Optimizing Power and Thermal Efficiency of an Irreversible Variable-Temperature Heat Reservoir Lenoir Cycle
Applying finite-time thermodynamics theory, an irreversible steady flow Lenoir cycle model with variable-temperature heat reservoirs is established, the expressions of power (<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semanti...
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2021-08-01
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Online Access: | https://www.mdpi.com/2076-3417/11/15/7171 |
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DOAJ |
language |
English |
format |
Article |
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DOAJ |
author |
Ruibo Wang Lingen Chen Yanlin Ge Huijun Feng |
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Ruibo Wang Lingen Chen Yanlin Ge Huijun Feng Optimizing Power and Thermal Efficiency of an Irreversible Variable-Temperature Heat Reservoir Lenoir Cycle Applied Sciences finite-time thermodynamics irreversible steady-flow Lenoir cycle cycle power thermal efficiency heat conductance distribution thermal capacity rate matching |
author_facet |
Ruibo Wang Lingen Chen Yanlin Ge Huijun Feng |
author_sort |
Ruibo Wang |
title |
Optimizing Power and Thermal Efficiency of an Irreversible Variable-Temperature Heat Reservoir Lenoir Cycle |
title_short |
Optimizing Power and Thermal Efficiency of an Irreversible Variable-Temperature Heat Reservoir Lenoir Cycle |
title_full |
Optimizing Power and Thermal Efficiency of an Irreversible Variable-Temperature Heat Reservoir Lenoir Cycle |
title_fullStr |
Optimizing Power and Thermal Efficiency of an Irreversible Variable-Temperature Heat Reservoir Lenoir Cycle |
title_full_unstemmed |
Optimizing Power and Thermal Efficiency of an Irreversible Variable-Temperature Heat Reservoir Lenoir Cycle |
title_sort |
optimizing power and thermal efficiency of an irreversible variable-temperature heat reservoir lenoir cycle |
publisher |
MDPI AG |
series |
Applied Sciences |
issn |
2076-3417 |
publishDate |
2021-08-01 |
description |
Applying finite-time thermodynamics theory, an irreversible steady flow Lenoir cycle model with variable-temperature heat reservoirs is established, the expressions of power (<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mi>P</mi></semantics></math></inline-formula>) and efficiency (<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mi>η</mi></semantics></math></inline-formula>) are derived. By numerical calculations, the characteristic relationships among <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mi>P</mi></semantics></math></inline-formula> and <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mi>η</mi></semantics></math></inline-formula> and the heat conductance distribution (<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mi>u</mi><mi>L</mi></msub></mrow></semantics></math></inline-formula>) of the heat exchangers, as well as the thermal capacity rate matching (<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mi>C</mi><mrow><mi>w</mi><mi>f</mi><mn>1</mn></mrow></msub><mo>/</mo><msub><mi>C</mi><mi>H</mi></msub></mrow></semantics></math></inline-formula>) between working fluid and heat source are studied. The results show that when the heat conductances of the hot- and cold-side heat exchangers (<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mi>U</mi><mi>H</mi></msub></mrow></semantics></math></inline-formula>, <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mi>U</mi><mi>L</mi></msub></mrow></semantics></math></inline-formula>) are constants, <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><mi>P</mi><mtext>-</mtext><mi>η</mi></mrow></semantics></math></inline-formula> is a certain “point”, with the increase of heat reservoir inlet temperature ratio (<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mi>τ</mi></semantics></math></inline-formula>), <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mi>U</mi><mi>H</mi></msub></mrow></semantics></math></inline-formula>, <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mi>U</mi><mi>L</mi></msub></mrow></semantics></math></inline-formula>, and the irreversible expansion efficiency (<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mi>η</mi><mi>e</mi></msub></mrow></semantics></math></inline-formula>), <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mi>P</mi></semantics></math></inline-formula> and <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mi>η</mi></semantics></math></inline-formula> increase. When <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mi>u</mi><mi>L</mi></msub></mrow></semantics></math></inline-formula> can be optimized, <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mi>P</mi></semantics></math></inline-formula> and <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mi>η</mi></semantics></math></inline-formula> versus <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mi>u</mi><mi>L</mi></msub></mrow></semantics></math></inline-formula> characteristics are parabolic-like ones, there are optimal values of heat conductance distributions (<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mi>u</mi><mrow><msub><mi>L</mi><mi>P</mi></msub><mo stretchy="false">(</mo><mi>o</mi><mi>p</mi><mi>t</mi><mo stretchy="false">)</mo></mrow></msub></mrow></semantics></math></inline-formula>, <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mi>u</mi><mrow><msub><mi>L</mi><mi>η</mi></msub><mo stretchy="false">(</mo><mi>o</mi><mi>p</mi><mi>t</mi><mo stretchy="false">)</mo></mrow></msub></mrow></semantics></math></inline-formula>) to make the cycle reach the maximum power and efficiency points (<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mi>P</mi><mrow><mi>max</mi></mrow></msub></mrow></semantics></math></inline-formula>, <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mi>η</mi><mrow><mi>max</mi></mrow></msub></mrow></semantics></math></inline-formula>). As <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mi>C</mi><mrow><mi>w</mi><mi>f</mi><mn>1</mn></mrow></msub><mo>/</mo><msub><mi>C</mi><mi>H</mi></msub></mrow></semantics></math></inline-formula> increases, <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mi>P</mi><mrow><mi>max</mi></mrow></msub><mtext>-</mtext><msub><mi>C</mi><mrow><mi>w</mi><mi>f</mi><mn>1</mn></mrow></msub><mo>/</mo><msub><mi>C</mi><mi>H</mi></msub></mrow></semantics></math></inline-formula> shows a parabolic-like curve, that is, there is an optimal value of <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mi>C</mi><mrow><mi>w</mi><mi>f</mi><mn>1</mn></mrow></msub><mo>/</mo><msub><mi>C</mi><mi>H</mi></msub></mrow></semantics></math></inline-formula> (<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mrow><mo stretchy="false">(</mo><msub><mi>C</mi><mrow><mi>w</mi><mi>f</mi><mn>1</mn></mrow></msub><mo>/</mo><msub><mi>C</mi><mi>H</mi></msub><mo stretchy="false">)</mo></mrow><mrow><mi>o</mi><mi>p</mi><mi>t</mi></mrow></msub></mrow></semantics></math></inline-formula>) to make the cycle reach double-maximum power point (<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mrow><mo stretchy="false">(</mo><msub><mi>P</mi><mrow><mi>max</mi></mrow></msub><mo stretchy="false">)</mo></mrow><mrow><mi>max</mi></mrow></msub></mrow></semantics></math></inline-formula>); as <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mi>C</mi><mi>L</mi></msub><mo>/</mo><msub><mi>C</mi><mi>H</mi></msub></mrow></semantics></math></inline-formula>, <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mi>U</mi><mi>T</mi></msub></mrow></semantics></math></inline-formula>, and <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mi>η</mi><mi>e</mi></msub></mrow></semantics></math></inline-formula> increase, <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mrow><mo stretchy="false">(</mo><msub><mi>P</mi><mrow><mi>max</mi></mrow></msub><mo stretchy="false">)</mo></mrow><mrow><mi>max</mi></mrow></msub></mrow></semantics></math></inline-formula> and <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mrow><mo stretchy="false">(</mo><msub><mi>C</mi><mrow><mi>w</mi><mi>f</mi><mn>1</mn></mrow></msub><mo>/</mo><msub><mi>C</mi><mi>H</mi></msub><mo stretchy="false">)</mo></mrow><mrow><mi>o</mi><mi>p</mi><mi>t</mi></mrow></msub></mrow></semantics></math></inline-formula> increase; with the increase in <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mi>τ</mi></semantics></math></inline-formula>, <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mrow><mo stretchy="false">(</mo><msub><mi>P</mi><mrow><mi>max</mi></mrow></msub><mo stretchy="false">)</mo></mrow><mrow><mi>max</mi></mrow></msub></mrow></semantics></math></inline-formula> increases, and <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mrow><mo stretchy="false">(</mo><msub><mi>C</mi><mrow><mi>w</mi><mi>f</mi><mn>1</mn></mrow></msub><mo>/</mo><msub><mi>C</mi><mi>H</mi></msub><mo stretchy="false">)</mo></mrow><mrow><mi>o</mi><mi>p</mi><mi>t</mi></mrow></msub></mrow></semantics></math></inline-formula> is unchanged. |
topic |
finite-time thermodynamics irreversible steady-flow Lenoir cycle cycle power thermal efficiency heat conductance distribution thermal capacity rate matching |
url |
https://www.mdpi.com/2076-3417/11/15/7171 |
work_keys_str_mv |
AT ruibowang optimizingpowerandthermalefficiencyofanirreversiblevariabletemperatureheatreservoirlenoircycle AT lingenchen optimizingpowerandthermalefficiencyofanirreversiblevariabletemperatureheatreservoirlenoircycle AT yanlinge optimizingpowerandthermalefficiencyofanirreversiblevariabletemperatureheatreservoirlenoircycle AT huijunfeng optimizingpowerandthermalefficiencyofanirreversiblevariabletemperatureheatreservoirlenoircycle |
_version_ |
1721218810578468864 |
spelling |
doaj-5ec0c9014f7a4b33bc6f1059961f4fb32021-08-06T15:19:59ZengMDPI AGApplied Sciences2076-34172021-08-01117171717110.3390/app11157171Optimizing Power and Thermal Efficiency of an Irreversible Variable-Temperature Heat Reservoir Lenoir CycleRuibo Wang0Lingen Chen1Yanlin Ge2Huijun Feng3Institute of Thermal Science and Power Engineering, Wuhan Institute of Technology, Wuhan 430205, ChinaInstitute of Thermal Science and Power Engineering, Wuhan Institute of Technology, Wuhan 430205, ChinaInstitute of Thermal Science and Power Engineering, Wuhan Institute of Technology, Wuhan 430205, ChinaInstitute of Thermal Science and Power Engineering, Wuhan Institute of Technology, Wuhan 430205, ChinaApplying finite-time thermodynamics theory, an irreversible steady flow Lenoir cycle model with variable-temperature heat reservoirs is established, the expressions of power (<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mi>P</mi></semantics></math></inline-formula>) and efficiency (<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mi>η</mi></semantics></math></inline-formula>) are derived. By numerical calculations, the characteristic relationships among <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mi>P</mi></semantics></math></inline-formula> and <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mi>η</mi></semantics></math></inline-formula> and the heat conductance distribution (<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mi>u</mi><mi>L</mi></msub></mrow></semantics></math></inline-formula>) of the heat exchangers, as well as the thermal capacity rate matching (<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mi>C</mi><mrow><mi>w</mi><mi>f</mi><mn>1</mn></mrow></msub><mo>/</mo><msub><mi>C</mi><mi>H</mi></msub></mrow></semantics></math></inline-formula>) between working fluid and heat source are studied. The results show that when the heat conductances of the hot- and cold-side heat exchangers (<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mi>U</mi><mi>H</mi></msub></mrow></semantics></math></inline-formula>, <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mi>U</mi><mi>L</mi></msub></mrow></semantics></math></inline-formula>) are constants, <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><mi>P</mi><mtext>-</mtext><mi>η</mi></mrow></semantics></math></inline-formula> is a certain “point”, with the increase of heat reservoir inlet temperature ratio (<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mi>τ</mi></semantics></math></inline-formula>), <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mi>U</mi><mi>H</mi></msub></mrow></semantics></math></inline-formula>, <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mi>U</mi><mi>L</mi></msub></mrow></semantics></math></inline-formula>, and the irreversible expansion efficiency (<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mi>η</mi><mi>e</mi></msub></mrow></semantics></math></inline-formula>), <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mi>P</mi></semantics></math></inline-formula> and <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mi>η</mi></semantics></math></inline-formula> increase. When <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mi>u</mi><mi>L</mi></msub></mrow></semantics></math></inline-formula> can be optimized, <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mi>P</mi></semantics></math></inline-formula> and <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mi>η</mi></semantics></math></inline-formula> versus <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mi>u</mi><mi>L</mi></msub></mrow></semantics></math></inline-formula> characteristics are parabolic-like ones, there are optimal values of heat conductance distributions (<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mi>u</mi><mrow><msub><mi>L</mi><mi>P</mi></msub><mo stretchy="false">(</mo><mi>o</mi><mi>p</mi><mi>t</mi><mo stretchy="false">)</mo></mrow></msub></mrow></semantics></math></inline-formula>, <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mi>u</mi><mrow><msub><mi>L</mi><mi>η</mi></msub><mo stretchy="false">(</mo><mi>o</mi><mi>p</mi><mi>t</mi><mo stretchy="false">)</mo></mrow></msub></mrow></semantics></math></inline-formula>) to make the cycle reach the maximum power and efficiency points (<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mi>P</mi><mrow><mi>max</mi></mrow></msub></mrow></semantics></math></inline-formula>, <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mi>η</mi><mrow><mi>max</mi></mrow></msub></mrow></semantics></math></inline-formula>). As <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mi>C</mi><mrow><mi>w</mi><mi>f</mi><mn>1</mn></mrow></msub><mo>/</mo><msub><mi>C</mi><mi>H</mi></msub></mrow></semantics></math></inline-formula> increases, <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mi>P</mi><mrow><mi>max</mi></mrow></msub><mtext>-</mtext><msub><mi>C</mi><mrow><mi>w</mi><mi>f</mi><mn>1</mn></mrow></msub><mo>/</mo><msub><mi>C</mi><mi>H</mi></msub></mrow></semantics></math></inline-formula> shows a parabolic-like curve, that is, there is an optimal value of <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mi>C</mi><mrow><mi>w</mi><mi>f</mi><mn>1</mn></mrow></msub><mo>/</mo><msub><mi>C</mi><mi>H</mi></msub></mrow></semantics></math></inline-formula> (<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mrow><mo stretchy="false">(</mo><msub><mi>C</mi><mrow><mi>w</mi><mi>f</mi><mn>1</mn></mrow></msub><mo>/</mo><msub><mi>C</mi><mi>H</mi></msub><mo stretchy="false">)</mo></mrow><mrow><mi>o</mi><mi>p</mi><mi>t</mi></mrow></msub></mrow></semantics></math></inline-formula>) to make the cycle reach double-maximum power point (<inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mrow><mo stretchy="false">(</mo><msub><mi>P</mi><mrow><mi>max</mi></mrow></msub><mo stretchy="false">)</mo></mrow><mrow><mi>max</mi></mrow></msub></mrow></semantics></math></inline-formula>); as <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mi>C</mi><mi>L</mi></msub><mo>/</mo><msub><mi>C</mi><mi>H</mi></msub></mrow></semantics></math></inline-formula>, <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mi>U</mi><mi>T</mi></msub></mrow></semantics></math></inline-formula>, and <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mi>η</mi><mi>e</mi></msub></mrow></semantics></math></inline-formula> increase, <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mrow><mo stretchy="false">(</mo><msub><mi>P</mi><mrow><mi>max</mi></mrow></msub><mo stretchy="false">)</mo></mrow><mrow><mi>max</mi></mrow></msub></mrow></semantics></math></inline-formula> and <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mrow><mo stretchy="false">(</mo><msub><mi>C</mi><mrow><mi>w</mi><mi>f</mi><mn>1</mn></mrow></msub><mo>/</mo><msub><mi>C</mi><mi>H</mi></msub><mo stretchy="false">)</mo></mrow><mrow><mi>o</mi><mi>p</mi><mi>t</mi></mrow></msub></mrow></semantics></math></inline-formula> increase; with the increase in <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mi>τ</mi></semantics></math></inline-formula>, <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mrow><mo stretchy="false">(</mo><msub><mi>P</mi><mrow><mi>max</mi></mrow></msub><mo stretchy="false">)</mo></mrow><mrow><mi>max</mi></mrow></msub></mrow></semantics></math></inline-formula> increases, and <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mrow><mo stretchy="false">(</mo><msub><mi>C</mi><mrow><mi>w</mi><mi>f</mi><mn>1</mn></mrow></msub><mo>/</mo><msub><mi>C</mi><mi>H</mi></msub><mo stretchy="false">)</mo></mrow><mrow><mi>o</mi><mi>p</mi><mi>t</mi></mrow></msub></mrow></semantics></math></inline-formula> is unchanged.https://www.mdpi.com/2076-3417/11/15/7171finite-time thermodynamicsirreversible steady-flow Lenoir cyclecycle powerthermal efficiencyheat conductance distributionthermal capacity rate matching |