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Wind-Fed Magnetospheres: Mass Budget & Spindown Stan Owocki University of Delaware Newark, Delaware USA Collaborators Asif ud-Doula Rich Townsend
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2 Questions What processes limit the build-up of mass in a wind-fed magnetosphere? –how/where does it leak? –how does total mass scale with B, vrot/vcrit, Mdot, etc. How does angular momentum loss & spindown scale with B *, Mdot, etc.? –can we explain slow rotators w/ magnetic spindown? –how to generalize for higher multipoles?
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Rigid Field - Hydro Model
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Wind Magnetic Confinement Ratio of magnetic to kinetic energy density: e.g, for dipole q=3; ~ 1/r 4 ** Alfven Radius: ( R A ) 1 For dipole (q=3) with beta=0: R A = * 1/4 R *
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Magnetic confinement vs. Wind + Rotation Alfven radius Kepler radius Rotation vs. critical Wind mag. confinement
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Field-aligned rotation * =100 R A =3.2R * V rot /V orb =1/2 R K =1.6 R * RKRK RARA
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Strong Field + Rapid rotation * =100 W=1/2 RKRK RARA
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Radial Mass Distribution
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Time evolution of Radial distribution of equatorial disk mass * = 100 & Vrot/Vcrit =1/2 RKRK RARA Time (ksec) Radius (R * )
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Corotation Parameter * = 100 & Vrot/Vcrit =1/2 RKRK RARA Time (ksec) Radius (R * )
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Two Parameter Study Stronger Magnetic Confinement ---> More Rapid Rotation --->
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Temporal evolution of radial distribution of equatorial disk mass Stronger Magnetic Confinement ---> More Rapid Rotation ---> r=1-5 t=0-3 Msec
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13 Strongest MHD sim * =1000 W=1/2 RKRK RARA
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14 Strongest MHD sim, no rotation 14 * =1000 W=0
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16 Breakout time & Asymptotic mass but for sigOriE, eta * ~10 6, for MHD sims with eta * =100, Independent of Mdot! (for W=1/2)
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18 Angular Momentum Loss & Spindown
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19 Weber & Davis 1967 At r= R A, M A =1 implies Tot. equat. Ang. mom/mass => & Frozen flux gasfield
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20 Gas fraction of angular momentum WD eqn.: at large radii
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23 Time Variation of Angular Momentum Loss
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24 Time variation of total Angular Momentum Loss Gas Field Total
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25 Angular Momentum Loss vs. latitude & time + + = =
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26 Angular Momentum Loss vs. Radius & Time GasFieldTotal
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27 Angular Momentum Loss: Gas vs. Field
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28 Magnetic confinement parameter =>
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29 Dipole spindown times
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30 Spindown age e.g. HD191612, with P o = 0.5 to 1 day:
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31 Extrapolated spindown law for higher order multipoles? p=2 monopole =3 dipole =4 quadrapole... etc. => Spindown weaker for more complex fields? If so, hard to explain tau Sco by spindown?? Need 3D MHD sims to test this!
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32 Summary Wind feeding of magnetosphere –balanced by inner & outer “leakage”? –observations should estimate M tot –breakout analysis predicts M tot indep of M dot ! Wind Magnetic Spindown –t spin ~ t mass /Sqrt[eta * ] for aligned dipole –complex field => slower spindown? –need 3D sims to confirm!
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Alfven speed Note: Compare sound speed
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