Tritium Breeders Li 2 OLi 2 AlO 2 Li 2 ZrO 3 Li 4 SiO 4 Li 2 TiO 3 Li Vaporization ( in additional H 2 ) > 600˚C> 900˚C> 800˚C> 700˚C> 800˚C Long period.

Slides:



Advertisements
Similar presentations
Implications of tritium burn fraction on fuel cycle Dai-Kai Sze, UCSD FNST Meeting August 18-20, 2009 UCLA, LA, Ca.
Advertisements

16th International Workshop on CERAMIC BREEDER BLANKET INTERACTIONS, 8-10 September, 2011 Portland, Oregon, USA. Status of research and development of.
SABR REACTOR CORE & TRITIUM BREEDING BLKT W. M. Stacey Georgia Tech September, 2009.
CBBI-16, Portland, 8-10, September Fabrication and performance of Li 4 SiO 4 pebbles by the melt spraying method Yongjin Feng Southwestern Institute of.
Energy From Chemical Reactions
Conceptual design of a demonstration reactor for electric power generation Y. Asaoka 1), R. Hiwatari 1), K. Okano 1), Y. Ogawa 2), H. Ise 3), Y. Nomoto.
KIT – University of the State of Baden-Wuerttemberg and National Research Center of the Helmholtz Association M.H.H. Kolb, R. Knitter INSTITUTE FOR APPLIED.
EXHAUST GAS RECIRCULATION IN DIESEL ENGINE
Physical States of Matter
Presented by: S. Suzuki, Blanket Engineering Lab., Japan Atomic Energy Research Institute, JAERI Contents 1.Outline of blanket development in JAERI 2.Design.
FNSF Blanket Testing Mission and Strategy Summary of previous workshops 1 Conclusions Derived Primarily from Previous FNST Workshop, August 12-14, 2008.
Associazione EURATOM ENEA sulla Fusione By Aldo Pizzuto Comparison of breeder blanket Design 9th Course on "TECHNOLOGY OF FUSION TOKAMAK REACTORS" – Erice,
1 Boyle’s Law (T and n constant) Charles’ Law (p and n constant) Combined Gas Law (n constant) Summary of Gas Laws p 1 ×V 1 = p 2 ×V 2.
June 14-15, 2007/ARR 1 Trade-Off Studies and Engineering Input to System Code Presented by A. René Raffray University of California, San Diego With contribution.
January 11-13, 2005/ARR 1 Ceramic Breeder Blanket Coupled with Brayton Cycle Presented by: A. R. Raffray (University of California, San Diego) With contributions.
November 8-9, Blanket Design for Large Chamber A. René Raffray UCSD With contributions from M. Sawan (UW), I. Sviatoslavsky (UW) and X. Wang (UCSD)
March 8-9, 2004/ARR 1 Some of the Major Considerations in Designing a Ceramic Breeder Blanket for ARIES-CS Presented by A. R. Raffray With contribution.
Resent Breeding Blanket Experiments - CONTENTS - - Objectives - - Resent breeding design at JAERI - - Brief history of FNS blanket experiments - - Resent.
Minimum Radial Standoff: Problem definition and Needed Info L. El-Guebaly Fusion Technology Institute University of Wisconsin - Madison With Input from:
The effect of the orientations of pebble bed in Indian HCSB Module Paritosh Chaudhuri Institute for Plasma Research Gandhinagar, INDIA CBBI-16, Sept.
Dalton’s Law of Partial Pressures Chapter 11 – Section 2 - Physical Characteristics of Gases.
Development of the FW Mobile Tiles Concept Mohamed Sawan, Edward Marriott, Carol Aplin University of Wisconsin-Madison Lance Snead Oak Ridge National Laboratory.
Basic Chemistry Copyright © 2011 Pearson Education, Inc. 1 Chapter 11 Gases 11.5 Temperature and Pressure (Gay-Lussac’s Law) An autoclave used to sterilize.
Matter. Review States of Matter Solid Liquid Gas Plasma.
1 Recent Progress in Helium-Cooled Ceramic Breeder (HCCB) Blanket Module R&D and Design Analysis Ying, Alice With contributions from M. Narula, H. Zhang,
Ideal gases and molar volume
Molar Volume. Avagadro’s Principle Equal volumes of gases contain equal numbers of molecules Volume of a gas varies directly with the number of molecules.
核工程计算物理实验室 Nuclear Engineering Computational Physics The Neutronics Studies of Fusion Fission Hybrid Power Reactor Youqi Zheng Ph. D Nuclear.
Fusion Blanket Technology
Neutronics Parameters for Preferred Chamber Configuration with Magnetic Intervention Mohamed Sawan Ed Marriott, Carol Aplin UW Fusion Technology Inst.
Chapter 12 Temperature and Heat Temperature – Average kinetic energy of molecules. Heat – Transfer of energy due to temperature difference; flows from.
Classification of Matter
October 27-28, 2004 HAPL meeting, PPPL 1 Thermal-Hydraulic Analysis of Ceramic Breeder Blanket and Plan for Future Effort A. René Raffray UCSD With contributions.
PROPERTIES OF MATTER PHYSICAL AND CHEMICAL. PHYSICAL PROPERTIES: can be used: -to identify a material, -to choose a material for a specific purpose, -to.
Neutronics Analysis for K-DEMO Blanket Module with Helium coolant June 26, 2013 Presented by Kihak IM Prepared by Y.S. Lee Fusion Engineering Center DEMO.
1.2 Properties and Changes of Matter 4 States of Matter - solid, liquid, gas, 4 th state – plasma.
Design study of advanced blanket for DEMO reactor US/JP Workshop on Fusion Power Plants and Related Advanced Technologies 23 th -24 th Feb at UCSD,
Growth Control of Li 2+x TiO 3+y for an Advanced Tritium Breeding Material The University of Tokyo School of Engineering, Department of Nuclear Engineering.
ITER test plan for the solid breeder TBM Presented by P. Calderoni March 3, 2004 UCLA.
Chemistry The study of the properties of matter and how matter changes. Element – a substance that cannot be broken down into any other substances by.
„I-1” – A CERAMIC COMPOSITE WITH EXTREMAL MECHANICAL STRENGTH AND THERMAL SHOCK RESISTANCY László A. GÖMZE, Milla GÖMZE University of Miskolc, Department.
1 Neutronics Assessment of Self-Cooled Li Blanket Concept Mohamed Sawan Fusion Technology Institute University of Wisconsin, Madison, WI With contributions.
Chapter 16 Chemical Reactions That Involve Heat. The study of the changes in heat in chemical reactions. Thermochemistry.
PHYSICAL AND CHEMICAL PROPERTIES Sections 2.2 and 2.3.
1 Neutronics Parameters for the Reference HAPL Chamber Mohamed Sawan Fusion Technology Institute University of Wisconsin, Madison, WI With contributions.
Physical and Chemical Properties. Physical Properties  Physical property: a characteristic of a substance that describes it such as the color, luster,
Development of tritium breeder monitoring for Lead-Lithium cooled ceramic breeder (LLCB) module of ITER presented V.K. Kapyshev CBBI-16 Portland, Oregon,
Materials Integration by Fission Reactor Irradiation and Essential Basic Studies for Overall Evaluation Presented by N.Yoshida and K.Abe At the J-US Meeting,
NOTES: Gases, Molar Volume, & Stoichiometry – a REVIEW!
{ Tritium Breeding Blanket Part I: Background, Choice of design, Choice of breeder, Tritium permeation and separation Matt Torrico NRE 4610: Intro to Fusion.
AAE 450 – Spacecraft Design Sam Rodkey 1 Active Thermal Control Design Sam Rodkey March 1 st, 2005 Project Management Project Manager.
Chemistry The study of matter and how matter changes.
Radiological Issues for Thin Liquid Wall Options L. El-Guebaly, P. Wilson, and D. Henderson Fusion Technology Institute University of Wisconsin - Madison.
Tritium Permeation Issue, Plan and Progress Dai-Kai Sze University of California, San Diego Presented at the ITER TBM Project Meeting UCLA, Feb ,
Tritium Breeding Blanket Part II: Coolant Properties, Shielding, and Tritium Breeding Ratio Nicholas Alfred NRE 4610-A :Intro to Fusion Dec 7 th, 2015.
FINAL REVIEW. 1 mole = 6.02 x of anything Molar mass – add up the mass of each element * number of each element CO 2 – 1 * * 16 = 44g/mole.
Introduction to Matter Describing Matter. Properties of Matter What is Matter? Matter is anything that has mass and takes up space.
CHAPTER 10 Reaction Energy Visual Concepts Heat Chapter 10.
The tritium breeding blanket in Tokamak fusion reactors T. Onjun1), S. Sangaroon2), J. Prasongkit3), A. Wisitsorasak4), R. Picha5), J. Promping5) 1) Thammasat.
Thermochemistry.
Can We achieve the TBR Needed in FNF?
Trade-Off Studies and Engineering Input to System Code
16th International Workshop on
בטיחות בתעשייה בהיבט חברות הביטוח
Saturday Morning Session, CBBI-16
Thermochemistry Heat and Energy.
11.5 – NOTES Heat of Combustion and Phase Changes
Chemical Equilibrium Mass transfer takes place from higher chemical potential to lower chemical potential. If the chemical potential of reactants are.
Ceramic Material Grades
Presentation transcript:

Tritium Breeders Li 2 OLi 2 AlO 2 Li 2 ZrO 3 Li 4 SiO 4 Li 2 TiO 3 Li Vaporization ( in additional H 2 ) > 600˚C> 900˚C> 800˚C> 700˚C> 800˚C Long period use (2 years) Instability (Li vaporization) StabilityInstability (crack) Instability (Li vaporization) Instability (Reduction of Ti) Tritium release ( easy release ) > 400˚C > 350˚C> 300˚C Optimum operating temp ˚C ˚C ˚C ˚C ˚C Tritium breeding ratio (TBR) HighLowerMiddle Thermal conductivity HighMiddle These tritium breeder are available in DEMO blanket? ˚C High Why we need advanced tritium breeder? ˚C Stability

Development target TBR Stability (high temperature use) Li 2 O Li 2 TiO 3 LiAlO 2 Li 2 ZrO 3 Li 4 SiO 4 DEMO Blanket Development target of advanced tritium breeder is influenced by requirement of DEMO blanket. Where is yellow area? Requirement 1) ?˚C 2) ? 3) ? Selection of important item

USAEUChinaKoreaIndiaJA Temperature 300 – 1000˚C Period of use < 2 years Purge gas 0.1%H 2 - He Local TBR> 1.05 Necessity of mixture (Li and Be) Yes ? Crash load - requirements - or - conditions - Candidate materials and new research project Li 2 TiO 3, Advanced breeder, etc. Requirement Condition

For Example 1 TBR Stability (high temperature use) Li 2 O Li 2 TiO 3 LiAlO 2 Li 2 ZrO 3 Li 4 SiO 4 DEMO Blanket in ●● Li 4 SiO 4 will be selected the tritium breeder for DEMO blanket in ●●. 7/20 Requirement 1) 300 – 800˚C →Requirement of stability is lower

For Example 2 TBR Stability (high temperature use) Li 2 O Li 2 TiO 3 LiAlO 2 Li 2 ZrO 3 Li 4 SiO 4 DEMO Blanket in ●● LiAlO 2 will be selected the tritium breeder for DEMO blanket in ●●. 8/20 Requirement 1) TBR is enough →Requirement of TBR is lower 2) More stability

Advanced Tritium Breeder in JA TBR Stability (high temperature use) Li 2 O Li 2 TiO 3 LiAlO 2 Li 2 ZrO 3 Li 4 SiO 4 DEMO Blanket in JA Li 2 TiO 3 with additional Li (Li 2+x TiO 3+y ) has higher stability at high temperatures in a reducing atmosphere. Why we need advanced tritium breeder? 9/20 Requirement 1) 300 – 1000˚C 2) 30% 6 Li burn up 3) Use for 2 years

Reference: Application of high temperature mass spectrometry and work function measurement to evaluation of thermochemical performance of ceramic breeders, Fusion Engineering and Design, Volumes 49-50, November 2000, Pages Atsushi Suzuki, Kenji Yamaguchi, Takayuki Terai, Michio Yamawaki Li Vaporization Li 2 O > Li 2 ZrO 3 = Li 4 SiO 4 = Li 2 TiO 3 > LiAlO 2 In my confidential experiment, I become dubious about the credibility of this results. So, I proposed that we try to this measurement again.

Li burn-up Loss of Li is 0.27mol Chemical formulaLi burn-up ( mol ) Li vaporization ( mol ) Chemical formula after 2 years Li 2 TiO XLi 1.88 TiO Y(aLi 4 Ti 5 O 12 + bLiTiO 2 ) TBR will be decreased. Condition: 30 % Li-6, 900 ℃( in 1%H 2 -He ), 2years This results are show in domestic conference by Hoshino. Li + n -> T + He Complex mixture Tritium release characteristic will be changes.