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1. magnetic confinement - ENEA - Fusione

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<strong>1.</strong> MAGNETIC CONFINEMENT<br />

35<br />

[<strong>1.</strong>43] M. Talvard, G.<br />

Giruzzi and W. D. Liu,<br />

Proc. 19th EPS Conf. on<br />

Contr. Fusion and Plasma<br />

Physics (Innsbruck 1992)<br />

Vol. 16C, 1103 (1992)<br />

[<strong>1.</strong>44] S. Preische, P. C.<br />

Efthimion and S. M. Kaye,<br />

Rev. Sci. Instrum. 68,<br />

409 (1997)<br />

<strong>1.</strong>2 FTU Facilities<br />

Oblique ECE measurements were performed for the first time at FTU. At present, this<br />

is the only oblique ECE diagnostic installed in a fusion device, and the potential of<br />

such a diagnostic appears to be still largely untapped [<strong>1.</strong>43-<strong>1.</strong>44]. High-field<br />

operations on FTU and access to enhanced <strong>confinement</strong> regimes [<strong>1.</strong>42] allow this<br />

diagnostic to have an excellent resolution in configuration and velocity space. This<br />

capability can be exploited to determine the bulk form of the electron distribution<br />

and the transition from the bulk to the tail of the distribution. This would allow a<br />

detailed study of the kinetic processes involved in heating and current drive, in a<br />

variety of transport mechanisms for which at present direct experimental evidence is<br />

lacking.<br />

New data acquisition system for the plasma-density laser interferometer<br />

The two-colour interferometer was developed to get reliable density measurements<br />

during pellet injection experiments. To calculate the density, the signal from the CO 2<br />

detectors, the HgCdTe room-temperature photo resistor and HeNe photodiode has<br />

to be acquired, amplified with the automatic gain control and then compared with<br />

the signal taken from the Bragg cell driver.<br />

A new acquisition system based on a PC with a 5-MHz ADC was installed to increase<br />

the sampling rate of the old system. The system also processes, stores and sends the<br />

signal data and density to the main pulse file (based on the UNIX system) so that<br />

they are available to users through the usual display program (SHOX) (fig. <strong>1.</strong>29).<br />

Fig. <strong>1.</strong>29 - Schematic of<br />

the new PC-based<br />

acquisition system.<br />

The ADC VME module of<br />

the old system was used<br />

to acquire the phase<br />

DAS<br />

comparator outputs. It did<br />

not have enough memory<br />

to acquire the whole<br />

discharge at the correct<br />

sampling rate so, during<br />

pellet injection or fast<br />

machine vibrations, some<br />

fringe jumps were<br />

observed. The problem<br />

was solved by acquiring<br />

CH2<br />

data with a National<br />

Lab View CH1<br />

Instruments NI6110E data<br />

acquisition card that has<br />

high performance, reliable<br />

data acquisition capabilities and high speed. The new program is written in LabView<br />

graphic language.<br />

It is possible to acquire four analog inputs at 5 MS/s, with a 12-bit resolution. Data<br />

are stored on the local hard disk and automatically processed to separate the density<br />

and vibration contributions to the interferometer phase. The data are then<br />

transferred via Ethernet to the main archive under “AFS” using a set of routines<br />

(FTUWIN DLL) for the standard formatting of FTU archive files, via the LabView<br />

program.<br />

Turbulence measurements with correlation reflectometry<br />

Turbulence physics is essential for understanding transport in tokamaks. It is<br />

important to scale turbulence characteristics with the main discharge parameters; the<br />

extension of turbulence measurements to high toroidal <strong>magnetic</strong> fields and densities<br />

can be done in FTU by means of the recently installed correlation reflectometer. The

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