The Drake Equation was developed in the infancy of the SETI project. The Search for Extra-Terrestrial Intelligence was a US-sponsored project starting over sixty years ago, designed to listen for any kind of electromagnetic broadcasts than another intelligent civilization might be emitting. The equation is simplicity itself, just a product of conditional probabilities. Here it is:
N = R*.fp
.Ne
.fl
.fi
.fc
.L
and N is the number of detectable alien
civilizations in the galaxy,
R* is the rate at which
stars form in the galaxy,
fp is the fraction of stars
which develop planets,
Ne is the number of planets
within a planetary systems which have the right conditions for life,
fl is the fraction of
planets with the right conditions for life which develop life,
fi is the fraction of
planets which develop life up to the level of intelligence,
fc is the fraction of
planets with intelligent life that build systems to radiate
electromagnetic waves,
L is the length of time such
civilizations persist in their radiation.
There are a number of assumptions made
which permit the formula for N to be expressed this way. Let us
discuss a few of them.
First,
the Milky Way galaxy is chosen as the basis for measuring everything.
We only know that life can originate on a spiral arm, far away from
the bulge and the black holes which inhabit the center. It seems
quite reasonable that life needs billions of years to evolve to the
stage where a civilization emerges and starts emitting radiation, and
in the bulge, distant stellar encounters happen much more frequently
than in the spiral arms. A stellar encounter can create a
gravitational pull on a planetary system to disturb it, and a planet
which had conditions for life prior to the encounter may be moved
either inward or outward relative to its star, where the conditions
do not hold. Two solutions might be done for this, either change R*
to only count spiral arm stars or modify all the subsequent
probabilities to take into account the different conditions between
the spiral arms and the central bulge.
Second, the term detectable can be
defined a number of ways. Since radiation dies off as the square of
the distance travelled, without absorption, and worse with
absorption, does detectable mean detectable with
some particular equipment? Imagining a ten kilometer aperture
radio dish out beyond Neptune's orbit, and compare that with the
original SETI equipment. If one wants to be able to detect a
civilization's emissions from the other side of the Milky Way,
assuming the central bulge does not intervene, something huge would
be required on both ends.
Third, the equation seems to be
assuming roughly isotropic radiation, spreading equally in every
direction, including the one direction that heads toward Earth. Why
would any civilization do that? There might be some transitory
period when they were broadcasting for their own planetary uses, but
if they wanted to communicate from solar system to solar system, they
would
develop a narrow beam system that would require only a tiny
fraction of the power of an isotropic radiator. But then detectable
means that Earth is in the beam of such a system. That would be
rather fortuitous.
Fourth, the fraction of stars which
develop planets might be, as we now know, approximately one, but
developing planets does not mean life can evolve on one of them, or
certainly not to the threshold of EM emissions. Stars heavier than
our star burn out quickly, and if one included them in the count,
they could have planets and one could have the right conditions for
life, but these conditions would soon change as the star evolved and
died. On the other end of the scale, M dwarfs, the most populous
kind of star, doesn't have enough energy output to have a planet with
the conditions for life, except if it is close in, and there it would
be likely phase-locked, with the same face always directed at the
star. There
are good objections to assuming life could evolve in such a system.
For the mid-range of stars, where our
sun resides, there might be planets, and one or two with the
conditions for life, but we know little about the migration of
planets, even without the evolution of the parent star. Do smaller
planets keep their orbits for billions of years in any planetary
system, or does it take billions of years for them to gradually
migrate inward or outward? If we change the definition to having a
planet of the right size in the liquid water zone for billions of
years, the number might drop from about 1.0 to 0.00001. Figuring out
long-term stability of orbits should be a fairly simple task for the
current state of mathematical astrophysics, but it does not seem to
have been done in a comprehensive way that enables on to figure out
this term in Drake's equation.
Fifth, exactly what does the
“conditions for life” entail? If it is made very loose, the
corresponding probability would be high, and the subsequent
probability would be less to make up for the looseness. If it is
made tight, the inverse happens. At the time the Drake equation was
written, mankind did not know how life forms, nor what were the
conditions needed for it. Now, sixty years later, the same situation
exists. We don't know. It is appalling that so little work is done
on the origination for life. One particular question is that, are
there some conditions in which life forms over a period of time,
something large compared to human lifetimes but small compared to
solar lifetimes, like a million years? Or is the situation
completely opposite, life
only forms if some event happens, and the probability of the
event might be very, very small.
Just suppose, as hypothesized in this
blog, a mild collision with a large planetoid, which becomes a
satellite, is necessary
for life. The collision would have occurred in the early part of
the solar system's existence. Earth-like planets which did not have
that collision in their history might be similar in many conditions
to ones which did, but, if the hypothesis is correct, only the latter
could have life. There are certainly other events in the history of
a planet which might affect the origination of life, such as the
chemical composition of the crust, volcanic heating, and asteroidal
bombardment.
To be generous, life originated three
or four billion years ago, and we do not know the conditions of the
Earth's surface, so we are limited in imagining how life could
originate. The delay in life origination work might be caused by the
delay in planet origination work. Neither is in a good state. There
is no reason to think that current conditions on the Earth could lead
to an origination of life, assuming all consequences of life were
removed. One of the conditions discussed in this blog is the
existence of organic
oceans on the surface, able to nurture membrane formation as well
as complex protein formation. Where might they come from? The mild
collision hypothesis is a possibility for this.
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