CHAPTER X

KEPLER, THE GREAT CALCULATOR

Most fortunate it was for the later development of astronomical theory

that Tycho Brahe not only was a practical or observational astronomer of

the highest order, but that he confined himself studiously for years to

observations of the places of the planets. Of Mars he accumulated an

especially long and accurate series, and among those who assisted him in

his work was a young and brilliant pupil named Johann Kepler.

Strongly impressed with the truth of the Copernican System, Kepler was

free to reject the erroneous compromise system devised by Tycho Brahe,

and soon after Tycho's death Kepler addressed himself seriously to the

great problem that no one had ever attempted to solve, viz: to find out

what the laws of motion of the planets round the sun really are. Of

course he took the fullest advantage of all that Ptolemy and Copernicus

had done before him, and he had in addition the splendid observations of

Tycho Brahe as a basis to work upon.

Copernicus, while he had effected the tremendous advance of substituting

the sun for the earth as the center of motion, nevertheless clung to the

erroneous notion of Ptolemy that all the bodies of the sky must perforce

move at uniform speeds, and in circular curves, the circle being the

only "perfect curve." Kepler was not long in finding out that this

could not be so, and he found it out because Tycho Brahe's observations

were much more accurate than any that Copernicus had employed.

Naturally he attempted the nearest planet first, and that was Mars--the

planet that Tycho had assigned to him for research. How fortunate that

the orbit of Mars was the one, of all the planets, to show practically

the greatest divergence from the ancient conditions of uniform motion in

a perfectly circular orbit! Had the orbit of Mars chanced to be as

nearly circular as is that of Venus, Kepler might well have been driven

to abandon his search for the true curve of planetary motion.

However, the facts of the cosmos were on his side, but the calculations

essential in testing his various hypotheses were of the most tedious

nature, because logarithms were not yet known in his day. His first

discovery was that the orbit of Mars is certainly not a circle, but oval

or elliptic in figure. And the sun, he soon found, could not be in the

center of the ellipse, so he made a series of trial calculations with

the sun located in one of the foci of the ellipse instead.

Then he found he could make his calculated places of Mars agree quite

perfectly with Tycho Brahe's observed positions, if only he gave up the

other ancient requisite of perfectly uniform motion. On doing this, it

soon appeared that Mars, when in perihelion, or nearest the sun, always

moved swiftest, while at its greatest distance from the sun, or

aphelion, its orbital velocity was slowest.

Kepler did not busy himself to inquire why these revolutionary

discoveries of his were as they were; he simply went on making enough

trials on Mars, and then on the other planets in turn, to satisfy

himself that all the planetary orbits are elliptical, not circular in

form, and are so located in space that the center of the sun is at one

of the two foci of each orbit. This is known as Kepler's first law of

planetary motion.

The second one did not come quite so easy; it concerned the variable

speed with which the planet moves at every point of the orbit. We must

remember how handicapped he was in solving this problem: only the

geometry of Euclid to work with, and none of the refinements of the

higher mathematics of a later day. But he finally found a very simple

relation which represented the velocity of the planet everywhere in its

orbit. It was this: if we calculate the area swept, or passed over, by

the planet's radius vector (that is, the line joining its center to the

sun's center) during a week's time near perihelion, and then calculate

the similar area for a week near aphelion, or indeed for a week when

Mars is in any intermediate part of its orbit, we shall find that these

areas are all equal to each other. So Kepler formulated his second great

law of planetary motion very simply: the radius vector of any planet

describes, or sweeps over, equal areas in equal times. And he found this

was true for all the planets.

But the real genius of the great mathematician was shown in the

discovery of his third law, which is more complex and even more

significant than the other two--a law connecting the distances of the

planets from the sun with their periods of revolution about the sun.

This cost Kepler many additional years of close calculation, and the

resulting law, his third law of planetary motion is this: The cubes of

the mean or average distances of the planets from the sun are

proportional to the squares of their times of revolution around him.

So Kepler had not only disposed of the sacred theories of motion of the

planets held by the ancients as inviolable, but he had demonstrated the

truth of a great law which bound all the bodies of the solar system

together. So accurately and completely did these three laws account for

all the motions, that the science of astronomy seemed as if finished;

and no matter how far in the future a time might be assigned, Kepler's

laws provided the means of calculating the planet's position for that

epoch as accurately as it would be possible to observe it. Kepler paused

here, and he died in 1630.

Astronomy: The Science of the Heavenly Bodies · 第 10 / 61 章