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Modelling saturated tearing modes in tokamaks.McLoud, Willem Stephanus. January 1992 (has links)
In this thesis a model for saturated tearing mode islands is developed. The equations for
the mode amplitudes are essentially those of R B White et al,after a pertubation
expansion has been made. It is well known that these equations are not then analytic at
the mode rational surface. In our model this problem is overcome when a suitable choice of
the axisymmetric current density perturbation is added to the unperturbed equilibrium
current density profile. The modelled axisymmetric current density perturbation flattens
the unperturbed profile locally at the rational surface and is sufficient to induce an island.
No modelling in the interior of the island is necessary.
The axisymmetric perturbation has a free variable which adjusts the amount of local
flattening. However, when the boundary conditions are taken into account, this free
parameter is determined, and the problem becomes an eigenvalue problem. The boundary
condition thus determines the amount of local flattening at the rational surface.
The saturated island widths are determined using D.' (W) criterion. The model allows
for non axsymmetric plasma surface in a simple way, requiring careful choice of D (W).
The different criteria are compared to establish the validity of the use of such criteria for
perturbed boundaries.
In the cylindrical approximation, one or two modes may be included in the model. In the
case of two modes, non-linear coupling via the current density profile is introduced.
Toroidal coupling between modes can also be simply introduced. Two modes that are
toroidally coupled are considered, but mode-mode coupling is ignored.
The emphasis falls in large part on the boundary conditions. Various boundary conditions
can be considered because distortion of the plasma surface can be fixed by wall effects,
plasma rotation, external DC coil currents, plasma rotation with external coil currents, etc.
Of particular interest is the case of toroidally coupled modes, coupled in turn to these
external conditions as this is the first study of such a nature.
Results flowing from the study include among others that:
for the special case of circular boundaries the model agrees reasonably with the
results of R B White et al.
No significant difference was found between the D. I (W) criterion of P H
Rutherford, which is valid for circular boundaries, and that of A H Reiman, which is
also valid for perturbed boundaries, when the boundary is perturbed significantly.
Toroidally coupled islands do not increase in size if the boundary condition of that
particular mode is not changed. If a coil current of particular helicity is switched
on, it will only affect the mode of that particular helicity.
Toroidally induced sideband islands have approximately the same width as natural
tearing islands when the size of the natural island is large. / Thesis (Ph.D.)-University of Natal, Durban, 1992.
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Development of a unified mass and heat integration framework for sustainable design an automated approach /Moodley, Anand. January 2007 (has links)
Thesis (M.Eng. (Chemical Engineering)) -- Universiteit van Pretoria, 2007. / Includes bibliographical references.
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Experimental and numerical investigation of the thermal performance of gas-cooled divertor modulesCrosatti, Lorenzo January 2008 (has links)
Thesis (Ph.D.)--Mechanical Engineering, Georgia Institute of Technology, 2008. / Committee Co-Chair: Minami Yoda, Co-Advisor; Committee Co-Chair: Said I. Abdel-Khalik; Committee Member: Donald R. Webster; Committee Member: Narayanan M. Komerath; Committee Member: S. Mostafa Ghiaasiaan; Committee Member: Yogendra Joshi
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Resistive Z-pinch equilibria and stabilityCulverwell, Ian Dennis January 1990 (has links)
No description available.
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Skakelmoduskragbron vir plasmatoepassingsRoos, Stefanus Dawid 14 August 2012 (has links)
M.Ing. / 50 Hz technology has led the plasma torch converters up to now. This technology was used. The high power levels of plasma torches made it difficult to implement high frequency technology. At this stage it is possible to use high-frequency technology in plasma torch applications. This thesis implements a high frequency converter suitable for plasma applications. The converter used for this application is the Partial Series Resonant Converter. A study launched to get the properties of plasmas showed that the control method used at this stage namely current control is not the ideal control method. Changing the control method of the converter made it possible to see what influence it has on the plasma. A thorough large signal analisis of the Partial Series Resonant Converter was done. From this analisis a transfer function of the converter was developed and the control parameters were calculated. This control parameters made it possible to change the control and to investigate the different control methods. The design of the plasma torch converter was based on the design of a distributed transformer, input and output filter and a non-linear controller. The results of the Partial Series Resonant Converter showed that power control leads to a more stable plasma. This thesis made a positive contribution to the knowledge of plasma torches and the knowledge of plasma torch converters. The thesis forms a summarry of plasmas and plasma-related topics, and futher study fields are defined by this thesis.
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Study of high-impurity accumulation and transport in the JET tokamak plasmas from soft X-ray tomographyRomanelli, Michele January 1998 (has links)
No description available.
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Particle orbits and diffusion in torsatronsPotok, Robert Edward January 1980 (has links)
Thesis (Sc.D.)--Massachusetts Institute of Technology, Dept. of Nuclear Engineering, 1980. / MICROFICHE COPY AVAILABLE IN ARCHIVES AND SCIENCE. / Includes bibliographical references. / by Robert Edward Potok. / Sc.D.
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An Electro- Magneto-static Field for Confinement of Charged Particle Beams and PlasmasPacheco, Josè L. 05 1900 (has links)
A system is presented that is capable of confining an ion beam or plasma within a region that is essentially free of applied fields. An Artificially Structured Boundary (ASB) produces a spatially periodic set of magnetic field cusps that provides charged particle confinement. Electrostatic plugging of the magnetic field cusps enhances confinement. An ASB that has a small spatial period, compared to the dimensions of a confined plasma, generates electro- magneto-static fields with a short range. An ASB-lined volume thus constructed creates an effectively field free region near its center. It is assumed that a non-neutral plasma confined within such a volume relaxes to a Maxwell-Boltzmann distribution. Space charge based confinement of a second species of charged particles is envisioned, where the second species is confined by the space charge of the first non-neutral plasma species. An electron plasma confined within an ASB-lined volume can potentially provide confinement of a positive ion beam or positive ion plasma. Experimental as well as computational results are presented in which a plasma or charged particle beam interact with the electro- magneto-static fields generated by an ASB. A theoretical model is analyzed and solved via self-consistent computational methods to determine the behavior and equilibrium conditions of a relaxed plasma. The equilibrium conditions of a relaxed two species plasma are also computed. In such a scenario, space charge based electrostatic confinement is predicted to occur where a second plasma species is confined by the space charge of the first plasma species. An experimental apparatus with cylindrical symmetry that has its interior surface lined with an ASB is presented. This system was developed by using a simulation of the electro- magneto-static fields present within the trap to guide mechanical design. The construction of the full experimental apparatus is discussed. Experimental results that show the characteristics of electron beam transmission through the experimental apparatus are presented. A description of the experimental hardware and software used for trapping a charged particle beam or plasma is also presented.
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MHD Stability and Confinement of Plasmas in a Single Mirror CellSavenko, Natalia January 2006 (has links)
<p>Thermonuclear fusion is a promising energy source for the future. If an economically efficient thermonuclear reactor would be built it has to be a cheap, safe, and highly productive electric power plant, or, a heating plant.</p><p>The emphasis of this thesis is on the single cell mirror trap with a marginally stable minimum B vacuum magnetic field, the straight field line mirror field, which provides MHD stability of the system, absence of the radial drift even to the first order in plasma β , and a reduced magnetic flux tube ellipticity. Strong density depletion at the mirrors is proposed as a mean to build up a strong potential barrier for the electrons and thereby increase the electron temperature. Conditions to obtain an energy gain factor Q>10 are briefly analyzed. Current coils which could generate the derived magnetic field are proposed. A sloshing ion distribution function is constructed for the three dimensional ‘straight line mirror field’. The gyro centre Clebsch coordinates are found to be a new pair of motional invariants for this magnetic field. The gyro centre Clebsch coordinate invariants can be used to obtain complete solutions of the Vlasov equation, including the diamagnetic drift. These solutions show that the equilibria satisfy the locally omniginuity criterion to the first order in β .</p><p>Contributions of the plasma diamagnetism to the magnetic flux tube ellipticity are studied for the straight field line mirror vacuum magnetic field and a sloshing ion distribution. Computations employing ray tracing have shown that there is a modest increase in the ellipticity, but the effect is small if β <0.2 .</p><p>Adiabatic charged particle motion in general field geometry has been studied. A set of four independent stationary invariants, the energy, the magnetic moment, the radial drift invariant, and the bounce average parallel velocity is proposed to describe adiabatic equilibria. </p>
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MHD Stability and Confinement of Plasmas in a Single Mirror CellSavenko, Natalia January 2006 (has links)
Thermonuclear fusion is a promising energy source for the future. If an economically efficient thermonuclear reactor would be built it has to be a cheap, safe, and highly productive electric power plant, or, a heating plant. The emphasis of this thesis is on the single cell mirror trap with a marginally stable minimum B vacuum magnetic field, the straight field line mirror field, which provides MHD stability of the system, absence of the radial drift even to the first order in plasma β , and a reduced magnetic flux tube ellipticity. Strong density depletion at the mirrors is proposed as a mean to build up a strong potential barrier for the electrons and thereby increase the electron temperature. Conditions to obtain an energy gain factor Q>10 are briefly analyzed. Current coils which could generate the derived magnetic field are proposed. A sloshing ion distribution function is constructed for the three dimensional ‘straight line mirror field’. The gyro centre Clebsch coordinates are found to be a new pair of motional invariants for this magnetic field. The gyro centre Clebsch coordinate invariants can be used to obtain complete solutions of the Vlasov equation, including the diamagnetic drift. These solutions show that the equilibria satisfy the locally omniginuity criterion to the first order in β . Contributions of the plasma diamagnetism to the magnetic flux tube ellipticity are studied for the straight field line mirror vacuum magnetic field and a sloshing ion distribution. Computations employing ray tracing have shown that there is a modest increase in the ellipticity, but the effect is small if β <0.2 . Adiabatic charged particle motion in general field geometry has been studied. A set of four independent stationary invariants, the energy, the magnetic moment, the radial drift invariant, and the bounce average parallel velocity is proposed to describe adiabatic equilibria.
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