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<Gradivo ID="147390" NadgradivoID="1257" NRID="19469792" OceID="0" DomainUrl="https://repozitorij.uni-lj.si/" IzpisPolniUrl="https://repozitorij.uni-lj.si/IzpisGradiva.php?lang=slv&amp;id=147390" StOgledov="1428" StPrenosov="391" StOcen="0" VsotaOcen="0" DatumIzvoza="2026-08-09 05:16:53" OcenaSkupna="0" StPodgradiv="0" StudijskiProgramEvsID="" JeIndeksirano="0" JeVecAvtorjev="0" DovoliZahtevkeZaDostop="0">
  <PID Url="http://hdl.handle.net/20.500.12556/RUL-147390">20.500.12556/RUL-147390</PID>
  <Naslov>Parametric analysis of fatigue-resistant elastocaloric regenerators</Naslov>
  <Podnaslov>tensile vs. compressive loading</Podnaslov>
  <TujJezik_Naslov></TujJezik_Naslov>
  <TujJezik_Podnaslov></TujJezik_Podnaslov>
  <Opis>Elastocaloric cooling has recently shown high potential as an environmentally friendly alternative to vapor-compression technology. Here, we have studied and analyzed the geometric characteristics of two active elastocaloric regenerators (AeCRs) that were proved to have high application potential, i.e., a shell-and-tube AeCR loaded in compression and a parallel-plate AeCR loaded in tension, with the goal of maximizing their cooling performance. For this purpose, a previously developed and experimentally verified 1D numerical model was used. We focused only on the geometries and operating conditions that allow for durable, i.e., buckling-free operation in compression and fatigue-resistant operation in tension. The results show that although the applied strain of the parallel-plate AeCR loaded in tension needs to be limited (below 2%) to ensure fatigue-resistant operation, it outperforms (in terms of cooling power and COP at 15 K of temperature span) the shell-and-tube AeCR, which due to buckling issues suffers from a poorer heat-transfer geometry, but can withstand higher strains due to compressive loading. At the maximum strain of 2%, the optimum parallel-plate AeCR can generate a maximum cooling power of 1825 W (corresponding to 7075 W kg$^{−1}$ of elastocaloric material) and a COP of 9.15 at a zero-temperature span. On the other hand, due to a higher applied strain (3%) the optimum shell-and-tube AeCR can generate a higher maximum temperature span at zero cooling power (up to 50 K) but has limited cooling performance at lower temperature spans. In addition, the layering of the shell-and-tube AeCR was investigated for the first time to improve its performance. This study shows the crucial impact of the heat-transfer geometry (heat-transfer area and hydraulic diameter), which needs to be further improved in compression-loaded AeCRs to improve their efficiencies (without compromising the buckling stability). The study also shows the importance of the applied strain, which needs to be at least 2% or more to achieve a high cooling performance of the AeCR. The obtained results should serve as guidelines for designing powerful and efficient AeCRs in the future.</Opis>
  <TujJezik_Opis></TujJezik_Opis>
  <KljucneBesede>
    <Beseda>elastocaloric effect</Beseda>
    <Beseda>caloric cooling</Beseda>
    <Beseda>Ni-Ti</Beseda>
    <Beseda>regenerators</Beseda>
    <Beseda>parametric analysis</Beseda>
  </KljucneBesede>
  <TujJezik_KljucneBesede>
    <Beseda>elastokalorični učinek</Beseda>
    <Beseda>kalorično hlajenje</Beseda>
    <Beseda>Ni-Ti</Beseda>
    <Beseda>regeneratorji</Beseda>
    <Beseda>parametrična analiza</Beseda>
  </TujJezik_KljucneBesede>
  <Potrjeno>true</Potrjeno>
  <JeZaklenjeno>false</JeZaklenjeno>
  <JeRecenzirano>true</JeRecenzirano>
  <Zaloznik></Zaloznik>
  <Izvor></Izvor>
  <Jezik ID="1033" ISO639-3="eng">Angleški jezik</Jezik>
  <TujJezik ID="1060" ISO639-3="slv">Slovenski jezik</TujJezik>
  <Povezave></Povezave>
  <Pokrivanje></Pokrivanje>
  <CasovnoPokritje></CasovnoPokritje>
  <AvtorskePravice></AvtorskePravice>
  <VrstaGradiva ID="dk_c" DRIVER="info:eu-repo/semantics/article">Članek v reviji</VrstaGradiva>
  <DatumVstavljanja>2023-07-04 11:29:07</DatumVstavljanja>
  <DatumObjave>2023-07-04 11:29:13</DatumObjave>
  <DatumSpremembe>2024-02-04 03:56:04</DatumSpremembe>
  <DatumTrajnegaHranjenja>0000-00-00 00:00:00</DatumTrajnegaHranjenja>
  <LetoIzida>2023</LetoIzida>
  <LetoIzidaDo>0</LetoIzidaDo>
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  <LetoIzvedbe>0</LetoIzvedbe>
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  <Opomba></Opomba>
  <StStrani>13 str.</StStrani>
  <StevilcenjeNivo1>Vol. 231, art. 120996</StevilcenjeNivo1>
  <StevilcenjeNivo2></StevilcenjeNivo2>
  <Kronologija>Aug. 2023</Kronologija>
  <Patent_Stevilka></Patent_Stevilka>
  <Patent_DatumVeljavnosti>0000-00-00</Patent_DatumVeljavnosti>
  <VerzijaDokumenta>Zaloznikova</VerzijaDokumenta>
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  <Identifikatorji>
    <Identifikator ID="4" Sifra="UDK" Naziv="UDK" URL="">519.876.5:621.57</Identifikator>
    <Identifikator ID="9" Sifra="ISSN-clanka" Naziv="ISSN pri članku" URL="">1359-4311</Identifikator>
    <Identifikator ID="15" Sifra="DOI" Naziv="DOI" URL="http://dx.doi.org/10.1016/j.applthermaleng.2023.120996">10.1016/j.applthermaleng.2023.120996</Identifikator>
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