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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:20260428T032950Z DTSTART;VALUE=DATE-TIME:20210226T160000 DTEND;VALUE=DATE-TIME:20210226T170000 SUMMARY:Laura Bercic (MSSL): Using in situ measured electron VDF to estim ate solar coronal temperature and ambipolar electric field in the solar wind TZID:Europe/London UID:20210226-8a17841a7763c46001776929ecb421ab@warwick.ac.uk CREATED:20210223T183810Z DESCRIPTION:Abstract: The solar coronal plasma which escapes the Sun’s gr avity and expands through our solar system is called the solar wind. It consists mainly of electrons and protons\, carries the Sun’s magnetic fi eld and\, at most heliocentric distances\, remains weakly-collisional. D ue to their small mass\, the solar wind electrons have much higher therm al velocity than their positively charged counterpart\, and play an impo rtant role in the solar wind energetics by carrying the heat flux away f rom the Sun. Their velocity distribution functions (VDFs) are complex\, usually modeled by three components. While the majority of electrons bel ong to the low-energetic thermal Maxwellian core population\, some reach higher velocities\, forming either the magnetic field aligned strahl po pulation\, or an isotropic high-energy halo population. This shape of th e electron VDF is a product of the interplay between Coulomb collisions\ , adiabatic expansion\, global and local electro-magnetic fields and tur bulence. During the talk I will focus on the effects of two of these: gl obal ambipolar electric field and Coulomb collisions. We compare the res ults of BiCoP kinetic solar wind model with the in situ solar wind measu rements provided by the Parker Solar Probe. Following the kinetic model results we can use features of in situ VDF to estimate plasma conditions in the solar corona and some global properties of the solar wind. We de monstrate that the fast streaming electrons forming the strahl populatio n do not strongly interact with the surrounding plasma and partially pre serve the shape of the VDF they had in the solar corona. This allows us to estimate coronal electron temperature at their origin. The interplay between ambipolar electron field and Coulomb collisions defines the loca tion of the transitions between separate electron populations in the vel ocity space. Recognizing the strahl break-point and the electron cutoff velocity in the in situ VDFs\, thus gives estimations about the strength of the ambipolar electric field and potential in the solar wind. LOCATION: CATEGORIES:CFSA Seminar LAST-MODIFIED:20210223T183810Z ORGANIZER;CN=Anne-Marie Broomhall: END:VEVENT END:VCALENDAR