{"title":"真空热管太阳能集热器","authors":"F. Mahdjuri","doi":"10.1016/0013-7480(79)90004-4","DOIUrl":null,"url":null,"abstract":"<div><p>A tubular evacuated solar collector with rectangular performance characteristics is introduced. The heat transfer from the absorber plate with selective coating to the water tubing occurs via a heat pipe system. In order to avoid any delay in the operation of the heat pipe due to superheating of the vapour, we have introduced a trap mechanism for the condensed liquid. To avoid the disadvantage of the high no-load condition of the vacuum collectors we have used the physical features of the critical point of the heat pipe working fluid.</p><p>Above the critical temperature, <em>T</em><sub><em>c</em></sub> of the working fluid the condensation effect will disappear. This means that above <em>T</em><sub><em>c</em></sub> the heat transfer property of a heat pipe will vanish. This will cause only a slight increase of the condenser temperature above <em>T</em><sub><em>c</em></sub> of the liquid used. For our heat pipe system we have chosen working liquids with critical temperature between 95–115°C.</p></div>","PeriodicalId":100466,"journal":{"name":"Energy Conversion","volume":"19 2","pages":"Pages 85-90"},"PeriodicalIF":0.0000,"publicationDate":"1979-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/0013-7480(79)90004-4","citationCount":"14","resultStr":"{\"title\":\"Evacuated heat pipe solar collector\",\"authors\":\"F. Mahdjuri\",\"doi\":\"10.1016/0013-7480(79)90004-4\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<div><p>A tubular evacuated solar collector with rectangular performance characteristics is introduced. The heat transfer from the absorber plate with selective coating to the water tubing occurs via a heat pipe system. In order to avoid any delay in the operation of the heat pipe due to superheating of the vapour, we have introduced a trap mechanism for the condensed liquid. To avoid the disadvantage of the high no-load condition of the vacuum collectors we have used the physical features of the critical point of the heat pipe working fluid.</p><p>Above the critical temperature, <em>T</em><sub><em>c</em></sub> of the working fluid the condensation effect will disappear. This means that above <em>T</em><sub><em>c</em></sub> the heat transfer property of a heat pipe will vanish. This will cause only a slight increase of the condenser temperature above <em>T</em><sub><em>c</em></sub> of the liquid used. For our heat pipe system we have chosen working liquids with critical temperature between 95–115°C.</p></div>\",\"PeriodicalId\":100466,\"journal\":{\"name\":\"Energy Conversion\",\"volume\":\"19 2\",\"pages\":\"Pages 85-90\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"1979-01-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"https://sci-hub-pdf.com/10.1016/0013-7480(79)90004-4\",\"citationCount\":\"14\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Energy Conversion\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://www.sciencedirect.com/science/article/pii/0013748079900044\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Energy Conversion","FirstCategoryId":"1085","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/0013748079900044","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
A tubular evacuated solar collector with rectangular performance characteristics is introduced. The heat transfer from the absorber plate with selective coating to the water tubing occurs via a heat pipe system. In order to avoid any delay in the operation of the heat pipe due to superheating of the vapour, we have introduced a trap mechanism for the condensed liquid. To avoid the disadvantage of the high no-load condition of the vacuum collectors we have used the physical features of the critical point of the heat pipe working fluid.
Above the critical temperature, Tc of the working fluid the condensation effect will disappear. This means that above Tc the heat transfer property of a heat pipe will vanish. This will cause only a slight increase of the condenser temperature above Tc of the liquid used. For our heat pipe system we have chosen working liquids with critical temperature between 95–115°C.