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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:20260427T213353Z DTSTART;VALUE=DATE-TIME:20170217T140000 DTEND;VALUE=DATE-TIME:20170217T150000 SUMMARY:Martin Laming (Space Science Division\, Naval Research Laboratory ): The First Ionization Potential (FIP) Effect in Open and Closed Magnet ic Field TZID:Europe/London UID:20170217-094d43f559df340e0159f3d62acf63ce@warwick.ac.uk CREATED:20170131T092336Z DESCRIPTION:The solar corona and both the slow and fast solar wind\, orig inating from closed and open field regions respectively\, show a degree of elemental abundance fractionation according to the First Ionization P otential (FIP) pattern. Elements with FIP below about 10 eV (e.g. Fe\, S i\, Mg) are enhanced in abundance relative to photospheric values\, by a factor of about 3-4 in the slow speed wind\, and by about 1.5 in the fa st wind\, relative to those elements (e.g. H\, N\, O\, Ar) with higher F IP. Further\, helium\, the element with highest FIP\, is often observed to be depleted in abundance relative to e.g. H\, N\, O\, Ar\, by varying amounts. A compelling explanation for these abundance anomalies invokes the ponderomotive force arising as Alfven and fast modes waves propagat e through or reflect from the chromosphere. These are fundamentally magn etic waves\, and provide the necessary ion-neutral separation. The diffe rent wave propagation in open and closed field regions of the solar coro na reproduces the observed variation in element abundances between fast and slow solar wind through the naturally occurring variation in the pon deromotive force. A careful consideration of the element abundance produ ced in a closed loop shows that the best match to observed values arises for a wave resonant with the loop\, i.e. the wave travel time from one footpoint to the other is an integral number of wave half-periods. This strongly suggests a coronal origin for the Alfven waves\, where such a r esonance would arise naturally\, as opposed to waves being generated in the photosphere or below and propagating up to the corona through the lo op footpoints\, (as in open field regions). This scenario is investigate d further\, by evaluating the their heating mechanism(s)\, and by consid eration of the different fractionation and other observables produced by shear and torsional Alfven waves\, with a view to diagnosing the wave o rigin. ponderomotive force arising in 3D compressible MHD simulations of coronal loops designed to understanding their heating mechanism(s)\, an d by consideration of the different fractionation and other observables produced by shear and torsional Alfven waves\, with a view to diagnosing the wave origin. LOCATION:PS128 CATEGORIES:CFSA Seminar LAST-MODIFIED:20170131T092336Z ORGANIZER;CN=Anne-Marie Broomhall: END:VEVENT END:VCALENDAR