BEGIN:VCALENDAR PRODID:-//SiteBuilder 2//University of ÌÇÐÄTV ITS Web Team//EN VERSION:2.0 CALSCALE:GREGORIAN METHOD:PUBLISH X-WR-TIMEZONE:Europe/London X-LIC-LOCATION:Europe/London BEGIN:VTIMEZONE TZID:Europe/London LAST-MODIFIED:20201010T011803Z TZURL:http://tzurl.org/zoneinfo/Europe/London X-LIC-LOCATION:Europe/London X-PROLEPTIC-TZNAME:LMT BEGIN:STANDARD TZNAME:GMT TZOFFSETFROM:+000115 TZOFFSETTO:+0000 DTSTART:18471201T000000 END:STANDARD BEGIN:DAYLIGHT TZNAME:BST TZOFFSETFROM:+0000 TZOFFSETTO:+0100 DTSTART:19160521T020000 RDATE:19170408T020000 RDATE:19180324T020000 RDATE:19190330T020000 RDATE:19200328T020000 RDATE:19210403T020000 RDATE:19220326T020000 RDATE:19230422T020000 RDATE:19240413T020000 RDATE:19270410T020000 RDATE:19300413T020000 RDATE:19330409T020000 RDATE:19340422T020000 RDATE:19350414T020000 RDATE:19380410T020000 RDATE:19390416T020000 RDATE:19400225T020000 RDATE:19460414T020000 RDATE:19470316T020000 RDATE:19480314T020000 RDATE:19490403T020000 RDATE:19530419T020000 RDATE:19540411T020000 RDATE:19570414T020000 RDATE:19600410T020000 RDATE:19680218T020000 END:DAYLIGHT BEGIN:STANDARD TZNAME:GMT TZOFFSETFROM:+0100 TZOFFSETTO:+0000 DTSTART:19161001T030000 RDATE:19170917T030000 RDATE:19180930T030000 RDATE:19190929T030000 RDATE:19201025T030000 RDATE:19211003T030000 RDATE:19221008T030000 RDATE:19391119T030000 RDATE:19471102T030000 RDATE:19481031T030000 RDATE:19491030T030000 RDATE:19711031T030000 END:STANDARD BEGIN:STANDARD TZNAME:GMT TZOFFSETFROM:+0100 TZOFFSETTO:+0000 DTSTART:19230916T030000 RRULE:FREQ=YEARLY;UNTIL=19240921T020000Z;BYMONTH=9;BYMONTHDAY=16,17,18,19 ,20,21,22;BYDAY=SU END:STANDARD BEGIN:DAYLIGHT TZNAME:BST TZOFFSETFROM:+0000 TZOFFSETTO:+0100 DTSTART:19250419T020000 RRULE:FREQ=YEARLY;UNTIL=19260418T020000Z;BYMONTH=4;BYMONTHDAY=16,17,18,19 ,20,21,22;BYDAY=SU END:DAYLIGHT BEGIN:STANDARD TZNAME:GMT TZOFFSETFROM:+0100 TZOFFSETTO:+0000 DTSTART:19251004T030000 RRULE:FREQ=YEARLY;UNTIL=19381002T020000Z;BYMONTH=10;BYMONTHDAY=2,3,4,5,6, 7,8;BYDAY=SU END:STANDARD BEGIN:DAYLIGHT TZNAME:BST TZOFFSETFROM:+0000 TZOFFSETTO:+0100 DTSTART:19280422T020000 RRULE:FREQ=YEARLY;UNTIL=19290421T020000Z;BYMONTH=4;BYMONTHDAY=16,17,18,19 ,20,21,22;BYDAY=SU END:DAYLIGHT BEGIN:DAYLIGHT TZNAME:BST TZOFFSETFROM:+0000 TZOFFSETTO:+0100 DTSTART:19310419T020000 RRULE:FREQ=YEARLY;UNTIL=19320417T020000Z;BYMONTH=4;BYMONTHDAY=16,17,18,19 ,20,21,22;BYDAY=SU END:DAYLIGHT BEGIN:DAYLIGHT TZNAME:BST TZOFFSETFROM:+0000 TZOFFSETTO:+0100 DTSTART:19360419T020000 RRULE:FREQ=YEARLY;UNTIL=19370418T020000Z;BYMONTH=4;BYMONTHDAY=16,17,18,19 ,20,21,22;BYDAY=SU END:DAYLIGHT BEGIN:DAYLIGHT TZNAME:BDST TZOFFSETFROM:+0100 TZOFFSETTO:+0200 DTSTART:19410504T020000 RDATE:19450402T020000 RDATE:19470413T020000 END:DAYLIGHT BEGIN:DAYLIGHT TZNAME:BST TZOFFSETFROM:+0200 TZOFFSETTO:+0100 DTSTART:19410810T030000 RRULE:FREQ=YEARLY;UNTIL=19430815T010000Z;BYMONTH=8;BYMONTHDAY=9,10,11,12, 13,14,15;BYDAY=SU END:DAYLIGHT BEGIN:DAYLIGHT TZNAME:BDST TZOFFSETFROM:+0100 TZOFFSETTO:+0200 DTSTART:19420405T020000 RRULE:FREQ=YEARLY;UNTIL=19440402T010000Z;BYMONTH=4;BYMONTHDAY=2,3,4,5,6,7 ,8;BYDAY=SU END:DAYLIGHT BEGIN:DAYLIGHT TZNAME:BST TZOFFSETFROM:+0200 TZOFFSETTO:+0100 DTSTART:19440917T030000 RDATE:19450715T030000 RDATE:19470810T030000 END:DAYLIGHT BEGIN:STANDARD TZNAME:GMT TZOFFSETFROM:+0100 TZOFFSETTO:+0000 DTSTART:19451007T030000 RRULE:FREQ=YEARLY;UNTIL=19461006T020000Z;BYMONTH=10;BYMONTHDAY=2,3,4,5,6, 7,8;BYDAY=SU END:STANDARD BEGIN:DAYLIGHT TZNAME:BST TZOFFSETFROM:+0000 TZOFFSETTO:+0100 DTSTART:19500416T020000 RRULE:FREQ=YEARLY;UNTIL=19520420T020000Z;BYMONTH=4;BYMONTHDAY=14,15,16,17 ,18,19,20;BYDAY=SU END:DAYLIGHT BEGIN:STANDARD TZNAME:GMT TZOFFSETFROM:+0100 TZOFFSETTO:+0000 DTSTART:19501022T030000 RRULE:FREQ=YEARLY;UNTIL=19521026T020000Z;BYMONTH=10;BYMONTHDAY=21,22,23,2 4,25,26,27;BYDAY=SU END:STANDARD BEGIN:STANDARD TZNAME:GMT TZOFFSETFROM:+0100 TZOFFSETTO:+0000 DTSTART:19531004T030000 RRULE:FREQ=YEARLY;UNTIL=19601002T020000Z;BYMONTH=10;BYMONTHDAY=2,3,4,5,6, 7,8;BYDAY=SU END:STANDARD BEGIN:DAYLIGHT TZNAME:BST TZOFFSETFROM:+0000 TZOFFSETTO:+0100 DTSTART:19550417T020000 RRULE:FREQ=YEARLY;UNTIL=19560422T020000Z;BYMONTH=4;BYMONTHDAY=16,17,18,19 ,20,21,22;BYDAY=SU END:DAYLIGHT BEGIN:DAYLIGHT TZNAME:BST TZOFFSETFROM:+0000 TZOFFSETTO:+0100 DTSTART:19580420T020000 RRULE:FREQ=YEARLY;UNTIL=19590419T020000Z;BYMONTH=4;BYMONTHDAY=16,17,18,19 ,20,21,22;BYDAY=SU END:DAYLIGHT BEGIN:DAYLIGHT TZNAME:BST TZOFFSETFROM:+0000 TZOFFSETTO:+0100 DTSTART:19610326T020000 RRULE:FREQ=YEARLY;UNTIL=19630331T020000Z;BYMONTH=3;BYDAY=-1SU END:DAYLIGHT BEGIN:STANDARD TZNAME:GMT TZOFFSETFROM:+0100 TZOFFSETTO:+0000 DTSTART:19611029T030000 RRULE:FREQ=YEARLY;UNTIL=19671029T020000Z;BYMONTH=10;BYMONTHDAY=23,24,25,2 6,27,28,29;BYDAY=SU END:STANDARD BEGIN:DAYLIGHT TZNAME:BST TZOFFSETFROM:+0000 TZOFFSETTO:+0100 DTSTART:19640322T020000 RRULE:FREQ=YEARLY;UNTIL=19670319T020000Z;BYMONTH=3;BYMONTHDAY=19,20,21,22 ,23,24,25;BYDAY=SU END:DAYLIGHT BEGIN:STANDARD TZNAME:BST TZOFFSETFROM:+0100 TZOFFSETTO:+0100 DTSTART:19681026T230000 END:STANDARD BEGIN:DAYLIGHT TZNAME:BST TZOFFSETFROM:+0000 TZOFFSETTO:+0100 DTSTART:19720319T020000 RRULE:FREQ=YEARLY;UNTIL=19800316T020000Z;BYMONTH=3;BYMONTHDAY=16,17,18,19 ,20,21,22;BYDAY=SU END:DAYLIGHT BEGIN:STANDARD TZNAME:GMT TZOFFSETFROM:+0100 TZOFFSETTO:+0000 DTSTART:19721029T030000 RRULE:FREQ=YEARLY;UNTIL=19801026T020000Z;BYMONTH=10;BYMONTHDAY=23,24,25,2 6,27,28,29;BYDAY=SU END:STANDARD BEGIN:DAYLIGHT TZNAME:BST TZOFFSETFROM:+0000 TZOFFSETTO:+0100 DTSTART:19810329T010000 RRULE:FREQ=YEARLY;BYMONTH=3;BYDAY=-1SU END:DAYLIGHT BEGIN:STANDARD TZNAME:GMT TZOFFSETFROM:+0100 TZOFFSETTO:+0000 DTSTART:19811025T020000 RRULE:FREQ=YEARLY;UNTIL=19891029T010000Z;BYMONTH=10;BYMONTHDAY=23,24,25,2 6,27,28,29;BYDAY=SU END:STANDARD BEGIN:STANDARD TZNAME:GMT TZOFFSETFROM:+0100 TZOFFSETTO:+0000 DTSTART:19901028T020000 RRULE:FREQ=YEARLY;UNTIL=19951022T010000Z;BYMONTH=10;BYDAY=4SU END:STANDARD BEGIN:STANDARD TZNAME:GMT TZOFFSETFROM:+0000 TZOFFSETTO:+0000 DTSTART:19960101T000000 END:STANDARD BEGIN:STANDARD TZNAME:GMT TZOFFSETFROM:+0100 TZOFFSETTO:+0000 DTSTART:19961027T020000 RRULE:FREQ=YEARLY;BYMONTH=10;BYDAY=-1SU END:STANDARD END:VTIMEZONE BEGIN:VEVENT DTSTAMP:20260428T195510Z DTSTART;VALUE=DATE-TIME:20190312T100000 DTEND;VALUE=DATE-TIME:20190312T110000 SUMMARY:Norbert Magyar (KU Leuven): Uniturbulence\, a new type of MHD tur bulence TZID:Europe/London UID:20190312-8a1785d868bd6a9a0168c7666de55639@warwick.ac.uk CREATED:20190304T131454Z DESCRIPTION:Abstract: The current understanding of the MHD turbulence gen eration mechanism originated in the works of Iroshnikov (1963) and Kraic hnan (1965) (IK for short)\, and is based on the Alfvén effect: the nonl inear cascade of energy\, essential in turbulence\, is the result of suc cessive collisions between counter-propagating Alfvén waves along the me an magnetic field. This theory is still at the basis of current models i n MHD turbulence. However\, this approach is strictly valid only in inco mpressible and homogeneous (and infinite) plasma\, under which condition s the only existing wave type is that of purely magnetically-driven Alfv én waves. Allowing for compressibility introduces a much richer spectrum of MHD waves\, especially if the plasma inhomogeneity is also accounted for. Recently\, using full 3D MHD numerical modelling of the propagatio n of Alfvénic waves in a plasma inhomogeneous in the perpendicular direc tion\, Magyar et al. (2017) showed that due to the modified nature of th e MHD waves in inhomogeneous plasmas\, characterised by linear coupling of incompressive and compressive perturbations\, the Elsässer variables usually representing the up and down-propagating pure Alfvén waves along a mean magnetic field are both nonzero even for unidirectionally propag ating waves. This leads to the same nonlinear advection term in the MHD equations being nonzero as in the IK phenomenology\, but now for the wav es propagating only in one direction. We name this new turbulence genera tion mechanism in inhomogeneous plasmas uniturbulence\, stemming from th e unidirectional wave cascade. Plasmas which are permeated mostly by wav es propagating in one direction include coronal holes and the solar wind \, thus these are expected to be the most influenced by the uniturbulenc e. This finding constitutes a paradigm shift in our understanding of the MHD turbulence as a whole\, opening up a new alley in turbulence studie s. Most excitingly\, it might be relevant to the decades-long unsolved p roblem of coronal heating\, especially in open magnetic field regions. LOCATION:PS017 CATEGORIES:CFSA Seminar LAST-MODIFIED:20190304T131454Z ORGANIZER;CN=Anne-Marie Broomhall: END:VEVENT END:VCALENDAR