Progress on Systems Code and Revision of Previous Results J. F. Lyon, ORNL ARIES Meeting Sept. 16, 2004.

Slides:



Advertisements
Similar presentations
Introduction to Plasma-Surface Interactions Lecture 6 Divertors.
Advertisements

First Wall Heat Loads Mike Ulrickson November 15, 2014.
ASIPP Zhongwei Wang for CFETR Design Team Japan-US Workshop on Fusion Power Plants and Related Advanced Technologies February 26-28, 2013 at Kyoto University.
April 23-24, 2009/ARR 1 Proposed Effort Over the Next 1-2 Years on ARIES-DB DCLL A. René Raffray, Siegfried Malang, Xueren Wang University of California,
PhD studies report: "FUSION energy: basic principles, equipment and materials" Birutė Bobrovaitė; Supervisor dr. Liudas Pranevičius.
Who will save the tokamak – Harry Potter, Arnold Schwarzenegger, Shaquille O’Neal or Donald Trump? J. P. Freidberg, F. Mangiarotti, J. Minervini MIT Plasma.
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.
September 15-16, 2005/ARR 1 Status of ARIES-CS Power Core and Divertor Design and Structural Analysis A. René Raffray University of California, San Diego.
Physics of fusion power Lecture 14: Anomalous transport / ITER.
Status of Systems Code Studies J. F. Lyon, ORNL ARIES Meeting June 14, 2005.
Overview of ARIES Compact Stellarator Power Plant Study: Initial Results from ARIES-CS Farrokh Najmabadi and the ARIES Team UC San Diego Japan/US Workshop.
January 8-10, 2003/ARR 1 Plan for Engineering Study of ARIES-CS Presented by A. R. Raffray University of California, San Diego ARIES Meeting UCSD San.
April 27-28, 2006/ARR 1 Finalizing ARIES-CS Power Core Engineering Presented by A. René Raffray University of California, San Diego ARIES Meeting UW, Madison.
Systems Code Status J. F. Lyon, ORNL ARIES Meeting June 14, 2006.
Systems Code Results: Impact of Physics and Engineering Assumptions J. F. Lyon, ORNL ARIES Meeting Sept. 15, 2005.
Physics and Technology Trade-Offs in Optimizing Compact Stellarators as Power Plants Farrokh Najmabadi and the ARIES Team UC San Diego 21 st IEEE Symposium.
Optimization of Stellarator Power Plant Parameters J. F. Lyon, Oak Ridge National Lab. for the ARIES Team Workshop on Fusion Power Plants Tokyo, January.
LPK Recent Progress in Configuration Development for Compact Stellarator Reactors L. P. Ku Princeton Plasma Physics Laboratory Aries E-Meeting,
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.
NCSX, MHH2, and HSR Reactor Assessment Results J. F. Lyon, ORNL ARIES Meeting March 8-9, 2004.
The ARIES Compact Stellarator Study: Introduction & Overview Farrokh Najmabadi and the ARIES Team UC San Diego ARIES-CS Review Meeting October 5, 2006.
Magnet System Definition L. Bromberg P. Titus MIT Plasma Science and Fusion Center ARIES meeting November 4-5, 2004.
Development of the New ARIES Tokamak Systems Code Zoran Dragojlovic, Rene Raffray, Farrokh Najmabadi, Charles Kessel, Lester Waganer US-Japan Workshop.
Optimization of a Steady-State Tokamak-Based Power Plant Farrokh Najmabadi University of California, San Diego, La Jolla, CA IEA Workshop 59 “Shape and.
Overview of ARIES Compact Stellarator Study Farrokh Najmabadi and the ARIES Team UC San Diego US/Japan Workshop on Power Plant Studies & Related Advanced.
Princeton Plasma Physics Laboratory
US-Japan Workshop on Fusion Power Plants and Related Advanced Technologies High Temperature Plasma Center, the University of Tokyo Yuichi OGAWA, Takuya.
IPP Stellarator Reactor perspective T. Andreeva, C.D. Beidler, E. Harmeyer, F. Herrnegger, Yu. Igitkhanov J. Kisslinger, H. Wobig O U T L I N E Helias.
Exploration of Compact Stellarators as Power Plants: Initial Results from ARIES-CS Study Farrokh Najmabadi and the ARIES Team UC San Diego 16 th ANS Topical.
ARIES-CS Systems Studies J. F. Lyon, ORNL Workshop on Fusion Power Plants UCSD Jan. 24, 2006.
Overview of the ARIES-CS Compact Stellarator Power Plant Study Farrokh Najmabadi and the ARIES Team UC San Diego Japan-US Workshop on Fusion Power Plants.
Determination of ARIES-CS Plasma & Device Parameters and Costing J. F. Lyon, ORNL ARIES-CS Review Oct. 5, 2006.
Use of Simple Analytic Expression in Tokamak Design Studies John Sheffield, July 29, 2010, ISSE, University of Tennessee, Knoxville Inspiration Needed.
Highlights of ARIES-AT Study Farrokh Najmabadi For the ARIES Team VLT Conference call July 12, 2000 ARIES Web Site:
Status of the ARIES-CS Power Core Configuration and Maintenance Presented by X.R. Wang Contributors: S. Malang, A.R. Raffray ARIES Meeting PPPL, NJ Sept.
ARIES Systems Studies: ARIES-I and ARIES-AT type operating points C. Kessel Princeton Plasma Physics Laboratory ARIES Project Meeting, San Diego, December.
Recent Results on Compact Stellarator Reactor Optimization J. F. Lyon, ORNL ARIES Meeting Sept. 3, 2003.
Progress on Systems Code J. F. Lyon, ORNL ARIES Meeting Nov. 4, 2004.
Y. ASAOKA, R. HIWATARI and K
Minimum Radial Standoff: Problem definition and Needed Info L. El-Guebaly Fusion Technology Institute University of Wisconsin - Madison With Input from:
Systems Code Refinements and Updated Information J. F. Lyon, ORNL ARIES Meeting Jan. 23, 2006.
Systems Analysis Development for ARIES Next Step C. E. Kessel 1, Z. Dragojlovic 2, and R. Raffrey 2 1 Princeton Plasma Physics Laboratory 2 University.
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.
ARIES-AT Physics Overview presented by S.C. Jardin with input from C. Kessel, T. K. Mau, R. Miller, and the ARIES team US/Japan Workshop on Fusion Power.
Systems Code – Hardwired Numbers for Review C. Kessel, PPPL ARIES Project Meeting, July 29-30, 2010.
Programmatic issues to be studied in advance for the DEMO planning Date: February 2013 Place:Uji-campus, Kyoto Univ. Shinzaburo MATSUDA Kyoto Univ.
ARIES- ACT, 21-22May 2013, Germantown, MD Page 1 L. Waganer Consultant for ARIES Project / UCSD / DOE ARIES Project Meeting May 2013 Hampton Inn,
1 Neutronics Assessment of Self-Cooled Li Blanket Concept Mohamed Sawan Fusion Technology Institute University of Wisconsin, Madison, WI With contributions.
Compact Stellarator Approach to DEMO J.F. Lyon for the US stellarator community FESAC Subcommittee Aug. 7, 2007.
Burning Simulation and Life-Cycle Assessment of Fusion Reactors Kozo YAMAZAKI Nagoya University, Nagoya , Japan (with the help of T. Oishi, K.
ARIES- ACT, Sept, 2012, Bethesda, MD Page 1 L. Waganer Consultant for ARIES Project / UCSD / DOE ARIES Project Meeting September 2012 Bethesda,
Characteristics of Transmutation Reactor Based on LAR Tokamak Neutron Source B.G. Hong Chonbuk National University.
Systems Analysis Development for ARIES Next Step C. E. Kessel 1, Z. Dragojlovic 2, and R. Raffrey 2 1 Princeton Plasma Physics Laboratory 2 University.
ZHENG Guo-yao, FENG Kai-ming, SHENG Guang-zhao 1) Southwestern Institute of Physics, Chengdu Simulation of plasma parameters for HCSB-DEMO by 1.5D plasma.
Presented by Yuji NAKAMURA at US-Japan JIFT Workshop “Theory-Based Modeling and Integrated Simulation of Burning Plasmas” and 21COE Workshop “Plasma Theory”
Analysis of Systems Code Results J. F. Lyon, ORNL ARIES Meeting Nov. 17, 2005.
ARIES Meeting University of Wisconsin, April 27 th, 2006 Brad Merrill, Richard Moore Fusion Safety Program Update of Pressurization Accidents in ARIES-CS.
Compact Stellarators as Reactors J. F. Lyon, ORNL NCSX PAC meeting June 4, 1999.
1 Radiation Environment at Final Optics of HAPL Mohamed Sawan Fusion Technology Institute University of Wisconsin, Madison, WI HAPL Meeting ORNL March.
Comments on ARIES-ACT 1/2011 Strawman L. El-Guebaly Fusion Technology Institute University of Wisconsin-Madison
Engineering models in the ARIES system code, Part II M. S. Tillack, X. R. Wang, et al. ARIES Project Meeting January 2011.
X.R. Wang, M. S. Tillack, S. Malang, F. Najmabadi and the ARIES Team
DCLL Blanket Analysis and Power Core Layout for ARIES-DB
Trade-Off Studies and Engineering Input to System Code
Progress on Systems Code Application to CS Reactors
Farrokh Najmabadi Professor of Electrical & Computer Engineering
Comments on ARIES-ACT 10/20/2010 Pre-Strawman
New Results for Plasma and Coil Configuration Studies
Analysis of Technical and Programmatic Tradeoffs with Systems Code
University of California, San Diego
Presentation transcript:

Progress on Systems Code and Revision of Previous Results J. F. Lyon, ORNL ARIES Meeting Sept. 16, 2004

What’s New Since June ARIES Meeting Progress on Systems/Optimization Code – changes required and progress to date – issues and next steps Revisions to 1-D POPCON calculations – corrected He calculation – edge T(r) and n(r) pedestals; profile and sensitivity studies Additional 0-D calculations – examined two A  cases for NCSX and extended scaling with for all cases Comments on LHD reactor systems study

Systems Code Purpose: integrate coil and plasma geometry, reactor constraints and costing Starting point -- last (mis)used in SPPS study – code written for tokamaks, revised for helical-coil stellarators (rotating ellipse, calculated B max interpolating from database) – has ~ 7400 lines of code, highly interconnected – written ~15 years ago and last used ~10 years ago on computer platforms using math routines that no longer exist Changes needed even for relative comparisons – incorporate modular coil geometry (main components) – update physics & engineering (scaling, profiles, limits) – consistent treatment of impurities and edge – new models for blankets, shields, coils, structure – new costing for main components (waiting for numbers) – updated costing of other cost accounts (need consultation) – incorporation of maintenance periods blue -- (partly) done, black -- in progress, red -- information needed

MHHOPT Reactor Optimization Code input: physics, coil, costing, geometry, reactor component parameters and constraints plasma/profile solver T e (r), T i (r), n e (r), n i (r), n Z (r), E r (r), , Z eff, P rad, P fusion, P ,loss, P wall, P divertor,  E, etc. masses of coil and structure, j, B max bl/sh volumes, TBR, access, radial build forces on coil and structure costs of all ARIES accounts, P electric evaluate all parameters & constraints output: all parameters and profiles nonlinear optimizer optimizes targets with constraints existing parts being updated waiting for information can update no plans to use

Systems Optimization Code Minimizes core cost or size or COE with constraints for a particular plasma and coil geometry using a nonlinear constrained optimizer Iterates on a number of optimization variables – plasma:,, H-ISS95; coils: width/depth of coils – reactor variables: B 0, Large number of constraints allowed (=, ) – P electric, ignition margin,  limit, ISS-95 multiplier, radial build, coil j and B max, plasma-coil distance, clearance between coils, blanket and shielding thicknesses, TBR, access for divertors and maintenance, etc. Large number of fixed parameters for plasma and coil configuration, plasma profiles, transport coefficients, cost component algorithms, and engineering model parameters Calculates a large number of parameters – plasma: , Z eff, power components (radiation,  i,  e),  losses, etc. – coils: components volumes and costs, j, B max, forces – reactor variables: blanket volumes, TBR, neutron wall loading, divertor area, access between coils, radial build, etc. – costs: equipment cost, annual operating cost, total project cost, CoE

Input Parameters Configuration geometry – plasma aspect ratio, surface area, coil aspect ratio, closest approach aspect ratio,  limit,  (r), ripple effective (r), etc. Reactor component parameters – inside & outside shield thickness; coil width and depth – blanket thickness inside & outside, under and between coils – coil case & vacuum vessel thickness, dimensions of modular coils and VF coils; scrapeoff thickness – first wall and reflector thickness; coil to vacuum vessel gap – allowable nuclear heating in coil; j max (B) – blanket energy multiplication Cost assumptions – modular and VF costs /kg – costs and multipliers for blanket and shield – duty factor, inflation, safety assurance

Four Configurations Now Studied NCSX MHH2 port or sectoraccess (end)through accessports both quasi-axisymmetric / constant for each case, can’t change separately

Cost Estimations

FOCI components: volume density frac. cost frac. thick. frac. density (1992) cost (kg/m^3) ($/kg) (m) SiC-comp PbLi Total FW breeding zone SiC-comp PbLi reflector Total BL(ib) breeding zone SiC-comp PbLi breeder SiC-comp PbLi W reflector Total BL(ob) reflector SiC-comp PbLi RAF Total BL(dv) reflector SiC-comp PbLi RAF Total BL(bv) HT shield SiC-comp PbLi W B-FS Total SH(ib) HT shield SiC-comp PbLi B-FS LT shield ( 0.000) Total SH(ob) HT shield RAF Void WC LT shield ( 0.400) RAF Void WC Total SH(BC) HT shield SiC-comp PbLi RAF LT shield ( 0.300) SiC-comp Void B-FS Total SH(dv) HT shield SiC-comp PbLi RAF LT shield ( 0.300) SiC-comp Void B-FS Total SH(bv) RAF Void WC Inboard VV RAF Void Outboard VV RAF Void B-FS O/B (UC) VV RAF Void B-FS Divertor VV

Cost Estimations HT shield RAF Void WC LT shield ( 0.400) RAF Void WC Total SH(BC) HT shield SiC-comp PbLi RAF LT shield ( 0.300) SiC-comp Void B-FS Total SH(dv) HT shield SiC-comp PbLi RAF LT shield ( 0.300) SiC-comp Void B-FS Total SH(bv) RAF Void WC Inboard VV RAF Void Outboard VV RAF Void B-FS O/B (UC) VV RAF Void B-FS Divertor VV RAF Void B-FS Bottom VV SS Void Cryostat SiC-comp PbLi

Output Plasma parameters and profiles –,, W plasma,  E, H factors,,  *, n Fe / n e, n O / n e, Z eff –, T i0, T i,edge, T e0, T e,edge,  0 / T e0,, n i0, n e0, / n Sudo, n DT / n e, – ignition margin, P fusion, P electric, P neutron, P charged, P divertor, components of P rad and P wall, P loss Coil parameters – modular & VF coil dimensions, currents, forces, inductance, stored energy, j, B max, case thickness Reactor parameters – blanket area accessible and blocked, inboard and outboard shield thickness, cryostat gap, access between coils

Output (cont.) Cost elements – land & structures; power supplies; impurity control; heat transport; power conversion; startup power – blankets & first wall; shields; modular & VF coils; structure; vacuum vessel – turbine plant equipment; electric plant equipment; misc. plant equipment; special materials; total direct cost – construction; home office; field office; owner’s costs; project contingency; construction interest; construction escalation; total capital cost – unit direct cost; unit base cost; total unit cost; capital return; O&M costs; blanket/first wall replacement; decommissioning allowance; fuel costs; cost of electricity Summary of all component masses & mass utilization Dimensions of each element in the radial build

Revision to 1-D (POPCON) Calculations Purpose of 1-D calculations: – test different profiles, physics models and assumptions for incorporation into systems code – examine effect of assumptions on operating point Corrected error in calculation of helium concentration – this affected n DT /n e, P fusion, etc. – removes earlier concern on  He /  E 6) Added edge pedestals to simulate edge cooling from enhanced (neoclassical impurity) edge radiation – small effect, but more consistent with large edge radiation Will later update confinement scaling ISS-95 --> ISS-04 – small effect, but dimensionally correct and fits data better  basis for assumed H-ISS values

Effect of Correction to n He Calculation Previously required  He */  E 6 OK Minimum H-ISS95 ==> 3.7 for a stable operating point

NCSX-1:  E /  E ISS-95 = 4.2, = 9.5 keV, = m –3, = 6.1% operating point thermally stable branch 2-GW P fus 6% ignition contour (P in = 0) n Sudo P in = 10 MW  E ISS-95 = 0.26P heating –  2/3 0.4 H-ISS95 =  E /  E ISS-95

Plasma Parameters from 1-D Power Balance ISS-95 of 3.75 to 4.2 is required; present stellarator experiments have up to 2.5 ISS-2004 scaling indicates  eff –0.4 improvement, so compact stellarators should have high H-ISS values

ISS-95 Confinement Scaling Is Being Updated  E ~  eff –0.4 should give large H-ISS for low  eff NCSX configuration Lays basis for higher H-ISS values ~  eff –0.4 ? H. Yamada, J. Harris et al. EPS 2004

H-ISS95 Is Sensitive to Some Assumptions Need to control alpha-particle power loss and helium recycling back into plasma -- both divertor issues

Parameters Insensitive to Profile Assumptions

0-D (Volume-Average) Calculations PURPOSE Allows analytic treatment of – connection between different device parameters – effect of different assumptions and constraints Validates modules needed for systems code ADDITIONS NCSX case with different A  (2/25/03 case) Superconducting coil constraint Varied p wall from 1 to 3.3 MW/m 2 (assumed peak 1.5 times higher) to study variation in global parameters

Added 2/25/03 (NCSX-2) Case Smaller plasma-coil spacing leads to less convoluted coils and lower B max / Minimum coil-coil separation distance determined k max

Scaling Relations for Reactor Parameters Fusion power red indicates configuration-specific parameters – P fusion ~ /A p – p n,wall /1.5 = = 0.8P fusion /[ 2 (A wall / 2 )] Coil-geometry related sh = sh 2 + c x ln( ) – = A  (so + fw + bl + sh + vv + gaps + 0.5dk 1/2 ) constraint – j coil = I coil /d 2 = [I coil / ]/d 2 – j SC (B max ) and d, k from B max / Cost-related (rationale for emphasis – blanket, shield, vacuum vessel, coil structure ~ wall area ~ P fusion /, but configuration constrained – fw/blanket replacement ~ frequency x cost ~ 1/ x P fusion / ~ P fusion independent of but actual cost depends on specifics – volume of coils ~ L coil I coil /j coil ~ C x P fusion 7/8 /( 5/8 1/2 j coil ) C = (L coil / )(I coil / )A p 1/2 /(A wall / 2 ) 5/8, C/j coil constant

NCSX-1 Values Determined by p n,max = 5 MW/m 2 = 6.22 m, = 6.48 T, B max = T j coil approximately constant,, B max & d are constrained for other cases by radial build to lower (2.13–2.67 MW/m 2 )

Main Reactor Parameters from 0-D Study Wall (blanket, shield, structure, vacuum vessel) area smallest for NCSX-1  chose NCSX-1 (8/1/03 case) for more detailed study

LHD Reactor Study (T. Dolan) Based on LHD plasma and coil configuration Uses port maintainence scheme and three blanket + cooling models (RAFS + Flibe, Va + Li, SiC + PBLi) Based on Miller’s costing code with some new values H-ISS95 limited to 2, to 4%, B max = 13 T – consistent with LHD performance, higher  eff value Base case has R = 14.4 m, B axis ~ 5.5 T, H-ISS95 = 1.7, = 3%, P fusion = 4.5 GW (P electric = 1.94 GW), = 2.1 MW/m 2, j coil = 30 MA/m 2, k = 2, f loss = 0.1,  = 40% Studied CoE variation with T 0, n & T profiles,, k, plasma-wall dist, shield-coil gap, B max,, P electric

Summary Progress on Systems/Optimization Code – added modular coil geometry and updated physics models – treatment of impurities and edge and new models for blankets, shields, coils, structure in progress – information needed on new costing for main components and updated costing of other cost accounts Revised 1-D POPCON calculations – corrected He calculation – insensitive to profiles, edge n(r) & T(r) pedestals – more sensitive to alpha-particle losses and helium  p * 0-D -- added 2/25 NCSX case, superconducting coil constraint, and extended scaling with Examined LHD reactor systems study