TY - JOUR
T1 - Irreversible performance of a quantum harmonic heat engine
AU - Rezek, Yair
AU - Kosloff, Ronnie
PY - 2006/5/31
Y1 - 2006/5/31
N2 - The unavoidable irreversible loss of power in a heat engine is found to be of quantum origin. Following thermodynamic tradition, a model quantum heat engine operating in an Otto cycle is analysed, where the working medium is composed of an ensemble of harmonic oscillators and changes in volume correspond to changes in the curvature of the potential well. Equations of motion for quantum observables are derived for the complete cycle of operation. These observables are sufficient to determine the state of the system and with it all thermodynamical variables. Once the external controls are set, the engine settles to a limit cycle. Conditions for optimal work, power and entropy production are derived. At high temperatures and quasistatic operating conditions, the efficiency at maximum power coincides with the endoreversible result ηq = 1 - √ Tc/Th. The optimal compression ratio varies from C = √ Th/Tc in the quasistatic limit where the irreversibility is dominated by heat conductance to C = (Th/Tc)1/4 in the sudden limit when the irreversibility is dominated by friction. When the engine deviates from adiabatic conditions, the performance is subject to friction. The origin of this friction can be traced to the noncommutability of the kinetic and potential energy of the working medium.
AB - The unavoidable irreversible loss of power in a heat engine is found to be of quantum origin. Following thermodynamic tradition, a model quantum heat engine operating in an Otto cycle is analysed, where the working medium is composed of an ensemble of harmonic oscillators and changes in volume correspond to changes in the curvature of the potential well. Equations of motion for quantum observables are derived for the complete cycle of operation. These observables are sufficient to determine the state of the system and with it all thermodynamical variables. Once the external controls are set, the engine settles to a limit cycle. Conditions for optimal work, power and entropy production are derived. At high temperatures and quasistatic operating conditions, the efficiency at maximum power coincides with the endoreversible result ηq = 1 - √ Tc/Th. The optimal compression ratio varies from C = √ Th/Tc in the quasistatic limit where the irreversibility is dominated by heat conductance to C = (Th/Tc)1/4 in the sudden limit when the irreversibility is dominated by friction. When the engine deviates from adiabatic conditions, the performance is subject to friction. The origin of this friction can be traced to the noncommutability of the kinetic and potential energy of the working medium.
UR - http://www.scopus.com/inward/record.url?scp=33744771952&partnerID=8YFLogxK
U2 - 10.1088/1367-2630/8/5/083
DO - 10.1088/1367-2630/8/5/083
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AN - SCOPUS:33744771952
SN - 1367-2630
VL - 8
JO - New Journal of Physics
JF - New Journal of Physics
M1 - 83
ER -