p.scarin, m.agostini, n.vianello, r.cavazzana, f.sattin, g.serianni, m.spolaore
DESCRIPTION
Analysis of edge turbulence in RFX-mod from GPI data and comparison with other toroidal devices. P.Scarin, M.Agostini, N.Vianello, R.Cavazzana, F.Sattin, G.Serianni, M.Spolaore Consorzio RFX, Associazione Euratom-ENEA, Padova, Italy S.J.Zweben - PowerPoint PPT PresentationTRANSCRIPT
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13th RFP Workshop October 9-11 2008 Stockholm 1
P.Scarin, M.Agostini, N.Vianello, R.Cavazzana, F.Sattin, G.Serianni, M.Spolaore Consorzio RFX, Associazione Euratom-ENEA, Padova, Italy
S.J.ZwebenPrinceton Plasma Physics Laboratory, Princeton, New Jersey, USA
R.J.Maqueda Nova Photonics, Princeton, New Jersey, USA
J.L.TerryPlasma Science and Fusion Center, MIT, Massachusetts, USA
Y.Yagi, H.Sakakita, H.Koguchi, S.Kiyama, Y.HiranoNational Institute of Advance Industrial Science and Technology, Japan
Analysis of edge turbulence in RFX-mod from GPI data and
comparison with other toroidal devices
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Introduction Turbulent structures are detected in the edge region of several plasma
devices: Tokamak, Stellerator, RFP, non fusionist machines
Structures are considered the main cause of transport and confinement degradation
Statistical analysis of edge turbulence reveals the presence of common properties that do not depend on the particular plasma device: indication of a
similar physical driving mechanism
Statistical properties of edge signals of four different fusion devices are analysed and the common properties are pointed out
The different turbulent time and space scales between the four experiments seems to be linked with the edge pressure gradient scale
Indication of pressure-driven instability
Introduction
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Edge Structures
t=0 t=12 s
t=24 s t=36 s
NSTX
RFX-modt=0 t=0.4 s t=0.8 s t=1.2 s
r [mm] r [mm]r [mm]r [mm]
[m
m]
[m
m]
[m
m]
[m
m]
G.Serianni et al., PPCF 49 2075 (2007)
In the edge region, potential, density and temperature signals are characterised by strong fluctuations
Strong bursts in the signals are related with the presence of coherent structures (blobs) propagating in the plane perpendicular to the main magnetic field
Introduction
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Main Diagnostic: GPIThe edge regions of
RFX-mod
TPE-RX
NSTX
Alcator C-mod
are studied with the Gas Puff Imaging diagnostic
GPI is a non intrusive spectroscopic diagnostic which measures the local emission fluctuations of H D HeI lines in the plane perpendicular to the main magnetic field
GPI e eI n T
R.Cavazzana et al. RSI 75 4152 (2004)
M.Agostini et al., RSI 77 10E513 (2006)
P.Scarin et al., JNM 363-366 669 (2007)
Zweben S. et al., NF 44 134 (2004)
Terry J. et al., JNM 290 757 (2001)
Introduction
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PDF of the Signals
NSTX
RFX-mod
TPE-RX
Alcator C-mod
PDF of raw signals are clearly non Gaussian in
all the devices
Deviation from Gaussianity increases
outward
Raw Signals
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Statistics Vs Radius
NSTX
Alcator C-mod
3
3/ 22
I IS
I I
4
22
I IF
I I
Flatness and skewness increase outside the separatrix
Edge fluctuations are more and more dominated by
positive (S>0) bursts with high amplitude (high F), relative to the mean value of the signals,
as one moves outward
Raw Signals
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Universal Statistics
F.Sattin et al. PPCF 48 1033 (2006)
F.Sattin et al. submitted to PPCF
Parabolic relation between F & S for the edge fluctuations in all the devices analysed: few conditions expected to
hold for different environments
B.Labit at al. PRL 98 255002 (2007)
Schopflocher T.P. et al. Boundary-Layer Meteorology 115 341 (2005)
Sura P. and Sardeshmukh, J.Phys. Oceanogr. 38 638 (2008)
Experimental PDF can be fitted with 2 Gamma functions: coefficient of
the curve provide information about the physics of the system
Raw Signals
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Power Spectra
Power spectra show (typically) different regions with
power law-decay
f *
f* should be linked to the turbulence injection scale
Time Scales
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NSTX
RFX-mod
TPE-RX
Alcator C-mod
Intermittency
The PDFs of the edge fluctuations
depend on the scale of the fluctuations
*
Time Scales
* assumes values similar to f* -1
Different time scales involved
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Flatness Comparison
For a set of different discharges F() has been evaluated for the different devices
Time scale multiplied for f*
For all the machines flatness reaches the Gaussian values of 3 for f*=1
Coherent structures develop for f *<1
τ f *=1 is linked with the largest spatial scale present in the system
No structures
Structures
Time Scales
Injection
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Edge Gradients
RFX-mod
The edge region of fusion devices are characterised by the presence of strong gradients that are possible sources of free energy for the development of
turbulence
[eV
]
NSTX
In tokamaks the edge region is fundamental in the rising and sustaining of
the H-mode regimes
Gradients
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Turbulence Vs Edge Gradients
NSTX
TPE-RX
Link between electron pressure gradient and
edge structures
Area occupied by edge structures (fp)
increases from inward to outward
Alcator C-mod Different experiments
characterised by different pressure gradient scales Lp
Gradients
Langmuir probes
RFX-mod
Langmuir probes
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Turbulence & Injection Scale Largest spatial scale present in the system:
*v / f v aAutocorrelation time
RFX-mod
NSTX
Alcator
Clear relation between the largest structures and the characteristic pressure gradient scale Lp
Gradients
v ⊥τ a
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Conclusions
Conclusions
Universal statistical properties have been detected in the edge region of four plasma fusion devices
A common largest spatial scale present in the systems can be identified
This spatial scale linked with the energy injection scale of the turbulence is clearly linked with the pressure gradient scale
Pressure-gradient instabilities should play a role in the generation and evolution of the edge turbulence
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Flatness (F) as a function of Skewness (S) for the GPI fluctuations (about 40000 points)
The data can be fitted with a quadratic polynomial, and the result are very similar to
the one reported for TORPEX machine in [B. Labit et al., PRL 98 (2007) 255002]
In the graphs different plasma conditions are considered (about 2000 different plasma
discharges)
The numerical values of the coefficients of the curve provide information about the
specific physics of the system
The analytical curve is a general consequence of a few conditions expected to hold for
different environments [Schopflocher T.P. et al. Boundary-Layer Meteorology 115 341 (2005), Sura P. and
Sardeshmukh, J.Phys. Oceanogr. 38 638 (2008),……………]
Statistical Properties of GPI signals in RFX-mod
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Statistical properties of GPI signals in RFP&Tokamak
F = a S2+b
for a large range of F and S values
An estimate of coefficient a would
bring information of underlying physical
mechanism
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Pressure Driven Instabilities in TPE-RX and RFX-mod
TPE-RX
RFX-mod In RFX-mod phase relation between Vp and ne
(measured at I < 350kA) varies from 90° to 0°
Different pressure driven instabilities
In TPE-RX device phase relation between Vf and GPI structures (link to ne) is 90°
Indication of curvature driven instabilities
[ M. Agostini et al., Plasma Phys. Control Fusion 50 (2008) to be published]
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GPI-Langmuir comparison
TPE-RX
• GPI and Langmuir diagnostics are active simultaneously in RFX-mod at I<350kA
although at different locations
• The (S, F) dataset of ne from Langmuir overlaps with the GPI database
• The good overlap supports the assumption that GPI provides a measure with an equivalent statistic to plasma density
fluctuations
• Time correlation between GPI and ion saturation current signals in TPE-RX taken simultaneously at almost the same location
• The high value of the correlation suggests that the 2 signals unveil the same
dynamic of the turbulence
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…..about the shape of Power Spectrum S(ƒ) (1)
S(ƒ) tails can
switch from exp to
power-law on the
same plasma pulse
Power-law exp
…it depends from the
distribution of burst times ?
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…..about the shape of Power Spectrum S(ƒ) (2)
…with the time scale analysis ones obtain different
distributions, with different width:
• S(ƒ) power-law wide distribution
• S(ƒ) exp narrow distribution
The S(ƒ) of edge turbulence may be interpreted as arising from superposition of signals
with different coherent structures and the time width distribution could depend from the
displacement of magnetic surface (radial component)
τ [μs]