J. Delgado, Joana C. Martinho, Ana Vaz Sá, A. S. Guimarães, Vítor Abrantes
{"title":"Conclusions","authors":"J. Delgado, Joana C. Martinho, Ana Vaz Sá, A. S. Guimarães, Vítor Abrantes","doi":"10.1007/978-3-319-97499-6_4","DOIUrl":"https://doi.org/10.1007/978-3-319-97499-6_4","url":null,"abstract":"","PeriodicalId":224320,"journal":{"name":"Thermal Energy Storage with Phase Change Materials","volume":"85 1","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"2018-08-10","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"132966094","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
J. Delgado, Joana C. Martinho, A. Sá, A. S. Guimarães, V. Abrantes
{"title":"Impregnation of PCMs in Building Materials","authors":"J. Delgado, Joana C. Martinho, A. Sá, A. S. Guimarães, V. Abrantes","doi":"10.1007/978-3-319-97499-6_2","DOIUrl":"https://doi.org/10.1007/978-3-319-97499-6_2","url":null,"abstract":"","PeriodicalId":224320,"journal":{"name":"Thermal Energy Storage with Phase Change Materials","volume":"98 1","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"2018-08-10","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"125566397","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
J. Delgado, Joana C. Martinho, A. Sá, A. S. Guimarães, V. Abrantes
{"title":"PCM Current Applications and Thermal Performance","authors":"J. Delgado, Joana C. Martinho, A. Sá, A. S. Guimarães, V. Abrantes","doi":"10.1007/978-3-319-97499-6_3","DOIUrl":"https://doi.org/10.1007/978-3-319-97499-6_3","url":null,"abstract":"","PeriodicalId":224320,"journal":{"name":"Thermal Energy Storage with Phase Change Materials","volume":"101 1","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"2018-08-10","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"123207945","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
{"title":"Impact of Energy Storage in Buildings on Electricity Demand Side Management","authors":"W. Qureshi, N. Nair, Mohammed M. Farid","doi":"10.1016/J.ENCONMAN.2010.12.008","DOIUrl":"https://doi.org/10.1016/J.ENCONMAN.2010.12.008","url":null,"abstract":"","PeriodicalId":224320,"journal":{"name":"Thermal Energy Storage with Phase Change Materials","volume":"1 1","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"2011-05-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"125867467","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
{"title":"The Role of Natural Convection during Melting and Solidification of PCM in a Vertical Cylinder","authors":"M. Farid, Yongsik Kim, T. Honda, A. Kanzawa","doi":"10.1080/00986448908940334","DOIUrl":"https://doi.org/10.1080/00986448908940334","url":null,"abstract":"Abstract Measurements of heat transfer during melting and solidfkation of n-eicosane and rt-hexadecane were performed in vertical cylinders with two different lengths and diameters. Radial temperature distibutions were measured with lime at different heights in all the tests. To evaluate the rate of heat charged and discharged from the cylinder at different heights, the data were recorded and processed directly usinj; on-line computer. A theoretical model was developed based on solving the one-dimensional unsteady heat conduction equation in both phases. Convection in the liquid was included using an effective thermal conductivity; a lumped parameter that includes also the effect of the two-dimensional heat transfer during melting. The model, which may be used for the prediction of both melting and solidfkation experiments, takes into account the effect of initial subcooling or superheating and includes the heat capacity of the cylinder containing the PCM. The agreement of the model was good not only with...","PeriodicalId":224320,"journal":{"name":"Thermal Energy Storage with Phase Change Materials","volume":"49 1","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"1989-10-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"116456960","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
{"title":"Effect of Natural Convection on the Process of Melting and Solidification of Paraffin Wax","authors":"M. Farid, A. Mohamed","doi":"10.1080/00986448708960492","DOIUrl":"https://doi.org/10.1080/00986448708960492","url":null,"abstract":"Abstract Temperature distribution and solid-liquid interface positions were measured during melting and solidification of paraffin wax (mixture of pentacosane and hexacosane) contained in a cylindrical cell, with an insulated wall to achieve one dimensional heat flow. The lower face of the cell was subjected to a sudden temperature change, while the condition of no heat flux was maintained at the upper face. Measurements of temperature distribution and interface positions during solidification from below were in excellent agreement with theoretical predictions based on pure conduction in both phases. Both the analytical solution of Neumann and the numerical solution of Murray and Landis were applied and found to have similar results. Although the experimental results of melting from below showed distinct temperature distribution in both phases, the agreement with the theoretical estimates based on pure conduction was very poor. In order to include the effect of convection, liquid thermal conductivity was ...","PeriodicalId":224320,"journal":{"name":"Thermal Energy Storage with Phase Change Materials","volume":"45 1","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"1987-07-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"132855674","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}