by which the times of sunset at two places could be
compared. He was acquainted with the fact, which
must indeed have been known from the very earliest
times, that the illumination of the moon is derived
entirely from the sun. He knew that an eclipse
of the moon was due to the interposition of the earth
which cuts off the light of the sun. It was,
therefore, plain that an eclipse of the moon must
be a phenomenon which would begin at the same instant
from whatever part of the earth the moon could be
seen at the time. Ptolemy, therefore, brought
together from various quarters the local times at
which different observers had recorded the beginning
of a lunar eclipse. He found that the observers
to the west made the time earlier and earlier the
further away their stations were from Alexandria.
On the other hand, the eastern observers set down
the hour as later than that at which the phenomenon
appeared at Alexandria. As these observers all
recorded something which indeed appeared to them simultaneously,
the only interpretation was, that the more easterly
a place the later its time. Suppose there were
a number of observers along a parallel of latitude,
and each noted the hour of sunset to be six o’clock,
then, since the eastern times are earlier than western
times, 6 p.m. at one station A will correspond to
5 p.m. at a station B sufficiently to the west.
If, therefore, it is sunset to the observer at A,
the hour of sunset will not yet be reached for the
observer at B. This proves conclusively that the
time of sunset is not the same all over the earth.
We have, however, already seen that the apparent
time of sunset would be the same from all stations
if the earth were flat. When Ptolemy, therefore,
demonstrated that the time of sunset was not the same
at various places, he showed conclusively that the
earth was not flat.
As the same arguments applied to all parts of the
earth where Ptolemy had either been himself, or from
which he could gain the necessary information, it
followed that the earth, instead of being the flat
plain, girdled with an illimitable ocean, as was generally
supposed, must be in reality globular. This
led at once to a startling consequence. It was
obvious that there could be no supports of any kind
by which this globe was sustained; it therefore followed
that the mighty object must be simply poised in space.
This is indeed an astonishing doctrine to anyone
who relies on what merely seems the evidence of the
senses, without giving to that evidence its due intellectual
interpretation. According to our ordinary experience,
the very idea of an object poised without support in
space, appears preposterous. Would it not fall?
we are immediately asked. Yes, doubtless it
could not remain poised in any way in which we try
the experiment. We must, however, observe that
there are no such ideas as upwards or downwards in
relation to open space. To say that a body falls
downwards, merely means that it tries to fall as nearly