Einstein, the searcher : $b his work explained from dialogues with EinsteinMoszkowski, Alexander
Philosophy
Einstein, the searcher : $b his work explained from dialogues with Einstein
Moszkowski, Alexander
Einstein, Albert, 1879-1955; Relativity (Physics)
Schopenhauer has, however, quite forgotten that he himself, some pages
earlier, trumpeted forth Newton's imperishable fame with the words: "To
form an estimate of the great value of the gravitational system which
was at least completed and firmly established by Newton, we must remind
ourselves how entirely nonplussed about the origin of the motion of
celestial bodies thinkers had previously been for thousands of years."
That bears the ring of truth. Newton's greatness can be grasped only if
thousands of years are used as a measure.
Whereas Schopenhauer argued from grounds drawn from psychology and the
principle of universal knowledge, his antagonist Hegel, who was still
more vague in these fields, sought to dispense with both Newton and
Kepler by calling to his aid the so-called pure intuition of the curved
line. In an exposition of truly comical prolixity, such as would have
delighted the hearts of scholiasts, he proves that the ellipse must
represent the fundamental type of planetary motion, this being quite
independent of Newton's laws, Kepler's observations, and resulting
mathematical relationships. And Hegel actually succeeds, with a nebulous
verbosity almost stultifying in its unmeaningness, in paraphrasing
Kepler's second law in his own fashion. It reads like an extract from
some carnival publication issued by scientists in a bibulous mood to
make fun of themselves.
But these extravagances, too, serve to add lustre to Newton, for his
genius shines out most brilliantly when it is a question of expressing
clearly, and without assumptions, a phenomenon of cosmic motion. Here
there are no forerunners, not even with regard to his own law of
gravitation. Newton showed with truly triumphant logic that Kepler's
second law belongs to those things that are really self-evident.
This law, taken alone, offers considerable difficulties to anyone who
learns of it for the first time. Every planet describes an ellipse; that
is accepted without demur. But the uninitiated will possibly or even
probably deduce from this that the planet will pass over equal lengths
of arc in equal times. By no means, says Kepler; the arcs traversed in
equal times are unequal. But if we connect every point of the elliptic
path with a definite point within the curve (the focus of the ellipse)
by means of straight lines, each of which is called a radius vector, we
get that the areas swept out by the radius vector in equal times (and
not the arcs) are equally great.
Why is this so? This cannot be understood _a priori_. But one might
argue that since the attraction of the sun is the governing force, this
will probably have something to do with Newton's law of gravitation, in
particular with the inverse square of the distance. And one might
further infer that, if a different principle of gravitation existed,
Kepler's law would assume a new form.
Public-domain text, read in full here on John Shaqi.
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