In this work the energy transfer in a one-dimensional harmonic crystal is investigated. In particular, a comparison between the discrete approach presented by Klein, Prigogine, and Hemmer with the continuum approach presented by Krivtsov is made. In the pioneering work of Klein and Prigogine the transfer of thermal energy is considered. In particular, an expression is obtained, which allows to calculate the thermal energy of each particle as a function of time. Later, Hemmer derived and used similar expressions to solve several particular problems in context of heat conduction. In the work of Krivtsov-in contrast to the discrete approach-a partial differential continuum equation is derived from the lattice dynamics of a 1D harmonic crystal. This so-called ballistic heat equation describes the propagation of heat at a finite speed in a continuous one-dimensional medium. The current work compares analyses based on the discrete equation of Klein, Prigogine, and Hemmer with those from the continuum-PDE-based one by Krivtsov. There is an important difference between the approaches. The continuum approach is derived from the dynamics of the crystal lattice, in which only kinetic degrees of freedom were excited and then thermal equilibration occurred. In contrast to that we consider in the discrete approach explicitly given equal kinetic and potential initial energies. Several exactly solvable initial problems are studied by using both methods. The problem of point perturbation shows a discrepancy in the results obtained in the framework of the continuous and discrete approaches. It is caused by the fact that the smoothness conditions of the initial perturbation is violated for the continuum approach. For other problems it is shown that at large spatial scales, where the one-dimensional crystal can be considered as a continuous medium, the discrete and the continuum relations converge. The asymptotic behavior of the difference between two aforementioned approaches is analyzed. (C) 2021 Elsevier Ltd. All rights reserved.
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Sungkyunkwan Univ, Dept Energy Sci, Suwon 16419, South KoreaSungkyunkwan Univ, Dept Energy Sci, Suwon 16419, South Korea
Yi, Hojoon
Bahng, Jaeuk
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Sungkyunkwan Univ, Dept Smart Fab Technol, Suwon 16419, South KoreaSungkyunkwan Univ, Dept Energy Sci, Suwon 16419, South Korea
Bahng, Jaeuk
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Park, Sehwan
Dang, Dang Xuan
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Sungkyunkwan Univ, Dept Energy Sci, Suwon 16419, South KoreaSungkyunkwan Univ, Dept Energy Sci, Suwon 16419, South Korea
Dang, Dang Xuan
Sakong, Wonkil
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Sungkyunkwan Univ, Dept Energy Sci, Suwon 16419, South Korea
Sungkyunkwan Univ, Ctr Integrated Nanostruct Phys, Inst Basic Sci, Suwon 16419, South KoreaSungkyunkwan Univ, Dept Energy Sci, Suwon 16419, South Korea
Sakong, Wonkil
Kang, Seungsu
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Sungkyunkwan Univ, Dept Energy Sci, Suwon 16419, South KoreaSungkyunkwan Univ, Dept Energy Sci, Suwon 16419, South Korea
Kang, Seungsu
Ahn, Byung-wook
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Sungkyunkwan Univ, Dept Energy Sci, Suwon 16419, South Korea
Sungkyunkwan Univ, Ctr Integrated Nanostruct Phys, Inst Basic Sci, Suwon 16419, South KoreaSungkyunkwan Univ, Dept Energy Sci, Suwon 16419, South Korea
Ahn, Byung-wook
Kim, Jungwon
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Korea Inst Sci & Technol, Inst Adv Composite Mat, Seoul 55324, South KoreaSungkyunkwan Univ, Dept Energy Sci, Suwon 16419, South Korea
Kim, Jungwon
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Kim, Ki Kang
Lim, Jong Tae
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Elect & Telecommun Res Inst, Real Devices Res Div, Daejeon 34129, South KoreaSungkyunkwan Univ, Dept Energy Sci, Suwon 16419, South Korea
Lim, Jong Tae
Lim, Seong Chu
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Sungkyunkwan Univ, Dept Energy Sci, Suwon 16419, South Korea
Sungkyunkwan Univ, Dept Smart Fab Technol, Suwon 16419, South KoreaSungkyunkwan Univ, Dept Energy Sci, Suwon 16419, South Korea
机构:
Univ Calif Santa Barbara, Calif NanoSyst Inst, Santa Barbara, CA 93106 USAUniv Calif Santa Barbara, Calif NanoSyst Inst, Santa Barbara, CA 93106 USA
Xu, Shuozhi
Chen, Xiang
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Univ Florida, Dept Mech & Aerosp Engn, Gainesville, FL USAUniv Calif Santa Barbara, Calif NanoSyst Inst, Santa Barbara, CA 93106 USA
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Equipo de Propulsion Espacial y Plasmas (EP2),Universidad Carlos Ⅲ de MadridSchool of Mechanical Engineering and Automation,Harbin Institute of Technology
Mario MERINO
万杰
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Laboratory for Space Environment and Physical Sciences,Harbin Institute of TechnologySchool of Mechanical Engineering and Automation,Harbin Institute of Technology
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Harbin Inst Technol, Sch Mech Engn & Automation, Shenzhen 518055, Peoples R ChinaHarbin Inst Technol, Sch Mech Engn & Automation, Shenzhen 518055, Peoples R China
Tian, Bin
Merino, Mario
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Univ Carlos III Madrid, Equipo Prop Espacial & Plasmas EP2, Leganes 28911, SpainHarbin Inst Technol, Sch Mech Engn & Automation, Shenzhen 518055, Peoples R China
Merino, Mario
Wan, Jie
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Harbin Inst Technol, Lab Space Environm & Phys Sci, Harbin, Peoples R ChinaHarbin Inst Technol, Sch Mech Engn & Automation, Shenzhen 518055, Peoples R China
Wan, Jie
Hu, Yuan
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Chinese Acad Sci, Inst Mech, State Key Lab High Temp Gas Dynam, Beijing 100190, Peoples R ChinaHarbin Inst Technol, Sch Mech Engn & Automation, Shenzhen 518055, Peoples R China
Hu, Yuan
Cao, Yong
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Harbin Inst Technol, Sch Mech Engn & Automation, Shenzhen 518055, Peoples R ChinaHarbin Inst Technol, Sch Mech Engn & Automation, Shenzhen 518055, Peoples R China
机构:
Equipo de Propulsion Espacial y Plasmas (EP),Universidad Carlos Ⅲ de MadridSchool of Mechanical Engineering and Automation,Harbin Institute of Technology
Mario MERINO
万杰
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Laboratory for Space Environment and Physical Sciences,Harbin Institute of TechnologySchool of Mechanical Engineering and Automation,Harbin Institute of Technology
万杰
胡远
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机构:
State Key Laboratory of High Temperature Gas Dynamics,Institute of Mechanics,Chinese Academy ofSchool of Mechanical Engineering and Automation,Harbin Institute of Technology