Moritz Faden , Andreas König-Haagen , Dieter Brüggemann
{"title":"立方体空腔熔化的不确定性和敏感性综合分析,B 部分:综合分析","authors":"Moritz Faden , Andreas König-Haagen , Dieter Brüggemann","doi":"10.1016/j.ijthermalsci.2024.109506","DOIUrl":null,"url":null,"abstract":"<div><div>Latent heat thermal energy storage systems are an attractive way to store thermal energy nearly isothermally. Nowadays, numerical methods are increasingly employed for their design. However, the results obtained with these methods are accompanied by a high degree of uncertainty, which results in leeway in the validation of the models. This leeway leads to seemingly perfectly validated numerical models, although they often contain strong simplifications and the input parameters have large uncertainties. To shed more light on this contradiction, we perform a combined uncertainty and sensitivity analysis of a classical validation problem — a paraffin melting from one side in a cuboid. The input parameters of the combined uncertainty and sensitivity analysis are the thermophysical properties of the phase change material (PCM) and the boundary and initial conditions of the experiment. We show that the uncertainty of the liquid fraction after <span><math><mrow><mtext>2</mtext><mspace></mspace><mtext>h</mtext></mrow></math></span> is around <span><math><mrow><mo>±</mo><mtext>7</mtext><mspace></mspace><mtext>%</mtext></mrow></math></span> if the thermophysical properties are implemented correctly. This is significantly lower than what would be expected considering the large variation of thermophysical property values found in the literature. The thermal conductivity of the solid, the melting point, and the solid density are the input parameters with the greatest influence on the global liquid fraction. Therefore, these parameters should be measured with higher accuracy to further improve the accuracy of the simulation. In addition to the liquid fraction, the heat flux flowing through the hot and cold sides of the simulation domain and the maximum velocity in the fluid phase are also considered targets of the combined uncertainty and sensitivity analysis. Here we see that the heat flux of the cold side is the target variable with the greatest uncertainty. Interestingly, for one time instance, the same liquid fraction and an almost identical phase front can be achieved with very different input variables, highlighting the importance of using several target variables for the validation.</div></div>","PeriodicalId":341,"journal":{"name":"International Journal of Thermal Sciences","volume":"209 ","pages":"Article 109506"},"PeriodicalIF":4.9000,"publicationDate":"2024-11-10","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"A combined uncertainty and sensitivity analysis of melting in a cubical cavity, Part B: Combined analysis\",\"authors\":\"Moritz Faden , Andreas König-Haagen , Dieter Brüggemann\",\"doi\":\"10.1016/j.ijthermalsci.2024.109506\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<div><div>Latent heat thermal energy storage systems are an attractive way to store thermal energy nearly isothermally. Nowadays, numerical methods are increasingly employed for their design. However, the results obtained with these methods are accompanied by a high degree of uncertainty, which results in leeway in the validation of the models. This leeway leads to seemingly perfectly validated numerical models, although they often contain strong simplifications and the input parameters have large uncertainties. To shed more light on this contradiction, we perform a combined uncertainty and sensitivity analysis of a classical validation problem — a paraffin melting from one side in a cuboid. The input parameters of the combined uncertainty and sensitivity analysis are the thermophysical properties of the phase change material (PCM) and the boundary and initial conditions of the experiment. We show that the uncertainty of the liquid fraction after <span><math><mrow><mtext>2</mtext><mspace></mspace><mtext>h</mtext></mrow></math></span> is around <span><math><mrow><mo>±</mo><mtext>7</mtext><mspace></mspace><mtext>%</mtext></mrow></math></span> if the thermophysical properties are implemented correctly. This is significantly lower than what would be expected considering the large variation of thermophysical property values found in the literature. The thermal conductivity of the solid, the melting point, and the solid density are the input parameters with the greatest influence on the global liquid fraction. Therefore, these parameters should be measured with higher accuracy to further improve the accuracy of the simulation. In addition to the liquid fraction, the heat flux flowing through the hot and cold sides of the simulation domain and the maximum velocity in the fluid phase are also considered targets of the combined uncertainty and sensitivity analysis. Here we see that the heat flux of the cold side is the target variable with the greatest uncertainty. Interestingly, for one time instance, the same liquid fraction and an almost identical phase front can be achieved with very different input variables, highlighting the importance of using several target variables for the validation.</div></div>\",\"PeriodicalId\":341,\"journal\":{\"name\":\"International Journal of Thermal Sciences\",\"volume\":\"209 \",\"pages\":\"Article 109506\"},\"PeriodicalIF\":4.9000,\"publicationDate\":\"2024-11-10\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"International Journal of Thermal Sciences\",\"FirstCategoryId\":\"5\",\"ListUrlMain\":\"https://www.sciencedirect.com/science/article/pii/S1290072924006288\",\"RegionNum\":2,\"RegionCategory\":\"工程技术\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q1\",\"JCRName\":\"ENGINEERING, MECHANICAL\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"International Journal of Thermal Sciences","FirstCategoryId":"5","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/S1290072924006288","RegionNum":2,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q1","JCRName":"ENGINEERING, MECHANICAL","Score":null,"Total":0}
A combined uncertainty and sensitivity analysis of melting in a cubical cavity, Part B: Combined analysis
Latent heat thermal energy storage systems are an attractive way to store thermal energy nearly isothermally. Nowadays, numerical methods are increasingly employed for their design. However, the results obtained with these methods are accompanied by a high degree of uncertainty, which results in leeway in the validation of the models. This leeway leads to seemingly perfectly validated numerical models, although they often contain strong simplifications and the input parameters have large uncertainties. To shed more light on this contradiction, we perform a combined uncertainty and sensitivity analysis of a classical validation problem — a paraffin melting from one side in a cuboid. The input parameters of the combined uncertainty and sensitivity analysis are the thermophysical properties of the phase change material (PCM) and the boundary and initial conditions of the experiment. We show that the uncertainty of the liquid fraction after is around if the thermophysical properties are implemented correctly. This is significantly lower than what would be expected considering the large variation of thermophysical property values found in the literature. The thermal conductivity of the solid, the melting point, and the solid density are the input parameters with the greatest influence on the global liquid fraction. Therefore, these parameters should be measured with higher accuracy to further improve the accuracy of the simulation. In addition to the liquid fraction, the heat flux flowing through the hot and cold sides of the simulation domain and the maximum velocity in the fluid phase are also considered targets of the combined uncertainty and sensitivity analysis. Here we see that the heat flux of the cold side is the target variable with the greatest uncertainty. Interestingly, for one time instance, the same liquid fraction and an almost identical phase front can be achieved with very different input variables, highlighting the importance of using several target variables for the validation.
期刊介绍:
The International Journal of Thermal Sciences is a journal devoted to the publication of fundamental studies on the physics of transfer processes in general, with an emphasis on thermal aspects and also applied research on various processes, energy systems and the environment. Articles are published in English and French, and are subject to peer review.
The fundamental subjects considered within the scope of the journal are:
* Heat and relevant mass transfer at all scales (nano, micro and macro) and in all types of material (heterogeneous, composites, biological,...) and fluid flow
* Forced, natural or mixed convection in reactive or non-reactive media
* Single or multi–phase fluid flow with or without phase change
* Near–and far–field radiative heat transfer
* Combined modes of heat transfer in complex systems (for example, plasmas, biological, geological,...)
* Multiscale modelling
The applied research topics include:
* Heat exchangers, heat pipes, cooling processes
* Transport phenomena taking place in industrial processes (chemical, food and agricultural, metallurgical, space and aeronautical, automobile industries)
* Nano–and micro–technology for energy, space, biosystems and devices
* Heat transport analysis in advanced systems
* Impact of energy–related processes on environment, and emerging energy systems
The study of thermophysical properties of materials and fluids, thermal measurement techniques, inverse methods, and the developments of experimental methods are within the scope of the International Journal of Thermal Sciences which also covers the modelling, and numerical methods applied to thermal transfer.