PPT-Exhaust Behavior and Mass Balance of Tritium
Author : elizabeth | Published Date : 2022-06-11
in Large Helical Device The tritium tracer study in the first deuterium plasma experiment in LHD was revealed that Tritium exhaust rate was 355 at the end of
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Exhaust Behavior and Mass Balance of Tritium: Transcript
in Large Helical Device The tritium tracer study in the first deuterium plasma experiment in LHD was revealed that Tritium exhaust rate was 355 at the end of the plasma experiment Thus . - What We Learned from TFTR -. C. A. Gentile. June 24, 2014. . PPPL / ITER Workshop. 1. From 1993 to 1997 the TFTR Project processed ~ 99 grams of . tritium in support of D-T operations.. Michael . Schantz. , Lorenzo . Tulipano. Phys 43, SRJC. 12 May 2009. Is nuclear power the answer?. . Transportation contributes to over 50% of CO. 2. emissions, but nuclear power cannot directly reduce this.. SAND No. 2012-1603C . Sandia is a . multiprogram. laboratory operated by Sandia Corporation, a Lockheed Martin Company,. for the United States Department of Energy’s National Nuclear Security Administration. Identifying & Dating Modern . Groundwaters. The “Age” of Groundwater. It’s not really age, rather it means “mean residence time (MRT)”. Types of GW (in terms of MRT). Modern GW: . Recharged within past few decades. mass. Stuart . Freedman memorial symposium. Berkeley, Jan 11, 2014. Hamish Robertson, University of Washington. a long wait for a little weight. 2. Neutrinos oscillate, have mass. Super-. Kamiokande. Blanket. Part I: Background, Choice of design, Choice of . breeder, Tritium permeation and separation. Matt Torrico. NRE 4610: Intro to Fusion. Dec. 7. th. , 2015. Introduction. The DD fuel cycle requires ion temperatures ~10x greater than. Part II: Coolant Properties, Shielding, and Tritium Breeding Ratio. Nicholas Alfred. NRE 4610-A :Intro to Fusion. Dec 7. th. , 2015. 500. Why Li17Pb83. High density . [~. 9015. . kg/(m^3. )] [1] . (and therefore a high mass flow rate can be obtained at lower velocities). A. W. Going. B. D. McClain. S. D. Wilson. Goals. Protect magnets and vacuum vessel from radiation. Produce tritium. Convert neutron energy into removable heat. ITER First Wall panels on blanket.. 1. Tokamak. fusion reactors. T. . Onjun1), S. . . Sangaroon2), . J. . Prasongkit3), . A. . . Wisitsorasak4), R. . . Picha5), . J. . Promping5). 1. ) . Thammasat. University, . Pathumthani. , Thailand. Tritium. Studies in TITAN for. Lead Lithium Eutectic Blankets. P. . Calderoni. - . Idaho National Laboratory. S. . Fukada. - . Kyushu University. Y. . Hatano. - . Toyama University. S. . Konishi. NOTICE OF DATE CHANGE. For further inquiries, please contact:. Don Inglis SLP Manager. E-mail: . dinglis@safeload.net.au. Phone: 02 9250 5161. REQUIRED . ACTIONS. FROM APRIL . 2013 . . Nov 2012. CONTENTS. Ⅰ. Characteristics of CANDU Reactor & . Tritium. Ⅱ. Tritium Measurements. Ⅲ. Needs of the equipment development. Ⅳ. Automatic Multiple Tritium Sampler(AMTS). Ⅴ. Conclusions & Expectations . Carlos Moreno. CIEMAT. 2. nd. EU-US DCLL Workshop University of California, Los Angeles, Nov. 14-15. th. , 2014. Roadmap . to DEMO. Fuel . Cycle schema. FC . requirements. FC . libraries. Current . Model. DEPTH PROFILES IN METALLIC . SAMPLES. Paper Number. FIP/P3-36 . Elina. . Pajuste. a. ,b. *. , . Gunta. . Kizane. a. , . Ieva. . Igaune. a. . a. Institute of Chemical Physics, University of Latvia, .
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