e tables or errors in the old observations. He
discussed them with minute care, and came to the conclusion that they
were not thus to be explained away. This part of the work he published
in November, 1845.
He then set to work to consider the perturbations produced by Jupiter
and Saturn to see whether they had been accurately allowed for, or
whether some minute improvements could be made sufficient to destroy the
irregularities. He introduced several fresh terms into these
calculations, but none of them of sufficient importance to do more than
partly explain the mysterious perturbations. He next examined the
various hypotheses that had been suggested to account for them. Were
they caused by a failure in the law of gravitation or by the presence of
a resisting medium? Were they due to some large but unseen satellite or
to a collision with some comet?
All these theories he examined and dismissed for various reasons. The
perturbations were due to some continuous cause--for instance, some
unknown planet. Could this planet be inside the orbit of Uranus? No, for
then it would perturb Saturn and Jupiter also, and they were not
perturbed by it. It must, therefore, be some planet outside the orbit of
Uranus, and in all probability, according to Bode's empirical law, at
nearly double the distance from the sun that Uranus is. Finally he
proceeded to determine where this planet was, and what its orbit must be
to produce the observed disturbances.
Not without failures and disheartening complications was this part of
the process completed. This was, after all, the real tug of war. Many
unknown quantities existed: its mass, its distance, its eccentricity,
the obliquity of its orbit, its position--nothing was known, in fact,
about the planet except the microscopic disturbance it caused in Uranus,
several thousand million miles away from it. Without going into further
detail, suffice it to say that in June, 1846, he published his last
paper, and in it announced to the world his theory as to the situation
of the planet.
Professor Airy received a copy of this paper before the end of the
month, and was astonished to find that Leverrier's theoretical place for
the planet was within 1 deg. of the place Adams had assigned to it eight
months before. So striking a coincidence seemed sufficient to justify a
Herschelian sweep for a week or two. But a sweep for so distant a planet
would be no easy matter. When seen through a large telescop
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