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Download The “Tuning Fork” Diagram Galaxy Properties 1 “Early”
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The “Tuning Fork” Diagram “Early” “Late” Galaxy Properties From M. Longair “Galaxy Formation” 1 Trends in spiral galaxies (see CO Tables 25.1/25.2) CO Fig 25.12 {,∆ z dE E S Irr • Mass/Light ratios E, dE • Sa Î Sc : M/LB = 6.2 Î2.6 but Longair’s plot Î constant • Sc’s dominated by younger, hotter, more massive stars. • Colors Red Blue • Sa Î Sc : B-V = 0.75 Î0.52 • Bluer colors Î Sc’s dominated by younger, hotter stars. • Mgas/Mtotal S, Irr Low L High L • Sa Î Sd: Mgas/Mtotal = 0.04 Î 0.25 • Molecular/atomic hydrogen • Sa Î Sd: MH2/MHI = 2.2 Î 0.3 • Metallicity • Depends on absolute magnitude • No. of Globular Clusters/Total Luminosity CO Fig 25.16 H I Spectra of Spiral Galaxies Vmax Vsys 2 Tully-Fisher Relation Rotation Curves • Maximum rotation velocity-Luminosity relation [FIG 25.10] • Tully-Fisher relation • MB = -9.95 log10VMax + 3.15 • MB = -10.2 log10VMax + 2.71 • MB = -11.0 log10VMax + 3.31 Semi-derivation of Tully-Fisher Relation: MB = -9.95 log10Vmax + 3.15 MB = -10.2 log10Vmax + 2.71 MB = -11.0 log10Vmax + 3.31 (Sa) (Sb) (Sc) (Sa) (Sb) (Sc) • Mass interior to outermost R where rotation curve can be measured: Mass = • Assume 2 Vmax R G L = Mass / const. • “Freeman Law” (observed fact ---maybe): L = const. Surf .Bright. = 4πR 2 4 L = const × Vmax Important as a DISTANCE calibrator! • Convert to Absolute B-band magnitudes: L = −10 log10 Vmax + const. M B = M sun − 2.5 log10 Lsun 3 Dwarf spheroidal (Leo I) Ellipticals Huge mass range: • • • • • Dwarf spheroidals: 107-108 M Blue compact dwarfs: ~109 M Dwarf ellipticals: 107-109 M Normal (giant) ellipticals: 108-1013 M cD galaxies in cluster centers: 1013-1014 M Dwarf ellipticals M32, NGC 205 Giant E (NGC 1407) cD (NGC 3311) Ellipticals cD Be s t r1/4 • R1/4 law usually fits radial surface brightness distribution od Go Be tte r • • I ( R ) = I e10 Also Hubble’s law I ( R) = Io R 1 + Ro 2 Modified Hubble’s law I ( R) = • + others HST images R 1 / 4 −1 −3.33 Re Diverges, but at least is projection of simple 3D distribution: Io 1 + R Ro 2 I ( R) = Io R 2 1 + Ro 3/ 2 4 The Virial Theorem [CO 2.4] • For gravitationally bound systems in equilibrium • Total energy = ½ time-averaged potential energy. E = total energy U = potential energy. K = kinetic energy. E=K+U • Can show from Newton’s 3 laws + law of gravity: where I = Σmiri2 = moment of inertia. • ½ (d2I/dt2 ) -2K = U • Time average < d2I/dt2 > = 0, or at least ~ 0. • Virial theorem Î -2<K> = <U> <K> = - ½ <U> <E> = <K> + <U> Î <E> = ½ <U> 2K = -U <v2> = 3 <vr2> Î σ2r = GM/(5R) U =− 3 GM 2 5 R • See pp. 959-962, + Sect. 2.4 • Applied to nuclei of spirals Î presence of massive black holes • Also often applied to Rot. Velocity • Virial Theorem Vel. Disp Mass determinations from absorption line widths • E galaxies • Galaxy clusters Nuclear bulge of M31 5 Mass determinations from absorption line widths Observed Spectrum • Virial Theorem U =− • 2K = -U • <v2> = 3 <vr2> • Î σ2r = GM/(5R) K star 3 GM 2 5 R E galaxy = K star convolved with Gaussian velocity distribution of stars. • See pp. 959-962, + Sect. 2.4 • Applied to nuclei of spirals Î presence of massive black holes Fourier Transforms Star • Also often applied to Galaxy • E galaxies • Galaxy clusters Ratio Gaussian fit: • Convolution turns into multiplication in F.T. space. • F.T. of a Gaussian is a Gaussian. Faber-Jackson relation: Le ~ σ04 (Absolute magnitude) 6 Homework Assignment 5 Due Monday Oct. 1 • CO 2nd edition problems 25.13, 25.14, 25.16 • Same as 1st edition problems 23.11, 23.12, 23.14 • There may be one addition derivation-type problem having to do with the stellar velocities found in E galaxies. It depends on whether I cover that in class with enough lead time. Do CO problem 25.20 ( = problem 23.18 in 1st edition) 7