Metal Matrix-Metal Nanoparticle Composites with Tunable Melting Temperature and High Thermal Conductivity for Phase-Change Thermal Storage
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作者:
Liu, Minglu
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Arizona State Univ, Dept Mech Engn, Tempe, AZ 85287 USAArizona State Univ, Dept Mech Engn, Tempe, AZ 85287 USA
Liu, Minglu
[1
]
Ma, Yuanyu
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Arizona State Univ, Dept Mat Sci & Engn, Tempe, AZ 85287 USAArizona State Univ, Dept Mech Engn, Tempe, AZ 85287 USA
Ma, Yuanyu
[2
]
Wu, Hsinwei
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Arizona State Univ, Dept Mat Sci & Engn, Tempe, AZ 85287 USAArizona State Univ, Dept Mech Engn, Tempe, AZ 85287 USA
Wu, Hsinwei
[2
]
Wang, Robert Y.
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Arizona State Univ, Dept Mech Engn, Tempe, AZ 85287 USA
Arizona State Univ, Dept Mat Sci & Engn, Tempe, AZ 85287 USAArizona State Univ, Dept Mech Engn, Tempe, AZ 85287 USA
Wang, Robert Y.
[1
,2
]
机构:
[1] Arizona State Univ, Dept Mech Engn, Tempe, AZ 85287 USA
[2] Arizona State Univ, Dept Mat Sci & Engn, Tempe, AZ 85287 USA
Phase-change materials (PCMs) are of broad interest for thermal storage and management applications. For energy-dense storage with fast thermal charging/discharging rates, a PCM should have a suitable melting temperature, large enthalpy of fusion, and high thermal conductivity. To simultaneously accomplish these traits, we custom design nanocomposites consisting of phase-change Bi nanoparticles embedded in an Ag matrix. We precisely control nanoparticle size, shape, and volume fraction in the composite by separating the nanoparticle synthesis and nanocomposite formation steps. We demonstrate a 50100% thermal energy density improvement relative to common organic PCMs with equivalent volume fraction. We also tune the melting temperature from 236252 degrees C by varying nanoparticle diameter from 8.114.9 nm. Importantly, the silver matrix successfully prevents nanoparticle coalescence, and no melting changes are observed during 100 meltfreeze cycles. The nanocomposites Ag matrix also leads to very high thermal conductivities. For example, the thermal conductivity of a composite with a 10% volume fraction of 13 nm Bi nanoparticles is 128 +/- 23 W/m-K, which is several orders of magnitude higher than typical thermal storage materials. We complement these measurements with calculations using a modified effective medium approximation for nanoscale thermal transport. These calculations predict that the thermal conductivity of composites with 13 nm Bi nanoparticles varies from 142 to 47 W/m-K as the nanoparticle volume fraction changes from 10 to 35%. Larger nanoparticle diameters and/or smaller nanoparticle volume fractions lead to larger thermal conductivities.
机构:
Rensselaer Polytech Inst, Dept Mat Sci & Engn, Troy, NY 12180 USACUNY City Coll, Dept Chem, New York, NY 10031 USA
Kumar, Ashavani
Vemula, Praveen Kumar
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CUNY City Coll, Dept Chem, New York, NY 10031 USA
CUNY Grad Sch & Univ Ctr, New York, NY 10031 USACUNY City Coll, Dept Chem, New York, NY 10031 USA
Vemula, Praveen Kumar
Ajayan, Pulickel M.
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CUNY Grad Sch & Univ Ctr, New York, NY 10031 USA
Rensselaer Polytech Inst, Dept Mat Sci & Engn, Troy, NY 12180 USACUNY City Coll, Dept Chem, New York, NY 10031 USA
Ajayan, Pulickel M.
John, George
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CUNY City Coll, Dept Chem, New York, NY 10031 USACUNY City Coll, Dept Chem, New York, NY 10031 USA
机构:
Rensselaer Polytech Inst, Dept Mat Sci & Engn, Troy, NY 12180 USACUNY City Coll, Dept Chem, New York, NY 10031 USA
Kumar, Ashavani
Vemula, Praveen Kumar
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机构:
CUNY City Coll, Dept Chem, New York, NY 10031 USA
CUNY Grad Sch & Univ Ctr, New York, NY 10031 USACUNY City Coll, Dept Chem, New York, NY 10031 USA
Vemula, Praveen Kumar
Ajayan, Pulickel M.
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机构:
CUNY Grad Sch & Univ Ctr, New York, NY 10031 USA
Rensselaer Polytech Inst, Dept Mat Sci & Engn, Troy, NY 12180 USACUNY City Coll, Dept Chem, New York, NY 10031 USA
Ajayan, Pulickel M.
John, George
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CUNY City Coll, Dept Chem, New York, NY 10031 USACUNY City Coll, Dept Chem, New York, NY 10031 USA