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DC Field | Value | Language |
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dc.contributor.advisor | Gorelenkov, Nikolai | en_US |
dc.contributor.author | Ghantous, Katy | en_US |
dc.contributor.other | Astrophysical Sciences Department | en_US |
dc.date.accessioned | 2013-12-07T23:15:19Z | - |
dc.date.available | 2013-12-07T23:15:19Z | - |
dc.date.issued | 2013 | en_US |
dc.identifier.uri | http://arks.princeton.edu/ark:/88435/dsp01w95050599 | - |
dc.description.abstract | The Line Broadened Quasilinear (LBQ) and the 1.5D reduced models are able to predict the effect of Alfvenic eigenmodes' interaction with energetic particles in burning plasmas. This interaction can result in energetic-particle losses that can damage the first wall, deteriorate the plasma performance, and even prevent ignition. The 1.5D model assumes a broad spectrum of overlapping modes and, based on analytic expressions for the growth and damping rates, calculates the pressure profiles that the energetic particles relax to upon interacting with the modes. 1.5D is validated with DIII-D experiments and predicted neutron losses consistent with observation. The model is employed to predict alpha-particle fusion-product losses in a large-scale operational parameter-space for burning plasmas. \par The LBQ model captures the interaction both in the regime of isolated modes as well as in the conventional regime of overlapping modes. Rules were established that allow quasilinear equations to replicate the expected steady-state saturation levels of isolated modes. The fitting formula is improved and the model is benchmarked with a Vlasov code, BOT. The saturation levels are accurately predicted and the mode evolution is well-replicated in the case of steady-state evolution where the collisions are high enough that coherent structures do not form. When the collisionality is low, oscillatory behavior can occur. LBQ can also exhibit non-steady behavior, but the onset of oscillations occurs for much higher collisional rates in BOT than in LBQ. For certain parameters of low collisionality, hole-clump creation and frequency chirping can occur which are not captured by the LBQ model. Also, there are cases of non-steady evolution without chirping which is possible for LBQ to study. However the results are inconclusive since the periods and amplitudes of the oscillations in the mode evolution are not well-replicated. If multiple modes exist, they can grow to the point of overlap which results in two-dimensional diffusion with cross terms. A diffusion scheme is proposed and validated to resolve this dynamics in (P,E) phase-space. | en_US |
dc.language.iso | en | en_US |
dc.publisher | Princeton, NJ : Princeton University | en_US |
dc.relation.isformatof | The Mudd Manuscript Library retains one bound copy of each dissertation. Search for these copies in the <a href=http://catalog.princeton.edu> library's main catalog </a> | en_US |
dc.subject | Alfvenic Eigenmodes | en_US |
dc.subject | burning plasmas | en_US |
dc.subject | energetic particles | en_US |
dc.subject | quasilinear thoery | en_US |
dc.subject | transport | en_US |
dc.subject | wave-particle interaction | en_US |
dc.subject.classification | Plasma physics | en_US |
dc.title | Reduced Quasilinear Models for Energetic Particles Interaction with Alfvenic Eigenmodes | en_US |
dc.type | Academic dissertations (Ph.D.) | en_US |
pu.projectgrantnumber | 690-2143 | en_US |
Appears in Collections: | Plasma Physics |
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Ghantous_princeton_0181D_10772.pdf | 4.57 MB | Adobe PDF | View/Download |
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