학술논문

Investigation of Ferrofluid Cooling for High Power Density Permanent Magnet Machines
Document Type
Periodical
Source
IEEE Transactions on Magnetics IEEE Trans. Magn. Magnetics, IEEE Transactions on. 59(1):1-11 Jan, 2023
Subject
Fields, Waves and Electromagnetics
Ferrofluid
Cooling
Force
Windings
Rotors
Magnetic separation
Magnetohydrodynamics
Ferrofluid (FF) cooling
magnetic body force
nanofluid (NF)
permanent magnet (PM) machines
thermomagnetic convection
Language
ISSN
0018-9464
1941-0069
Abstract
This article investigates an advanced thermal management method adopting ferrofluid (FF) for improving the end-winding cooling of permanent magnet (PM) machines. An oil-based liquid with nano-sized ferromagnetic particles (which is known as FF) is used to fill in the cavity around the end windings. This is to establish an effective heat flux path between the end winding that is often regarded as hot spot in electrical machines and the external cooling system, i.e., water jacket, to improve the cooling performance of the PM machines. This improvement does not only result from the higher thermal conductivity and thermal expansion of the nanofluid with metal particles but also from strong thermomagnetic convection generated by the magnetic body force of the ferromagnetic particles within the FF. Multiphysics models considering the interaction between the electromagnetic field, the heat transfer, and the fluid dynamics have been built to study the thermal performances of a PM machine under different load conditions. Several factors affecting the thermomagnetic convection, such as the temperature-dependent magnetization curve of the FF, the concentration, and different ferromagnetic materials as well as different current densities, have been investigated to analyze their influences on cooling performance. One major finding is that, compared with other coolant without magnetic body force, the FF can significantly reduce machine peak temperature, e.g., by around ${36.4}~^{\circ }\text{C}$ when the current density is $\boldsymbol {22.1}~\text {A} / {\text {mm}}^{ \boldsymbol {2}}$ .