Radiation |
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wavelength x frequency = velocity |
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wavelength x frequency = 300,000 km/sec |
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Nature's primary charged particles are: | ||
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Its light output depends only on its temperature.> The sun and stars emit radiation like a blackbody following the Blackbody spectrum.> As an object (a blackbody) is heated, the radiation it emits will always be described by the blackbody spectrum for the temperature of the body, with the curve peaking to higher and higher frequency. > >
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(b.) a dim, young star (T=600 K) (c.) the Sun, with a surface temperature of 6000 K (d.) a globular cluster of bright stars, Messier 2 (T=60,000 K)
(b.) infrared wavelengths (c.) visible wavelengths (d.) X-ray wavelengths (e.) gamma-ray wavelengths |
> We refer to the amount of radiation for the star at our location as the apparent brightness.> > The apparent brightness of a star is inversely proportional to the square of its distance:> >
> > This Law results from the spreading of the energy in the radiation.> |
> The observed speed will not depend on relative motion.> > However, the wavelength of the light does change with relative motion.> > Stars moving away from us appear red-shifted and stars moving toward us appear blue-shifted.> > This can be illustrated by considering the wave crests of the wave motion.> |
The Light-year (ly):> The parsec (pc)> 1 parsec = 3.26 light-years The "local" neighborhood |