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Asymmetric Halo Current Rotation in Post-Disruption Plasmas- [electronic resource]
Asymmetric Halo Current Rotation in Post-Disruption Plasmas - [electronic resource]
Asymmetric Halo Current Rotation in Post-Disruption Plasmas- [electronic resource]

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자료유형  
 학위논문파일 국외
최종처리일시  
20240214101237
ISBN  
9798379793159
DDC  
530
저자명  
Saperstein, Alex R. .
서명/저자  
Asymmetric Halo Current Rotation in Post-Disruption Plasmas - [electronic resource]
발행사항  
[S.l.]: : Columbia University., 2023
발행사항  
Ann Arbor : : ProQuest Dissertations & Theses,, 2023
형태사항  
1 online resource(183 p.)
주기사항  
Source: Dissertations Abstracts International, Volume: 85-01, Section: B.
주기사항  
Advisor: Mauel, Michael.
학위논문주기  
Thesis (Ph.D.)--Columbia University, 2023.
사용제한주기  
This item must not be sold to any third party vendors.
초록/해제  
요약Halo currents (HCs) in post-disruption plasmas can be large enough to exert significant electromagnetic loads on structures surrounding the plasma. These currents have axisymmetric and non-axisymmetric components, both of which pose threats to the vacuum vessel and other components. However, the non-axisymmetric forces can rotate, amplifying the displacements they cause when the rotation is close to the structures' resonant frequencies. A new physically motivated scaling law has been developed that describes the rotation frequencies of these HCs and has been validated against measurements on HBT-EP, Alcator C-Mod, and other tokamaks [1, 2]. This scaling law can describe the time-evolution of the asymmetric HC rotation throughout disruptions on HBT-EP as well as the time-averaged rotation on C-Mod. The scaling law can also be modified to include the edge safety factor at the onset of rotation (qonset), which significantly improves its validity when applied to machines like C-Mod, where qonset changes frequently. The qonset dependence is explained by the relationship between the poloidal structure of the HC asymmetries and the MHD instabilities that drive them, which has been observed experimentally for the first time using a novel set of current sensing limiter tiles installed on HBT-EP. The 1/a2 and qonset-dependence of the rotation suggest that the HCs predominantly rotate poloidally. This remains consistent with the toroidal rotation observed on HBT-EP and other tokamaks through the "Barber Pole Illusion" and the direction of rotation's dependence on the direction of Ip. This scaling law is used to make projections for next generation tokamaks like ITER and SPARC, which predicts that rotation will be resonant on ITER. However, resonant effects can still be avoided if the duration of the disruption is kept short enough to prevent two rotations from being completed [3].
일반주제명  
Plasma physics.
일반주제명  
Electromagnetics.
키워드  
Fusion
키워드  
Halo currents
키워드  
Tokamaks
키워드  
Non-axisymmetric components
키워드  
Vacuum vessel
기타저자  
Columbia University Applied Physics
기본자료저록  
Dissertations Abstracts International. 85-01B.
기본자료저록  
Dissertation Abstract International
전자적 위치 및 접속  
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■001000016933359
■00520240214101237
■006m          o    d                
■007cr#unu||||||||
■020    ▼a9798379793159
■035    ▼a(MiAaPQ)AAI30528051
■040    ▼aMiAaPQ▼cMiAaPQ
■0820  ▼a530
■1001  ▼aSaperstein,  Alex  R.  .
■24510▼aAsymmetric  Halo  Current  Rotation  in  Post-Disruption  Plasmas▼h[electronic  resource]
■260    ▼a[S.l.]:▼bColumbia  University.  ▼c2023
■260  1▼aAnn  Arbor  :▼bProQuest  Dissertations  &  Theses,  ▼c2023
■300    ▼a1  online  resource(183  p.)
■500    ▼aSource:  Dissertations  Abstracts  International,  Volume:  85-01,  Section:  B.
■500    ▼aAdvisor:  Mauel,  Michael.
■5021  ▼aThesis  (Ph.D.)--Columbia  University,  2023.
■506    ▼aThis  item  must  not  be  sold  to  any  third  party  vendors.
■520    ▼aHalo  currents  (HCs)  in  post-disruption  plasmas  can  be  large  enough  to  exert  significant  electromagnetic  loads  on  structures  surrounding  the  plasma.  These  currents  have  axisymmetric  and  non-axisymmetric  components,  both  of  which  pose  threats  to  the  vacuum  vessel  and  other  components.  However,  the  non-axisymmetric  forces  can  rotate,  amplifying  the  displacements  they  cause  when  the  rotation  is  close  to  the  structures'  resonant  frequencies.  A  new  physically  motivated  scaling  law  has  been  developed  that  describes  the  rotation  frequencies  of  these  HCs  and  has  been  validated  against  measurements  on  HBT-EP,  Alcator  C-Mod,  and  other  tokamaks  [1,  2].  This  scaling  law  can  describe  the  time-evolution  of  the  asymmetric  HC  rotation  throughout  disruptions  on  HBT-EP  as  well  as  the  time-averaged  rotation  on  C-Mod.  The  scaling  law  can  also  be  modified  to  include  the  edge  safety  factor  at  the  onset  of  rotation  (qonset),  which  significantly  improves  its  validity  when  applied  to  machines  like  C-Mod,  where  qonset  changes  frequently.  The  qonset  dependence  is  explained  by  the  relationship  between  the  poloidal  structure  of  the  HC  asymmetries  and  the  MHD  instabilities  that  drive  them,  which  has  been  observed  experimentally  for  the  first  time  using  a  novel  set  of  current  sensing  limiter  tiles  installed  on  HBT-EP.  The  1/a2  and  qonset-dependence  of  the  rotation  suggest  that  the  HCs  predominantly  rotate  poloidally.  This  remains  consistent  with  the  toroidal  rotation  observed  on  HBT-EP  and  other  tokamaks  through  the  "Barber  Pole  Illusion"  and  the  direction  of  rotation's  dependence  on  the  direction  of  Ip.  This  scaling  law  is  used  to  make  projections  for  next  generation  tokamaks  like  ITER  and  SPARC,  which  predicts  that  rotation  will  be  resonant  on  ITER.  However,  resonant  effects  can  still  be  avoided  if  the  duration  of  the  disruption  is  kept  short  enough  to  prevent  two  rotations  from  being  completed  [3].
■590    ▼aSchool  code:  0054.
■650  4▼aPlasma  physics.
■650  4▼aElectromagnetics.
■653    ▼aFusion
■653    ▼aHalo  currents
■653    ▼aTokamaks
■653    ▼aNon-axisymmetric  components
■653    ▼aVacuum  vessel
■690    ▼a0759
■690    ▼a0607
■71020▼aColumbia  University▼bApplied  Physics.
■7730  ▼tDissertations  Abstracts  International▼g85-01B.
■773    ▼tDissertation  Abstract  International
■790    ▼a0054
■791    ▼aPh.D.
■792    ▼a2023
■793    ▼aEnglish
■85640▼uhttp://www.riss.kr/pdu/ddodLink.do?id=T16933359▼nKERIS▼z이  자료의  원문은  한국교육학술정보원에서  제공합니다.
■980    ▼a202402▼f2024

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