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6. Star Colors and the Hertzsprung
6. Star Colors and the Hertzsprung

... H is a constant Ho called the Hubble constant. One gets a linear relation between expansion speed (as measured by redshift) and distance v = Ho d ...
Big Bang and Beyond
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What we will do today:
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Gravitational Collapse with Negative Energy Field
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Chapter 12 Our Place in the Universe
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Echoes of the Early Universe

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... Doppler Shift and the Expanding Universe Your instructor will discuss the Doppler shift of light waves from a moving source. a) A stationery light source emits waves of light uniformly in all directions as shown in the diagram. How do the wavelengths of light from the right side of the diagram compa ...
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... The universe began about 13 thousand million years ago, in a hot Big Bang. During a brief period known as “inflation”, which lasted only for a tiny fraction of a second, the universe expanded rapidly. Immediately after inflation, the rate of expansion dropped dramatically; but the universe continued ...
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... could be many worlds that had plenty of time for life to arise and evolve. These worlds might have had civilizations millions or billions of years ago. The scale of time holds sobering lessons for our own future. Species have come and gone in the months of the cosmic calendar, and there is no reason ...
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1_Introduction - Department of Astronomy

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PSCI 1414 General Astronomy

... • Star system – A star and all the material that orbits it, including planets, dwarf planets like Pluto, and other small solar system bodies • Galaxy – A gravitationally bound system of stars, gas, and dust • Galaxy cluster (or group) – A collection of galaxies bound together by gravity • Superclust ...
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1_Introduction

... A single shell will produce a tiny flux here at Earth. For a shell 1 parsec thick, flux = t × n × L = 40 nanowatts/meter2 ...
The Island Universe of Immanuel Kant - EU-HOU
The Island Universe of Immanuel Kant - EU-HOU

... much farther galaxies could be measured. As can be easily noticed in the previous slide (right panel), Hubble law works very well: velocity/distance ratio remains constant in a wide range of these two quantities, particularly for more distant galaxies where the proper motions velocities become negli ...
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Flatness problem



The flatness problem (also known as the oldness problem) is a cosmological fine-tuning problem within the Big Bang model of the universe. Such problems arise from the observation that some of the initial conditions of the universe appear to be fine-tuned to very 'special' values, and that a small deviation from these values would have had massive effects on the nature of the universe at the current time.In the case of the flatness problem, the parameter which appears fine-tuned is the density of matter and energy in the universe. This value affects the curvature of space-time, with a very specific critical value being required for a flat universe. The current density of the universe is observed to be very close to this critical value. Since the total density departs rapidly from the critical value over cosmic time, the early universe must have had a density even closer to the critical density, departing from it by one part in 1062 or less. This leads cosmologists to question how the initial density came to be so closely fine-tuned to this 'special' value.The problem was first mentioned by Robert Dicke in 1969. The most commonly accepted solution among cosmologists is cosmic inflation, the idea that the universe went through a brief period of extremely rapid expansion in the first fraction of a second after the Big Bang; along with the monopole problem and the horizon problem, the flatness problem is one of the three primary motivations for inflationary theory.
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