CHAPTER NINE

According to Prof. Newcomb, for instance, the distance of the sun is

about 380 times the distance of the moon—as determined by triangulation.

But, upon page 22, _Popular Astronomy_, Newcomb tells of another

demonstration, with strikingly different results—as determined by

triangulation.

A split god.

The god Triangulation is not one undivided deity.

The other method with strikingly different results is the method of

Aristarchus. It cuts down the distance of the sun, from 380 to 20 times

the distance of the moon. When an observer upon this earth sees the moon

half-illumined, the angle at the moon, between observer and sun, is a

right angle; a third line between observer and sun completes a triangle.

According to Aristarchus, the tilt of the third line includes an angle

of 86 degrees, making the sun-earth line 20 times longer than the

moon-earth line.

“In principle,” says Newcomb, “the method is quite correct and very

ingenious, but it can not be applied in practice.” He says that

Aristarchus measured wrong; that the angle between the moon-earth line

and the earth-sun line is almost 90 degrees and not 86 degrees. Then he

says that the method can not be applied because no one can determine

this angle that he had said is of almost 90 degrees. He says something

that is so incongruous with the inflations of astronomers that they’d

sizzle if their hypnotized readers could read and think at the same

time. Newcomb says that the method of Aristarchus can not be applied

because no astronomer can determine when the moon is half-illumined.

We have had some experience.

Does anybody who has been through what we’ve been through suppose that

there is a Prof. Keeler in the world who would not declare that

trigonometrically and spectroscopically and micrometrically he had

determined the exact moment and exasperating, or delightful, decimal of

a moment of semi-illumination of the moon, were it not that, according

to at least as good a mathematician as he, determination based upon that

demonstration does show that the sun is only 20 times as far away as the

moon? But suppose we agree that this simple thing can not be done.

Then instantly we think of some of the extravagant claims with which

astronomers have stuffed supine credulities. Crawling in their unsightly

confusion that sickens for simplification, is this offense to harmony:

That astronomers can tell under which Crusade, or its decimalated moment

a shine left a star, but can not tell when a shine reaches a line on the

moon—

Glory and triumph and selectness and inflation—or that we shall have

renown as evangelists, spreading the homely and wholesome doctrine of

humility. Hollis, in _Chats on Astronomy_, tells us that the diameter of

this earth, at the equator, is 41,851,160 feet. But blessed be the meek,

we tell him. In the _Observatory_, 19-118, is published the

determination, by the astronomer Brenner, of the time of rotation of

Venus, as to which other astronomers differ by hundreds of days.

According to Brenner, the time is 23 hours, 57 minutes, and 7.5459

seconds. I do note that this especial refinement is a little too

ethereal for the Editor of the _Observatory_: he hopes Brenner will

pardon him, but is it necessary to carry out the finding to the fourth

decimal of a second? However, I do not mean to say that all astronomers

are as refined as Brenner, for instance. In the _Jour. B. A. A._, 1-382,

Edwin Holmes, perhaps coarsely, expresses some views. He says that such

“exactness” as Capt. Noble’s in writing that the diameter of Neptune is

38,133 miles and that of Uranus is 33,836 miles is bringing science into

contempt, because very little is known of these planets; that, according

to Nelson, these diameters are 27,000 miles and 28,500 miles.

MacPherson, in _A Century’s Progress in Science_, quotes Prof. Serviss:

that the average parallax of a star, which is an ordinary astronomic

quantity, is “about equal to the apparent distance between two pins,

placed one inch apart, and viewed from a distance of one hundred and

eighty miles.” Stick pins in a cushion, in New York—go to Saratoga and

look at them—be overwhelmed with the more than human powers of the

scientifically anointed—or ask them when shines half the moon.

The moon’s surface is irregular. I do not say that anybody with brains

enough to know when he has half a shoe polished should know when the sun

has half the moon shined. I do say that if this simple thing can not be

known, the crowings of astronomers as to enormously more difficult

determinations are mere barnyard disturbances.

Triangulation that, according to his little priests, straddles orbits

and on his apex wears a star—that he’s a false Colossus; shrinking, at

the touch of data, back from the stars, deflating below the sun and

moon; stubbing down below the clouds of this earth, so that the

different stories that he told to Aristarchus and to Newcomb are the

conflicting vainglories of an earth-tied squatter—

The blow that crumples a god:

That, by triangulation, there is not an astronomer in the world who can

tell the distance of a thing only five miles away.

Humboldt, _Cosmos_, 5-138:

Height of Mauna Loa: 18,410 feet, according to Cook; 16,611, according

to Marchand; 13,761, according to Wilkes—according to triangulation.

In the _Scientific American_, 119-31, a mountain climber calls the

Editor to account for having written that Mt. Everest is 29,002 feet

high. He says that, in his experience, there is always an error of at

least ten per cent. in calculating the height of a mountain, so that all

that can be said is that Mt. Everest is between 26,100 and 31,900 feet

high. In the _Scientific American_, 102-183, and 319, Miss Annie Peck

cites two measurements of a mountain in India: they differ by 4000 feet.

The most effective way of treating this subject is to find a list of

measurements of a mountain’s height before the mountain was climbed, and

compare with the barometric determination, when the mountain was

climbed. For a list of 8 measurements, by triangulation, of the height

of Mt. St. Elias, see the _Alpine Journal_, 22-150: they vary from

12,672 to 19,500 feet. D’Abruzzi climbed Mt. St. Elias, Aug. 1, 1897.

See a paper, in the _Alpine Journal_, 19-125. D’Abruzzi’s barometric

determination—18,092 feet.

Suppose that, in measuring, by triangulation, the distance of anything

five miles away, the error is, say ten per cent. But, as to anything ten

miles away, there is no knowing what the error would be. By

triangulation, the moon has been “found” to be 240,000 miles away. It

may be 240 or 240,000,000 miles away.

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