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A Whole-Heliosphere View of the Solar Wind Hale Lecture American Astronomical Society 5/24/2010 Marcia Neugebauer University of Arizona
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A Better Title: The Things that Happen to the Solar Wind After it Leaves the Sun
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The Complex Solar Atmosphere
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The Sun creates both slow and fast solar wind
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But, it’s a complicated process
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Model of open and closed field lines (Wang et al., 2007)
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The Source-Surface Model (Cravens, 1997)
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Major Processes in the Solar Wind Expansion Collision Reconnection Pickup (mass loading) All of which leads to: –Turbulence –The interstellar medium
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Expansion
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First Adiabatic Invariant (Conservation of Magnetic Moment ) = mw 2 /2B T /B = constant As B , expect T , and T || / T
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Magnetic Moment versus Distance from Sun
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(Hellinger et al., 2009)
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Proton Distribution functions (Marsch et al., 1981) Distance from Sun --> Solar wind speed -->
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The Strange Behavior of Alpha Particles Abundance highly variable n a /n p = 0 -.03 in slow wind (~0 at HCS) n a /n p =.04-.05 in fast wind Greatly enhanced in CMEs (up to 0.40!) Hotter than protons T a /T p = 4 to 6 in fast wind Approaches isothermal in slow wind Faster than protons V ap up to 100 km/s in fast wind V ap -> 0 in dense, slow wind Anisotropic and double peaked
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V ap vs Distance in Fast Wind (Neugebauer et al., 1996)
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Collision
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Magnetized Plasmas Don’t Easily Mix
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Note Boundaries Between Winds from Streamers & Coronal Holes
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(Gosling et al., 1978) Some Stream Interfaces are Stable over Many AU
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Heliospheric Current Sheets, Embedded in the Slow Wind, are Also Stable Solar MaximumSolar MinimumDeclining Activity
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Result of the Solar Dipole Tilt (Ballerina Skirt) (Jokipii & Thomas, 1981)
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Solar Rotation Creates Corotating Interaction Regions (Pizzo, 1978)
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Signatures of a CIR at ~5 AU (Lazarus et al., 1999) SI at density drop HCS on Day 138
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Coronal Mass Ejections
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Interplanetary CMEs (Richardson, 1997)
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Interaction Regions at Solar Max and Min
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Evolution of Interaction regions from 1 to 60 AU Formation of MIRs (Wang & Richardson, 2003)
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Ecliptic plane view of pileup out to 100 AU
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Effect of GMIRs on Cosmic Rays (Burlaga et al., 2003)
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Anti-Correlation of Sunspots and Cosmic Rays
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Reconnection
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Petschek Reconnection Mechanism (Gosling, 2005)
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Reconnection Exhaust Fans (Gosling, 2010) Bifurcated structure Opposite V/ /B Decreased B, Increased V, T Observed even for small angle changes Created by turbulence?
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Pickup
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Pick-up is sometimes associated with Mass Loading
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Non-Solar Sources of Solar Wind Ions Atoms and ions –Interstellar medium –Dust –Comets –Planets Dust –Comets and Asteroids –Interstellar medium –Jupiter
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The Pick-up Process B U In solar-wind frameIn inertial frame Photoionization adds mass to wind. Charge exchange creates fast neutral and slow ion. Both processes provide drag on wind.
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Proton Spectrum with Pickup Ions (Gloeckler et al., 2001)
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Inner Source of Pick-up Ions (Gloeckler et al., 2001)
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High-Energy Tails of H and He (Gloeckler, 2003)
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Effect of Pickup Ions on the Wind Photoionization adds mass Charge exchange may conserve mass –Results in a fast neutral atom and a slow ion Both processes result in: –Acceleration of slow ions up to V sw –Drag –Hot ions with V th V sw
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Slow-Down of Solar Wind due to Pick-up Ions
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Turbulence
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OGO 5 Density fluctuations (Neugebauer, 1976) f/f pg Helios 2 Field vector spectra (Bruno & Carbone, 2005) Power Spectra
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2-D Simulation of MHD Turbulence (Greco et al., 2010) Field lines + Current density (gray shade) Current sheets generated locally Reconnection heats plasma
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The End of the Road (Approach to Alaska’s Bridge to Nowhere)
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Interaction with the Interstellar Medium
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Model of Outer Heliosphere
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Anomalous Cosmic Rays at TS and in Heliosheath (Courtesy A. Cummings, 2010)
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“The Ribbon”
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Summary A lot of interesting physics in the solar wind Several unsolved issues –Turbulent processes –Relaxation of anisotropic and multi-beams –Physics of high-energy tails –Acceleration of ACR –Prevalence of reconnection –Stability/sources of discontinuities Applications to many other astrophysical settings
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