Concept of a Magnetocaloric Generator with Latent Heat Transfer for the Conversion of Heat into Electricity
Second‐order and first‐order magnetocaloric materials (MCMs) not experiencing hysteresis are characterized by a reversible temperature change when exposed to an applied magnetic field. Due to this property described by the magnetocaloric effect, MCMs are used in magnetic cooling applications. Conver...
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Veröffentlicht in: | Energy technology (Weinheim, Germany) Germany), 2022-03, Vol.10 (3), p.n/a |
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Sprache: | eng |
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Zusammenfassung: | Second‐order and first‐order magnetocaloric materials (MCMs) not experiencing hysteresis are characterized by a reversible temperature change when exposed to an applied magnetic field. Due to this property described by the magnetocaloric effect, MCMs are used in magnetic cooling applications. Conversely, a rapid variation of the MCM's temperature around its specific Curie temperature causes a fast change in its magnetic permeability. Cycling the MCM's temperature within a magnetic field allows the possibility of inducing voltage, which would be higher for rapid cycling rates. Herein, latent heat transfer is introduced as an approach to obtain higher heating/cooling cycle frequency in a magnetocaloric generator that converts heat to electricity. In practice, rapid condensation/evaporation cycles of the water on a first‐order magnetocaloric La(Fe,Si) alloy are observed in a high vacuum system. This leads to the fast change of magnetization in an applied magnetic field from which an induced voltage is picked up. With the constructed set‐up, a peak induced voltage 2.75 mVp is obtained from low‐grade heat having reservoir temperature differences of △T = 56 °C. At higher temperature differences, a peak‐to‐peak voltage of around 3.5 mVpp at a cycle frequency of 2 Hz is achieved.
The thermomagnetic generator, herein, makes use of latent heat transfer from the working fluid to heat up and cool down a magnetocaloric material (MCM) around its Curie temperature. High temperature cycling frequencies that result in the more rapid change of magnetization lead to an induced peak‐to‐peak voltage of 3.5 mVpp at a cycle frequency of 2 Hz. |
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ISSN: | 2194-4288 2194-4296 |
DOI: | 10.1002/ente.202100891 |