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As we mentioned in The Spectra of Stars (and Brown Dwarfs) section, astronomers use the term “metals” to refer to all elements heavier than hydrogen and helium. The fraction of a star’s mass that is composed of these elements is referred to as the star’s metallicity . The metallicity of the Sun, for example, is 0.02, since 2% of the Sun’s mass is made of elements heavier than helium.

Appendix K lists how common each element is in the universe (compared to hydrogen); these estimates are based primarily on investigation of the Sun, which is a typical star. Some very rare elements, however, have not been detected in the Sun. Estimates of the amounts of these elements in the universe are based on laboratory measurements of their abundance in primitive meteorites, which are considered representative of unaltered material condensed from the solar nebula (see the Cosmic Samples and the Origin of the Solar System chapter).

Radial velocity

When we measure the spectrum of a star, we determine the wavelength of each of its lines. If the star is not moving with respect to the Sun, then the wavelength corresponding to each element will be the same as those we measure in a laboratory here on Earth. But if stars are moving toward or away from us, we must consider the Doppler effect (see The Doppler Effect section). We should see all the spectral lines of moving stars shifted toward the red end of the spectrum if the star is moving away from us, or toward the blue (violet) end if it is moving toward us ( [link] ). The greater the shift, the faster the star is moving. Such motion, along the line of sight between the star and the observer, is called radial velocity    and is usually measured in kilometers per second.

Doppler-shifted stars.

Diagram illustrating the Doppler Shift. At bottom is the wavelength scale in nanometers (nm), starting at 400 nm on the left and progressing to 750 nm at right. Above the scale are three spectra, one above the other. The spectrum in the center shows a stationary object, with five hypothetical spectral lines shown at their rest positions. At top red-shift is illustrated with the same five lines each equally moved slightly to the right, or to the red part of the spectrum. At bottom blue-shift is illustrated with the same five lines each equally moved slightly to the left, or to the blue part of the spectrum. This image is for illustrative purposes, and no exact red- or blue-shift value is given.
When the spectral lines of a moving star shift toward the red end of the spectrum, we know that the star is moving away from us. If they shift toward the blue end, the star is moving toward us.

William Huggins , pioneering yet again, in 1868 made the first radial velocity determination of a star. He observed the Doppler shift in one of the hydrogen lines in the spectrum of Sirius and found that this star is moving toward the solar system. Today, radial velocity can be measured for any star bright enough for its spectrum to be observed. As we will see in The Stars: A Celestial Census , radial velocity measurements of double stars are crucial in deriving stellar masses.

Proper motion

There is another type of motion stars can have that cannot be detected with stellar spectra. Unlike radial motion, which is along our line of sight (i.e., toward or away from Earth), this motion, called proper motion    , is transverse : that is, across our line of sight. We see it as a change in the relative positions of the stars on the celestial sphere ( [link] ). These changes are very slow. Even the star with the largest proper motion takes 200 years to change its position in the sky by an amount equal to the width of the full Moon, and the motions of other stars are smaller yet.

Large proper motion.

Photographs of Barnard’s Star demonstrating its large proper motion. At left (a) the star is seen in the center of an image taken in 1985, along with several background stars. At center (b) is the same field as photographed in 1995. The background stars have not moved, but Barnard’s Star has moved downward from the center of the image (where is was seen in 1985). At right (c) is the same field in 2005. The background stars have again not moved, and Barnard’s Star is now near the bottom of the image.
Three photographs of Barnard’s star, the star with the largest known proper motion, show how this faint star has moved over a period of 20 years. (modification of work by Steve Quirk)

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Source:  OpenStax, Astronomy. OpenStax CNX. Apr 12, 2017 Download for free at http://cnx.org/content/col11992/1.13
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