{"id":7685,"date":"2021-09-09T14:17:12","date_gmt":"2021-09-09T14:17:12","guid":{"rendered":"https:\/\/www.istp.cnr.it\/?post_type=product&#038;p=7685"},"modified":"2022-06-21T14:41:08","modified_gmt":"2022-06-21T14:41:08","slug":"no2v-collisions-reactive-inelastic-and-dissociation-rates-for-state-to-state-vibrational-kinetic-models-2","status":"publish","type":"product","link":"https:\/\/www.istp.cnr.it\/it\/research-product\/no2v-collisions-reactive-inelastic-and-dissociation-rates-for-state-to-state-vibrational-kinetic-models-2\/","title":{"rendered":"N+O2(v) collisions: reactive, inelastic and dissociation rates for state-to-state vibrational kinetic models"},"content":{"rendered":"<p>The reactive, inelastic and dissociation vibrationally-detailed rate coefficients of the N+O2 collision processes, previously calculated by means of a QCT method, have been interpolated as a function of the initial and final vibrational levels and of the temperature, in the range 1000 &#8211; 20000 K. These rates have been implemented in a N2\/N\/O2\/O\/NO mixture state-to-state kinetic model. The model has been tested in a couple of applications. The first consists in its time evolution, for 10-3 s, from an equilibrium composition at 4000\/3000K towards a new composition obtained by suddenly decreasing the temperature to 1000K. This is a preliminary study that could open the way to a new approach in the investigation of some biomedical applications governed by plasma sources at atmospheric pressure.  The second test regards the boundary layer formed around the nose of a hypersonic vehicle in the framework of the fast transportation and space tourism applications.<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Armenise I.; Esposito F.<\/p>\n","protected":false},"featured_media":2274,"comment_status":"closed","ping_status":"closed","template":"","meta":[],"product_cat":[574],"product_tag":[3033,3034,3035,3036],"class_list":["post-7685","product","type-product","status-publish","has-post-thumbnail","hentry","product_cat-journal-articles","product_tag-rate-coefficients-interpolation","product_tag-no2v-collisions","product_tag-state-to-state-vibrational-kinetics","product_tag-n2-n-o2-o-no-mixture","prodpage-style2"],"acf":[],"_links":{"self":[{"href":"https:\/\/www.istp.cnr.it\/it\/wp-json\/wp\/v2\/product\/7685","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=7685"}],"wp:featuredmedia":[{"embeddable":true,"href":"https:\/\/www.istp.cnr.it\/it\/wp-json\/wp\/v2\/media\/2274"}],"wp:attachment":[{"href":"https:\/\/www.istp.cnr.it\/it\/wp-json\/wp\/v2\/media?parent=7685"}],"wp:term":[{"taxonomy":"product_cat","embeddable":true,"href":"https:\/\/www.istp.cnr.it\/it\/wp-json\/wp\/v2\/product_cat?post=7685"},{"taxonomy":"product_tag","embeddable":true,"href":"https:\/\/www.istp.cnr.it\/it\/wp-json\/wp\/v2\/product_tag?post=7685"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}