{"title":"纯氧化镁和掺杂氧化镁在环己烷中的浸没热。微孔效应","authors":"R. Mikhail, S. Nashed, A. Khalil","doi":"10.1039/DF9715200187","DOIUrl":null,"url":null,"abstract":"Heats of immersion of pure and doped magnesia in cyclohexane were measured at 35°C for samples heated at different temperatures in vacuo. For the pure samples, rise in temperature of thermal treatment leads to a gradual decrease in the heats of immersion normalized per unit area (h1, ergs cm–2), till a certain limiting value of 44.5 ergs cm–2 is reached. Pore structure analyses lead to certain correlations between the heat of immersion and the fraction of the total surface located in micropores. Pores which could effectively play a role in altering the heat of immersion were assessed to possess a mean hydraulic radius of 10 A or less. Doping on the surface leads to the same behaviour, except that the decline in the heat of immersion is followed by an increase in the hi values for the high temperature samples heated at or above 560°C. For the doped samples, formation of a solid solution between Li+ and Mg2+, and a spinel between Al3+ and Mg2+ complicates the results obtained.","PeriodicalId":11262,"journal":{"name":"Discussions of The Faraday Society","volume":"45 1","pages":"187-195"},"PeriodicalIF":0.0000,"publicationDate":"1971-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"17","resultStr":"{\"title\":\"Heats of immersion of pure and doped magnesia in cyclohexane. Effects of micropores\",\"authors\":\"R. Mikhail, S. Nashed, A. Khalil\",\"doi\":\"10.1039/DF9715200187\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Heats of immersion of pure and doped magnesia in cyclohexane were measured at 35°C for samples heated at different temperatures in vacuo. For the pure samples, rise in temperature of thermal treatment leads to a gradual decrease in the heats of immersion normalized per unit area (h1, ergs cm–2), till a certain limiting value of 44.5 ergs cm–2 is reached. Pore structure analyses lead to certain correlations between the heat of immersion and the fraction of the total surface located in micropores. Pores which could effectively play a role in altering the heat of immersion were assessed to possess a mean hydraulic radius of 10 A or less. Doping on the surface leads to the same behaviour, except that the decline in the heat of immersion is followed by an increase in the hi values for the high temperature samples heated at or above 560°C. For the doped samples, formation of a solid solution between Li+ and Mg2+, and a spinel between Al3+ and Mg2+ complicates the results obtained.\",\"PeriodicalId\":11262,\"journal\":{\"name\":\"Discussions of The Faraday Society\",\"volume\":\"45 1\",\"pages\":\"187-195\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"1971-01-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"17\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Discussions of The Faraday Society\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1039/DF9715200187\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Discussions of The Faraday Society","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1039/DF9715200187","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Heats of immersion of pure and doped magnesia in cyclohexane. Effects of micropores
Heats of immersion of pure and doped magnesia in cyclohexane were measured at 35°C for samples heated at different temperatures in vacuo. For the pure samples, rise in temperature of thermal treatment leads to a gradual decrease in the heats of immersion normalized per unit area (h1, ergs cm–2), till a certain limiting value of 44.5 ergs cm–2 is reached. Pore structure analyses lead to certain correlations between the heat of immersion and the fraction of the total surface located in micropores. Pores which could effectively play a role in altering the heat of immersion were assessed to possess a mean hydraulic radius of 10 A or less. Doping on the surface leads to the same behaviour, except that the decline in the heat of immersion is followed by an increase in the hi values for the high temperature samples heated at or above 560°C. For the doped samples, formation of a solid solution between Li+ and Mg2+, and a spinel between Al3+ and Mg2+ complicates the results obtained.