A Class of Reduced-Order Regenerator Models
We present a novel class of reduced-order regenerator models that is based on Endoreversible Thermodynamics. The models rest upon the idea of an internally reversible (perfect) regenerator, even though they are not limited to the reversible description. In these models, the temperatures of the worki...
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2021
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oai:doaj.org-article:c7e846df09e8435cb46cbe145459f9f42021-11-11T16:02:14ZA Class of Reduced-Order Regenerator Models10.3390/en142172951996-1073https://doaj.org/article/c7e846df09e8435cb46cbe145459f9f42021-11-01T00:00:00Zhttps://www.mdpi.com/1996-1073/14/21/7295https://doaj.org/toc/1996-1073We present a novel class of reduced-order regenerator models that is based on Endoreversible Thermodynamics. The models rest upon the idea of an internally reversible (perfect) regenerator, even though they are not limited to the reversible description. In these models, the temperatures of the working gas that alternately streams out on the regenerator’s hot and cold sides are defined as functions of the state of the regenerator matrix. The matrix is assumed to feature a linear spatial temperature distribution. Thus, the matrix has only two degrees of freedom that can, for example, be identified with its energy and entropy content. The dynamics of the regenerator is correspondingly expressed in terms of balance equations for energy and entropy. Internal irreversibilities of the regenerator can be accounted for by introducing source terms to the entropy balance equation. Compared to continuum or nodal regenerator models, the number of degrees of freedom and numerical effort are reduced considerably. As will be shown, instead of the obvious choice of variables energy and entropy, if convenient, a different pair of variables can be used to specify the state of the regenerator matrix and formulate the regenerator’s dynamics. In total, we will discuss three variants of this endoreversible regenerator model, which we will refer to as <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mi mathvariant="italic">ES</mi></semantics></math></inline-formula>, <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mi mathvariant="italic">EE</mi></semantics></math></inline-formula>, and <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mi mathvariant="italic">EEn</mi></semantics></math></inline-formula>-regenerator models.Raphael PaulKarl Heinz HoffmannMDPI AGarticleregeneratornumerical modelendoreversible thermodynamicsstirlingvuilleumierirreversibilityTechnologyTENEnergies, Vol 14, Iss 7295, p 7295 (2021) |
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regenerator numerical model endoreversible thermodynamics stirling vuilleumier irreversibility Technology T |
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regenerator numerical model endoreversible thermodynamics stirling vuilleumier irreversibility Technology T Raphael Paul Karl Heinz Hoffmann A Class of Reduced-Order Regenerator Models |
description |
We present a novel class of reduced-order regenerator models that is based on Endoreversible Thermodynamics. The models rest upon the idea of an internally reversible (perfect) regenerator, even though they are not limited to the reversible description. In these models, the temperatures of the working gas that alternately streams out on the regenerator’s hot and cold sides are defined as functions of the state of the regenerator matrix. The matrix is assumed to feature a linear spatial temperature distribution. Thus, the matrix has only two degrees of freedom that can, for example, be identified with its energy and entropy content. The dynamics of the regenerator is correspondingly expressed in terms of balance equations for energy and entropy. Internal irreversibilities of the regenerator can be accounted for by introducing source terms to the entropy balance equation. Compared to continuum or nodal regenerator models, the number of degrees of freedom and numerical effort are reduced considerably. As will be shown, instead of the obvious choice of variables energy and entropy, if convenient, a different pair of variables can be used to specify the state of the regenerator matrix and formulate the regenerator’s dynamics. In total, we will discuss three variants of this endoreversible regenerator model, which we will refer to as <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mi mathvariant="italic">ES</mi></semantics></math></inline-formula>, <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mi mathvariant="italic">EE</mi></semantics></math></inline-formula>, and <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mi mathvariant="italic">EEn</mi></semantics></math></inline-formula>-regenerator models. |
format |
article |
author |
Raphael Paul Karl Heinz Hoffmann |
author_facet |
Raphael Paul Karl Heinz Hoffmann |
author_sort |
Raphael Paul |
title |
A Class of Reduced-Order Regenerator Models |
title_short |
A Class of Reduced-Order Regenerator Models |
title_full |
A Class of Reduced-Order Regenerator Models |
title_fullStr |
A Class of Reduced-Order Regenerator Models |
title_full_unstemmed |
A Class of Reduced-Order Regenerator Models |
title_sort |
class of reduced-order regenerator models |
publisher |
MDPI AG |
publishDate |
2021 |
url |
https://doaj.org/article/c7e846df09e8435cb46cbe145459f9f4 |
work_keys_str_mv |
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1718432438882926592 |