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Association

Euratom-Cea





TORE SUPRA









The control of magnetically confined plasmas

(in tokamak facilities)



S. Brémond





Institut de Recherches sur la Fusion par confinement Magnétique (IRFM)

CEA Centre de Cadarache









Large Scale Initiative « fusion » Summer School (September 2009) S. Brémond 1

Outline

Association

Euratom-Cea





TORE SUPRA



• A short reminder of the fusion energy source development issue



• Basics of tokamak operation



• Control issues overview

- Basic controls

- Performance optimisation, advanced scenario

- Machine protection



• Control design needs



• Conclusion





Large Scale Initiative « fusion » Summer School (September 2009) S. Brémond 2

A SHORT REMINDER OF THE FUSION

Fusion reaction ENERGY SOURCE DEVELOPMENT ISSUE 1/3

Association

Euratom-Cea 9 Fe









Binding energy by nucleon (MeV / nucleon)

8

Ne

TORE SUPRA O

C U

7 He



FISSION of heavy nucleus

6 Be FUSION of light nucleus

D + T  He + n

5 Li

(3.6 MeV) + (14 MeV)

4





3

T

2

Requires to give the two light nucleus enough

energy so that they have a chance to jump through

1 D

the electrostatic barrier Nb of

0

nucleons

0 50 100 150 200 250





FUEL AND HEAT IT UP ! (to about 100 million degrees, plasma state)



EXTERNAL HEATING required

before internal heating takes over (collisions of the He with the D-T nucleus)



Large Scale Initiative « fusion » Summer School (September 2009) S. Brémond 3

A SHORT REMINDER OF THE FUSION

Power balance ENERGY SOURCE DEVELOPMENT ISSUE 2/3

Association

Euratom-Cea CONFINE IT (to avoid power losses and fuel dilution) ! Gravitational confinement



Condition for overall power gain (Lawson criteria)

TORE SUPRA

Huge mass

n x T x tE > threshold required

(sun and stars)

Fuel density Temperature Confinement time



G 

Inertial confinement

G 1

Compression of a

milimetric target

n ~ 103 x standard solids

1995- tE ~ 10-9 seconde

JET

1990

Magnetic confinement

1980

Effect of magnetic field

Pfusion on charged particles

1968 G

Pexternal heating

n ~ 10-5 air in this room

tE ~ 1 seconde



Large Scale Initiative « fusion » Summer School (September 2009) S. Brémond 4

A SHORT REMINDER OF THE FUSION

Magnetic confinement 1/2 ENERGY SOURCE DEVELOPMENT ISSUE 3/3

Association

Euratom-Cea

The Issue: losses at

principle both ends

TORE SUPRA









Issue: vertical drift



B = m0 Ibob / 2p R

The toroidal

configuration Giration radius a 1/B









Issue (collective

Helicoïdal effects between

I particles) : hoop

field lines p force



The tokamak configuration







Large Scale Initiative « fusion » Summer School (September 2009) S. Brémond 5

A SHORT REMINDER OF THE FUSION

Magnetic confinement 2/2 ENERGY SOURCE DEVELOPMENT ISSUE 3/3

Association

Euratom-Cea



Equilibrium

TORE SUPRA

field

external

coils



SET OF MAGNETIC

CONFINEMENT COILS







Two options







Wall



Scrape-off layer (SOL)



Last closed flux surface



Limiter configuration divertor configuration

Large Scale Initiative « fusion » Summer School (September 2009) S. Brémond 6

BASICS OF TOKAMAK

Tokamak plasma actuators 1/2 OPERATION 1/4

Association

Euratom-Cea

Central

TORE SUPRA solenoid coil

(transformer

FUEL primary)

Gaz valves, pellets injector,

Pumps

Poloidal

CONFINE Field coils

Fuelling (plasma

-Transformer primary coil system (gas position

(limited time duration) + non valve, pellet and shape)

inductive current drive systems injector not

-> drive plasma current represented

here)

- Poloidal Field coils

-> set plasma position and

shape Pumping

(cryo

pumps)

HEAT UP

- “ohmic” heating (limited

capabilities)

- Wave, Beam heating systems ITER project view



Large Scale Initiative « fusion » Summer School (September 2009) S. Brémond 7

BASICS OF TOKAMAK

Tokamak plasma actuators 2/2 OPERATION 2/4

Association

Euratom-Cea

Heating / Current Drive

TORE SUPRA









NEUTRAL BEAM







ION CYCLOTRON WAVE

Tens of MHz (tetrode sources)



ELECTRON CYCLOTRON

WAVE

Around 100 GHz (gyrotrons)





LOWER HYBRID WAVES

2.5 GHz, 3.7 GHz (klystrons)









Large Scale Initiative « fusion » Summer School (September 2009) S. Brémond 8

BASICS OF TOKAMAK

Example of Tore Supra (CEA Cadarache) OPERATION 3/4

Association

Euratom-Cea

PERMANENT TOROIDAL MAGNETIC FIELD :

supercondutctor NbTi coils

TORE SUPRA

ACTIVELY COOLED PLASMA FACING

COMPONENTS : water cooling, exhaust

capability ~ 10 MW/m2 (within ITER range)



Circular cross-section

Current 1.5 MA

CONFINED

Major radius 2.4 m

PLASMA

Minor radius ~ 0.72 m

Volume ~25 m3









2 Lower hybrid 3 Ion Cyclotron 1 Electron Cyclotron

antennas (3.7 GHz) antennas (40-80 MHz) antenna (118 GHz)

~ 6 MW max, 1 GJ ~ 10 MW max, 250 MJ 0.8 MW max , 25 MJ

Large Scale Initiative « fusion » Summer School (September 2009) S. Brémond 9

BASICS OF TOKAMAK

Plasma discharge schedule OPERATION 4/4

Association

Euratom-Cea ITER discharge foresseen schedule



TORE SUPRA









Large Scale Initiative « fusion » Summer School (September 2009) S. Brémond 10

CONTROL ISSUES 1/2

Control issues overview

Association

Euratom-Cea second

-3 -2 -1 0 1 2 3 4

TORE SUPRA 10 10 10 10 10 10 10 10







Plasma MHD Energy confinement Current diffusion





Thermal ELM’s - Disruption Cooling of PFCs





Particles Particle confinement Wall inventory









Basic controls Machine protection

(MHD equilibrium, density) Safety



Performance optimisation

Advanced scenario







Large Scale Initiative « fusion » Summer School (September 2009) S. Brémond 11

CONTROL ISSUES 2/2

Feedback control need

Association

Euratom-Cea Target scenario

CONTROLER / DIAGNOSTICS

TORE SUPRA

• INTRINSIC INSTABILITIES SUPERVISOR measurements



• PERTURBATIONS (state of the Sequencing, tracking of

references and machine

wall, internal profiles “self- protection

organisation”, etc. )

• COMPLEXITY OF THE PHYSICS at

stake (accurate prediction very ACTUATORS Tokamak

plasma

difficult) - magnetic coils

- fuelling / pumping systems

 - heating / current drive

systems

Real time feedback control required







Reliable real-time

measurements

needed

(not covered here)





Large Scale Initiative « fusion » Summer School (September 2009) S. Brémond 12

JET diagnostics overview

BASIC CONTROL 1/4

Equilibrium control – basics 1/3

Association

Euratom-Cea BASIC MODELING (PLASMA POSITION)

 

TORE SUPRA

MOTION EQUATION

(Magneto Hydro Dynamic



dv

dt



v 

t



  



 v . grad v  j  B  grad p

description)

  

RIGID DISPLACEMENT MODEL    r ( t )u r   z ( t )u z





m p R  2pf R m p Z  2pf Z





     

f  jt  B p plasma  jt  B p ext  j p  Bt  grad p



m0 I p

2



 

Zero order m0 I p

2

m0 I p  p  1 8p u R p

2

development   8R  li  RI p BZext u R  BRe xt u Z uR

ln     1u R 8p

in R 4p   a  2 



a



m 0 I p   8R 

2

l 3



m p R  2pRI p BZext  ln     p  i   

m p Z  2pRI p BRe xt

2   a  2 2

(Poloidal) beta: ratio of

kinetic / magnetic pressure Plasma self inductance

Large Scale Initiative « fusion » Summer School (September 2009) S. Brémond 13

BASIC CONTROL 2/4

Equilibrium control – basics 2/3

Association

Euratom-Cea VERTICALLY ELONGATED CROSS SECTION



TORE SUPRA - happens to allow better plasma performance

require outward curvature

- but require outward field curvature







Vertical position unstable









Huge force : Tesla * MAmp * 2pR

Low mass: 800m3 * 1020 (per m3) * 10-27 (kg/ion) • •

Very fast time scale : ~ ms (MHD Alfven time)



But we don’t have to react that fast (we could not actually)

Ip

because eddy current will be induced in the metallic

structures of the vessel which will – on certain conditions-

slow down the motion to their L/R characteristic time where

feedback controlled active coils may take over





Large Scale Initiative « fusion » Summer School (September 2009) S. Brémond 14

BASIC CONTROL 3/4

Equilibrium control – basics 3/3

Association

Euratom-Cea

PLASMA SHAPING

TORE SUPRA









ITER Poloidal cross section

Numerical Modeling :

•Direct / Inverse problem (PF coils current -> magnetic surfaces topology or the inverse): 2D

free boundary equilibrium codes (CEDRES++ developed with Univ. Nice)

•Reconstruction problem (magnetic probes at the vessel -> plasma last closed surface): 2D

free boundary reconstruction code (EQUINOX developed with Univ. Nice, other approach for

plasma boundary reconstruction only developed with INRIA Sophia)



Large Scale Initiative « fusion » Summer School (September 2009) S. Brémond 15

BASIC CONTROL 4/4

Particle density control

Association

Euratom-Cea

ne

TORE SUPRA FUELLING SOURCES

Gaz

•Recycling : a badly controlled dominant puffing

fuelling source (depending of the history / +

state of the wall) Recycling

•Gaz puffing : edge fuelling

•Pellets injection : more internal fuelling Pellets







Complex particle transport phenomena 





Control target / issues: Gaz puffing

pellet

- impurity exhaust (He ashes)

- density profile optimisation (burn control)

- radiation control (divertor) recycling









Large Scale Initiative « fusion » Summer School (September 2009) S. Brémond 16

PERFORMANCE OPIMISATION –

Advanced scenario ADVANCED SCENARIO 1/2

Association

Euratom-Cea

• internal confinement enhancement

Control of the internal profiles (plasma

TORE SUPRA

current density, pressure, etc.)



• MHD instables modes control

Edge localised modes, sawteeth,

neoclassical tearing modes, resistive

wall modes, etc.









Large Scale Initiative « fusion » Summer School (September 2009) S. Brémond 17

PERFORMANCE OPIMISATION –

Internal profiles control (current density) ADVANCED SCENARIO 2/2

Association

Euratom-Cea

Distributed plasma current

density real-time

TORE SUPRA

measurement



RT equilibrium reconstruction with the EQUINOX

code (developed with Univ. Nice)



Identification of the plasma current profile

(and free boundary equilibrium) from external

measurements





Distributed plasma current density

real-time control design



New design approach based on a distributed non linear control oriented model



  //     jT  

1    

 x    // R 0 j ni (1, t ) x 

m 0 R 0 a 2 x x  x 

t m 0 a 2 x x  x 

a 2 xB 0

q



“Diffusivity - interior - boundary” control x

 magnetic flux, //parallell electric resistivity, jninon inductive current density

Large Scale Initiative « fusion » Summer School (September 2009) S. Brémond 18

MACHINE PROTECTION ISSUES 1/1

Machine protection issues

Association

Euratom-Cea

• Disruption detection

TORE SUPRA



• Disruption mitigation



• Plasma First Wall Component protection from overheating





Needs :





- IR imaging wrapping to PFCs geometry

- High level real time data processing

(pattern recognition, heat flux

assessment,multi diagnostic processing,

etc.)

collaboration under way with INRIA Sophia









Large Scale Initiative « fusion » Summer School (September 2009) S. Brémond 19

CONTROL DESIGN PROCESS 1/1

Control design process

Association

Euratom-Cea

• Existing control mainly based on “semi empirical” design

TORE SUPRA • Model based control: needs for integrated modeling

Plateforme de

simulation

(Kepler)

Boite à outils

contrôleurs Modèles orientés

(Scicos) contrôle

Paramétrage

avec éditeur TS

TS

Structure de

données ITM Contrôleurs





Paramétrage avec éditeur

générique ITM Diagnostics TR









Installation actuelle Outils ITM en cours Briques ou connexions

Tore Supra de développement à développer





Plasma discharge flight simulator under development



Large Scale Initiative « fusion » Summer School (September 2009) S. Brémond 20

Conclusion

Association

Euratom-Cea





TORE SUPRA Control of tokamak plasmas: an old problem, new issues

Performance target requires to (ITER needs) :

- operate very close to technological limits (while ensuring machine

protection)

- optimise plasma performance by controlling not only global variables,

but also local ones (plasma internal profiles)

- develop an integrated management of the plasma discharge

-pre-qualify control algorithms (safety – licensing)





Main needs

- real-time data processing algorithms development

- Integrated modeling tools (model based control design)







Large Scale Initiative « fusion » Summer School (September 2009) S. Brémond 21



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