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Classifications of Galaxy Morphology? |
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Bulge to Disk ratio, lumpiness of spiral arms, tightness of spiral arms |
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"a" has a larger bulge, tighter arms, and less dusty gas |
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tightly wound arms, big bulge |
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lumpy, open arms, small bulge |
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no bulge, disorganized, lumpy |
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Morphology stats (vol limited) |
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.33 spiral, .54 irregular |
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Dirr most common, DE high density regions, Dsph faintest |
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Color, Stellar Pop, Gas content of Elliptical? |
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Color, Stellar Pop, Gas content of Lenticular |
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(in between E and Spr): Greenish, Old and Intermediate, modest gas content |
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Color, Stellar Pop, Gas content of Spiral |
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Blue, old + int + young, high gas content |
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Color, Stellar Pop, Gas content of Irregular |
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Bluer, mostly young, unpredictable gas content |
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quantify surface brightness as function of position (radially along major axis). leads to mass distribution |
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Intensity (I or capital Sigma) |
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Surface Brightness (I or cap sigma) = Luminosity / Area = flux / angular area; u = mag of 1 arcsec^2 patch; |
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line of constant surface brightness |
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Exponential Surface Brightness (r) = ? |
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Ee * e ^ (-1.679((r/re) - 1)) |
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de Vauc Surface Brightness (r) = ? |
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Ee * e ^ (-7.67 * ((r/re)^(1/4) - 1 )) where re = radius w/ half light Ee = E(re) |
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E(r) = Ee * e ^ (-k((r/re)^(1/n) - 1)), where K is coupled with n; for n = 1, k = 1.679; for n = 4, k = 7.67 |
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use scale length( n for disk); find r where E(r) falls below some limit, eg. r = re |
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integral from 0 to r of I(r) * 2pir * dr |
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a --> c; younger, opposite of late. |
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explore parameter space, create statistical samples, search of particular obj or phenomena |
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A * omega = 4 * pi * r^2 * (solid angle in deg^2) |
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biased towards most luminous; # depends on density and volume surveyed; if density constant --> N ~ L^(3/2) |
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(IMF) Use of Schechter Function? |
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#(M1,M2) = integral from M1 to M2 of schechter function phi(M) or phi(L). Mt(M1,M2) = integral from M1 to M2 of squiggle(M) where squiggle(M) = M * phi(M) generally (integ of salpeter IMF) |
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function for number of stars in a galaxy. phi = squiggle / M |
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most mass in low mass stars; most L in high mass stars; color depends on mean age of stellar pop. |
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stellar population synthesis |
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IMF + isochrones/evol. trails + lib of stell. spectra = spectral evol of single burst of SF |
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burst = brightens --> fades; const. SFR = const UV spectra, build up of red/optical/NIR |
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initial UV from O and B stars, massive dominate; after long while shrinks and reddens; post burst is dominated by A type (.5 Gyrs) |
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Sections of Interstellar Medium? |
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Hot ionized gas(HII), neutral atomic gas(HI), cold molecular gas(H2 or CO), dust |
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Detecting sections of ISM? |
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HII --> Halpha; HI --> 21cm line; molecular gas --> mostly CO rot. line, H2; Dust --> Blackbody Radiation |
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rank ISM components by density (low to high) |
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1) hot ionized gas (1/2 atoms /cm3); 2) neutral atomic gas(1-10 atoms / cm3); 3) cold molecular gas(10^2 - 10^5 atoms / cm3; 4) dust (solid) |
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ISM component proportions by most common? |
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1) neutral atomic gas 65%; 2) cold molecular gas 20%; 3) hot ionized gas 15%; 4) dust <5% |
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med cold ( between neutral atomic gas and cold molecular gas ) |
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recombination of electron from n = 3 to n = 2 emitting photon with wavelength 6563 angstroms |
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21cm wavelength emitted from change to parallel to antiparallel spins; smallest energy;
galactic plane; extends past stars |
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quantization of angular momentum |
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scatters blue light; transparent to red light; extinction and reddening; emits IR from absorbing UV/V |
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Halpha; compact region of SF; cna be in spiral arms; |
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HIneutralhot --(compressed/cooled)--> H2molecular --(ionization by O stars)--> HIIionizedhot --(massive stars die, recombination)--> HIneutralhot |
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Structure of HII region? (r from 0 to r) |
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H2(new stars) --> HII --> Dust --> HI |
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mass of stars / time of universe |
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Esfr = (2.5 E -4) * (Egas)^(1.4) |
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Purpose of Global Schmidt Law? |
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determining star formation rate per unit area |
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SFRefficiency * (density of gas) ^ (1.5); SFReff = Esfr / Egas |
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Components of Galaxy Kinematics? |
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Rotation and Velocity dispersion |
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random, dominant in ellipticals |
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(vdisp)^2 = (1/N) sum from 1 to N of (Vi - <V>)^2; where Vi is observed velocity; |
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Vobs = Vcsin(i) where i is inclination and Vc is rotation velocity |
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determines mass distribution |
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90% of galaxy mass, probably huge |
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NFW profile --> p(r) = p0 / ((r/rc)(1+(r/rc))^2) |
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Vc^2 = (Vc,DM)^2 + (Vc,bulge)^2 + (Vc,star)^2 + (Vc,gas)^2 Vc observed, Vbulge,star,gas from surface density |
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How to get rotation curve? |
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1) stars -measure surface photometry -convert to surface density using appropriate M/L 2) Gas -measure HI surface density -add correction for metals and molecular gas 3) Dark Matter -subtract first two components -fit function for DM density profiles |
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context of Tully-Fisher Relation? |
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Luminous galaxies have higher max Vc |
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L prop to (Vc)^N N = 3,4 M(abs) = C - 2.5*N*log10(Vc); more accurate with inclusion of gas |
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conclusion of tully-fisher? |
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faster rotation = more massive = more luminous; implies mass of Baryons through luminosity and velocity --> Vflat^2 = G*Menc / rmax |
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slow moving; interacts only through gravity; WIMPs or Axions. |
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Elliptical Galaxy Kinematics? |
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V is mostly random, therefore V = vdisp; Vdisp is anisotropic; some with kinematically distinct cores; vdisp rises to center; |
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M prop V^2 * R / G; for ellipticals? M prop vdisp^2 * R / G; |
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n = M / R^2 = V^2 /G * R; REVIEW WITH FUNDAMENTAL PLANE |
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Fundamental Plane theory vs observed? |
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theory : R prop E ^ -1 * vdisp ^ 2; obs: R prop E ^ -0.8 * vdisp^1.53 |
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Cause for error between theory and observed fundamental plane? |
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1) M/L not constant at all masses 2) structure non-homologous (e.g. ellipticals are not self-similar versions of each other) 3) Measurements are not consistent for all galaxy sizes |
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E = V^2 / G*R*Y; E*R/V^2 = const., where const depends on M/L; allows for trace of evolution of stellar mass/light ratio with time/redshift |
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Evol. of FP with redshift? |
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-assume structure of ellip. same at all redshifts and stars formed long ago -stars fade as bright massive stars die - same mass, lower L, M/L increases with time |
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Galaxy Formation Constraints? |
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Spirals: -formed from gas accretion with high angular momentum - gas --> stars Ellipticals: -repeated random mergers of gas and stars -gas streamed to center forming high density of stars |
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how does reionization affect galaxy evolution? |
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intense UV in early universe keeps gas too hot to form low mass galaxies |
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How does "feedback" affect galaxy evolution? |
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feedback - energy input from within galaxy drives out gas or shuts down accretion -SN - starburst - lots of SN in same location -AGN - central BH accretes gas, emits light, powers jets, injects energy into surrounding gas |
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how are galaxy mass and CBH mass related? |
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High L makes galaxy look like star, from washing out of galaxy light |
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luminous QSOs w/ radio emission and maybe radio jets |
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broad emission lines; blue; depends on viewing angle. |
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most massive gravitationally bound structures in Universe; too fast to stay together w/o DM |
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Rich = 30-300 bright galaxies poor = 5-10 bright galaxies (local group) |
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virial theorem --> Mtot = (5/3) R * vdisp^2 / G - 10 - 30% gas; hot ionized >10^7 K - metals - gas blown out or stripped away from other galaxies |
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Exogalactic Distance Ladder |
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radar (SS) --> stellar parallax (nearby stars) --> spectroscopic parallax(MW) --> Variable stars (nearby galaxies) --> TullyFisher --> Standard Candles (galaxies and galaxy clusters) |
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Distance through MS fitting? |
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apparent mag prop L/4pid^2; compare apparent mags with constant L; |
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distance through variable stars |
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1) measure period 2) derive luminosity 3) measure apparent brightness 4) derive distance |
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distance through TF relation |
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distance through fundamental plane |
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compare angular size to physical size R derived from vdisp and E surface brightness; estimate L for galaxy using cluster |
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extreme L common among type 1a; measure apparent brightness; derive d |
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light curve: broader is brighter; more L --> fades slower; Mmax,B = -21.726 + 2.698*deltam15b; |
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1. Random -use average to reduce 2. systematic - offset in one direction - miscalibration - fix by improving calibration - fix by using galaxies at large distances. |
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