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Astrophysics and Cosmology

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Presentation on theme: "Astrophysics and Cosmology"— Presentation transcript:

1 Astrophysics and Cosmology
Lecture #26 11/19/2018 Lecture XXVI

2 Concepts Parsec, light year Curved space Hubble’s law Big Bang
Early universe 11/19/2018 Lecture XXVI

3 Units to measure large distances
Light second = cx1s=3x108 m = 3x105 km Earth circumference = 40,000 km = 0.13 light seconds Earth – Moon = 1.28 light seconds Light minute = cx60s=1.8x1010 m Earth – Sun = 8.3 light minutes Earth – Pluto = 311 light minutes Light year = cx1y=9.46x1015 m 11/19/2018 Lecture XXVI

4 Scales of the universe Distance from Earth
Proxima Centauri (next door neighbor) – 4.3 ly Center of our Galaxy (Milky Way) 3x104 ly Our galaxy (Milky Way) is a disk D=100,000 ly thickness 2,000ly total number of stars in Milky Way ~1011 Nearest galaxy (Andromeda nebula) 2x106 ly Farthest galaxies 1010 ly 11/19/2018 Lecture XXVI

5 How to measure heavenly distances?
Cannot clock the light, cannot use a ruler… Parallax – apparent motion of a star against the background of more distant stars f=90-q D=d/tan(f) d=1.5x108km Parallax angle in seconds – distance to the star in Parsec = 3.26 ly q f d D 11/19/2018 Lecture XXVI

6 Other information from the sky
Apparent brightness  on average related to distances Spectrum  temperature Red shift – related to relative velocity  distances High energy radiation Neutrinos (m=~0, weak interaction) – propagate great distances Experiment  observation SLOAN digital sky survey: Hubble telescope: 11/19/2018 Lecture XXVI

7 Hubble deep field 11/19/2018 Lecture XXVI

8 Hertzsprung-Russel (H-R) diagram
Luminosity increases with star’s mass Temperature related to the wavelength lT=2.9x10-3mK By measuring l we can find T, then using H-R diagram we can predict the absolute brightness (L). The apparent brightness (l) is related to L and the distance to the star: 11/19/2018 Lecture XXVI

9 Evolution of the stars-I
Stars are born when gaseous clouds (mostly hydrogen) contract due to gravity Gravity accelerates the particles of the star inward  kinetic energy is increasing, could be large enough (1keV~107K) to overcome coulomb repulsion and start nuclear fusion HHe (In our Sun – yellow dwarf) Pressure from the energy released in fusion keeps the star from collapsing When the hydrogen in the core burns out the core contracts and T goes up  the outer envelope expands and cools down (Red giant) The core continues to heat up and He starts burning in fusion and continue to higher Z’s ending nucleosynthesis at Fe and Ni No pressure from fusion – gravitational collapse – white dwarf Pauli principle for orbital e keeps the star from further collapse T goes down white draft becomes black dwarf (cloud of ash) 11/19/2018 Lecture XXVI

10 Evolution of the stars-II
Heavier stars continue to burn beyond Fe and Ni in endoergic reactions In addition the following process can occur e-+pn+n Neutrons are formed in abundance – neutron star (>~1.5 mass of Sun, D~10km) Pauli principle for neutrons limit the size No electrostatic repulsion – leads to a catastrophic collapse – supernova explosion If mass of neutron star >2-3xSolar mass – black hole – not even light can escape 11/19/2018 Lecture XXVI

11 Gravity and curvature of space
Einstein’s general relativity: No observer can determine by experiment if he is accelerating or is rather in a gravitational field Explain gravity (interaction) through curvature of space (geometry) Establish equivalence between gravitational and inertial mass Experimental proof: Curving light: straight line becomes curved in gravitational field Extreme curvature – black hole: black because not even light can escape it 11/19/2018 Lecture XXVI

12 Expanding universe v=Hd The universe is expanding.
Redshift – spectral lines shifted – object is moving In 1929 Edwin Hubble, measured the redshifts of a number of distant galaxies. the redshift of distant galaxies increased as a linear function of their distance Hubble’s law v=Hd v- velocity of galaxies, d – distance H=80km/s/Mpc The universe is expanding. 11/19/2018 Lecture XXVI

13 Age of the universe v=Hd v- velocity of galaxies, d – distance
H=80km/s/Mpc = 20km/s/million ly Farthest galaxy 1010ly t=d/v=d/(dH)=1/H=15x109yr 11/19/2018 Lecture XXVI

14 Universe evolution Age of the universe 1010 years
Cosmic Microwave background – echo of the Big Bang 11/19/2018 Lecture XXVI

15 Cosmic microwave background
Discovered in 1964 by Arno Penzias and Robert Wilson as a “noise” in radio telescope Cosmic microwave background at l=7.35 cm Blackbody radiation at T=~3K Present precise measurement 2.7K Echo of the Big Bang, predicted in 1940 by George Gamow Radiation “decoupled” from matter when atoms were formed and there were no free electrons to scatter light (~3000K, 0.3 Myears after birth) 11/19/2018 Lecture XXVI

16 Fate of the Universe Gravity slows down the expansion
Depending on the density the universe might Continue to expand infinitely Collapse back to a point 11/19/2018 Lecture XXVI

17 WMAP Launched from cape Canaveral on June 30 2001
11/19/2018 Lecture XXVI

18 Trajectory Lunar swingby Phasing loops
WE ARE LIKE OUR OWN LITTLE PLANET… WE ORBIT THE SUN. Official arrival date: Oct 1, 2001 100 days to L2, 1.5e6 km from Earth. 11/19/2018 Lecture XXVI

19 COBE 1992 Bennett et al 2003 WMAP 2003 11/19/2018 Lecture XXVI

20 Facts first, then the conclusions!
11/19/2018 Lecture XXVI

21 BEYOND LCDM model FLATNESS + HST meas. of Ho (Spergel et al 2003)
Riess et al. 2001 + HST meas. of Ho de Bernardis et al 2000 Verde et al 2002 (Spergel et al 2003) 11/19/2018 Lecture XXVI After

22 We (and all of chemistry) are a small minority in the Universe.
Compare gravitational rotation of galaxies with luminous matter 11/19/2018 Lecture XXVI


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