Plasma Current Start-up Experiments without the Central Solenoid in TST-2 and Future Plans Y. Takase...
-
date post
19-Dec-2015 -
Category
Documents
-
view
221 -
download
2
Transcript of Plasma Current Start-up Experiments without the Central Solenoid in TST-2 and Future Plans Y. Takase...
Plasma Current Start-up Experiments without the Central Solenoid in TST-2 and Future Plans
Y. TakaseGraduate School of Frontier Sciences, University of Tokyo
for TST-2 and TST-2@K Groups
Joint Meeting of the 3rd IAEA Technical Meeting on Spherical Toriand the 11th Internat Workshop on Spherical Torus
St. Petersburg State University, Russia3-6 October 2005
Compact, high plasma with good confinement can be realized in ST
compact burning plasma experiment and fusion reactor
Motivation for CS-less Ip Start-up
Lower aspect ratio and
elimination of central solenoid (CS)
improves economic competitiveness
TST-2 Spherical Tokamak
Design parameters of TST-2:R = 0.38 m / a = 0.25 (A = 1.6)
Bt = 0.3 T (0.3 T achieved)
Ip = 0.2 MA (0.14 MA achieved)
tpulse = 0.05 s (0.3 s achieved)
Main research topics: Plasma start-up optimization RF heating and wave physics MHD instability and reconnection Control of turbulence and transport
CL
1 m
TST-2
R = 0.36 ma = 0.23 mB = 0.4 TI = 0.2 MAtpulse = 0.05 sOH = 0.13 Vs
Achieved (6/01)B = 0.21 TI = 0.11 MAtpulse = 0.10 s
TST-2
Relocation of TST-2(Twice in 2 Years)
U. TokyoHongo~2002
U. TokyoKashiwa2004~
Kyushu U.Fukuoka
2003
TST-2
TST-2 EBW Antenna
Waveguides from8.2GHz klystrons
Typical plasma equilibrium
TST-2 at Kyushu University (2003)
Heating / current drive By ECW and/or EBW
TST-2@K
Plasma Stored Energy Increase (Heating)Observed during RF Injection
15% increase in Wtotal
RF on no RF
Wtotal = Wkin + Wmag(pol)
Wkin
TST-2@K
Plasma Current Formation by ECH
• 1 kA / 1 kW achieved by ECH (2.45 GHz)
• Higher current for
low gas pressure low collisionality is important
• Requires vertical field with positive curvature trapped particles are important
TST-2
Solenoidless Start-up Experiments
• Forest scenario – “pressure driven current” with mirror Bv
– 4kA maintained for 0.27 s
(with static Bv ~ 2 mT, no induction)
– Te = 160 eV (plasma is collisionless)
0
2
4
6#301567
I p [
kA
]
(a)
0
0.1
0.2
Bt [
T]
@R
0.38
[m]
(b)
RF (~100 kW)
0
0.2
0.4
0.6
0 50 100 150 200 250 300
nel [
1018
m-2
]
@R
0.39
[m]
Time [ms]
(c)
no = ce res.inside vac.ves.
1
10
100
1000
0.6 0.8 1 1.2 1.4 1.6 1.8
#301559-#301570 t=100-300ms
Cou
ntx
E [
keV
/0.0
5keV
]
Energy [keV]
Exp(-E/160eV)
TST-2@K
Reconstructed Equilibrium of the RF Start-up Plasma (I)
8~ ,1~ are paramters Obtained
channels) 80(about tsmeasuremen magnetic toFitted
A - 11
2 4
1
. and parametes free hasfunction Flux
0
2n
00
000
020
0
A
r
r
r
rj
rBff
fr
prj
A
p
pp
p
0.4 0.8
0
-0.4
-0.8
0.4
0.8
R [m]
Z [m]
0
Plasma is limited by the outboard limiter,j is truncated at top and inboard
Features of RF Start-up Plasma Equilibrium
R [m]
R [m]
0
0.7
0 0.7
-80
4
0
j [kA/m2] @ z=0
p [Pa] @ z=0
0
• high p
• large outboard boundary currentOutboard co-PS current is dominant, while inboard counter-PS current is truncted.
• Steep pressure gradient at the outboard boundary
Soft X-ray flux and temperature are roughly consistent with the pressure deduced from equilibrium reconstruction.
(a)
(b)
(c)
(d)
#302405
(e)
VL01(outboard)
IPF3(kA/turns)
PRF(kW)
Ip(kA)
IPF2-5(KA/turns)
-3
-2
-1
0
1
I PF
3(k
A)
0
2
4
6
8
10
I p(k
A)
-202468
10
VL(V
olt
s)
-2
-1
0
1
I PF
25(k
A)
(f)
-0.2
-0.1
0
0.1
0.2
-0.2
-0.1
0
0.1
0.2
Rp-0.38 Zp
0.137 0.139 0.141 0.143 0.145 0.147
Rp(m
)
Zp(m
)
Time (s)
0
50
100
150
200
Prf(k
W)
Completely CS-less Start-up to Ip = 10 kAAchieved in TST-2
CL
1 m
TST-2
R = 0.36 ma = 0.23 mB = 0.4 TI = 0.2 MAtpulse = 0.05 sOH = 0.13 Vs
Achieved (6/01)B = 0.21 TI = 0.11 MAtpulse = 0.10 s
PF1
PF2
PF4
PF3
PF5
CS
1 turn
6 turns
24 turns
TST-2@K
New Start at the Univ. Tokyo Kashiwa Campus
• Resume operation at Kashiwa
– Solenoidless start-up• Based on results of JT-60U
– Reconnection physics • Reconnection Events• Ion heating
– Turbulence and transport• Develop fluctuation diagnostics
– HHFW heating / current drive• 10-30MHz / 400 kW• k|| control (new antenna)
– Prepare LHCD system• 200MHz / 400kW (from JFT-2M)
TST-2
100kW of RF Power Injected Successfully
Full-wave calculation by TASK/WMHHFW AntennaTST-2
Bt = 0.3 T, f = 21 MHz, n = 10, ne = 2 1019 m-3, Te = 0.3 keV
E
Preparation in Progress for 200 MHz Experiments
E
Bt = 0.3 T, f = 200 MHz, n = 10, ne = 2 1018 m-3, Te = 0.3 keV
Full-wave calculation by TASK/WM
TST-2
Combline antenna
200 MHz transmitters (from JFT-2M)
Reconnection Events
TST-2
li
W(J)
25.0 26.0 27.01.4
radiation
H_alpha
Hard X ray
mag. fluct.
log(b^2)
15.0
40.0
0.0
2.0
0.0
2.0
4.0
-4.0
0.0
-5.0
-1.0
-1.5
1.0
26.025.0
2.2
27.0
Ip
20.0
0.71
0.76
50.0
1.4
2.2
Detailed Time Evolution
q_0
TST-2 t=26.2ms t=26.6ms
0
20
40
60
80
100
35534
Ip[kA]
0
2
4
6
8
Intensty CV [a.u.]
0
150
300
450
600
18 20 22 24 26
T CV [a.u.]
Time[ms]
CV intensity decreases while CIII, OIII intensities increase (loss of electron energy)
CV (core) , andOV, CIII, OIII ( edge)ion temperatures increaseat reconnection events
Reconnection events
Conversion of magnetic energyto ion kinetic energy
Ion Heating Observed at Reconnection Events
TST-2
A New Experiment to Explore Ultra-High Plasma Formation by Plasma Merging
UTST
TST-2 Magnetic Diagnostics
Megawatts of heating power can be obtained by plasma merging / reconnection
Rapid Heating by Plasma Merging / Reconnection
TS-3
Y. Ono, et al.
time [msec]
I tfc=0dW/dt~10[MW]
I tfc=10kA
dW/dt~6[MW]
I tfc=35kAdW/dt~4[MW]
10 20 30
Merging
Single
Merging
Single
Merging
Single0
40
80
120
0
40
80
0
40
80
B +Bt ext
Bp
Iz
B +Bt ext
ST#1 ST#2Bp Bp
IzB +Bt ext High ST
Comparison of thermal energy evolution for merging (solid line) and single (dashed line) formation
FRC
High q ST
Low q ST
Start-up without Center Solenoid Demonstrated
• VTin coil disconnected
• Use VR and VTout only
Discharge duration increases with
improvement of plasma position control
JT-60U
Demonstration of Advanced Tokamak Operation without the Center Solenoid
2002.06.21
Start-up and initial ramp-up
Noninductive ramp-up Transition to self-driven phase
JT-60U
ITB + H-mode (Ip = 0.7MA)p = 3.6, N = 1.6, HH = 1.6, fBS > 90%
Profiles of CS-less Advanced Tokamak with Very High Self-Driven Current Fraction
JT-60U
transport barriers
Backup(I)
0 0.4 0.8
0
-0.4
-0.8
0.4
0.8
R [m]
Z [m]
V.V
1st 2nd 3rd
PF2 Coil
Antennas
n2
n0
00
00
020
- 1 - 11
2 4
1
Arr
rr
j
rBff
fr
prj
pp
The following flux function was tried, but parameters and were not efficient.
External poloidal field
This implies that the present magnetics cannot resolve edge fine structure.
fitting. orseslightly w yields
- 1 of instead - 1 2n
3n AA
Backup (II)
Fitting was poor for inboard Bz
poloidal angle
Flux loop
Pickup coils
Flux function (red) and area of large j (blue).