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Fig. 6.23 a Manipulation of
the ferrofluid drop by a
uniform magnetic eld,
b Manipulation of the
ferrofluid drop by a
nonuniform magnetic eld
6.4.3 Magnetohydrodynamics
Magnetohydrodynamics (MHD) represents the interaction of an electric and a
magnetic
uids (e.g. plasma, electrolytes, liquid
metals, etc.). This results in a Lorentz force on the
eld with electrically conducting
fl
fl
uid, and as a consequence, the
fl
ow (Fig. 6.24 ). With respect to magnetic refrigeration, the most interesting
applications represent the use of liquid metals, such as Hg, NaK and liquid metal
alloys based on Ga and In. The MHD principle can be also applied for the liquid
metal bi-directional
uid
fl
ow, which is common in active magnetic regenerators
(AMRs). Therefore, it could also serve for the principle shown in Fig. 6.22 .
In this case we place the electrodes over the two regions of the AMRs
(Fig. 6.25 ). Instead of a ferro
fl
uid, a liquid metal will be applied as the working
fluid. In the case of Fig. 6.25 a, one pair of AMRs is being magnetized. Since the
magnetic
fl
eld is applied to this region, the electrodes are switched ON and
therefore propel the liquid metal from the magnetized AMR to the HHEX. Since the
Fig. 6.24 Example of the MHD
fl
uid
fl
ow induced by an electric and magnetic eld
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