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State of the Lab

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in the ion cyclotron range of frequencies: theory and experiment ... ln (flux / Energy1/2) beam injection. energy. at RF end 10 ms 20 ms. noise level. 108251 ... – PowerPoint PPT presentation

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Title: State of the Lab


1
Wave - plasma interactions in the ion cyclotron
range of frequencies theory and experiment in
NSTX
Cynthia K. Phillips Princeton Plasma Physics
Laboratory for the NSTX Team APS meeting April
2003
2
NSTX IS STUDYING HIGH HARMONIC FAST WAVES IN HIGH
BETA PLASMAS
  • HHFW are compressional fast Alfvén waves
  • ??? k VA N WD (6 - 12) WD
  • plasma beta 4 - 38
  • choose w / k// electron thermal speed
  • strong electron absorption via transit time
    magnetic pumping and Landau damping
  • ion cyclotron damping generally weak, except for
    energetic ions and low k//
  • For NSTX, find k????i 1 and ??? / a ltlt 1
  • Since BP BT , 2D magnetic equilibrium effects
    important

B0
x
k
3
RADIO FREQUENCY (RF) WAVES USED FOR HEATING AND
CURRENT DRIVE
  • STs need auxiliary heating (H) and current drive
    (CD)
  • choose wave spectra for H or CD
  • absorption profile depends on plasma parameters
  • HHFW are absorbed by electrons in high beta
    plasmas
  • competitive absorption by ions degrades CD
    efficiency

4
POWER SPECTRUM OF ANTENNA IS PROGRAMMABLE OVER A
WIDE RANGE OF k ( 2 to 14 m-1)
Antenna phasing controls heating or current drive
12 element antenna for 6 MW _at_ 30 MHz
co-CD
B
counter-CD
Heating
-20
0
20
antenna extends almost 90 toroidally
kz (m-1)
4
5
HHFW STRONGLY HEATS ELECTRONS
4He Discharge
Te gt Ti
keV
Major Radius (m)
  • B 0.44 T
  • kT 14 m-1
  • ne0 4.0 x 1019 m-3

Note decay of Te after RF turn-off
6
CENTRAL ELECTRON HEATING PREDICTED BY THEORETICAL
MODELS
Full wave code
WKB ray tracing codes
3
3
ray tracing codes
AORSA - 2D
HPRT
Pabs ( MW / m3 )
Pabs ( MW / m3 )
CURRAY
0
0
0
0.4
0.8
normalized minor radius
normalized minor radius
7
HHFW HEATS FAST DEUTERIUM IONS INJECTED WITH
NEUTRAL BEAMS
Neutral particle analyzer
2
12
12
108251
2
10
Te0(keV)
beam injection energy
8
ln (flux / Energy1/2)
8
1
ln ( flux / energy 1/ 2 )
ne ( 1019 m-3)
Ip (MA)
at RF end 10 ms 20 ms
6
4
4
RF 2.4
noise level
2
NBI 1.6 MW
0
0
0
40
80
120
Time (s)
Energy (keV)
  • fast D tail builds up during and decays after
    HHFW

8
THEORY PREDICTS SIGNIFICANT ABSORPTION BY FAST
IONS
  • fast ion and electron absorption comparable
  • no thermal ion absorption for this k// range
  • fast ion absorption degrades CD efficiency
  • BUT
  • fast ion absorption decreases at lower BT ,
    higher b
  • observed and predicted

1
0.6
beam
e-
0.2
9
CURRENT DRIVE INFERRED FROM DIFFERENCES IN LOOP
VOLTAGE WITH PHASED WAVES
  • 2 discharges with similar ne(r),Te(r)
  • inductance similar
  • ?V not caused by dli/dt
  • less loop voltage required for constant IP with
    co-CD phasing

Counter - CD
DV .2V
Loop Voltage (V)
Co - CD
RF on
Time (s)
  • circuit analysis (0D) IP (V-
    0.5IPdLi/dt)/RP IBS ICD
  • ICD 110 kA inferred vs 96 160 kA predicted by
    codes
  • driven current consistent with previous tokamak
    experience

10
WAVE-PLASMA INTERACTIONS PLAY A CRITICAL ROLE IN
NSTX RESEARCH
  • HHFW provides means of electron heating
  • Interaction between HHFW and fast ions observed
  • ion interaction decreases with increasing
    electron beta
  • Initial evidence found for HHFW current drive
  • driven current consistent with modeling and
    previous FWCD experiments
  • higher Te needed to achieve NSTX research goals

11
HHFW CURRENT DRIVE CONSISTENT WITH D-IIID AND
TFTR CD EXPERIMENTS
C. Petty et al., Plasma Physics and Controlled
Fusion 43 (2001) 1747
  • Operation at higher Te required to meet NSTX
    goals
  • Increased power and improved confinement should
    allow this
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