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Record W2805310589 · doi:10.11159/ffhmt18.189

Optimal Control of a Stirling Engine

2018· article· en· W2805310589 on OpenAlexvenueno aff
Karsten Schwalbe, Abdellah Khodja, Mathias Scheunert, Karl Heinz Hoffmann

Bibliographic record

VenueProceedings of the ... International Conference on Fluid Flow, Heat and Mass Transfer · 2018
Typearticle
Languageen
FieldEngineering
TopicAdvanced Thermodynamic Systems and Engines
Canadian institutionsnot available
Fundersnot available
KeywordsStirling engineStirling cycleComputer scienceControl (management)Environmental scienceEngineeringMechanical engineeringArtificial intelligence

Abstract

fetched live from OpenAlex

Many industrial engines, like machine tools for example, produce a lot of waste heat during operation.To reduce energy costs, this heat can be recuperated using an appropriate heat engine.The Stirling engine is such a heat engine as it can make use of the external heat source and produce usable mechanical power.Although the Stirling engine can theoretically reach the Carnot efficiency in the reversible limit, in reality effects like irreversible heat and mass transfer as well as friction losses lower its performance significantly.Therefore, thermodynamic models are needed to estimate the performance of real Stirling engines.In this study an endoreversible model of the Stirling engine is presented.In Endoreversible Thermodynamics [1] all irreversibilities are restricted to interactions between reversibly working subsystems.The model of the Stirling engine consists of two gas chambers with pistons and a regenerator in between.The gas chambers are in contact with an external heat source and a heat sink for cooling, respectively.The pistons can be moved freely and independent from each other with the help of linear motors.The investigated system can be described using, among others, the ideal gas assumption, the Newtonian heat transport law, a simplified mass transfer law, and friction losses proportional to the squared rotation speed.The needed transport coefficients are derived using experimental data.On the basis of this model the optimal trajectory of the engine's pistons is calculated using Pontryagin's maximum principle.This leads to an ordinary differential equation system with mixed start and final conditions for which a special solution method has to be used to ensure convergence.It is found that the optimized paths differ significantly from the conventional harmonic paths.While the latter show a sinusoidal behaviour, the former exhibit a relatively long isochoric phase.As a result, the power output is much larger than in case of a conventional piston movement.For the considered engine parameters the power output nearly doubles.Additionally, the influence of the time period of the cyclic piston motion on the performance of the engine is investigated.We find that there is a local maximum of the power output for a certain time period depending on the engine parameters.Consequently, there exists an optimal time period for the Stirling engine that should be used for operation.Investigating the influence of the friction coefficient on the power output, it turns out that the power output decreases monotonously with an increasing friction coefficient.Furthermore it follows from the numerical data that the decrease of the power is relatively large for small friction coefficients, so that it is very crucial to lower the friction losses of a high performing Stirling engine as much as possible.Finally, some possible modifications for the Stirling engine model are discussed.Here, Endoreversible Thermodynamics shows one of its greatest benefits: A high degree of adaptability while the model equations remain manageable.

Fetched live from OpenAlex and de-inverted. Abstracts are not stored in this database: the inverted indexes are 8.6 GB of the frame’s 9.3 GB of text, and the host has 13 GB free.

How this classification was reachedexpand

Full frame machine prediction

Teacher imitation

Not calibrated prevalence, not ground truth. Human validation pending. The Gemma side is a direct model label for every work in the frame, read from the title-only record. The Codex side is a classifier learned from the 10,348 direct Codex labels and calibrated to design-weighted sample rates; fields without enough sample support carry no Codex call. Candidate is the union of the two sides; consensus is their intersection. These outputs are machine_predicted_unvalidated and are not human labels.

metaresearch head score (Codex)0.001
metaresearch head score (Gemma)0.001
Version: metacan-v3-hybrid-931329e0061cValidation status: machine_predicted_unvalidated
Candidate categoriesnone
Consensus categoriesnone
DomainCandidate signal: none · Consensus signal: none
Study designCandidate signal: Simulation or modeling · Consensus signal: Simulation or modeling
GenreCandidate signal: Empirical · Consensus signal: none
Teacher disagreement score0.013
Threshold uncertainty score0.026

Distilled classifier scores by category (both heads)

CategoryCodexGemma
Metaresearch0.0010.001
Meta-epidemiology (narrow)0.0010.001
Meta-epidemiology (broad)0.0010.001
Bibliometrics0.0010.000
Science and technology studies0.0010.001
Scholarly communication0.0020.001
Open science0.0010.001
Research integrity0.0010.001
Insufficient payload (model declined to judge)0.0040.001

Machine scores (provisional)

The two teacher heads of the student model, read on this work. A score orders the frame for review; it never asserts a category, and the validation status ships verbatim with every row.

Baseline scores from an immature model (maturity gate not passed, 7 training rounds). Scores rank; they never assert a category.

Opus teacher head0.011
GPT teacher head0.212
Teacher spread0.201 · how far apart the two teachers sit on this one work
Validation statusscore_only:v0-immature-baseline · verbatim from the scoring run: score_only means the number may rank works, and no category label ships from it

Classification

machine, unvalidated

Machine predicted; a candidate call from one source (direct Gemma or distilled Codex), not a consensus.

The models applied no category: nothing in the taxonomy fit this work.
Study designSimulation or modeling
Domainnot available
GenreEmpirical

How this classification was reached, model by model and score by score, is at the end of the page under "How this classification was reached".

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Citations0
Published2018
Admission routes1
Has abstractyes

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