control of fusion reactor plasma y. miyoshi frontier science,university of tokyo

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Control of fusion reactor plasma Y. Miyoshi Frontier Science ,University of Tokyo

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Page 1: Control of fusion reactor plasma Y. Miyoshi Frontier Science,University of Tokyo

Control of fusion reactor plasma

Y. MiyoshiFrontier Science ,University of Tokyo

Page 2: Control of fusion reactor plasma Y. Miyoshi Frontier Science,University of Tokyo

Introduction

ITER [1]

DEMO [2]Commercial [2]

Under construction

Construction of control system is needed.

Construction of control system for high performance plasma with limited actuators or diagnostics is needed.

Page 3: Control of fusion reactor plasma Y. Miyoshi Frontier Science,University of Tokyo

Control Logic Construction

Control paramete

rs

actuators and

diagnostics

② Control

logic

Control System construction

Page 4: Control of fusion reactor plasma Y. Miyoshi Frontier Science,University of Tokyo

Example of Parameter Categorization

ItemControl parameter

mid parameter

measurable parameter

Electrical output

Pfusne,Z ,f ,f ,Ti,Te

Safety operation

q ,Wqra ,q ,nτ,Zeff ,f

Plasma stability

β , n ,qmin, rotation

Ip,ap ,j(r),Bt

Plasma shape, position

R ,ap,κ,δ,d Ip,j(r)

Detailed discussion is needed.

div

load

N GW min

p p gap

p

eff

D T

rad

elm

edgef

fimp

Page 5: Control of fusion reactor plasma Y. Miyoshi Frontier Science,University of Tokyo

  gas-puffpellet NBI RF coil

ne ○ ○ △    Zeff ○ ○      fd,fT,fimp ○ ○ △    

Ti     ○    Te     ○ ○  qrad ○ ○      qelm   ○     ○

Ip     ○ ○ ○

j(r)     △ ○ △

Rp,ap         ○

κ,δ         ○

dgap         ○

rotation    ○    

Example of Actuator Categorization

For multiple control, Coupling effect must be taken into account.

Page 6: Control of fusion reactor plasma Y. Miyoshi Frontier Science,University of Tokyo

Multiple Control Experiment

Ti

Difference in Ti

Ref

NBI power

q-minimu

m

Ref

LHCD power

Time

q-minimum real time control ΔTi real time

control

qminITG

current profilepressure gradient

NBI

LHCD

JT-60 experiment

[3]T.Suzuki, J.Plasma Fusion Res. Vol86, No9 530-535 (2010) (in Japanese)

Page 7: Control of fusion reactor plasma Y. Miyoshi Frontier Science,University of Tokyo

1.5D transport code simulation

qmin

ITG

current profile

pressure gradient

NBI

LHCD

JT-60 experiment

NBI

gas-puff

Fusion power

minimum q-value

transport code simulation [4]

Page 8: Control of fusion reactor plasma Y. Miyoshi Frontier Science,University of Tokyo

Fusion power

Gas-puff

Target value

Fusion power control simulation

Current profile movie

Density profile movie

Gas-

puff

[1

0^

19/s

ec]

Page 9: Control of fusion reactor plasma Y. Miyoshi Frontier Science,University of Tokyo

q-minimum control simulationq-

min

Energ

y

[MW

]

r/a (q

-m

in)

Current profile

Page 10: Control of fusion reactor plasma Y. Miyoshi Frontier Science,University of Tokyo

Simultaneous control simulation

Energ

y

[MW

]

Gas-

puff

[1

0^

19/s

ec]

q-

min

r/a (q

-m

in)

Page 11: Control of fusion reactor plasma Y. Miyoshi Frontier Science,University of Tokyo

Summary of 1.5D simulation

gas-puff

Fusion power

Single Control

NBI minimum q-value

Single Control

NBI

gas-puff

Fusion power

minimum q-value

Simultaneous Control

It is difficult to determine the appropriate gain matrix from only the response characteristics.

Easy to control

Difficult to control because of their interaction

Page 12: Control of fusion reactor plasma Y. Miyoshi Frontier Science,University of Tokyo

Using modern control theory

0-D analysis

1.5-D analysis

Plasma Experiment

JT-60 experiment

Simultaneous control simulation

Classical control

Modern control

This research

Page 13: Control of fusion reactor plasma Y. Miyoshi Frontier Science,University of Tokyo

Classical and Modern control theory

Control Physical Model

Model differen

ce

True system

+-

yuer

Managed as disturbance

Control

True system

+-

yuerBlack Box

Classical control

Modern control

Page 14: Control of fusion reactor plasma Y. Miyoshi Frontier Science,University of Tokyo

State space modelTo determine actuator value, we use this ‘State space model’

actuator vector

state vector

output vector

We can get appropriate actuator value u.

Control requirement

Page 15: Control of fusion reactor plasma Y. Miyoshi Frontier Science,University of Tokyo

0-D Plasma Physics Model

a=2 (m), R=6.2 (m)

0.7

Page 16: Control of fusion reactor plasma Y. Miyoshi Frontier Science,University of Tokyo

State Equation

State vectorActuator vector

Output vector x u

we get an

d

From

Page 17: Control of fusion reactor plasma Y. Miyoshi Frontier Science,University of Tokyo

Linearized State Equation

P control

ne

Page 18: Control of fusion reactor plasma Y. Miyoshi Frontier Science,University of Tokyo

Adding the Integrator

Add the integral term to avoid the disturbance.

PI control

Page 19: Control of fusion reactor plasma Y. Miyoshi Frontier Science,University of Tokyo

2 degree of freedom control

Feedback 

Control

Plasma

+-

yuer Δu

Feed forward 

Control

ueq

Find the equilibrium point from the reference and physical model

Find the feed back gain from physical model

Page 20: Control of fusion reactor plasma Y. Miyoshi Frontier Science,University of Tokyo

Simulink

We use the software ‘MATLAB/Simulink’ to do simulation.

MATLAB/Simulink

Page 21: Control of fusion reactor plasma Y. Miyoshi Frontier Science,University of Tokyo

Summary

For control logic construction, categorizing of control parameters, actuators and diagnostics is necessarily.

In this research, we determine the PI gain from 0-D plasma physics model, and we demonstrate the 0-D control simulation.

The simulation using a transport code or plasma control experiment are future work.

Page 22: Control of fusion reactor plasma Y. Miyoshi Frontier Science,University of Tokyo

Reference

[1] http://www.naka.jaea.go.jp/ITER/iter/index.html[2] http://www.asahi-net.or.jp/~rt6k-okn/subject.htm[3] 3]T.Suzuki, J.Plasma Fusion Res. Vol86, No9 530-535 (2010) (in Japanese)[4] Y. Miyoshi et.al PFR Vol.7 2405135 (2012)[5] Control system design (G. C. Goodwin et.al)

Page 23: Control of fusion reactor plasma Y. Miyoshi Frontier Science,University of Tokyo

Appendix

Page 24: Control of fusion reactor plasma Y. Miyoshi Frontier Science,University of Tokyo

The Effect of Disturbance

Control Nominal Model

Model err

True system

+-

yuer

d

If controller has integrator (1/s), the effect of step disturbance will vanish.

Page 25: Control of fusion reactor plasma Y. Miyoshi Frontier Science,University of Tokyo

Linearize

In this simulation, we assume that equation point = reference point.