. Bertorello, J. Magn. Magn. Mater. 272–276 (2004) 2253-2254. [12]. S.D. Shenoy, P.A. Joy, M.R. Anantharaman, J. Magn. Magn. Mater. 269 (2004) 217-226. [13]. S. A. Morrison, C. L. Cahill, E. E. Carpenter, S. Calvin, R. Swaminathan, M. E. McHenry, V. G. Harris, J.Appl.Phys. 95 (2004) 6392-6395. [14]. J. Sun, J. Li, G. Sun, W. Qu, Ceramics International. 28 (2002) 855-858. [15]. A. Verma, T.C. Goel, R.G. Mendiratta, M.I. Alam. Mat. Sci. Engg. B60 (1999) 156-162. [16]. G. Pozo Lopez, S.P. Silvetti, S.E. Urreta, E.D. Cabanillas. Physica B. 398 (2007) 241-244. [17]. C. Upadhyay, D. Mishra, H.C. Verma, S. Anand, R.P. Das. J. Magn. Magn. Mater. 260 (2003) 188-194. [18]. S.Mahalakshmi , K.Srinivasa Manja J.alloys.comp457(2008)522-525 [19]. D.Ravinder, J.Vijaya Bhasker Redddy, Mater.Lett.57(2003)4344-4350
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  • 4. K.S. Nagaraju et al.Int. Journal of Engineering Research and Application www.ijera.com ISSN : 2248-9622, Vol. 6, Issue 9,(Parte-5) September.2016, pp.39-42 www.ijera.com 42|P a g e