{"id":2491,"date":"2021-12-13T00:00:46","date_gmt":"2021-12-13T00:00:46","guid":{"rendered":"https:\/\/www.istp.cnr.it\/?post_type=product&#038;p=2491"},"modified":"2022-05-29T15:57:51","modified_gmt":"2022-05-29T15:57:51","slug":"h-mode-plasmas-in-the-pre-fusion-power-operation-1-phase-of-the-iter-research-plan","status":"publish","type":"product","link":"https:\/\/www.istp.cnr.it\/it\/research-product\/h-mode-plasmas-in-the-pre-fusion-power-operation-1-phase-of-the-iter-research-plan\/","title":{"rendered":"H-mode plasmas in the pre-fusion power operation 1 phase of the ITER research plan"},"content":{"rendered":"<p>The optimum conditions for access to and sustainment of H-mode plasmas and their expected plasma parameters in the pre-fusion power operation 1 (PFPO-1) phase of the ITER research plan, where the additional plasma heating will be provided by 20 MW of electron cyclotron heating, are assessed in order to identify key open R&#038;D issues. The assessment is performed on the basis of empirical and physics-based scalings derived from present experiments and integrated modelling of these plasmas including a range of first-principle transport models for the core plasma. The predictions of the integrated modelling of ITER H-mode plasmas are compared with ITER-relevant experiments carried out at JET (low-collisionality high-current H modes) and ASDEX Upgrade (significant electron heating) for both global H-mode properties and scale lengths of density and temperature profiles finding reasonable agreement. Specific integration issues of the PFPO-1 H-mode plasma scenarios are discussed taking into account the impact of the specificities of the ITER tokamak design (level of ripple, etc).<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Loarte A.; Polevoi A.R.; Schneider M.; Pinches S.D.; Fable E.; Militello Asp E.; Baranov Y.; Casson F.; Corrigan G.; Garzotti L.; Harting D.; Knight P.; Koechl F.; Parail V.; Farina D.; Figini L.; Nordman H.; Strand P.; Sartori R.<\/p>\n","protected":false},"featured_media":2687,"comment_status":"closed","ping_status":"closed","template":"","meta":[],"product_cat":[574,524],"product_tag":[765,766,767,768,769,770],"class_list":["post-2491","product","type-product","status-publish","has-post-thumbnail","hentry","product_cat-journal-articles","product_cat-thermonuclear-fusion","product_tag-h-mode","product_tag-iter","product_tag-pre-fusion-power","product_tag-core-transport","product_tag-pedestal","product_tag-core-edge-integration","prodpage-style2"],"acf":[],"_links":{"self":[{"href":"https:\/\/www.istp.cnr.it\/it\/wp-json\/wp\/v2\/product\/2491","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=2491"}],"wp:featuredmedia":[{"embeddable":true,"href":"https:\/\/www.istp.cnr.it\/it\/wp-json\/wp\/v2\/media\/2687"}],"wp:attachment":[{"href":"https:\/\/www.istp.cnr.it\/it\/wp-json\/wp\/v2\/media?parent=2491"}],"wp:term":[{"taxonomy":"product_cat","embeddable":true,"href":"https:\/\/www.istp.cnr.it\/it\/wp-json\/wp\/v2\/product_cat?post=2491"},{"taxonomy":"product_tag","embeddable":true,"href":"https:\/\/www.istp.cnr.it\/it\/wp-json\/wp\/v2\/product_tag?post=2491"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}