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    Heat, Mass, and Fluid Flow in a Solar Reactor for Fullerene Synthesis

    Source: Journal of Solar Energy Engineering:;2001:;volume( 123 ):;issue: 002::page 153
    Author:
    T. Guillard
    ,
    D. Laplaze
    ,
    G. Flamant
    DOI: 10.1115/1.1352736
    Publisher: The American Society of Mechanical Engineers (ASME)
    Abstract: Experimental results with a 2 kW solar furnace, in a wide range of vaporization rates (0.1–4 g/h), under variable pressure and flow rate of argon, are used with numerical simulation to define key parameters for large scale synthesis of fullerenes with solar energy. The vaporization process is controlled by diffusion in the temperature and pressure ranges 3000-3700 K and 70-250 hPa respectively. In the solar reactor, fullerene yield is governed by the dilution of carbon vapor in argon and the temperature gradient in the cooling zone. Criteria for both parameters are suggested. Consequently, these data, combined with a validated numerical model of the reactor, may be used for the design of large-scale solar process.
    keyword(s): Temperature , Carbon , Solar energy , Fullerenes , Graphite , Pressure , Vapors AND Flow (Dynamics) ,
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      Heat, Mass, and Fluid Flow in a Solar Reactor for Fullerene Synthesis

    URI
    http://yetl.yabesh.ir/yetl1/handle/yetl/125849
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    contributor authorT. Guillard
    contributor authorD. Laplaze
    contributor authorG. Flamant
    date accessioned2017-05-09T00:05:57Z
    date available2017-05-09T00:05:57Z
    date copyrightMay, 2001
    date issued2001
    identifier issn0199-6231
    identifier otherJSEEDO-28300#153_1.pdf
    identifier urihttp://yetl.yabesh.ir/yetl/handle/yetl/125849
    description abstractExperimental results with a 2 kW solar furnace, in a wide range of vaporization rates (0.1–4 g/h), under variable pressure and flow rate of argon, are used with numerical simulation to define key parameters for large scale synthesis of fullerenes with solar energy. The vaporization process is controlled by diffusion in the temperature and pressure ranges 3000-3700 K and 70-250 hPa respectively. In the solar reactor, fullerene yield is governed by the dilution of carbon vapor in argon and the temperature gradient in the cooling zone. Criteria for both parameters are suggested. Consequently, these data, combined with a validated numerical model of the reactor, may be used for the design of large-scale solar process.
    publisherThe American Society of Mechanical Engineers (ASME)
    titleHeat, Mass, and Fluid Flow in a Solar Reactor for Fullerene Synthesis
    typeJournal Paper
    journal volume123
    journal issue2
    journal titleJournal of Solar Energy Engineering
    identifier doi10.1115/1.1352736
    journal fristpage153
    journal lastpage159
    identifier eissn1528-8986
    keywordsTemperature
    keywordsCarbon
    keywordsSolar energy
    keywordsFullerenes
    keywordsGraphite
    keywordsPressure
    keywordsVapors AND Flow (Dynamics)
    treeJournal of Solar Energy Engineering:;2001:;volume( 123 ):;issue: 002
    contenttypeFulltext
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    DSpace software copyright © 2002-2015  DuraSpace
    نرم افزار کتابخانه دیجیتال "دی اسپیس" فارسی شده توسط یابش برای کتابخانه های ایرانی | تماس با یابش
    yabeshDSpacePersian