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8/2/2019 Ferro Magnetic Materials
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FERROMAGNETIC MATERIALS
DKR-JIITN-PH611-MAT-SCI-2010
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DKR-JIITN-PH611-MAT-SCI-2010
Ferromagnetic Materials
MHB 00 +=
Certain metallic materials posses permanent magnetic moment inthe absence of an external field, and manifests very large andpermanent magnetization which is termed as spontaneousmagnetization. Example: Fe, Co, Ni and some rare earth metals
such as Gd.
Magnetic susceptibility as high as 106 are possible for ferromagneticmaterials. Therefore, H
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Atomic magnetic moments due to un-cancelled electron spin is
responsible for Spontaneous magnetization. Orbital motion alsocontributes but its contribution is very small in comparison to theelectron spin.
Coupling interaction causes net spin magnetic moments ofadjacent atoms to align with one another even in absence ofexternal field. This mutual spin alignment exists over a relativelylarger volume of the crystal called domain.
The maximum possible magnetizationis called saturation magnetization. Itresults when all magnetic dipoles in a
solid piece are mutually aligned withthe external field. There is also acorresponding saturation flux densityBs.
NMs = (3)
DKR-JIITN-PH611-MAT-SCI-2010
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1. Weiss theory of spontaneous magnetization classical theory
Hypothesis of Weiss theory:
1. A ferromagnetic specimen contains, in general, large number ofsmall regions called domains (dimension ~ 10-2 cm andcontaining as many as 1015 to 1017 atoms) which arespontaneously magnetized. The magnitude of spontaneousmagnetization of the specimen is determined by vector sum ofdipole moment of individual domains.
2. Within each domain spontaneous magnetization is due to theexistence of a molecular field which tends to produce a parallelalignment of the atomic dipoles despite effect of thermal energy.This internal field is equivalent to a magnetic field Hm, which is
proportional to the magnetization M of within a domain i.e.
MHm =
Where is constant independent of temperature, called molecularfield constant or Weiss constant.
(1.1)
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Effective field experienced by each dipole would be then,
MHHe +=
Let us consider a ferromagnetic solid containing N number ofatoms/ m3, then magnetization due to spins can be given as
])(
tanh[]tanh[ 00
kT
MHN
kT
HNM BB
BB
+==
At sufficiently high temperature,
1)(
0
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Where,
kT
MHNM B
)(2
0 +=
kT
MN
kT
HNM BB
2
0
2
0 +=kT
HN
kT
NM BB
2
0
2
0 )1(
=
)1(
2
0
2
0
kT
NkT
N
H
M
B
B
==
)(
2
0
2
0
k
NTk
N
H
M
B
B
==
)(
=T
C
Ck
NkNC BB ===
2
0
2
0 and
Therefore,(1.3)
(1.4)
(1.5)
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T
1/
Ferromagnetic
Paramagnetic
0 Now when H = 0, then
]tanh[])(
tanh[ 00
kT
MN
kT
MHNM B
B
B
B
=
+=
]tanh[ 0
kT
M
M
M
N
M B
sB
==
(1.5)
tanh==sB M
M
N
M
Where, kT
MB
0
=
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)(aBNgJM JB=
Where
and
kT
MHgJ
kT
HgJa BB
)(00 +==
We know that,Bs NgJM =)0( Therefore
)()0()( aBMTMJs
=
)()0(
)(aB
M
TMJ
s
=
Further,kT
MgJ
kT
MHgJa BB 00 )( =+=
J
a
J
a
J
J
J
JJB
2coth
2
1
2
)12(coth
2
12)(
++=
2. Weiss theory of spontaneous magnetization Quantum theory
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kT
MgJa B
0=
BgJ
kTaTM
0
)( =
BBs NgJgJ
kTa
M
TM
1
)0(
)(
0
=
2
0
22)0(
)(
Bs JNg
kTa
M
TM=
)0(
)(
sM
TM
a
)(aBJ
T =T
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)0(
)(
sM
TM
T
1
15.00
)0(sM
T
1
5.0
Ms(0) is spontaneous magnetization at 0K.
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Let us consider Brillouin function (BJ) again,
Ja
JJaJ
JJaBJ
2coth
21
2)12(coth
212)( ++=
For a
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+
+++=
aJ
aJ
aJ
aJJJaBJ 2
22
2
222
12
12
12
)414(12)(
+++=
aJ
aJJaaaJJaBJ 2
2222222
12
124412)(
+=
aJ
JaaJaBJ 2222
12
44)(
+=
aJ
JJaaBJ 2
2
12
)1(4)(
+=J
JaaBJ
3
)1()(
Therefore, from the equation of magnetization
)()0()( aBMTM Js=J
JaMTM s
3
1)0()(
+=
Thus, slope of the curve for a
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2
0
22)0()(
Bs JNgkTa
MTM =
We also know that,
2
0
22)0()(
Bs JNgkT
aMTM =
Thus,
(B)
Comparing (A) and (B) at T = ,
J
J
JNg
k
B3
12
0
22
+=
k
JJNg B
3
)1(2
0
2 += (C)
Equation gives relation between curie temperature, and molecular fieldconstant, .
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Now let us consider the case of T>, a
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)3
)1(1(
3
)1(
20
2
2
0
2
kTJJNg
kT
JJNg
H
M
B
B
+
+
==
)3
)1((
)1(
2
0
2
2
0
2
kJJNgTk
JJNg
H
M
B
B
+
+==
)(
=T
C(C)
Where,k
JJNgC B
)1(2
0
2 +=
and k
JJNg B
3
)1(20
2 +=
(D)
(E)
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3. Exchange interaction in magnetic materials
212 sJsEexch =
2
1
2.2 ZJSSSJEj
jiijexch = =rr
Heisenberg in 1928 gave theoretical explanation for large Weissfield in ferromagnetic materials.
According to his theory, parallel arrangements of spins inferromagnetic materials arises due to exchange interaction inwhich two neighboring spins in the solid are coupled togetherwith an energy given as
Here J is known as exchange integral. Its value depends uponseparation between atoms as well as overlap of electron chargecloud. When J > 0, lower energy is obtained for parallel
configuration of spins, while for J < 0, spins are anti-parallel.
(3.1)
If there are Z nearest neighbors to a central ith spin, theexchange energy for this spin is
(3.2)
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ijJ
02r
rab
Cr
Mn
Fe
Co
Ni
Gd
22ZS
KJ
KZJS 22
This energy must be equal to K as at , ferromagnetic order isdestroyed. Thus,
(rab is inter-atomic distance
and r0 is atomic radius).
0>J
0