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The Doppler Effect in Astronomy and Cosmology The Doppler Effect A passing ambulance A passing train Doppler Effect in Cosmology 2 The Doppler Effect for Sound The radio emits a series of “beeps,” with period T. If the Flash is stationary, he will hear the beeps with a period T’ = T. There is no Doppler shift. Doppler Effect in Cosmology 3 The Doppler Effect for Sound Now the Flash starts running away from the radio. The Flash is running away, and so the beeps take longer to reach him, and so he hears a period T’, which is not equal to T, but is bigger. Doppler Effect in Cosmology 4 The Doppler Effect for Sound Now the Flash starts running away from the radio. Suppose the Flash is running at a constant velocity, v, and the sound is traveling at a speed vS. They start an initial distance d apart. Flash hears the first beep at time d t1 = vs " v Doppler Effect in Cosmology 5 The Doppler Effect for Sound Now the Flash starts running away from the radio. The radio waits a time T to send out the next beep, while the Flash is running the whole time. So, he hears the next beep at time d + v sT t2 = vs " v Doppler Effect in Cosmology 6 The Doppler Effect for Sound Now the Flash starts running away from the radio. So, the Flash hears a period T’=t2 - t1. vs T T" = T= vs # v 1# v v S Doppler Effect in Cosmology 7 The Doppler Effect for Sound Now the Flash starts running away from the radio. Since the frequency is f =1/T’, then we can write $ v' f " = &1# ) f % vS ( Doppler Effect in Cosmology 8 The Doppler Effect for Sound What if both are moving? If the speed of the source is v0, the speed of sound is vS, and the speed of the receiver is vR, then # vS m vR & f "=% (f $ vS ± v0 ' Doppler Effect in Cosmology 9 The Doppler Effect for Light Because light behaves like a wave, it still has a Doppler effect. However, the equations are different! c±v f "= f c mv The Special Theory of Relativity. ! Doppler Effect in Cosmology 10 The Doppler Effect for Light Redshift. Blueshift. A source of light moving at v = 0.7c. Doppler Effect in Cosmology 11 Spectral Lines When electrons in an atom make a transition from a bigger orbit to a lower one, they emit light. Every atom has a characteristic spectrum. Doppler Effect in Cosmology 12 Spectrum of a Star The Sun emits a continuous spectrum like a blackbody with a temperature of 5800 K. The spectrum of the Sun shows absorption lines. By looking at the spectrum, we can determine the chemical composition of a star. Doppler Effect in Cosmology 13 Spectrum of Stars in a Distant Galaxy The stars (of a certain type) have the same spectrum, no matter where they are. The spectrum from stars shows same absorption lines. Doppler Effect in Cosmology The lines are shifted! 14 Edwin Hubble The Universe is expanding!!! v = H0d Doppler Effect in Cosmology 15 Doppler Effect in Cosmology 16 The Evolution of the Universe Doppler Effect in Cosmology 17 The Cosmic Microwave Background The Universe started off extremely hot and dense, with LOTS of high-energy photons around. As the Universe expands, the UV photons can start freestreaming from the Surface of Last Scattering at z ~ 1100. Doppler Effect in Cosmology 18 The Cosmic Microwave Background The photon wavelength grows with the expansion! The Universe has expanded by a factor of z ~ 1100 since the LSS, and so the photons are in the microwave region. If the Big Bang picture is correct, there should be a Cosmic Microwave Background! Doppler Effect in Cosmology 19 Penzias and Wilson The CMB was discovered (accidentally) in 1964, and has a perfect blackbody spectrum with tiny deviations! Doppler Effect in Cosmology 20 Tiny Deviations Lead to Structure in the Universe COBE WMAP This is an area of active research today, and is based very much on the Doppler effect! Doppler Effect in Cosmology 21