{"id":6774,"date":"2019-07-11T15:53:06","date_gmt":"2019-07-11T15:53:06","guid":{"rendered":"https:\/\/www.istp.cnr.it\/?post_type=product&#038;p=6774"},"modified":"2022-06-21T10:35:46","modified_gmt":"2022-06-21T10:35:46","slug":"high-n-tearing-mode-dynamics-in-fast-rotating-rfp-plasmas","status":"publish","type":"product","link":"https:\/\/www.istp.cnr.it\/it\/research-product\/high-n-tearing-mode-dynamics-in-fast-rotating-rfp-plasmas\/","title":{"rendered":"High-n tearing mode dynamics in fast rotating RFP plasmas"},"content":{"rendered":"<p>The Reversed Field Pinch (RFP) configuration is often characterized by a wide spectrum of unstable  tearing  modes  (TMs)  involved  in  the  generation  and  sustainment  of  the  magnetic field  in  the  plasma.  This  dynamo  process  is  heavily  influenced  also  by  other  processes  or parameters  like  intrinsic  plasma  flow  (no  external torque  sources  are  normally  present), wall  resistivity  and  interaction  with  external  non axi-symmetric  magnetic  fields  provided by active coils. The  transition  between  fast-slow  rotation  branches under  the  application  of  magnetic feedback boundary conditions was studied in [1] for the case of RFX-mod, a medium size (a = 0.459 m, R0 = 2m) flexible toroidal magnetic confinement device. In particular, RFX-mod is equipped with an advanced and sophisticated feedback system realized by a grid of independently controlled 48 (toroidal) x4 (poloidal) active saddle coils. In  this  contribution  the  interaction  of  the  m=1,  n>9  tearing  modes  with  the  bulk  plasma close to the fast-slow transition threshold is investigated with the help of a systematic set of experiments where the active feedback control is selectively switched on and off on specific modes during the discharge dynamics. The peculiar result found is that also in fast rotating discharges,  although  the  radial  component  at  the  wall  of  high  n  tearing  modes  is  almost zero, in the absence of active feedback control a gradual modification (growth) of the total mode  amplitude  is  measured,  leading  potentially  to wall  locking  of  that  mode  and  to  the back  transition  to  the  slow  rotation  branch.  Data  showing  the  mode-mode  and  mode-wall interaction will be presented for several combinations of non-controlled TMs. The process is  discussed  also  in  function  of  the  dynamics  of  the  plasma  flow,  following  the  lines presented in [2], and showing the clear correlation between active control, MHD dynamics and plasma flow.<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Bolzonella T.; Cavazzana R.; Innocente P.; Zanca P.; Zaniol B.; Zuin M.<\/p>\n","protected":false},"featured_media":1294,"comment_status":"closed","ping_status":"open","template":"","meta":[],"product_cat":[704],"product_tag":[763,820,1260,1274],"class_list":["post-6774","product","type-product","status-publish","has-post-thumbnail","hentry","product_cat-conference-proceedings","product_tag-reversed-field-pinch","product_tag-tearing-modes","product_tag-rfp","product_tag-tms","prodpage-style2"],"acf":[],"_links":{"self":[{"href":"https:\/\/www.istp.cnr.it\/it\/wp-json\/wp\/v2\/product\/6774","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/www.istp.cnr.it\/it\/wp-json\/wp\/v2\/product"}],"about":[{"href":"https:\/\/www.istp.cnr.it\/it\/wp-json\/wp\/v2\/types\/product"}],"replies":[{"embeddable":true,"href":"https:\/\/www.istp.cnr.it\/it\/wp-json\/wp\/v2\/comments?post=6774"}],"wp:featuredmedia":[{"embeddable":true,"href":"https:\/\/www.istp.cnr.it\/it\/wp-json\/wp\/v2\/media\/1294"}],"wp:attachment":[{"href":"https:\/\/www.istp.cnr.it\/it\/wp-json\/wp\/v2\/media?parent=6774"}],"wp:term":[{"taxonomy":"product_cat","embeddable":true,"href":"https:\/\/www.istp.cnr.it\/it\/wp-json\/wp\/v2\/product_cat?post=6774"},{"taxonomy":"product_tag","embeddable":true,"href":"https:\/\/www.istp.cnr.it\/it\/wp-json\/wp\/v2\/product_tag?post=6774"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}