The Energetics of Sunspots and Faculae: Fluid Dynamics vs. Magnetic Inhibition Kenneth Schatten ai-solutions & Hans Mayr NASA –GSFC Code 910.4 Sunspots and Faculae: Fluid Dynamics vs. Magnetic Inhibition • SOME “HOME PHOTOS” • METEOROLOGICAL CONCEPTS: WHAT • MAKES CLOUDS & HURRICANES FLUID DYNAMICS VS. MAGNETIC INHIBITION – WHAT IS THIS ALL ABOUT? • MAGNETIC FIELD PLAYS AN IMPORTANT ROLE IN • • • • 2004 THE STRUCTURE ABOVE PHOTOSPHERE FLUID DYNAMICS MAY PLAY AN IMPORTANT ROLE IN ENERGETICS OF ACTIVE REGION FEATURES FACULA OBSERVATIONS TOUGH OBSERVATIONAL QUESTION: ARE FACULAE UPLIFTED STRUCTURES? RELATION TO CLIMATE & USRA OPPORTUNITY 2 2004 3 2004 4 2004 5 2004 6 2004 7 2004 8 2004 9 METEOROLOGICAL CONCEPTS • MAIN POINT: FOR STORMS, THERE ARE 2 • • • • • 2004 KINDS OF INSTABILITIES: 1) CONDITIONAL INSTABILITY (FOR CLOUDS); 2) HURRICANES ARE A 2ND KIND OF INSTABILITY STABILITY OF THE ATMOSPHERE CONDITIONAL INSTABILITY (CI) HURRICANE DEVELOPMENT AND ENERGETICS CISK (CONDITIONAL INSTABILITY OF THE SECOND KIND) – CHARNEY AND ELIASSEN IMPORTANCE OF OCEANS: KERRY EMANUEL 10 Atmospheric Stability Compare an air parcel’s temperature (Tp) with the environmental temperature (Te) at a given altitude if Tp > Te, parcel rises if Tp = Te parcel does not move up or down if Tp < Te parcel sinks 2004 11 CONDITIONAL INSTABILITY Determining Air Parcel Temperature: Rising air parcels and adiabatic cooling consider a rising parcel of air -->> As the parcel rises, it will adiabatically expand and cool (recall our discussion in chapter 5 about rising parcels of air) adiabatic - a process where the parcel temperature changes due to an expansion or compression, no heat is added or taken away from the parcel the parcel expands since the lower pressure outside allows the air molecules to push out on the parcel walls since it takes energy for the parcel molecules to "push out" on the parcel walls, they use up some of their internal energy in the process. 2004 therefore, the parcel also cools since temperature is proportional to molecular internal energy Dry versus Moist-Adiabatic Process the moist adiabatic lapse rate is less than the dry adiabatic lapse rate because as vapor condenses into water (or water freezes into ice) for a saturated parcel, latent heat is released into the parcel, mitigating the adiabatic cooling 12 Atmospheric Stability 2004 Absolute Stability Absolute Stability Absolute Instability Conditional Instability 13 CONDITIONAL INSTABLILITY: 1ST KIND:CLOUDS COMPETE FOR ENERGY Photograph by: Holle 2004 The downward motion inhibits further convection and the growth of additional thermals from below, which is why fair weather cumulus typically have expanses of clear sky between them. Without a continued supply of rising air, the cloud 14 begins to erode and eventually disappears. OVERVIEW OF HURRICANES: CISK • Convergence at the surface leads to convergence of moisture. • The convection or thunderstorms that form release latent heat which intensifies the surface low. • The warm core column of air will create an upper level high pressure center. • The weak shear allows the storm to remain vertical and allows for the latent heat release to enhance the surface low. 2004 15 Hurricane Structure:CISK This feedback mechanism continues as long as the favorable conditions for hurricane growth continue to exist. The energy for the growth of the storm comes from the ocean (evaporation). 2004 16 Hurricane Development: CISK H L 2004 Latent energy (the conversion of Water vapor to liquid water) releases energy which drives the circulation and causes the “strong heating” Shown. Strong Heating L Strong Convergence 17 RELEVANCE TO GLOBAL CHANGE: CISK, AND THERMODYNAMICS WHAT MAKES HURRICANES SO FEROCIOUS? 2004 KERRY EMANUEL: OCEANS RESUPPLY OF MOIST AIR IS KEY TO ENERGETICS OF HURRICANES (AND THEY LIVE OFF (DRIVEN LIKE A HEAT ENGINE) OF ∆Τ ΒΕΤWEEN LOWER TROPOSPHERE AND STRATOSPHERE) –GLOBAL WARMING INTENSIFIES THE ENERGY AVAILABLE (KERRY PREDICTED STRONGER AND MORE FREQUENT HURRICANES DUE TO GLOBAL WARMING) 18 HOW DOES ALL THIS RELATE TO THE SUN? - FLUID DYNAMICS VS. MAGNETIC INHIBITION •GRANULATION – CLOUDS ACTIVE REGION FEATURES: SPOTS AND FACULAE – HURRICANES? 2004 19 FLUID DYNAMICS VS. MAGNETIC INHIBITION TWO DISTINCT REGIONS: 1. Above the photosphere (τ<1), the magnetic field is in a low beta environment (plasma press. to field press.). 2. Below the photosphere (τ>1), a high beta environment largely exists. So, Hans and I ask ?: what is the role of FLUID DYNAMICS VS. FIELD INHIBITION, below the photosphere? 2004 20 SOLAR VS. TERR. METEOROLOGY • SOLAR (FOR TAU >1); THE SAHA EQN. GOVERNS AMOUNT OF • • • • • 2004 IONIZATION STATE; CHEMICAL ABUNDANCE ESSENTIALLY CONSTANT; THUS ‘RELATIVE HUMIDITY’ IS GOVERNED BY THERMO. STATE VARIABLES NEVERTHELESS, DENSITYAND IONIZATION STATE CAN BE A LOCAL FUNCTION OF TEMP. (HOT AND COLD LOCATIONS), WITH TIME HISTORY. IONIZATION PLAYS THE SAME ROLE AS LATENT ENERGY GRANULES MAY BE THE 1ST KIND OF INSTABILITY IN OUR VIEW, SUNSPOTS MAY BE A 2ND KIND OF INSTABILITY, WITH MAGNETIC FIELD PLAYING THE ROLE OF GUIDING THE CIRCULATION INTO A LARGE SCALE MOTION, WHICH MAKES THE PROCESS OF CONVECTION MORE EFFICIENT – THIS LAST POINT AFFECTS HOW ACTIVE REGIONS AFFECT CLIMATE!!! – THE SECULAR EFFECT OF ACTIVE REGIONS 21 Fountains of fire on the sun, who can reach a height of half a million km. These arcs of fire follow the lines of the electromagnetic field and not of the gravitation 2004 22 field of the sun. Photo in the ultraviolet light via NASA satellite TRACE. 2004 23 2004 Gas Movement in the Convection Layer Courtesy: McREL 24 FIELD INHIBITION VS FLUID DYNAMICS • FIELD INHIBITION 2004 • FLUID DYNAMICS 25 SPRUIT FIELD INHIBITION “WELL” SUNSPOT & FACULA MODELS 2004 26 SCHATTEN & MAYR “IONHURRICANE” MODEL 2004 27 2004 28 Number of authors also thought about Flows around and below spots • Meyer et al. (1974) predicted the existence of • • the converging flow ( 1 km s-1, at a depth of several Mm) as a collar around the sunspot, to provide it with confinement and stability. Parker (1979) cluster model for sunspots, and a downdraft beneath the sunspot, in the convection zone, is needed for cooling. Zhao, Kosovichev and Duvall, Jr. (2001) used time-distance helioseis. to examine flows. 2004 29 FIELD INHIBITION VS FLUID DYNAMICS (SUNSPOTS ARE WELLS IN BOTH MODELS) • FIELD INHIBITION (FI) • FIELD PRESSURE • • • 2004 CREATES WELLS FOR SPOTS AND FACULAE FACULAE BRIGHT DUE TO “HOT WALLS” EXTRA BRIGHTNESS NEAR LIMB REQUIRES ‘HOT GAS’ OVERALL EFFECT OF FI MODEL IS TO REDUCE ENERGY TRANSPORT • FLUID DYNAMICS (FD) • VERTICAL MOMENTUM • • EQN. DRIVES “HEIGHT” OF FEATURES. FACULAE HILLOCKS BECAUSE OF LARGER “SCALE HEIGHT” FACULAE - BRIGHT : UPLIFTED STRUCTURES WHICH FACE OBSERVER MORE “NORMALLY” OVERALL EFFECT OF FD MODEL IS THAT FIELD ENHANCES ENERGY TRANSPORT FACULAE: KEY TO OBSERVATIONALLY DECIDING AN ANSWER BETWEEN 2 VIEWS 30 A TOUGH OBSERVATIONAL QUESTION: • ONE OBSERVES A “HOT WALL.” HOW DO WE DECIDE WHETHER IT IS UPLIFTED (A HILLOCK OR MESA) VS. DEPRESSED (A WELL), WHEN THERE IS NO “SEA LEVEL” ON THE SUN? 2004 31 In Hillock Model, it was recognized that field does play a role in evacuating the flux tube. 2004 32 FACULAR OBSERVATIONS • GENERAL APPEARANCE OF FACULAE (CENTER TO LIMB VARIATIONS & COLOR) • FACULAE BLANKET SUNSPOTS • STELLMACHER & WIEHR • RECENT BERGER ET AL. OBSERVATIONS? 2004 33 GENERAL APPEARANCE OF FACULAE (CENTER:LIMB CONTRAST & COLOR). SOLID LINES ARE SIMPLE THEORETICAL MODEL OF HILLOCKS, AND DASHED LINES ARE OBSERVATIONS AT THREE DIFFERENT COLORS. 2004 34 FACULAE BLANKET SUNSPOTS •UPLIFTED FACULAE CAN REDUCE THE APPARENT AREA OF SUNSPOTS DUE TO “SHIELDING”, WHICH THE NEXT FIGURE SHOWS (A GRAPH OF AREA OF SUNSPOTS VS. DISK POSITION AND PLAGE /FACULAR SIZE) 2004 35 SOLAR ACTIVITY FEATURES THE APPARENT AREA OF SUNSPOTS IS FAIRLY FLAT (LEFT SIDE OF LOWER GRAPH) WHEN PLAGE ARE SMALL, BUT IS REDUCED NEAR LIMB DUE TO “SHIELDING”, WHEN PLAGE ARE LARGE (RIGHT SIDE OF LOWER GRAPH). 2004 36 2004 37 Time-Distance Helioseismology • Zhao & Kosovichev (2001, 2003) – Blue – cool; Red – hot • Inward flows near surface help to confine and stabilise spot 2004 38 SUN-CLIMATE: WHAT IS THE EFFECT OF ACTIVE REGIONS? Composite TSI from Fröhlich (2000) • Willson (1997) and Willson and Mordvinov (2003) used the Nimbus 7/ERB results to relate the nonoverlapping ACRIM I and ACRIM II data sets. • Fröhlich and Lean (1998) and Fröhlich (2000) used ERBS to relate ACRIM I and ACRIM II. • HOW DO WE UNDERSTAND ∆Ε ∼ Rz ? 2004 39 HOW DO WE UNDERSTAND ∆Ε∼Rz? • IN EARLY MODELS OF ACTIVE REGIONS, ∆Ε ∼ 0. • PRESENT VIEW, ACTIVE REGIONS SERVE AS AN AID IN • • • 2004 TRANSPORTING ENERGY OUTWARD BY AIDING LARGE SCALE FLOW. THIS HAPPENS AS THE TURBULENT VISCOSITY IS REDUCED WHEN THE FIELD AIDS LARGE SCALE FLOW PATTERNS AS A CONSEQUENCE, B FIELD OF ACTIVE REGION INCREASES THE EFFICIENCY OF CONVECTIVE ENERGY TRANSPORT. Thus ∆Ε >0 PROPORTIONAL TO ACTIVITY HOW DOES ∆Ε∼Rz OCCUR? (NEXT FIGURE) 40 ENERGETICS:HOW DOES ∆Ε∼Rz OCCUR? • We offer following simplified global picture: • The photosphere ~ a surface of constant • temperature (like the surface of pot of boiling water), so it has an area, “A” Energy radiating from surface ~ σA T**4. • To reduce radiation, since T~ constant: reduce A • So a sunspot, effectively removes area, ∆A, from the radiating photosphere. • Faculae, by crinkling surface, increases ∆A • OVERALL, SINCE ACTIVITY AIDS OVERALL FLOW, ∆Α increases , thus ∆Ε∼ ∆Α ∼Rz. • NEVERTHELESS, DEEP SECULAR CHANGES:???? 2004 41 CLIMATE EFFECTS/USRA INTERESTS A Workshop To Formulate a New Research Approach on SOLAR VARIABILITY ON DECADAL TO MILLENIAL TIMESCALES: Influence on Earth Climate Change and Prediction April 26-27, 2004 Patuxent Wildlife Center 10901 Scarlet Tanager Loop, Laurel, MD 20708 Sponsored by The Universities Space Research Association http://www.usra.edu/hq/meetings/scw/ 2004 42 CONCLUSIONS • FACULAE MAY HOLD THE CLUE TO: • • 2004 FLUID DYNAMICS VS. FIELD INHIBITION TOUGH OBSERVATIONAL QUESTION: ARE FACULAE UPLIFTED STRUCTURES? EFFECT ON CLIMATE: THE OVERALL EFFECT OF FLUID DYNAMICAL MODEL IS THE MAGNETIC FIELD ENHANCES ENERGY TRANSPORT, ALLOWING A POSITIVE EFFECT OF ACTIVITY UPON ENERGY FLOW: ∆Ε∼Rz. 43