{"id":1646,"date":"2019-12-13T16:22:20","date_gmt":"2019-12-13T16:22:20","guid":{"rendered":"http:\/\/www.icterra.pt\/?p=1646"},"modified":"2019-12-18T11:40:10","modified_gmt":"2019-12-18T11:40:10","slug":"the-unprecedented-2017-2018-stratospheric-smoke-event-decay-phase-and-aerosol-properties-observed-with-the-earlinet","status":"publish","type":"post","link":"https:\/\/www.icterra.pt\/legacy\/index.php\/2019\/12\/13\/the-unprecedented-2017-2018-stratospheric-smoke-event-decay-phase-and-aerosol-properties-observed-with-the-earlinet\/","title":{"rendered":"The unprecedented 2017\u20132018 stratospheric smoke event: decay phase and aerosol properties observed with the EARLINET"},"content":{"rendered":"<p style=\"text-align: justify;\">Baars, H., Ansmann, A., Ohneiser, K., Haarig, M., Engelmann, R., Althausen, D., Hanssen, I., Gausa, M., Pietruczuk, A., Szkop, A., Stachlewska, I. S., Wang, D., Reichardt, J., Skupin, A., Mattis, I., Trickl, T., Vogelmann, H., Navas-Guzm\u00e1n, F., Haefele, A., Acheson, K., Ruth, A. A., Tatarov, B., M\u00fcller, D., Hu, Q., Podvin, T., Goloub, P., Veselovskii, I., Pietras, C., Haeffelin, M., Fr\u00e9ville, P., Sicard, M.,\u00a0 Comer\u00f3n, A., Fern\u00e1ndez Garc\u00eda, A. J., Molero Men\u00e9ndez, F., C\u00f3rdoba-Jabonero, C., Guerrero-Rascado, J. L., Alados-Arboledas, L., Bortoli, D., Costa, M. J., Dionisi, D., Liberti, G. L., Wang, X., Sannino, A., Papagiannopoulos, N., Boselli, A., Mona, L., D&#8217;Amico, G., Romano, S., Perrone, M. R., Belegante, L., Nicolae, D., Grigorov, I., Gialitaki, A., Amiridis, V., Soupiona, O., Papayannis, A., Mamouri, R.-E., Nisantzi, A., Heese, B., Hofer, J., Schechner, Y. Y., Wandinger, U., and Pappalardo, G.: The unprecedented 2017\u20132018 stratospheric smoke event: decay phase and aerosol properties observed with the EARLINET,<br \/>\nAtmos. Chem. Phys., 19, 15183\u201315198,<\/p>\n<p style=\"text-align: justify;\">Six months of stratospheric aerosol observations with the European Aerosol Research Lidar Network (EARLINET) from August 2017 to January 2018 are presented. The decay phase of an unprecedented, record-breaking stratospheric perturbation caused by wildfire smoke is reported and discussed in terms of geometrical, optical, and microphysical aerosol properties. Enormous amounts of smoke were injected into the upper troposphere and lower stratosphere over fire areas in western Canada on 12\u00a0August 2017 during strong thunderstorm\u2013pyrocumulonimbus activity. The stratospheric fire plumes spread over the entire Northern Hemisphere in the following weeks and months. Twenty-eight European lidar stations from northern Norway to southern Portugal and the eastern Mediterranean monitored the strong stratospheric perturbation on a continental scale. The main smoke layer (over central, western, southern, and eastern Europe) was found at heights between 15 and 20\u2009km since September 2017 (about 2 weeks after entering the stratosphere). Thin layers of smoke were detected at heights of up to 22\u201323\u2009km. The stratospheric aerosol optical thickness at 532\u2009nm decreased from values <span class=\"inline-formula\">&gt;<\/span>\u20090.25 on 21\u201323\u00a0August 2017 to 0.005\u20130.03 until 5\u201310 September and was mainly 0.003\u20130.004 from October to December\u00a02017 and thus was still significantly above the stratospheric background (0.001\u20130.002). Stratospheric particle extinction coefficients (532\u2009nm) were as high as 50\u2013200\u2009Mm<span class=\"inline-formula\"><sup>\u22121<\/sup><\/span> until the beginning of September and on the order of 1\u2009Mm<span class=\"inline-formula\"><sup>\u22121<\/sup><\/span> (0.5\u20135\u2009Mm<span class=\"inline-formula\"><sup>\u22121<\/sup><\/span>) from October\u00a02017 until the end of January\u00a02018. The corresponding layer mean particle mass concentration was on the order of 0.05\u20130.5\u2009<span class=\"inline-formula\">\u00b5<\/span>g\u2009m<span class=\"inline-formula\"><sup>\u22123<\/sup><\/span> over these months. Soot particles (light-absorbing carbonaceous particles) are efficient ice-nucleating particles (INPs) at upper tropospheric (cirrus) temperatures and available to influence cirrus formation when entering the tropopause from above. We estimated INP concentrations of 50\u2013500\u2009L<span class=\"inline-formula\"><sup>\u22121<\/sup><\/span> until the first days in September and afterwards 5\u201350\u2009L<span class=\"inline-formula\"><sup>\u22121<\/sup><\/span> until the end of the year 2017 in the lower stratosphere for typical cirrus formation temperatures of <span class=\"inline-formula\">\u2212<\/span>55\u2009<span class=\"inline-formula\"><sup>\u2218<\/sup><\/span>C and an ice supersaturation level of 1.15. The measured profiles of the particle linear depolarization ratio indicated a predominance of nonspherical smoke particles. The 532\u2009nm depolarization ratio decreased slowly with time in the main smoke layer from values of 0.15\u20130.25 (August\u2013September) to values of 0.05\u20130.10 (October\u2013November) and <span class=\"inline-formula\">&lt;<\/span>\u20090.05 (December\u2013January). The decrease of the depolarization ratio is consistent with aging of the smoke particles, growing of a coating around the solid black carbon core (aggregates), and thus change of the shape towards a spherical form. We found ascending aerosol layer features over the most southern European stations, especially over the eastern Mediterranean at 32\u201335<span class=\"inline-formula\"><sup>\u2218<\/sup><\/span>\u2009N, that ascended from heights of about 18\u201319 to 22\u201323\u2009km from the beginning of October to the beginning of December\u00a02017 (about 2\u2009km per month). We discuss several transport and lifting mechanisms that may have had an impact on the found aerosol layering structures.<\/p>\n<p>Read the full article <a href=\"https:\/\/doi.org\/10.5194\/acp-19-15183-2019\">here<\/a>.<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Baars, H., Ansmann, A., Ohneiser, K., Haarig, M., Engelmann, R., Althausen, D., Hanssen, I., Gausa, M., Pietruczuk, A., Szkop, A., Stachlewska, I. S., Wang, D., Reichardt, J., Skupin, A., Mattis, I., Trickl, T., Vogelmann, H., Navas-Guzm\u00e1n, F., Haefele, A., Acheson, K., Ruth, A. A., Tatarov, B., M\u00fcller, D., Hu, Q., Podvin, T., Goloub, P., Veselovskii, [&hellip;]<\/p>\n","protected":false},"author":3,"featured_media":0,"comment_status":"closed","ping_status":"closed","sticky":false,"template":"","format":"standard","meta":{"footnotes":""},"categories":[16,163],"tags":[89,86,161,160,159],"_links":{"self":[{"href":"https:\/\/www.icterra.pt\/legacy\/index.php\/wp-json\/wp\/v2\/posts\/1646"}],"collection":[{"href":"https:\/\/www.icterra.pt\/legacy\/index.php\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/www.icterra.pt\/legacy\/index.php\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/www.icterra.pt\/legacy\/index.php\/wp-json\/wp\/v2\/users\/3"}],"replies":[{"embeddable":true,"href":"https:\/\/www.icterra.pt\/legacy\/index.php\/wp-json\/wp\/v2\/comments?post=1646"}],"version-history":[{"count":1,"href":"https:\/\/www.icterra.pt\/legacy\/index.php\/wp-json\/wp\/v2\/posts\/1646\/revisions"}],"predecessor-version":[{"id":1647,"href":"https:\/\/www.icterra.pt\/legacy\/index.php\/wp-json\/wp\/v2\/posts\/1646\/revisions\/1647"}],"wp:attachment":[{"href":"https:\/\/www.icterra.pt\/legacy\/index.php\/wp-json\/wp\/v2\/media?parent=1646"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/www.icterra.pt\/legacy\/index.php\/wp-json\/wp\/v2\/categories?post=1646"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.icterra.pt\/legacy\/index.php\/wp-json\/wp\/v2\/tags?post=1646"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}