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SUNISTSUNIST
SUNIST- Sino UNIted Spherical Tokamak
Status of SUNIST spherical tokamak in 2006
HE Yexi, ZHANG Liang, *FENG Chunhua, FU Hongjun, GAO Zhe, TAN Yi, WANG Wenhao, *WANG Long, *YANG Xuanzong, XIE Lifeng
[email protected], 86-10-62791874 (o), 86-10-62782658 (fax)
SUNIST United LaboratoryDepartment of Engineering Physics, Tsinghua University, Beijing 100084, P.R.China
*Institute of Physics, Chinese Academy of Science, Beijing 100080, P.R.China
This work was supported by National Nature and Science Fund of China (Grant numbers: 10275041 and 10375089) , and International Atomic Energy Agency (Research contract No. 12935/R0) .
The 2nd Research Coordinate Meeting
on Joint Research Using Small Tokamak, IAEAOctober 23 - 26, Beijing
OUTLINE
UNISTUNISTSUNISTSUNIST
SUNIST spherical tokamak
Preliminary resultECR plasma current startupthe 1st step modification for double swing operation of BOH
Further plan
SUNIST spherical tokamak
SUNISTSUNIST
SUNIST main parameters:
major radius R 0.3m
minor radius a 0.23m
Aspect ratio A ~1.3
elongation κ ~1.6
toroidal field ( R0) BT 0.15T
plasma current IP 0.05MA
flux (double swing) ΔΦ 0.06Vs
SUNIST spherical tokamak
SUNIST spherical tokamak magnets and power supply
UNISTUNISTSUNISTSUNIST
coil turn L(H) R(m) ID(kA) VC(V) Capacitor(mF)
TF 24 508 4.72 9.4 200 2560(1280)
HF 236 519 17.8 13 3000 13.3/1280
EF 26 684 15 1.5 1200/120 1(2)/476(18.8)
Vacuum vessel and BV magnet assembling
toroidal magnet pre-assembling
Cross section and designed magnetic surface
SUNIST spherical tokamak
SUNIST spherical tokamak vacuum and vacuum vessel
SUNISTSUNIST
main parameters – vacuum vessel:outer diameter 1.2 m inner diameter 0.13 mheight 1.2 mvolume ~ 1 m3
surface area ~ 2.3 m2
vacuum pumps: TMP (1000l//s)
sputtering Ti pump (200l/s)
cryogenic pump (1500l/s to N2)
wall conditioning: baking: PTC( Curie point 160 0C)glowing discharge,
siliconization
background pressure: ~ 6×10-5 Pa (between shot
s)
leaking rate on cross seal: ≯=2×10-7 Pam3/s
SUNIST spherical tokamak
OUTLINE
UNISTUNISTSUNISTSUNIST
SUNIST spherical tokamak
Preliminary resultECR plasma current startupthe 1st step modification for double swing operation of BOH
Further plan
SUNISTSUNIST
Typical discharge of ECR startup in 2005
Preliminary result
Microwave: Pout < 100kW, t pulse ~ 30 ms, f = 2.45 GHz
background pressure ~ 110-4 Pascalhydrogen pressure ~ 110-2 Pascal during discharge
SUNISTSUNIST
Improving vacuum condition
Preliminary result
top view of the movement of the piezo valveinstalled a cryogenic pump (CRYO-PL
EX 8LP), background pressure down to 5~8x10-5 Pa (between shots)
pulsed gas puffing, moving valve to chamber, shorter puffing duration (~
2ms) and shorter interval between filling and PRF (~3ms)
siliconization, SiH4 + He, DC glow dis
charge
the piezo valve
vacuum vessel
Conduit for pumping
t0~30ms
~8mspuffing pulse
power pulse
t0 ~3ms
~2ms
SUNISTSUNIST Preliminary result
• spiky still• oscillations of H and microwave
reflection causing during lower Bv
• BV effect on ECR startup
2 4 6 8 10
0
1
2W
Time (ms)
2 4 6 8 10
0.0
0.2
0.4
0.6
Ip (k
A)
2 4 6 8 10
01020304050
H (
a.u.
)
2 4 6 8 1006
121824
Bv (G
)
0 2 4 6 8 10 12 14 16 18
0.0
0.2
Vlo
op, V
Time (ms)
0 2 4 6 8 10 12 14 16 18
08
16
Pin
0 2 4 6 8 10 12 14 16 18
08
1624
H,
a.u
.
0 2 4 6 8 10 12 14 16 18-0.8-0.40.00.4
Ip, k
A
0 2 4 6 8 10 12 14 16 18
0153045
Iv, G
current startup with a later BV
current startup with one-up BV
Typical discharge of ECR startup in 2006
SUNISTSUNIST
The effect of BV to H emission and wave reflection
Preliminary result
0 2 4 6 8 10 12 14 16 18
0
10
20
30
0 2 4 6 8 10 12 14 16 18
-20-10
0102030405060
H
(a.u
.)
Time (ms)
Ref
lect
ion
(%)
0 2 4 6 8 10 12 14 16 18
0
10
20
30
0 2 4 6 8 10 12 14 16 18
-20-10
0102030405060
H
(a.u
.)
Time (ms)
Refle
ctio
n (%
)
with Bv (~30G)without Bv
SUNISTSUNIST
Performances of preliminary ECR current startup
Preliminary result
The effects of BV on plasma current startup on SUNIST:
- BV applied leading PRF _ plasma current is just spikes.
The dependence of driven IP on vertical field is consistent with
the toroidal plasma current produced by BV drift effect in ECR plasma.
- BV applied during ECR plasma _ plasma current has higher value,
longer duration.
- BV influences on H and reflection of PRF.
The effect of electrode discharge to ECR plasma current
- in co-direction _ IP could increase above 10% (Fig. 7).
- in counter-direction _ IP would be counteracted more obviously
(Fig.8).
OUTLINE
UNISTUNISTSUNISTSUNIST
SUNIST spherical tokamak
Preliminary resultECR plasma current startupthe 1st step modification for double swing operation of BOH
Further plan
modification for double swing operation of BOH
UNISTUNISTSUNISTSUNIST
Modifications of the circuit
shutdown the SCR
increasing ramp-down rate
To
From
t
Iohm,I’
C13.6mF
3000V
SCR DCoil519uH
SCR’C’500uF
3000V
L’ 12uH
R200mOhm
0
Imax
I’
t
s 50
C13.6mF
3000V
SCRD
Coil519uH
modification for double swing operation of BOH
UNISTUNISTSUNISTSUNIST
• With < 10kA Iohm and 200
mohm R, ~20kA Ip is gene
rated and a small flat-top
revealed that could be adj
usted by R and IP.
• Compare to normal ramp-
up ohmic discharge, ≯10k
A Iohm ~30kA Ip
• If loop voltage can be kep
t, the plasma current can
be maintained.4 6 8 10 12 14 16 18
02468
10 4 6 8 10 12 14 16 18
0.00.20.40.60.8 4 6 8 10 12 14 16 18
0
8
16
24 4 6 8 10 12 14 16 18-10-505
1015
Iohm
(kA)
time(ms)
Iv(k
A) Ip
(kA)
Vlo
op(V
)
modification for double swing operation of BOH
UNISTUNISTSUNISTSUNIST
Adding a capacitor bank in order to reverse Iohm , and get longer duration of Ip
C
13.6mF
3000V
SCR
SCR’C’
500uF
3000V
L’ 12uH
R
200mOhm
SCR’’
C’’
1.28F
300V
Iohm
0t
IohmIp
OUTLINE
UNISTUNISTSUNISTSUNIST
SUNIST spherical tokamak
Preliminary resultECR plasma current startupthe 1st step modification for double swing operation of BOH
Further plan
SUNISTSUNIST
Further plan
1 upgrade system
*modification of ohmic field power supply to double swing mode
*upgrade diagnostics: H and SX arrays, visible and UV spectroscopy, W interferometer and reflectometer…
*magnet discharge and plasma configuration controls
2 SUNIST discharge performance
*operation regime, equilibrium and MHD
*edge plasma
*vacuum vessel conditioning effects to discharge3 current startup and RF wave effect on plasma*ECR current startup with or without electrode assistance and BV effects
*possibility transit to typical discharge from non induced start plasma current
*Alfven wave effects on low aspect ratio toroidal plasma.