M.R. Burleigh 2601/Unit 3 DEPARTMENT OF PHYSICS AND ASTRONOMY LIFECYCLES OF STARS Option 2601
M.R. Burleigh 2601/Unit 3 Stellar Physics Observational properties of stars Stellar Spectra The Sun Stellar Structure Stellar Evolution Stars of particular interest
M.R. Burleigh 2601/Unit 3 DEPARTMENT OF PHYSICS AND ASTRONOMY Unit 3 The Sun
M.R. Burleigh 2601/Unit 3 The Sun Basic physical parameters Structure of interior and atmosphere Surface features Magnetic field Solar activity, flares and pulsations Relationship to other stars
M.R. Burleigh 2601/Unit 3 Our nearest star Nearest, therefore studied in most detail Standard against which other stars are compared –Radius = 6.96x10 5 km (~109R ) –Mass = 1.99x10 30 kg (~333,000M ) –Luminosity = 3.86x10 26 W –Spectral type/luminosity class = G2 V
M.R. Burleigh 2601/Unit 3 Structure Core – region of nuclear burning Radiative zone Convection zone Photosphere Chromosphere Corona Only regions directly observable
M.R. Burleigh 2601/Unit 3
Solar interior Helioseismology Solar oscillations used to study the structure similar to seismology on Earth Periods range from 5 min to 2h 40min –Detected by periodic changes in Doppler shifts of spectral lines
M.R. Burleigh 2601/Unit 3
Photosphere Granulation Base of photosphere is deepest region observable Patchwork of granules –d~700 km –Transient (5-10mins) –Bright irregular formations surrounded by darker lanes Top layer of convection zone
M.R. Burleigh 2601/Unit 3 Photosphere Bright regions are rising hot gas (convection cells) Dark regions are falling cooler gas
M.R. Burleigh 2601/Unit 3 Sunspots Cooler regions (appear darker) than surrounding photosphere Temperatures ~3800K cf. 5800K elsewhere Associated with high magnetic fields More later…
M.R. Burleigh 2601/Unit 3
Limb darkening Brightness of solar disk decreases from centre to limb (edge of disk) Arises because we see deeper hotter gas at centre, cooler layers at limb
M.R. Burleigh 2601/Unit 3
Limb darkening
M.R. Burleigh 2601/Unit 3 In a slab of thickness dx, density , fraction of flux F absorbed is: Optical depth: Absorption in photosphere Units of opacity κ are m 2 /kg (or cm 2 /g) Main source of opacity in solar photosphere is H ¯
M.R. Burleigh 2601/Unit 3 Absorption lines Discussed in detail in last Unit First mapped by Fraunhoffer ( )
M.R. Burleigh 2601/Unit 3 Absorption lines Alphabetic designation… capital letters for strong, lower case for weak lines Hence… Na D lines, CaII H & K, Mg b
M.R. Burleigh 2601/Unit 3 Chromosphere Spectrum contains emission features from highly excited/ionized species (e.g. H Balmer, HeII) High temperatures (see last lecture)
M.R. Burleigh 2601/Unit 3 Chromosphere
Chromosphere Photospheric continuum absorbed by Chromospheric gas Absorption lines projected against solar disk Emission lines seen against dark space
M.R. Burleigh 2601/Unit 3 Chromospheric fine structure Some absorption lines have large optical depth (e.g. H , CaII H & K) Monochromatic photos show large bright and dark patches… plages and filaments
M.R. Burleigh 2601/Unit 3 Chromospheric fine structure Structure appears over whole disk Bright network associated with magnetic fields at boundaries of supergranules Brightening (i.e. less absorption) of CaII K increasing magnetic field strength
M.R. Burleigh 2601/Unit 3 Chromospheric fine structure See spicules at the limb, jets of glowing gas emerging at 20-25km/s – km across, 10000km high Form a network following supergranule boundaries Probably play a significant role in mass transport… chromosphere corona wind
M.R. Burleigh 2601/Unit 3 Transition Region
M.R. Burleigh 2601/Unit 3 Transition Region Gives rise to UV spectral features –e.g. Lyman , CIII, NIII, OVI Network continues through this region Disappears at ~1.6x10 6 K in MgX images
M.R. Burleigh 2601/Unit 3 Solar Corona
M.R. Burleigh 2601/Unit 3 Solar Corona In visible light… K Corona – dominates near the Sun –Light scattered by (1-2)x10 6 K electrons –Strongly affected by solar activity F Corona – visible at a few solar radii –Light scattered from dust
M.R. Burleigh 2601/Unit 3 Solar Corona
M.R. Burleigh 2601/Unit 3 Solar Corona Radio Corona: arises from free-free transitions of free electrons & atoms/ions Line emission: “forbidden” lines due to high temperature & low density EUV lines: e.g. FeVIII-XVI… high ionization states
M.R. Burleigh 2601/Unit 3 Solar Corona
M.R. Burleigh 2601/Unit 3 Coronal Loops & Holes Coronal gas hot enough to emit low energy X-rays X-ray images show irregular gas distribution Large loop structures hot gas trapped in magnetic loops
M.R. Burleigh 2601/Unit 3 Coronal Loops & Holes Dark regions (gas less hot and dense) coronal holes Holes correspond to magnetic field lines that do not reconnect with the surface
M.R. Burleigh 2601/Unit 3 Solar Corona
M.R. Burleigh 2601/Unit 3 Solar Wind Solar gravity is insufficient to retain high temperature coronal gas Gas is a plasma (ionized but electrically neutral on a large scale) Thermal conductivity high high T prevails out to large distances
M.R. Burleigh 2601/Unit 3 Solar Wind Wind accelerates as it expands –300km/s at 30R 400km/s at 1 AU Proton/electron energy ~10 3 eV Density at Earth ~( )x10 6 m -3
M.R. Burleigh 2601/Unit 3 Solar Wind
M.R. Burleigh 2601/Unit 3 Solar Activity We can easily observe transient phenomena These are manifestations of Solar Activity Linked through solar rotation and magnetic field
M.R. Burleigh 2601/Unit 3 Sunspots Field strengths (deduced from Zeeman effect) ~0.1T (up to 0.4T) Fields may inhibit convective energy transport Any given spot has an associated magnetic polarity May be paired with spot of opposite polarity (or diffuse region no observed as a spot)
M.R. Burleigh 2601/Unit 3 Sunspots
Sunspots Can measure solar rotation rate by following spots P equator ~25d P 40 o ~27d P 70 o ~30d
M.R. Burleigh 2601/Unit 3 Sunspots Spot numbers vary with an 11 year cycle (except Maunder Minimum) Spot latitudes vary during cycle Spot lifetimes days to months
M.R. Burleigh 2601/Unit 3 Sunspots
Sunspots Bipolar spot pair – preceding spot always has same polarity through cycle Polarities are opposite in each hemisphere Reverse at end of 11yr cycle – overall 22 year cycle Spots always follow constant latitude
M.R. Burleigh 2601/Unit 3
Sunspot Cycle
M.R. Burleigh 2601/Unit 3
Active Regions As spot numbers increase so does solar activity Each sunspot group is associated with an active region several x 10 5 km across Magnetic activity is concentrated in these Usually bipolar (Bipolar Magnetic Regions – BMRs)
M.R. Burleigh 2601/Unit 3 Active Regions
M.R. Burleigh 2601/Unit 3 Active Regions Bright areas associated with BMRs in various zones In photosphere – faculae Chromosphere – plages Corona – streamers
M.R. Burleigh 2601/Unit 3 Prominences Streams of chromospheric gas – dark when viewed against disk Quiescent –Long lived (weeks) curtain-like gas along neutral line separating poles of BMR Active –Few hours – loops closely associated with solar flares
M.R. Burleigh 2601/Unit 3 Prominences
Prominences
Solar Flares
M.R. Burleigh 2601/Unit 3 Solar Flares Transient outbursts – probably originate by magnetic reconnection Radiate from radio to -rays Emit high energy particles (solar cosmic rays)
M.R. Burleigh 2601/Unit 3 Solar Flares km in size Brighten within 5 min Decay in ~20min (up to 3hrs for largest) The larger the flare, more energetic and longer lived At solar max – small flares hourly, large flares monthly
M.R. Burleigh 2601/Unit 3
The Sun Basic physical parameters Structure of interior and atmosphere Surface features Magnetic field Solar activity, flares and pulsations Relationship to other stars
M.R. Burleigh 2601/Unit 3 Next lectures Tuesday 8 th March 10am and 1pm LRB No lecture Monday 7 th March
M.R. Burleigh 2601/Unit 3 DEPARTMENT OF PHYSICS AND ASTRONOMY Unit 3 The Sun
M.R. Burleigh 2601/Unit 3 DEPARTMENT OF PHYSICS AND ASTRONOMY LIFECYCLES OF STARS Option 2601