TY - JOUR
T1 - Direct measurements of the magnetic entropy change
AU - Nielsen, Kaspar Kirstein
AU - Neves Bez, Henrique
AU - von Moos, Lars
AU - Bjørk, Rasmus
AU - Eriksen, Dan
AU - Bahl, Christian
PY - 2015
Y1 - 2015
N2 - An experimental device that can accurately measure the magnetic entropy change, Δs, as a function
of temperature, T, and magnetic field, H, is presented. The magnetic field source is in this case
a set of counter-rotating concentric Halbach-type magnets, which produce a highly homogeneous
applied field with constant orientation. The field may be varied from 0 to 1.5 T in a continuous
way. The temperature stability of the system is controlled to within ±10 mK and the standard
range for the current setup is from 230 K to 330 K. The device is under high vacuum and we
show that thermal losses to the ambient are negligible in terms of the calorimetric determination
of the magnetic entropy change, while the losses cannot be ignored when correcting for the actual
sample temperature. We apply the device to two different types of samples; one is commercial grade
Gd, i.e., a pure second-order phase transition material, while the other is Gd5Si2Ge2, a first order
magnetic phase transition material. We demonstrate the device’s ability to fully capture the thermal
hysteresis of the latter sample by following appropriate thermal resetting scheme and magnetic
resetting scheme. © 2015 AIP Publishing LLC.
AB - An experimental device that can accurately measure the magnetic entropy change, Δs, as a function
of temperature, T, and magnetic field, H, is presented. The magnetic field source is in this case
a set of counter-rotating concentric Halbach-type magnets, which produce a highly homogeneous
applied field with constant orientation. The field may be varied from 0 to 1.5 T in a continuous
way. The temperature stability of the system is controlled to within ±10 mK and the standard
range for the current setup is from 230 K to 330 K. The device is under high vacuum and we
show that thermal losses to the ambient are negligible in terms of the calorimetric determination
of the magnetic entropy change, while the losses cannot be ignored when correcting for the actual
sample temperature. We apply the device to two different types of samples; one is commercial grade
Gd, i.e., a pure second-order phase transition material, while the other is Gd5Si2Ge2, a first order
magnetic phase transition material. We demonstrate the device’s ability to fully capture the thermal
hysteresis of the latter sample by following appropriate thermal resetting scheme and magnetic
resetting scheme. © 2015 AIP Publishing LLC.
U2 - 10.1063/1.4932308
DO - 10.1063/1.4932308
M3 - Journal article
C2 - 26520967
SN - 0034-6748
VL - 86
JO - Review of Scientific Instruments
JF - Review of Scientific Instruments
IS - 10
M1 - 103903
ER -