Download Free Analysis Of Mhd Activity Using Ece Diagnostics On Alcator C Mod Tokamak Book in PDF and EPUB Free Download. You can read online Analysis Of Mhd Activity Using Ece Diagnostics On Alcator C Mod Tokamak and write the review.

An Active MHD Diagnostic has been installed and operated on Alcator C--Mod to study Toroidal Alfven Eigenmodes (TAEs). The diagnostic consists of two broadband amplifiers and two antennas which can excite stable modes in the TAE frequency range. The plasma response to this excitation is measured by existing magnetic fluctuation diagnostics. Analysis of the fluctuation data provides information about the TAE frequencies and damping rates as well as mode structure. The Active MHD diagnostic has evolved since its first operation in 2002, when it could only operate over a limited, preprogrammed frequency band. Recent improvements include automatic tuning to cover frequencies from 100 to 750 kHz, and an interface to the Alcator C--Mod Digital Plasma Control System (DPCS). The DPCS monitors plasma parameters, calculates the nominal TAE frequency, and adjusts the frequency input to the MHD amplifiers, all in real time. Now the Active MHD Diagnostic can measure TAEs over an entire plasma shot. This paper is focused on the requirements and design of the MHD Amplifiers, particularly the tuning bandwidth. It will also present some preliminary results from the recent run campaign.
In a tokamak plasma, knowledge of the thermal particle and supra-thermal ion populations, and their dynamics is essential for controlled operation as the plasma pressure and current gradients provide the energy required to trigger various types of (MagnetoHydroDynamic) MHD instabilities that act to degrade plasma control and performance. Therefore studying the behaviour of MHD instabilities will reveal considerable information about the various particle populations in the plasma. In particular, a sensitive and readily excitable class of MHD instability in a tokamak plasma is the Toroidicity induced Alfvén Eigenmode (TAE). This mode is excited by supra-thermal ions and its frequency depends on the magnetic field strength, mass density profile, safety factor and the major radius of a tokamak, making it a rich source of information. At ASDEX Upgrade plasma ions are accelerated to energies of 1MeV and higher by Ion Cyclotron Resonance Heating. The interactions between TAEs and the resulting supra-thermal ion population is used to infer the effects that TAEs will have on fusion-born {uF061}-particles in a thermonuclear fusion reactor. This is of paramount importance to ITER and any future fusion devices, as {uF061}-particles are envisioned to be the main source of energy used to maintain a burning plasma. The aim of this research was to characterise typically observed fast ion excited TAEs at ASDEX Upgrade, to study the stability of fast ion excited TAEs at ASDEX Upgrade, to demonstrate that such TAEs could be driven by ICRF (Ion Cyclotron Radio Frequency) beat waves, and to improve equilibrium reconstructions using TAE derived safety factor information. To this end all milestones were achieved demonstrating that the techniques developed to drive TAEs with ICRF beat waves provides the basis for a new diagnostic, which complements existing safety factor profile diagnostics.
Lower Hybrid Current Drive (LHCD) is a promising technique to sustain tokamak plasmas and provide control over the current profile--two important capabilities required for the development of tokamak fusion reactors. Upgraded measurement capabilities on the Alcator C-Mod Tokamak create a unique opportunity to study the plasma's toroidal electric current profile at magnetic fields, plasma densities, and magnetic geometries anticipated in future reactors in stationary discharges dominated by lhcd. The Motional Stark Effect (MSE) diagnostic uses polarized light to infer the plasma's internal current profile. The MSE diagnostic deployed on the Alcator C-Mod Tokamak previously experienced unacceptable calibration drift and sensitivity to partially-polarized background light that limited its ability to measure magnetic field pitch-angles. A comprehensive analytic study of the origin of polarization angle errors in MSE diagnostics and an experimental study using a robotic calibration system were conducted. Insight from this study guided the fabrication and installation of a first-of-a-kind in-situ calibration system for MSE diagnostics--a long sought capability-- and the development of thermal isolation schemes for the periscope. An experimental study of the effect of partially polarized background light identified this as a significant source of systematic error. Partial-polarization upon reflection was identified as the mechanism that leads to polarized light in a tokamak. Visible bremsstrahlung, divertor emission, and blackbody emission were identified as the dominant sources of light. A new technique, MSE multi-spectral line polarization (MSE-MSLP), was developed to measure the polarization on a single sight line in multiple wavelengths simultaneously using a high-throughput polarization polychromator. Wavelength-interpolation of the background light polarization utilizing this hardware decreases the error from background subtraction by a factor of 5-10 relative to time-interpolation, drastically improving the measurement quality while eliminating the need for neutral beam pulsing. The method also allows for simultaneous measurement of multiple polarized transitions within the Stark multiplet. The upgraded MSE diagnostic was used to measure the magnetic field pitch angle profile in plasmas with some or all of the plasma current driven by lhcd. Measurements were made across a range of single-parameter scans: lhcd power, loop voltage, plasma density, plasma current, and launched n// spectrum. The current profile is observed to broaden during lhcd, but consistently has significant on-axis current density, even in fully non-inductive plasmas. The current profile and hard x-ray (HXR) profiles are observed to be most sensitive to plasma current, with higher current yielding broader profiles. The current and HXR profiles as well as global current-drive efficiency are insensitive to changes in n// or loop voltage. Numerical simulations by the ray-tracing Fokker-Planck GENRAY/CQL3D code reproduce the total measured current in non-inductive conditions but fail to accurately predict the current and HXR profiles; the simulations consistently predict more current drive in the outer half of the plasma than is observed. This leads to a flattening of the HXR profile compared to the experimental profiles. These qualitative discrepancies persist across the range of plasma parameters scanned. Varying code inputs within their measurement uncertainties and adding experimentally-constrained levels of fast-electron diffusion do not reconcile profile discrepancies. Some qualitative profile trends in single parameter scans are reproduced by the simulations including broadening of profiles at higher current, and a weak dependence on the launched n//spectrum. However, HXR profile self-similarity across different densities and powers is not reproduced. These new comparisons between profile measurements and simulation suggest that the simulations are missing important physics in this operational regime.