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Submitted on 1 Jan 1971
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MAGNETOCALORIC EFFECT AND CRITICAL PHENOMENA OF IRON, COBALT AND NICKEL
NEAR THE CURIE TEMPERATURE
W. Rocker, R. Kohlhaas, H. Schöpgens
To cite this version:
W. Rocker, R. Kohlhaas, H. Schöpgens. MAGNETOCALORIC EFFECT AND CRITICAL PHE-
NOMENA OF IRON, COBALT AND NICKEL NEAR THE CURIE TEMPERATURE. Journal de
Physique Colloques, 1971, 32 (C1), pp.C1-652-C1-653. �10.1051/jphyscol:19711225�. �jpa-00214052�
JOURNAL DE PHYSIQUE
Colloque C I, ~upplkment au no 2-3, Tome 32, Fkvrier-Mars 1971, page C 1 - 652
MAGNETOCALORIC EFFECT AND CRITICAL PHENOMENA OF IRON, COBALT AND NICKEL NEAR THE CURIE TEMPERATURE
by W. ROCKER, R. KOHLHAAS and H. W. SCH~PGENS
Max-Planck-Institut fur Eisenforschung, Diisseldorf and Abt. Metallphysik im 1I.Physikalischen Institut der Universjtat Koln
Rdsumk. -
Les propriktts magnetiques de Fe, Co et Ni et I'effet magnCtocalorique ont
6teCtudiCs dans les environs du point de Curie. L'aimantation spontanke et I'inverse de
lasusceptibilite initiale ant
C t tcalculkes. Les exposants
j?, y, 6et
TCont Bte donnts.
Abstract.
- The magnetic properties of Fe, Co and Ni have been measured together with the magnetocaloric effect
inthe neighbourhood of the Curie temperature. Spontaneous magnetization and reciprocal initial susceptibility have been computed. The critical indices 8,
7, 6and
nare given.
Till now there have been given uniform exponents
b and
yconcerning the magnetization-field-tempera- ture behaviour of a ferromagnetic in a great tempera- ture range about the critical point. These critical indices were combinable with scaling laws and they allowed to calculate the exponents 6 of the magneti- zation and
nof the magnetocaloric effect at T,.
Following theoretical discussions of Kadanoff [I]
two values for /? were to be expected according to the distance from the critical point.
This supposition was confirmed by exact measure- ments of Arajs [2] on nickel from which /? was calcu- lated
:b
=0.50 for
E =I 1 - TIT, I
=4
x...
5 xB
=0.34 for
E =I 1 - TIT,
( =5
x... 3
x1 0 - I . We have studied with a modified Faraday force technique the magnetization behaviour of Fe, Co and Ni spheres together with the magnetocaloric effect in a wide temperature range about the Curie point with external fields from 100 to 25 000 Oe. The appa- ratus and the measuring procedure have been des- cribed by Lange [3]. Fig. 1 shows some of these magnetization curves of Fe, Co and Ni as a function of temperature with the external field as a parameter.
In fig. 2 there are plotted some curves of the magne-
tocaloric effect as a function of temperature without field.
FIG. 2.
- Magnetocaloric effect of Fe,
Coand Ni plotted
vstemperature
TOwithout
field.The numerous automatically measured points were given into a PDP-10 digital computer to calculate according to Kouvel [4] with a parabolic extrapola- tion process [3] the temperature dependence of the spontaneous magnetization
soand the reciprocal initial susceptibility 1 / ~ , . In fig. 3 there are plotted the square of spontaneous magnetization and the reciprocal initial susceptibility versus temperature.
The temperature dependence of both quantities is not linear in the whole temperature range.
Fra. 1.
- Specific magnetization of Fe, Co and Ni plotted
vs RG. 3.- Square
ofspontaneous magnetization and reciprocal temperature with external field as a parameter initial susceptibility vs temperature.
Article published online by EDP Sciences and available at http://dx.doi.org/10.1051/jphyscol:19711225
MAGNETOCALORIC EFFECT AND CRITICAL PHENOMENA O F IRON, COBALT AND NICKEL C 1
-
653A log-log plot of a. vs
E =I 1 - TITc I respecti- vely of 1/x0 vs
Eshown in fig. 4 allows the deter-
FIG.
5. -Log-log plot of magnetization vs internal field and magnetocaloric effect vs magnetization at
Te.FIG. 4.
- Log-log plot of spontaneous magnetization and reciprocal initial susceptibility vs
E =I
1 - TITc[.mination of the exponents p and
y.There is no uni- form value for p and y in the whole investigated tem- perature range. Fig. 5 shows the log-log plot of the magnetization a t Tc vs internal field and of the magne- tocaloric effect vs magnetization to determine the critical indices 6 and
n.In the table there are given the exact values of the determined exponents P, y, 6 and n and the ranges of their validity. The mean deviation of these values is about
f3 %. Moreover the values for 6 and
acal- culated with the scaling laws
6
=1 + y/Pand
n
=2 + (y - 1)/p (according to Wohlfarth
[ 5 ] )by using the experimental values for and
yare noticed in parenthesis. The agreement between the calculated and the experimental values for 6 and n is not very satisfactory.
To conclude there is to remark that the exact behaviour of a ferromagnetic transition metal at the critical point seems to be more complicated than it was first assumed. Here is the behaviour near T, not exactly to be described by the scaling laws.
Acknowledgements.
-We thank Prof. Arajs for sending us the preprint [2].
Experimental values of the exponents
P, y, 6
andn
and range of validity.In
parenthesis : values for6
anda
calculated b y using the scaling laws and the experimental values forP
andy .
Range
~ = 4x ...
& = 4 x... H i = 1 ... 25 kOe Tc
8
x...
4 x6
x... 4 x lo-'
Exponent 0 Y 6
n OKReferences
[I]