"In the beginning, there was nothing at all. Earth was not found, nor Heaven above, a Yawning-Gap there was, but grass nowhere."In this lecture period we discuss:
09/19/05
The activity below
explores the main steps in its evolution (requires free Macromedia
plug-in;
http://www.macromedia.com/downloads/ ).
RadiationElectromagnetic
Radiation includes visible light, radio waves, microwaves, x-rays,
gamma rays, and infra-red (heat) rays. All these forms of radiation
are characterized by traveling oscillations of a combined electric
and magnetic field. These electromagnetic waves differ by the
wavelength of the oscillation, with shorter wavelength radiation
carrying more energy than longer wavelength radiation.
All possible wavelengths make up the
electromagnetic
spectrum.
Planck's LawPlanck's Law is sometimes
called the "black-body" formula works very well for
celestial bodies:
Where E (lambda) is the
amount of radiant energy emitted at a given wavelength, lambda. T is
the temperature of the object, and a and b are constants.
The spectrum of wavelengths emitted by a body at a temperature, T, has a characteristic shape that is strongly dependent on the wavelength (to the inverse fifth power).
This law describes the spectral distribution of radiation emitted by a black body. Very hot bodies (3000 - 20,000 K) like our Sun emit a lot of light at visible wavelengths. The Sun acts like a black body near 6000K, whereas the Earth acts like a black body near 300 K (can you guess where its curve would lie?). Stefan-Boltzmann Law ("E equals sigma T to the fourth")
where E is the total energy emitted (calculated by adding up the areas
under the curves of Figure 1), sigma is a constant, and T is temperature.
Wein's LawThe wavelength
of the peak radiance [lambda (max)] decreases linearly as the temperature
increases, where c is a constant:
Summary of radiation laws
The Doppler Effect
Click here to see how the speed of an object affects wavelength. The Doppler Effect for Light is calculated by:
Big Bang TheoryThe Big Bang theory states that the Universe began when primordial mass exploded. This fireball gradually cooled as it expanded outward, and giant clouds of swirling gas formed the celestial bodies. The Big Bang theory does not explain why the bang occurred, but predicts (with surprising accuracy) what the consequences of the event. Evidence #1: atomic physicsIf the big bang occurred, the initial temperatures must have been so unimaginably high that matter could only have existed in exotic and unstable forms. As the temperature cooled in the first second, free hydrogen nuclei (atomic mass 1) were formed that could undergo fusion reactions to give heavier forms of hydrogen (atomic mass 2, 3) and helium (atomic mass 3 and 4). Thus, the theory predicts a early universe with only a mixture of ~75% hydrogen and 25% helium (by weight) and no heavier species. This ratio is exactly what is observed in stars. Evidence #2: red shiftMeasurements of the red shifts of virtually all galaxies (except a few in our immediate vicinity) show that the visible universe is expanding in all directions. The constant of proportionality between the distance and velocity of recession is known as Hubble's constant. Evidence #3: microwave radiationMeasurements of low energy microwave radiation show that the visible universe is permeated by "cosmic background" microwave radiation, coming from all directions and similar to what is expected from a black body at 3K. The Big Bang theory predicts that such radiation is the red-shifted remnant of the radiation released when matter and light became decoupled about 1 million years after the Big Bang. The American scientists who first made this measurement in 1965 (Penzias and Wilson) obtained the Nobel Prize.
COBE satellite results show that the cosmic ray background is not completely uniform in direction (see Figure), but that there is some clumping in preferred directions with differences in effective temperature of only one hundred millionth of a degree. This clumpiness would have been necessary for the big bang to produce galaxies, since a perfectly uniform explosion would not produce localized high densities.
All materials © the Regents of the University of Michigan unless noted otherwise. |
||||||||||||||||||