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<metadata xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xmlns:dc="http://purl.org/dc/elements/1.1/"><dc:title>Electrocaloric cooling</dc:title><dc:creator>Plaznik,	Uroš	(Avtor)
	</dc:creator><dc:creator>Vrabelj,	Marko	(Avtor)
	</dc:creator><dc:creator>Kutnjak,	Zdravko	(Avtor)
	</dc:creator><dc:creator>Malič,	Barbara	(Avtor)
	</dc:creator><dc:creator>Poredoš,	Alojz	(Avtor)
	</dc:creator><dc:creator>Kitanovski,	Andrej	(Avtor)
	</dc:creator><dc:subject>heat regeneration</dc:subject><dc:subject>electrocaloric cooling</dc:subject><dc:subject>electric-energy recovery</dc:subject><dc:subject>energy analysis</dc:subject><dc:description>Here we explore the effect of electric-energy recovery and heat regeneration on the energy efficiency of an electrocaloric-cooling system. Furthermore, the influence of the polarizationelectric field hysteresis on the energy efficiency of the system is analysed. For the purposes of the analysis, the properties of (1 % x)Pb(Mg1/3Nb2/3)O3-xPbTiO3 (PMN-100xPT) with x = 0, x = 0.1, and x = 0.35 are characterized. We show that if no heat is regenerated, even small irreversibilities in the electric circuit used to recover the electric energy can cause a significant drop in the achievable energy efficiency. On the other hand, when a heat regeneration process is considered and a realistic value for the degree of electric-energy recovery equal to 80% is assumed, the limit for the energy efficiency of a system employing PMN ceramics is estimated to be equal to 81% of the efficiency of a Carnot heat pump.</dc:description><dc:date>2015</dc:date><dc:date>2021-04-20 22:26:27</dc:date><dc:type>Članek v reviji</dc:type><dc:identifier>126396</dc:identifier><dc:identifier>UDK: 621.5:620.9(045)</dc:identifier><dc:identifier>ISSN pri članku: 0295-5075</dc:identifier><dc:identifier>DOI: 10.1209/0295-5075/111/57009</dc:identifier><dc:identifier>COBISS_ID: 14221083</dc:identifier><dc:language>sl</dc:language></metadata>
