Project Cyclops, A Design... - Department of Earth and Planetary ...
Project Cyclops, A Design... - Department of Earth and Planetary ...
Project Cyclops, A Design... - Department of Earth and Planetary ...
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intooceans, <strong>and</strong>withthesmallerUV<strong>and</strong>X-rayfluxat 1<br />
AU,theearlytectonicatmosphere <strong>of</strong> the<strong>Earth</strong>would<br />
havebeenstable.However, even<strong>Earth</strong>couldnothave<br />
engendered life,givenasmuchCO2buildupasoccurred on<br />
Venus.Most<strong>of</strong> thecarbonin the<strong>Earth</strong>'scrustislocked<br />
upin limestone. Calcium<strong>and</strong>magnesium silicatesreact<br />
with CO2in waterto form silica<strong>and</strong>calciumor<br />
magnesium carbonates. OnVenus,thelack<strong>of</strong> oceans<br />
prevented thisreaction.<br />
A greatdeal<strong>of</strong>limestone aswellasallcoal<strong>and</strong>oil are<br />
the fossil remnants <strong>of</strong> early life. It may well be that<br />
life appeared quite early <strong>and</strong>, through photosynthesis,<br />
started removing CO2 from the atmosphere before<br />
tectonic activity had released anywhere near the amount<br />
that has accumulated on Venus. We must remember that<br />
volcanic activity is due to heat produced by the decay <strong>of</strong><br />
long-lived istopes <strong>and</strong>, while it may have been greater<br />
initially, it has continued for billions <strong>of</strong> years. Vegetation<br />
<strong>and</strong> plankton are responsible for the extremely<br />
small percentage <strong>of</strong> COz in the present<br />
atmosphere despite all our burning <strong>of</strong> fossil fuels. Living<br />
systems have certainly assisted in the CO2 removal <strong>and</strong><br />
may have been the decisive factor. If so, then life may be<br />
what saved <strong>Earth</strong> from the heat death <strong>of</strong> Venus, <strong>and</strong> is as<br />
much responsible for our fleecy skies <strong>and</strong> blue seas as it<br />
is beholden to them. Let us hope this symbiosis will<br />
continue!<br />
ECOSPHERES AND GOOD SUNS<br />
The ecosphere is the region surrounding a star within<br />
which planetary conditions can be right to support life.<br />
Too close to the star, any planet will be too hot; too far<br />
away, any planet will be too cold. We do not know<br />
precisely the limits <strong>of</strong> insolation that define the ecosphere.<br />
Dole, in his study <strong>of</strong> the probability <strong>of</strong> planets<br />
being habitable by man (ref. 4), choses the limits at 65<br />
percent <strong>and</strong> 135 percent <strong>of</strong> the solar flux on <strong>Earth</strong> on<br />
the basis that 10 percent <strong>of</strong> the surface would then be<br />
habitable. If we consider the adaptability <strong>of</strong> life <strong>and</strong> do<br />
not require man to survive the environment these limits<br />
may be pessimistic. On the other h<strong>and</strong>, the factors<br />
responsible for appropriate atmospheric evolution may<br />
be more limiting than the temperature that would later<br />
exist on an <strong>Earth</strong>like planet at various distances.<br />
We can say that for an <strong>Earth</strong>-size planet, the inner<br />
ecosphere limit in the solar system lies somewhere<br />
between <strong>Earth</strong> <strong>and</strong> Venus. Rasool feels that the limit is<br />
not closer to the Sun than 0.9 AU, corresponding to ! 23<br />
percent <strong>of</strong> <strong>Earth</strong>'s insolation. On the other h<strong>and</strong>, Mars,<br />
at i.5 AU <strong>and</strong> with 43 percent as much solar flux, is<br />
probably barren, not because <strong>of</strong> too little sunlight, but<br />
because it is too small to have had enough tectonic<br />
activity to give it much <strong>of</strong> an atmosphere. With a heavier<br />
atmosphere than ours, the greenhouse effect could make<br />
conditions on Mars quite livable.<br />
The greater the ratio <strong>of</strong> the outer to inner radius <strong>of</strong><br />
ecosphere the greater the probability <strong>of</strong> finding one or<br />
more planets within it. Dole has computed these<br />
probabilities using the data on planetary spacings <strong>of</strong> the<br />
solar system. Taking (rmax/rmin) = 1.5, his curves show<br />
a 66 percent probability <strong>of</strong> one favorably situated planet<br />
<strong>and</strong> a 5 to 6 percent probability <strong>of</strong> two. Since we do not<br />
have statistics for other planetary systems, all we can do<br />
is fall back on the assumption <strong>of</strong> mediocrity <strong>and</strong> say that<br />
something over half <strong>of</strong> all planetary systems should have<br />
at least one favorably situated planet.<br />
As we consider stars <strong>of</strong> increasing luminosity, the<br />
ecosphere moves out <strong>and</strong> widens. As Cameron observes,<br />
if Bode's law holds generally-if the planetary spacing is<br />
proportional to distance from the primary-this exactly<br />
compensates for the widening <strong>of</strong> the ecosphere <strong>and</strong> gives<br />
a constant probable number <strong>of</strong> planets per ecosphere,<br />
regardless <strong>of</strong> the size <strong>of</strong> the primary star. Assuming that<br />
the more luminous stars were able to dissipate their<br />
nebulae to proportionately greater distances so that<br />
terrestrial planets could evolve, the upper limit <strong>of</strong><br />
luminosity for a good sun is reached when the stellar<br />
lifetime becomes too short. If intelligent life typically<br />
requires the 4-1/2 billion years it has taken to evolve on<br />
<strong>Earth</strong> we see from Figure I-7 that we should exclude all<br />
stars hotter than F4 stars.<br />
As we consider stars <strong>of</strong> decreasing luminosity, the<br />
ecosphere shrinks <strong>and</strong> a new difficulty arises, if the tidal<br />
braking becomes great enough to stop the planet's<br />
rotation, the entire atmosphere will probably freeze out<br />
on the dark side <strong>and</strong> all life will die. To estimate the<br />
limit imposed by this effect, let us divest the <strong>Earth</strong> <strong>of</strong> its<br />
moon <strong>and</strong> bring the <strong>Earth</strong> closer to the Sun, decreasing<br />
the Sun's luminosity (<strong>and</strong> mass) to keep the insolation<br />
constant, until the solar tide equals the present combined<br />
solar <strong>and</strong> lunar tide. Since the solar tide is 46<br />
percent <strong>of</strong> the lunar tide we can afford to increase the<br />
solar tide by the<br />
factor:<br />
k =<br />
x/! + (0.46) 2<br />
- 2.4 (6)<br />
0.46<br />
without changing the tidal drag <strong>Earth</strong> has experienced.<br />
The tide raising force is proportional to M/r 3, while the<br />
insolation is proportional to M3"S/r 2. Thus if we keep<br />
the insolation constant, M will vary as r2/3"s <strong>and</strong> the<br />
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