Overview of Astronomical Concepts I. Radiation, Magnitudes, Distances PHY 688, Lecture 3 Stanimir Metchev Outline • Radiation – blackbody radiation, luminosity – magnitudes, colors – extinction, optical depth • Detection and Measurement of Light – Earth’s atmosphere, photometric bands – detectors • Astronomical yardsticks – parallax – absolute magnitude, distance modulus Jan 30, 2009 PHY 688, Lecture 3 2 Blackbody Radiation • Planck’s law – specific intensity – [erg s–1 cm–2 Hz–1 sterad–1] or [Jy sterad–1] – 1 Jy = 10–23 erg s–1 cm–2 Hz–1 • Wien displacement law • Stefan-Boltzmann law T λmax= 0.29 K cm F = σ T4 – energy flux density – [erg s–1 cm–2] • Stellar luminosity 2# 5 k 4 "= 15c 2 h 3 L* = 4 "R*2#Teff4 ! – [erg s–1] Jan 30, 2009 PHY 688, Lecture 3 ! 3 Blackbody Radiation Teff, Sun = 5777 K Jan 30, 2009 PHY 688, Lecture 3 4 The Dreaded Magnitudes • Stefan-Boltzmann Law: • apparent magnitude: F = σ T4 [erg s–1 cm–2] m = –2.5 lg F/F0 – m increases for fainter objects! – m = 0 for Vega; m ~ 6 mag for faintest naked-eye stars – faintest galaxies seen with Hubble: m ≈ 30 mag • 109.5 times fainter than faintest naked-eye stars – dependent on observing wavelength • mV, mB, mJ, or simply V (550 nm), B (445 nm), J (1220 nm), etc • bolometric magnitude (or luminosity): mbol (or Lbol) – normalized over all wavelengths Jan 30, 2009 PHY 688, Lecture 3 5 Magnitudes and Colors • magnitude differences: – relative brightness of two objects at the same wavelength V1 – V2 = –2.5 lg FV1/FV2 • ∆m = 5 mag approx. equivalent to F1/F2 = 100 – relative brightness of the same object at different wavelengths (color) B – V = –2.5 (lg FB/FV – lg FB,Vega/FV,Vega) – by definition Vega has a color of 0 mag at all wavelengths, i.e. (B – V)Vega = 0 mag Jan 30, 2009 PHY 688, Lecture 3 6 Magnitudes and Colors 2MASS GD 165 A/B Jan 30, 2009 J H K PHY 688, Lecture 3 (Zuckerman & Becklin 1988) 1.2, 1.6, 2.2 µm color composite ~10,000 K ~2,200 K 7 Color of Blackbody Radiation Jan 30, 2009 PHY 688, Lecture 3 8 Extinction and Optical Depth • Light passing through a medium can be: – transmitted, absorbed, scattered • dLν(s) = –κν ρ Lν ds = –L dτν – medium opacity κν [cm2 g–1] – optical depth τν = κν ρs [unitless] • Lν = Lν,0e–τ = Lν,0e–κρs =Lν,0e–s/l – photon mean free path: lν = (κν ρ)–1 = s/τν [cm] • If there is extinction along the line of sight, apparent magnitude mν is attenuated by Aν = 2.5 lg (Fν,0/Fν) = 2.5 lg(e)τν = 0.43τν mag – reddening between two frequencies (ν1, ν2) or wavelengths is defined as Eν1,ν2 = mν1 – mν2 – (mν1 – mν2)0 [mag] – (mν1 – mν2)0 is the intrinsic color of the star AV / E(B–V) ≈ 3.0 Jan 30, 2009 PHY 688, Lecture 3 9 Interstellar Extinction Law extinction is highest at ~100 nm = 0.1 µm unimportant for >10 µm Jan 30, 2009 PHY 688, Lecture 3 10 Interstellar Extinction: Dust Jan 30, 2009 PHY 688, Lecture 3 11 Atmospheric Transmission Jan 30, 2009 PHY 688, Lecture 3 12 Outline • Radiation – blackbody radiation, luminosity – magnitudes, colors – extinction, optical depth • Detection and Measurement of Light – Earth’s atmosphere, photometric bands – detectors • Astronomical yardsticks – parallax – absolute magnitude, distance modulus Jan 30, 2009 PHY 688, Lecture 3 13 Photometric Bands: Near-Infrared Jan 30, 2009 PHY 688, Lecture 3 14 Photometric Bands: Visible Jan 30, 2009 PHY 688, Lecture 3 15 Photometric Systems • UBVRI(ZY) (visible) – Johnson, Bessel, Cousins, Kron, etc • ugriz (visible) – Thuan-Gunn, Strömgren, Sloan Digital Sky Survey (SDSS), etc • JHKLM(NQ) (infrared) – Johnson, 2-micron All-Sky Survey (2MASS), Mauna Kea Observatory (MKO), etc Jan 30, 2009 PHY 688, Lecture 3 16 Detection of Light Quantum efficiencies of the 4 CCD chips on the Hubble WFPC2 camera A charge-coupled device (CCD) converts photons to electrons Jan 30, 2009 PHY 688, Lecture 3 17 Detection of Light: The Sloan Digital Sky Survey (SDSS) SDSS 2.5 m telescope at Apache Point, NM Jan 30, 2009 PHY 688, Lecture 3 Ritchey-Chretien design (Cassegrain-like) 18 Detection of Light: The Sloan Digital Sky Survey (SDSS) Jan 30, 2009 PHY 688, Lecture 3 19 Detection of Light: The Sloan Digital Sky Survey (SDSS) u g r i z (ansgtroms) Jan 30, 2009 PHY 688, Lecture 3 20 Proxima Cen Jan 30, 2009 PHY 688, Lecture 3 21 Outline • Radiation – blackbody radiation, luminosity – magnitudes, colors – extinction, optical depth • Detection and Measurement of Light – Earth’s atmosphere, photometric bands – detectors • Astronomical yardsticks – parallax – absolute magnitude, distance modulus Jan 30, 2009 PHY 688, Lecture 3 22 Measuring Distance: The Trigonometric Parallax • • • distance to nearby star is 1 parsec (pc) when angle p = 1 arc second (1") 1 pc = 3.26 light years (ly) = 2.06x105 AU = 3.09x1018 cm Proxima Cen is at 1.3 pc ~ 4.3 ly Jan 30, 2009 PHY 688, Lecture 3 23 Absolute Magnitude and Distance Modulus • The apparent magnitude of a star at 10 pc – used to compare absolute brightnesses of different stars M = m + 2.5 lg F(r) / F(10 pc) • Distance modulus (DM) – a proxy for distance m – M = 5 lg (r / 10 pc) – DM = 0 mag for object at 10 pc – DM = –4.4 mag for Proxima Cen – DM = 14.5 mag to Galactic center Jan 30, 2009 PHY 688, Lecture 3 24