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News
from MAST - April 2004
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MAST Development
The 9 month MAST Engineering Break (see MAST News
Bulletin Dec 2003 for a detailed description) was completed
on schedule. Following vessel closure, leak testing was carried
out followed by an extensive period (1½ weeks) of high temperature
baking, resulting in a base pressure close to 10-8mbar.
Power supply and electrical system commissioning has progressed
rapidly and is almost complete. The new central solenoid has been
operated at ±45kA ( ~ 80% of maximum capability) and the
toroidal field (TF) system has been taken up to 85kA (Irod
~2MA). The maximum TF power supply current is 92kA
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Figure 1. Installation of the new
MAST centre column |
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Commissioning of the 60GHz electron Bernstein wave (EBW) heating
system is also well-underway with 5 of the 7 gyrotrons having been
operated at high power. EBW experiments are scheduled to take place
early in the 2004 (M4) campaign (see below).
Commissioning of the South West (SW) neutral beam injector has
also started, power levels > 1MW being rapidly achieved in hydrogen.
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Neutral Beam System Upgrade
Until July 2003, the MAST NBI System was operated using two duopigatron
neutral beam injectors on loan from Oak Ridge National Laboratory
which together gave a maximum total injected deuterium beam power
into MAST of 3.3MW for 250ms in plasma pulse 9502. In order to further
develop the long pulse high power capability of the NBI system the
decision was taken in 2003 to replace the two duopigatron injectors
with Positive Ion Neutral Injectors (PINIs), which have been successfully
used over many years on JET and other fusion facilities in Europe.
The MAST PINI is based on the JET PINI design with a supercusp ion
source and tetrode accelerator modified to match the existing geometry
of the MAST NBI beamlines. It will be capable of delivering ~ 2.5MW
(per injector) into the MAST plasma for a pulse duration in excess
of 5 seconds when operated in deuterium at 75kV/65A. The predicted
deuterium beam power distribution at the MAST plasma axis is shown
in Figure 2.
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Figure 2. Predicted neutral
power density distribution on plasma axis (75kV/65A deuterium
beam corresponding to 2.5MW of injected neutral power). This
simulation is based on accelerator alignment measurements
of the first MAST PINI. The contour indicates the 1/e fraction
of the peak power density |
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The first MAST PINI (Figure 3) has been designed, manufactured,
fully assembled and installed on the MAST South (S) beamline in
April 2004. In addition, many components of the NBI beamlines had
to be modified or re-designed: new PINI support and steering structure,
new second stage neutraliser, modified bend magnet (reduced pole
gap), additional HV area above the injector to accommodate the snubber,
etc. A new PLC controlled gas introduction system for the PINI ion
source and the neutraliser has been designed, manufactured and installed.
New long-pulse calorimeters and Residual Ion Dumps (RIDs), based
on hypervapotrons, were installed into both beamlines (see MAST
News Bulletin Feb 2004). The calorimeters and RIDs are instrumented
with a large number of thermocouples allowing accurate measurement
of beam power density distribution, beam position and neutralisation
efficiency. Most of the power supplies and corresponding controls
are being modified or replaced to allow long-pulse PINI operation.
Major changes include fast switching of the arc at high voltage
(HV) turn-on (arc notching), reapplication after PINI HV breakdown
and HV regulation. This new scheme will also allow pulse width modulation
of the beam power. New components required for PINI operation have
been designed, procured and are being installed: filament transformer
and power supply, gradient (G2) resistor, arc current feedback control,
etc. A new HV transmission line, connecting the PINI to the HVPS,
has been designed, installed and tested. The new transmission line
also incorporates the snubber to protect the PINI from stored energy
in the transmission line during HV breakdowns. A new bending magnet
control circuit allowing automatic setting of the bending magnet
current based on working gas and set beam voltage has been designed
and manufactured. The new Beam Interlock System, based on the Fast
Beam Interlock System (FBIS) used on JET, has been designed, manufactured
and is being installed. This system will protect both beamline and
MAST vessel components by stopping the beam extraction in case of
the following fault conditions: beamline over-pressure, neutraliser
gas introduction valve malfunction, bending magnet current/beam
voltage mismatch, excessive shinethrough power on MAST vessel components
at low plasma densities (Beam Bremsstrahlung Interlock). Electrical
and thermal data acquisition system and timer controls were also
upgraded to allow fast collection and storage of an increased number
of signals: 16 fast electrical data channels, 96 thermal data channels
and 8 timing channels were added to each beamline.
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Figure 3. MAST PINI M01 (rear view) in
the D1 building
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The first MAST PINI will be brought into operation on the S beamline
in Summer 2004 whilst continuing to operate the SW beamline with
the ORNL duopigatron injector. The second PINI will be assembled
in Summer 2004, installed on the SW beamline during the November
2004 MAST Engineering Break and brought into MAST operation at the
beginning of 2005. |
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The latest MAST operating schedule is shown below: |
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Experimental Activities
The experimental proposals (>80) for the forthcoming campaign
have been reviewed and prioritised by the Campaign Drivers and the
MAST Experiments Committee (MEC) has given a provisional indication
of the experimental time likely to be allocated to each of the main
thrusts. A set of targets, by which the success of the 2004 campaign
can be judged, has also been drawn up. Detailed planning of the
experimental programme is now underway. After an initial period
of plasma conditioning discharges and diagnostic commissioning,
the main focus will be on start-up studies and electron Bernstein
wave heating tests. Scientists from ENEA Frascati will visit Culham
to participate in the start-up studies.
A number of MAST presentations have been given at the recent round
of ITPA (International Tokamak Physics Activity) meetings. At the
6th ITPA Pedestal Physics Group Meeting at Culham 1-3 Mar 2004 Andrew
Kirk delivered a presentation on the pedestal database whilst Hendrik
Meyer gave a presentation on improvements in H-mode access in connected
double null configurations in MAST. MAST results were also included
in a presentation by Rajesh Maingi (ORNL), of the NSTX team, who
compared edge pedestal data in MAST and NSTX. Martin Valovic gave
a presentation on the incorporation of new MAST data in the H-mode
confinement database at the 6th meeting of the ITPA Confinement
Database and Modelling Topical Group at Naka, 8 - 11 March 2004.
The incorporation of MAST ITB (Internal Transport Barrier) data
in the Profile Database was also discussed by Martin at the Transport
Topical Group meeting held in Naka at the same time.
MAST presentations were prominent at the recent APS High Temperature
Plasma Diagnostics conference in San Diego, April 2004. Paddy Carolan
gave an invited talk on "High Definition Imaging in the MAST
Spherical Tokamak from Soft X-rays to Infrared". This was backed
up by contributed papers from Mike Walsh of Walsh Scientific ("Incorporation
of fast laser beam shunting and a broadband polariser in the MAST
Thomson scattering systems"), Ash Patel ("A versatile
multi-wavelength imaging diagnostic in the Mega Ampere Spherical
Tokamak, MAST") and Michaela Nelson of Queen's University,
Belfast, ("THEMIS, a high resolution soft x-ray spectrometer
on the MAST tokamak"). Of particular interest is a novel diagnostic
that provides narrow spectral bandwidth imaging which accommodates
the wide field of view, uniquely available in MAST, of the full
plasma diameter. Flexibility was built into the design, first exploited
in measuring the Zeff profile from the visible bremsstrahlung and
more recently used to measure the neutral beam characteristics as
well as availing of the diagnostic opportunities provided by the
neutral beams. One configuration of the diagnostic is shown below
(Fig. 4) which allowed the beam divergence evolution to be measured
(Fig. 5) across the full vessel diameter. The viewing geometry of
the beam meant that there was a range of Doppler shifts. A slightly
tilted interference filter, used in the convergent region of the
optics, coped with this complication by taking advantage of the
filter bandpass variation with light incident angle. In another
application (Fig 6) the Charge Exchange Recombination, CXR, of two
elements were monitored as well as the Balmer Dα
light from the beam neutrals. This is important in determining impurity
density profiles.
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| Figure 4. Beam
emission diagnostic in MAST |
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| Figure 5. Beam
emission measurements in MAST |
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| Figure 6 Combined beam emission
and charge exchange recombination spectroscopy measurements |
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Recent MAST journal publications include:
A. Kirk et al, ELM characteristics in MAST, Plasma Phys. Contr.
Fusion 46 (2004) 551
H. Meyer et al, Formation of transport barriers in the MAST spherical
tokamak, Plasma Phys. Contr. Fusion 46 (2004) A291
A. Kirk et al, H-mode pedestal characteristics in MAST, Plasma Phys.
Contr. Fusion 46 (2004) A187
Other News
A group of senior Polish scientists visited MAST on 30th March
2004 to discuss opportunities for future collaboration on fusion
research.
A MAST Data Access Policy has been developed outlining the responsibilities
of those granted access to unpublished MAST data.
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