{"id":7970,"date":"2022-05-02T17:00:12","date_gmt":"2022-05-02T17:00:12","guid":{"rendered":"https:\/\/www.istp.cnr.it\/?post_type=product&#038;p=7970"},"modified":"2023-01-13T11:06:26","modified_gmt":"2023-01-13T11:06:26","slug":"dynamics-of-ultralow-q-plasmas-in-the-rfx-mod-device","status":"publish","type":"product","link":"https:\/\/www.istp.cnr.it\/it\/research-product\/dynamics-of-ultralow-q-plasmas-in-the-rfx-mod-device\/","title":{"rendered":"Dynamics of ultralow-q plasmas in the RFX-mod device"},"content":{"rendered":"<p>The results are presented of an experimental activity performed in the RFX-mod device aimed at characterizing plasma dynamics in the so-called Ultralow-q (ULq) magnetic configuration, which corresponds to edge safety factor values below 1. The role of the edge safety factor in determining plasma dynamics is studied. In particular, a characterization of MHD activity is performed. The results of dedicated non-linear 3D visco-resistive MHD simulations are in good quantitative agreement with the experimental observations. In particular, the predicted tendency for ULq plasmas to be characterized by magnetic spectra dominated by a single mode (either a kink or a double resonant internal mode) is confirmed by experiment. Magnetic reconnection plays a relevant role in determining the dynamics of the magnetic topology. Both almost quiescent and largely fluctuating plasmas are observed with a strong sensitivity on the edge safety factor. The main MHD properties of the ULq are compared to those of RFP and tokamak discharges, also produced in the RFX-mod device. MHD modes exhibit toroidal rotation at a frequency depending on mode amplitude. Differently from what encountered in RFP plasmas at comparable current levels, no wall locking is detected.<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Zuin, M.; Agostini, M.; Auriemma, F.; Bonfiglio, D.; Cappello, S.; Carraro, L.; Cavazzana, R.; Cordaro, L.; Franz, P.; Marrelli, L.; Martines, E.; Puiatti, M. E.; Piovan, R.; Spizzo, G.; Terranova, D.; Vianello, N.; Zanca, P.; Zaniol, B.; Zanotto, L.<\/p>\n","protected":false},"featured_media":1294,"comment_status":"closed","ping_status":"open","template":"","meta":[],"product_cat":[574],"product_tag":[760,835,1260,1291,3519,3520],"class_list":["post-7970","product","type-product","status-publish","has-post-thumbnail","hentry","product_cat-journal-articles","product_tag-mhd","product_tag-magnetic-confinement","product_tag-rfp","product_tag-reconnection","product_tag-ultra-low-q","product_tag-mode-control","prodpage-style2"],"acf":[],"_links":{"self":[{"href":"https:\/\/www.istp.cnr.it\/it\/wp-json\/wp\/v2\/product\/7970","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=7970"}],"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=7970"}],"wp:term":[{"taxonomy":"product_cat","embeddable":true,"href":"https:\/\/www.istp.cnr.it\/it\/wp-json\/wp\/v2\/product_cat?post=7970"},{"taxonomy":"product_tag","embeddable":true,"href":"https:\/\/www.istp.cnr.it\/it\/wp-json\/wp\/v2\/product_tag?post=7970"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}