Polywell Fusion J A E YO UNG PA R K E NN F USION SYMPOSIUM, A P R I L

Similar documents
arxiv: v1 [physics.plasm-ph] 1 Jun 2014

The Dynomak Reactor System

Chapter IX: Nuclear fusion

TWO FUSION TYPES NEUTRONIC ANEUTRONIC

The GDT-based fusion neutron source as a driver of subcritical nuclear fuel systems

Magnetic Confinement Fusion and Tokamaks Chijin Xiao Department of Physics and Engineering Physics University of Saskatchewan

Aspects of Advanced Fuel FRC Fusion Reactors

Regeneration factor as a function of neutron energy for the different fissile isotopes. Breeding in the Thorium-U 233 fuel cycle can be achieved with

Helium Catalyzed D-D Fusion in a Levitated Dipole

Inertial Confinement Fusion DR KATE LANCASTER YORK PLASMA INSTITUTE

INTRODUCTION TO MAGNETIC NUCLEAR FUSION

A Faster Way to Fusion

The Path to Fusion Energy creating a star on earth. S. Prager Princeton Plasma Physics Laboratory

GA A22689 SLOW LINER FUSION

Toward the Realization of Fusion Energy

Plasma Wall Interactions in Tokamak

Comments About Varied IEC Approaches to Fusion Power

Plasma & Fusion on Earth: merging age-old natural phenomena into your present and future

Compact, spheromak-based pilot plants for the demonstration of net-gain fusion power

240NU211 - Fusion Technology

Introduction to Fusion Physics

PHYSICS BASIS FOR THE GASDYNAMIC MIRROR (GDM) FUSION ROCKET. Abstract

Developing a Robust Compact Tokamak Reactor by Exploiting New Superconducting Technologies and the Synergistic Effects of High Field D.

GA A23168 TOKAMAK REACTOR DESIGNS AS A FUNCTION OF ASPECT RATIO

240 ETSEIB Escola Tècnica Superior d Enginyeria Industrial de. European Master in Innovation in Nuclear Energy (EMINE)

Development of Long Pulse Neutral Beam Injector on JT-60U for JT-60SA

The Levitated Dipole Experiment: Towards Fusion Without Tritium

Toroidal confinement devices

Conceptual design of an energy recovering divertor

A Polywell p+11b Power Reactor Joel G. Rogers, Ph.D.

Lecture 14, 8/9/2017. Nuclear Reactions and the Transmutation of Elements Nuclear Fission; Nuclear Reactors Nuclear Fusion

Neutron Sources Fall, 2017 Kyoung-Jae Chung Department of Nuclear Engineering Seoul National University

Imposed Dynamo Current Drive

Smaller & Sooner: How a new generation of superconductors can accelerate fusion s development

Discovery of an Electron Gyroradius Scale Current Layer: Its Relevance to Magnetic Fusion Energy, Earth s Magnetosphere and Sunspots

0 Magnetically Confined Plasma

ª 10 KeV. In 2XIIB and the tandem mirrors built to date, in which the plug radius R p. ª r Li

Unpressurized steam reactor. Controlled Fission Reactors. The Moderator. Global energy production 2000

ELECTROMAGNETIC LIQUID METAL WALL PHENOMENA

Possibilities for Long Pulse Ignited Tokamak Experiments Using Resistive Magnets

Magnetic Confinement Fusion-Status and Challenges

Fluctuation Suppression during the ECH Induced Potential Formation in the Tandem Mirror GAMMA 10

Der Stellarator Ein alternatives Einschlusskonzept für ein Fusionskraftwerk

Capacitive Probe for Plasma Potential Measurements in a Vacuum diode and Polywell Device

Thorium Fuel Cycle Using Electrostatic and Electrodynamic Neutron Generators

A is called the mass number gives, roughly, the mass of the nucleus or atom in atomic mass units = amu = u

Quasi-Symmetric Stellarators as a Strategic Element in the US Fusion Energy Research Plan

Introduction to Plasma Physics

Fusion Nuclear Science - Pathway Assessment

Purposed Polywell Mechanism

Overview of Pilot Plant Studies

Plans for a laboratory electron-positron plasma experiment

Spherical Torus Fusion Contributions and Game-Changing Issues

Observation of Neo-Classical Ion Pinch in the Electric Tokamak*

Estimations of Beam-Beam Fusion Reaction Rates in the Deuterium Plasma Experiment on LHD )

Mission Elements of the FNSP and FNSF

Advancing Local Helicity Injection for Non-Solenoidal Tokamak Startup

Plasmoid Motion in Helical Plasmas

purposes is highly encouraged.

Burn Stabilization of a Tokamak Power Plant with On-Line Estimations of Energy and Particle Confinement Times

Plasma and Fusion Research: Regular Articles Volume 10, (2015)

STELLARATOR REACTOR OPTIMIZATION AND ASSESSMENT

Observations of Counter-Current Toroidal Rotation in Alcator C-Mod LHCD Plasmas

Implementation of a long leg X-point target divertor in the ARC fusion pilot plant

School and Conference on Analytical and Computational Astrophysics November, 2011

Fusion Energy: How it works, Why we want it, & How to get it sooner

Non-Solenoidal Plasma Startup in

Advanced Tokamak Research in JT-60U and JT-60SA

Electron Trapping in High-Current Ion Beam Pipes

A SUPERCONDUCTING TOKAMAK FUSION TRANSMUTATION OF WASTE REACTOR

Introduction to the Sun

Fusion Principles Jef ONGENA Plasma Physics Laboratory Royal Military Academy Brussels

Neutron Testing: What are the Options for MFE?

Fusion-Enabled Pluto Orbiter and Lander

Self-consistent modeling of ITER with BALDUR integrated predictive modeling code

A Virtual Reactor Model for Inertial Fusion Energy. Michel Decroisette Noël Fleurot Marc Novaro Guy Schurtz Jacques Duysens

D-D FUSION NEUTRONS FROM A STRONG SPHERICAL SHOCK WAVE FOCUSED ON A DEUTERIUM BUBBLE IN WATER. Dr. Michel Laberge General Fusion Inc.

Simulation of alpha particle current drive and heating in spherical tokamaks

How Is Nuclear Fusion Going?

Atomic physics in fusion development

Recent Development of LHD Experiment. O.Motojima for the LHD team National Institute for Fusion Science

Neutral beam plasma heating

Small Spherical Tokamaks and their potential role in development of fusion power

Magnetized Target Fusion: Prospects for low-cost fusion energy

Issues for Neutron Calculations for ITER Fusion Reactor

Prospects of Nuclear Fusion Energy Research in Lebanon and the Middle-East

MHD. Jeff Freidberg MIT

Configuration Optimization of a Planar-Axis Stellarator with a Reduced Shafranov Shift )

General Physics (PHY 2140)

Toroidal confinement of non-neutral plasma. Martin Droba

What we ve learned so far about the Stability of Plasma Confined by a Laboratory Dipole Magnet

Space Weather Prediction with Exascale Computing

Magnetically-Channeled SIEC Array (MCSA) Fusion Device for Interplanetary Missions

Lecture PowerPoints. Chapter 31 Physics: Principles with Applications, 7th edition Giancoli

Confinement of toroidal non-neutral plasma

Studies of Charge Separation Characteristics for Higher Density Plasma. in a Direct Energy Converter Using Slanted Cusp Magnetic Field

Double Null Merging Start-up Experiments in the University of Tokyo Spherical Tokamak

Terry Kammash and Myoung-Jae Lee Department of Nuclear Engineering The University of Michigan Ann Arbor, MI (313)

Chapter 14 Our Star Pearson Education, Inc.

Recent results on non-inductive startup of highly overdense ST plasma by electron Bernstein wave on LATE

Transcription:

Polywell Fusion J A E YO UNG PA R K E NERGY MAT T E R CONVERSION CORPORATION E NN F USION SYMPOSIUM, A P R I L 20 20 1 8

History of EMC2 1985 Energy Matter Conversion Corporation is a US-incorporated, San Diego-based company developing nuclear fusion 1985: EMC2 founded by the late Dr. Robert Bussard Polywell technology is based on high pressure magnetic confinement of plasma called the Wiffle-Ball and plasma heating with an electrostatic potential well by e-beams 1992 1995: First Polywell device was built with DARPA funding. Successfully demonstrated electrostatic potential well using electron beams. 2013 2017 1995-2013 1995-2013: EMC2 continued R&D efforts utilizing a series of 19 test Polywell devices to demonstrate and examine Wiffle-Ball (WB) plasma confinement backed by the US Navy. 2013: Successful formation of WB and demonstration of enhanced confinement. 2014-2017: EMC2 filed two patents, published a peer-reviewed paper, and provided public disclosures of the Polywell technology. 2017: EMC2 developed computer code to validate and began optimizing the Polywell technology. 2

EMC2 San Diego Laboratory 3

EMC2 Teams and Collaborations KU Leuven Plasma Simulation Power Systems, Magnets Particle Diagnostics Reactor Engineering, Neutronics & Modeling Neutral beam injector plasma sources m-wave & laser diagnostics 4

Why EMC2 Pursues Polywell Fusion? Lawson Criteria for Polywell n* t * T - High density using stable magnetic cusp trap: 10n compared to tokamak (5x10 20 m -3 ) - Sufficient confinement using Wiffle- Ball (i.e. high beta cusp): 0.1 t compared to tokamak (0.1-1s) - High temperature using electron beam heating: 1.5-2T compared to tokamak (30-50 kev) Additional Metrics Critical to Fusion Energy - Plasma stability: uncontrolled plasma behaviors degrade reactor performance and damage reactor - Efficient fuel heating allows 2 nd generation fuels (D 3 He and p- 11 B) - Needs to address engineering and materials limitations - Size and cost of reactor matters to compete against other power plants An important Question: how to make a better fusion reactor than tokamak or stellarator? Bonus question: Can we use a fusion engine to travel within and outside the solar system? 5

What is Polywell Fusion? 1. Magnetic cusp - Cusp has the best stability property - Key to achieve high density and compact reactor size 2. Electrostatic heating - Potential well to heat & confine ions - Cusp is compatible with electron beams 3. Wiffle-Ball (WB) Confinement - High pressure plasma in the cusp generates a unique equilibrium - WB can greatly enhance energetic electron confinement Polywell fusion: Polyhedral magnets and Electrostatic potential well for fusion power reactor + e - e - e - + + 6

Magnetic Cusp: Stable but leaky magnetic trap Simple magnetic cusp can be produced by 2 coils with opposite currents From Project Sherwood: The U. S. Program in Controlled Fusion by Amasa Bishop (1958). Magnetic cusp was proposed as a fusion concept in 1954 due to its favorable stability ~ 20 cusp devices were built for fusion From Principles of Plasma Physics Krall & Trivelpiece (1973) Cusp is stable due to its curvature note that B-field increase from center to boundary Various types of cusp systems from Dolan s review article (1994) 7

Electrostatic Heating of Ions: A Potential Game Changer - The simplest known method of heating ions to fusion temperature (100M degree or more) - Pioneered by Farnsworth and Hirsch in 1960s for Inertial Electrostatic Confinement (IEC) fusion system - Electron beam approach compatible with magnetic cusp system - Potential well formation inside magnetic cusp demonstrated in 1995-8 kv electron beam injection yielded 7kV potential well very high efficiency - Due to poor confinement of energetic electrons, the potential well failed with increasing plasma density - That s why EMC2 started focusing on improving confinement of energetic electrons Forming and Maintaining a Potential Well in a Quasispherical Magnetic Trap, Krall et al, Physics of Plasma (1995) 8

WB: A critical missing piece for Polywell Fusion How is WB formed and what does it do? - WB (also known as high beta cusp) was proposed by Grad between 1954-1958. - WB is formed when the plasma pressure becomes high and comparable to magnetic filed pressure in the cusp boundary - For example, the critical density (beta=1) is 6x10 20 /m 3 at 50 kev for 5T B-field - Due to diamagnetic nature of plasma, the magnetic fields are pushed outward and forms a sharp boundary with strong plasma current on the surface - This diamagnetic current is responsible to change the magnetic field topology to enhance plasma confinement in the center. 9

WB formation Simulation Results

Experimental Validation of WB Formation and Confinement Property LaB 6 Electron Gun (7 kev, 1 3 A) Plasma Gun (350 MW solid arc) X-ray diode (2 kev x-rays and up, corner and face views) Chamber size: 45 cm cube, Coil major radius; 6.9 cm Distance between two coils: 21.6 cm, B-field at cusp (near coil center) 0.6 2.7 kg I(t): x-ray intensity - di(t)/dt ~ I(t)/t 11

X-ray intensity / I injection (a.u.) e X-ray intensity / Electron current (a.u.) X-ray intensity (a.u.) Face and corner cusp chord n e bulk (in unit of 10 15 cm -3 ) Flux exclusion (%) WB confirmation: enhanced confinement of 7 kev electrons 1 0.8 0.6 0.4 0.2 0-0.2 n e bulk B High shot 15610 High Phase X-ray face X-ray corner X-ray from impurities (e.g. W) 16 8 0 "High-Energy Electron Confinement in a Magnetic Cusp Configuration, Park et al, Physical Review X 5, 021024, 2015 Quote from Navy Review Committee - EMC2 has made a major breakthrough in its development of the Polywell... It has clearly and repeatedly demonstrated so-called wiffle ball plasma formation with dramatically enhanced plasma confinement, a major achievement and a prerequisite to concept success. 0.5 0.5 0.4 0.3 0.2 shot 15631@220 MW shot 15650@340 MW shot 15630@450 MW shot 15640@700 MW 0.4 0.3 0.2 shot 15621@B=0 shot 15677@B=0.6 kg shot 15640@B=2.7 kg 0.1 0.1 0 0-0.1-0.1 WB requires high condition WB requires balance between plasma and B-field pressure 12

Plasma Simulation A tool to understand how Polywell works & how we can optimize it ECsim:Energy Conserving semiimplicit method 1980 s Early development Simple solvers J.U. Brackbill, D. Forslund, JCP, 46, 271, (1982). 1992-2005 Vector computers (Crays) Advanced solvers G. Lapenta, J.U. Brackbill, P. Ricci, PoP, 13, 055904, (2006). 2005-2008 First Massively parallel implementation S. Markidis et al, Astronomical Society of Conference Series, vol 406, page. 237, (2009). - Latest version of the implicit particle code developed over 35 years - First-Principles code: solves Newton Eq. and Maxwell Eqs. - EMC2 now uses ECsim for Polywell as well as other magnetic geometry like mirror and pinch Venus 08-Now Massively Parallel Vectorized operations 3D production Review in Lapenta, JCP, 231, 795 (2011) & Lapenta et al, Nature Physics 11, 690 695 (2015) ipic3d Celeste Parsek 2015-Now Solves 3 rd order matrix equation to conserve energy within machine accuracy Optimized for high beta fusion reactor simulation ECsim G. Lapenta, D. Gonzelez-Herrero, E. Boella, J. of Plasma Physics, 83, 705830205 (2017). 13

Magnetic Mirror Simulation 14

(Confinement time) Path to Polywell Fusion Power 1 s Polywell Reactor Performance Matrix Net power Polywell 10 years Waste Lawson Crit 10 8 6 4 2 0 Stability 10-5 s Today 1-2 Proof-of Principle devices Size & Cost Simplicity Efficiency 2 kg 10 cm 7 kev (Magnetic field) (Reactor size) (Electron Heating) 5 T 2 meter 80 kev 15

Polywell Fusion Power Plant: how it will look EMC2 Vision: Compatible with existing power conversion technology 1 st generation Polywell Power Plant will utilize existing HTGR technology (high temperature gas cooled reactor): ~40% efficiency at 725 C Helium cooling Initial cost breakdown for 500 MWe plant - $150M for Polywell Fusion Engine - $400M for secondary loop/generator - $150M for tritium breeding system To achieve 7-9 cents per kwh electricity cost 16

Proposed Maintenance of Polywell Fusion Core Use of D-T requires routine replacement of Polywell Fusion core Simulation almost ready for e-beam driven potential well and dynamics equilibrium for advanced fuels 17

Summary EMC2 has been working on a compact fusion reactor based on Polywell approach combining electrostatic fusion with magnetic cusp system. Recent breakthrough in confinement and simulation will catalyze our efforts toward the demonstration of net power generation in a compact Polywell fusion test device If proven, Polywell technology would offer a low cost and rapid development path to power the world economically and sustainably. Unique Advantages of Polywell Plasma stability: economical and reliable reactor High beta cusp (WB) confinement: confinement and compact size Use of electron beam driver: efficient heating 18