Astronomy: The Science of the Heavenly Bodies — John Shaqi
Astronomy: The Science of the Heavenly BodiesTodd, David P. (David Peck)
History
Astronomy: The Science of the Heavenly Bodies
Todd, David P. (David Peck)
Astronomy
Newton was born in 1643, the year after the death of Galileo. He had a
thorough training in the mathematics of his day, and addressed himself
first to an investigation and definite formulation of the general laws
of motion, which he found to be three in number, and which he was able
to put in very simple terms. The first one is: Any body, once it is set
in motion, will continue to move forward in a straight line with a
uniform velocity forever, provided it is acted upon by no force
whatever. In other words, a state of motion is as natural as a state of
rest (rest in relation to things everywhere adjacent) in which we find
all things in general.
Here on earth where gravity itself pulls all objects downward toward the
earth, and where resistance of the air tends to hold a moving body back
and bring it to rest, and where friction from contact with whatever
material substance may be in its path is perpetually tending to
neutralize all motion--with all three of these forces always at work to
stop a moving body, the truth of this first and fundamental law of
motion was not apparent on the surface.
Till Galileo's time everyone had made the mistake of supposing that some
force or other must be acting continually on every moving body to keep
it in motion. Ptolemy, Copernicus, Kepler, Leonardo da Vinci--all failed
to see the truth of this law which Newton developed in the immortal
_Principia_. And at the present day it is not always easy to accept at
first, although the progress of mechanical science, by reducing friction
and resistance, has produced machines in which motion of large masses
may be kept up indefinitely with the application of only the merest
minimum of force.
Once a planet is set in motion round the sun, it would go on forever
through frictionless, non-resistant space; but there must be a central
force, as Huygens saw clearly, to hold it in its orbit. Otherwise it
would at any moment take the direction of a tangent to the orbit. Here
is where Newton's second law of motion comes in, and he formulated it
with great definiteness. When any force acts on a moving body, its
deviation from a straight line will be in the direction of the force
applied and proportional to that force.
In accord with this law, Newton first began to inquire whether the force
of attraction here on earth, which everyone commonly recognizes as
gravity, drawing all things down toward the center of the earth, might
not extend upward indefinitely. It is found in operation on the summits
of mountain peaks, and the clouds above them and the rain falling from
them are obviously drawn downward by the same force. May it not extend
outward into space, even as far as the moon?
Public-domain text, read in full here on John Shaqi.
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