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Project Cyclops, A Design... - Department of Earth and Planetary ...

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Red Giant. The transition from main sequence star to<br />

red giant is very short, as evidenced by the scarcity <strong>of</strong><br />

stars observed in this phase. Hydrogen burning in the<br />

shell stabilizes the star as a red giant for a time, but as<br />

the shell grows the rate <strong>of</strong> burning drops <strong>and</strong> the star<br />

again contracts. This time the contraction raises the<br />

temperature in the core to the point where helium<br />

fusion can commence <strong>and</strong> the star, now obtaining energy<br />

from both hydrogen <strong>and</strong> helium fusion, again exp<strong>and</strong>s.<br />

Eventually, a core <strong>of</strong> elements heavier than helium forms<br />

<strong>and</strong> the hydrogen <strong>and</strong> helium burning shells approach<br />

each other. Here the interaction becomes complicated<br />

<strong>and</strong> computer modeling has not as yet been successful<br />

beyond this stage.<br />

Advanced Age. When gravitational contraction can no<br />

longer increase the core temperature <strong>and</strong> density sufficiently<br />

to initiate the next series <strong>of</strong> reactions, the star<br />

evolves away from the red giant region. Its path is to the<br />

left in the HR diagram <strong>of</strong> Figure 2-3 at roughly constant<br />

luminosity. During this time, the star may enter a<br />

pulsating phase, return briefly to the red giant regime,<br />

then conclude by slowly or violently ejecting its surface<br />

layers. Most frequently, the end result is a white dwarf.<br />

It is a configuration in which the material is almost<br />

completely degenerate from center to surface. The<br />

physical size <strong>of</strong> these objects is about the same as the<br />

<strong>Earth</strong>, but. their mass is between 0.2 <strong>and</strong> 1.2 solar<br />

masses. The surface temperature is typically 6,000 to<br />

12,000 ° K. Because <strong>of</strong> the small radius, the luminosity is<br />

very low compared with the Sun, even though the<br />

temperature is higher [see eq. (1)].<br />

A more violent, explosive end for a star is called a<br />

supernova (Lma x typically 108 Lo) <strong>and</strong> produces large<br />

quantities <strong>of</strong> heavy elements. These elements are ejected<br />

with velocities <strong>of</strong> roughly 104 km/sec <strong>and</strong> so soon<br />

become well mixed with the interstellar medium. The<br />

star may not always be entirely destroyed by the<br />

process: At the center <strong>of</strong> the exp<strong>and</strong>ing clouds, rotating<br />

neutron stars (pulsars) have been discovered. Such<br />

explosive fates await stars <strong>of</strong> 10 solar masses or larger.<br />

They are the primary source <strong>of</strong> elements heavier than<br />

neon <strong>and</strong> provide a large fraction <strong>of</strong> the elements<br />

between helium <strong>and</strong> neon.<br />

Clearly when a star leaves the main sequence the<br />

effects on its planets are catastrophic. It is doubtful if<br />

even very intelligent life could remain in the planetary<br />

system <strong>and</strong> avert disaster. (Our Sun will not enter the<br />

giant phase before approximately seven billion more<br />

years.) So far as intelligent life is concerned we should<br />

therefore confine our attention to main sequence stars,<br />

<strong>and</strong> probably only to those cooler than F0. When we<br />

come to consider atmospheric evolution <strong>and</strong> tidal effects<br />

we will want to exclude M stars. Thus, the stars <strong>of</strong><br />

greatest interest are F, G, <strong>and</strong> K main sequence stars,<br />

which amount to about 25 percent <strong>of</strong> all stars. If we<br />

exclude binary <strong>and</strong> multiple star systems, because <strong>of</strong><br />

unstable planetary orbits, this still leaves over 20 billion<br />

stars in the galaxy as possible suns for intelligent life.<br />

The Solar<br />

Neighborhood<br />

ls ours in any way a special neighborhood? Photographs<br />

<strong>of</strong> spiral galaxies give the impression that most<br />

stars are concentrated in the nucleus <strong>and</strong> along the spiral<br />

arms. Our Sun is located midway between two spiral<br />

arms-actually, on the fringe <strong>of</strong> a spur extending <strong>of</strong>f one<br />

arm. We are about 33,000 light-years from the galactic<br />

center or two-thirds <strong>of</strong> the way to the rim. The disk is<br />

about 1500 light-years thick at this radius, <strong>and</strong> the Sun<br />

is only a few tens <strong>of</strong> light-years <strong>of</strong>f the midplane. At first<br />

glance, it might appear that we are in a somewhat<br />

isolated neighborhood but this is not the case.<br />

It is true that the star density in the nucleus is<br />

extremely high-a hundred or more times that in the<br />

solar neighborhood. This means that the average separation<br />

between stars is only 20 to 25 percent as great as<br />

here. But only 10 percent <strong>of</strong> the total stellar mass is in<br />

the nucleus.<br />

Contrary to common belief, the spiral arms are not<br />

regions <strong>of</strong> higher star density. They are regions <strong>of</strong> high<br />

gas <strong>and</strong> dust density, the maternity wards <strong>of</strong> the Galaxy,<br />

where new stars are being born at a higher rate. The gas<br />

clouds fragment to form clusters <strong>of</strong> hundreds <strong>of</strong> thous<strong>and</strong>s<br />

<strong>of</strong> new stars including a large number <strong>of</strong> shortlived<br />

O <strong>and</strong> B stars. These stars die before their motions<br />

carry them very far from their birthplace. It is these very<br />

bright stars scattered along tile spiral arms that give the<br />

arms their extra brightness.<br />

The rotation about the galactic center <strong>of</strong> the stars in<br />

the disk is quite different from that <strong>of</strong> the spiral arm<br />

pattern. The Sun, along with most other stars in our<br />

neighborhood, circles the galactic center once each 240<br />

million years <strong>and</strong> in one orbit will cross all components<br />

<strong>of</strong> the spiral arms. Stars born in the spiral arms drift out<br />

<strong>of</strong> the arms <strong>and</strong>, because <strong>of</strong> their velocity dispersion,<br />

become thoroughly mixed with older stars. While we can<br />

find the common age <strong>of</strong> stars in a cluster by noting the<br />

mass <strong>and</strong> hence the age <strong>of</strong> those leaving the main<br />

sequence, we can only estimate the general population<br />

class <strong>of</strong> isolated stars. Thus, if we should decide that 4<br />

billion years were needed to evolve a technological<br />

civilization, we have no way <strong>of</strong> determining whether a<br />

particular population ! star is too young or too old. The<br />

thorough mixing <strong>of</strong> stars with time means that there is<br />

12

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