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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:20260428T221313Z DTSTART;VALUE=DATE-TIME:20211216T150000 DTEND;VALUE=DATE-TIME:20211216T160000 SUMMARY:Elizabeth Paul (Princeton): Adjoint methods for stellarator shape optimization and sensitivity analysis TZID:Europe/London UID:20211216-8a17841b7b77d624017be4dda3d74988@warwick.ac.uk CREATED:20211208T153940Z DESCRIPTION:Abstract: Modern stellarator design requires numerical optimi zation to navigate the high-dimensional spaces used to describe their ge ometry. Physical insight into the self-adjointness properties of the und erlying equations enables advanced optimization methods through the effi cient calculation of sensitivity information. The first applications of the adjoint method to stellarator design are reviewed. An adjoint drift- kinetic equation is derived based on the self-adjointness property of th e Fokker-Planck collision operator [1]. This adjoint method allows one t o understand the sensitivity of neoclassical quantities\, such as the ra dial collisional transport and bootstrap current\, to perturbations of t he magnetic field strength. The well-known self-adjointness property of the MHD force operator is generalized to include perturbations of the ro tational transform and the currents outside the confinement region [2-3] . This adjoint method enables evaluation of the sensitivity of equilibri um properties to perturbations of coil shapes or the plasma boundary. Ad joint methods have also been developed to reduce stellarator coil comple xity [4]\, eliminate magnetic islands [5]\, and obtain quasisymmetric va cuum fields. Applications of these adjoint methods for sensitivity analy sis and optimization are reviewed [6]. [1] E. J. Paul\, I. G. Abel\, M. Landreman\, and W. Dorland\, “An adjoint method for neoclassical stellar ator optimization\,” Journal of Plasma Physics 85\, 795850501 (2019). [2 ] T. Antonsen\, Jr.\, E. J. Paul\, and M. Landreman\, “Adjoint approach to calculating shape gradients for 3D magnetic confinement equilibria\,” Journal of Plasma Physics 85\, 905850207 (2019). [3] E. J. Paul\, T. An tonsen\, Jr.\, M. Landreman\, and W. A. Cooper\, “Adjoint approach to ca lculating shape gradients for 3D magnetic confinement equilibria\,” Jour nal of Plasma Physics 86\, 905860103 (2020). [4] E. J. Paul\, M. Landrem an\, A. Bader\, and W. Dorland\, “An adjoint method for gradient-based o ptimization of stellarator coil shapes\,” Nuclear Fusion 58\, 076015 (20 18). [5] A. Geraldini\, M. Landreman\, and E. J. Paul\, “An adjoint meth od for determining the sensitivity of island size to magnetic field vari ations\,” Journal of Plasma Physics 87\, 905870302 (2021). [6] E. J. Pau l\, M. Landreman\, and T. M. Antonsen\, “Gradient-based optimization of 3D MHD equilibria\,” Journal of Plasma Physics 87\, 905870214 (2021). 1 LOCATION: CATEGORIES:CFSA Seminar LAST-MODIFIED:20211208T153940Z ORGANIZER;CN=Anne-Marie Broomhall: END:VEVENT END:VCALENDAR