Some comets approach much closer to the sun than others. The majority

of all comets observed have come within the earth's orbit and no

known comet has its perihelion beyond the orbit of Jupiter. It is, of

course, possible that there may be a number of comets that never come

within the orbit of Jupiter, but it is very unlikely that any such

comet would ever be discovered. The majority of comets are simply

small, fuzzy points of light that are only visible telescopically and

the greater the perihelion distance of the comet the less likely is

it to be seen with the naked eye.

Since comets as well as planets obey Kepler's first law, known as

the law of areas, and sweep over equal areas in equal times, it is

evident that when a comet is at perihelion, or nearest to the sun, it

is moving at maximum speed and when it is at aphelion, or farthest

from the sun, it is moving at minimum speed. Moreover, its speed at

these two points in its orbit varies tremendously since the orbits of

comets are ellipses of very high eccentricity. The speed with which

the planets are traveling is, on the other hand, remarkably uniform

since their orbits are nearly circular.

The leisurely speed with which a comet travels through the frigid

outer regions of the solar system is gradually accelerated as the

comet draws nearer and nearer to the sun until it has acquired near

the time of perihelion passage a velocity that occasionally exceeds

two hundred miles a second. Here, also, the great increase in light

and heat and the strong magnetic field of the sun produce complex

changes in the gaseous and meteoric substances of which the comet is

composed until the characteristic tail and peculiar cometary features

are fully developed. As the comet again recedes from the sun after

perihelion passage its speed slackens once more. It soon parts with

its tail and other spectacular features and fades rapidly from view

even in the largest telescopes.

XXIII

METEORITES

Meteorites, bolides or fireballs, as they are variously called, are

stones that fall to the earth from the heavens. They furnish the one

tangible evidence that we possess, aside from that furnished by the

spectroscope, as to the composition of other bodies in space and

it is a significant fact that no unknown elements have ever been

found in meteorites, though the forms in which they appear are so

characteristic that they make these stones readily distinguishable

from stones of terrestrial origin.

The origin of meteorites is not definitely known, but the evidence is

very strong in favor of the theory that they are the larger fragments

of disintegrated comets of which meteors and shooting stars are the

smaller; the distinction between the two being simply that the latter

class includes all bodies that are completely consumed by friction

with the earth's atmosphere and, therefore, only reach the surface in

the form of meteoric dust.

According to other theories meteorites may be fragments of shattered

worlds that have chanced to come too near to a larger body and have

been disrupted, or they may possibly be the larger fragments of the

disintegrated comets of which the meteoric swarms are the smaller.

Interplanetary space is not altogether a void. Our own planet

sweeps up in the course of a single day, it has been estimated,

approximately twenty million shooting stars or meteors of sufficient

size to be visible to the naked eye, while the estimate for the

telescopic particles runs up to four hundred million.

Meteorites on the other hand are comparatively rare. On the average

it has been estimated about one hundred meteorites strike the earth

in the course of a year, of which number only two or three are

actually seen. According to _Bulletin 94, U. S. National Museum_,

approximately six hundred and fifty falls and finds of meteorites

have been reported, representatives of which appear in museums and

private collections.

Meteorites, as well as shooting stars and meteors, frequently appear

in showers. In such instances the fall usually consists of several

hundred or thousand individual stones and the area over which they

fall is several square miles in extent and roughly ellipsoidal

in shape. One of the most remarkable of such falls [...] hundred

thousand stones, varying in weight from fifteen pounds to a small

fraction of an ounce, fell near Pultusk, Poland. Another remarkable

fall of meteorites occurred at L'Aigle, France, in 1803. Between two

thousand and three thousand stones fell over an ellipsoidal area of

six and two-tenths miles in greatest diameter, the aggregate weight

of the stones being not less than seventy-five pounds.

This fall of stones is of particular interest since it took place at

a time when men were still very doubtful as to whether or not stones

actually fell to earth from the heavens.

After this fall had occurred in a most populous district of France

in broad daylight and attended by violent explosions that lasted for

five or six minutes and were heard for a distance of seventy-five

miles, no reasonable doubt could longer be held as to the actuality

of such phenomena.

Meteorites are without exception of an igneous nature, that is,

they are rocks that have solidified from a molten condition. They

can be classified into three groups, Aerolites or Stony Meteorites,

Siderolites or Stony-iron Meteorites, and Siderites or Iron

Meteorites.

More iron meteorites seem to have fallen in Mexico and Greenland than

in any other part of the world--at least of its land surface.

Yet strange to say, of all the meteorites that have been seen to

fall only nine belong to the group of Siderites or Iron Meteorites,

though the three largest meteorites known, Peary's meteorite from

Cape York, Greenland, weighing 37-1/2 tons, the meteorite lying on

the plain near Bacubirito, Mexico, weighing about 20 tons, and the

Willamette, Oregon, meteorite, weighing 15-1/2 tons all belong to

this group. Moreover, all the Canyon Diablo meteorites, which are

strewn concentrically around Coon Mountain crater in northern Arizona

to a distance of about five miles, are members of this same group.

Coon Mountain or Meteor crater itself is a perfectly round hole,

about six hundred feet deep and over four thousand feet in diameter

and was formed, it is believed, by the impact of a huge meteorite

which has never been found. It is believed that the Canyon Diablo

meteorites, of which there are nearly four hundred individuals in

the U. S. National Museum alone, were all members of this same fall.

It is possible that these meteorites of the Canyon Diablo district,

with the huge meteorite that produced the crater itself, formed the

nucleus of a comet that struck the earth not more than five thousand

years ago, according to the geological evidence.

All iron meteorites or siderites (from the Greek sideros, iron) are

composed chiefly of alloys of nickel and iron. The percentage of

nickel in these iron meteorites is very small, usually from five to

ten per cent., while the iron forms about ninety or ninety-five per

cent. of the whole. Cobalt is also present in practically all iron

meteorites in small quantities of 1 per cent. or less. Usually small

quantities of iron sulphide and phosphide as well as graphite or

some other form of carbon appear in the iron meteorites and in some

instances black and white diamonds have been found, as in some of the

Canyon Diablo irons.

A very interesting and beautiful feature of many iron meteorites

is the Widmanstätten figures which appear when a section of such a

stone is polished and treated by means of a weak acid. These figures

are due to the unequal solubility of the three different alloys of

nickel and iron of which the stones are composed. The irons giving

the Widmanstätten figures are known as octahedral irons. Other irons

known as hexahedral irons give figures of a different type known as

Neumann figures when the polished section is treated with weak acid,

while other irons are so homogeneous in their composition that they

show no figures at all.

Aerolites or Stony Meteorites occur more abundantly than iron or

stony-iron types, and they are classified into many divisions and

subdivisions according to their composition. In these stones appear

certain compounds that are commonly met with in terrestrial igneous

rocks. The mineral that is most abundant in the stony meteorites,

composing sometimes nearly seventy-five per cent. of the stone,

is a magnesium and iron silicate known as olivine, which is also

usually present in terrestrial rocks of an igneous nature. Certain

compounds found in the stony meteorites are rarely if ever found in

terrestrial rocks, however, and these serve to distinguish the stony

meteorites readily from stones of terrestrial origin. The alloys of

iron and nickel, for instance, that occur in minor quantities in the

stony meteorites and make up usually about ninety-five per cent.

of the mass of the iron meteorites, are never found in terrestrial

rocks. Although about thirty of the terrestrial elements are to be

found in meteorites, the forms and compounds in which they appear

are so characteristic and on the whole so different from those

occurring in terrestrial rocks, that the analyst has no difficulty

in distinguishing between the two. There are, for instance certain

formations known as chondrules, peculiar spherical and oval shapes,

varying in size from minute particles to objects the size of walnuts,

appearing in many varieties of stony meteorites that are never found

in terrestrial rocks, and that are one of the most puzzling features

associated with the origin and nature of these stones. Sometimes

the chondrules are so loosely embedded in the stone that they fall

away when it is broken. In some instances almost the entire stone is

made up of these chondrules. According to one theory the chondrules

were originally molten drops, like fiery rain, and their internal

structure, which is greatly varied, depends upon their conditions of

cooling.

Stony meteorites, in which these chondrules are to be found,

are spoken of as chondrites. There are white and gray and black

chondrites and crystalline and carbonaceous chondrites, according to

the nature of the chondrules found in the stones.

Stony meteorites also contain minute quantities of iron and nickel

alloys in the form of drops or stringers.

Upon entering the earth's atmosphere stony meteorites become coated

with a thin black crust which is a glass formed by the fusion of its

surface materials by the heat generated during its passage through

the atmosphere.

In many of the stony meteorites there also appear fine thread-like

veins which are due to the fracturing of the stone prior to its

entrance into the atmosphere. The material filling these veins is

coal black in color, opaque and of an unknown composition.

Many meteorites show signs of collisions and encounters with other

meteorites outside of the atmosphere as would be expected as they

travel in swarms and groups. Sometimes the entire meteorite is

composed of fragments of two or more distinct stones cemented

together. Such a stone is spoken of as a _breccia_.

In the third class of meteorites to which we now come, known as the

stony-iron meteorites, there is a network or sponge of nickel-iron

alloy, the interstices of which are filled with stony material.

When this network or sponge is continuous the meteorite is spoken of

as a stony-iron pallasite. When the network of metal is more or less

disconnected the meteorite is a meso-siderite.

If meteorites are heated in a vacuum, the conditions existing in

interplanetary space being thus produced to a certain extent, they

give forth their occluded gases and it has been found that these

gases give spectra identical with the spectra of certain comets.

Meteoric irons give forth hydrogen as their characteristic gas while

the gases occluded in the stony meteorites are chiefly the oxides

of carbon, carbon monoxide and carbon dioxide. It has been found

that the amount of gases contained in a large meteorite or shower of

meteorites is sufficient to form the tail of a comet. These facts all

tend to strengthen the belief that meteorites are indeed cometary

fragments.

In view of the fact that some geologists believe meteorites may be

fragments of other worlds, it is of interest to know that so far no

fossil-bearing meteorites have been found, and if meteorites are

fragments of a shattered world, such worlds must have been reduced to

a molten condition at the time of the catastrophe.

The rapid passage of the meteorite through the air leaves a partial

vacuum in its trail into which rush the molecules of air from all

sides, producing the characteristic noises that accompany the passage

of a meteorite, which have been variously compared to the rattle of

artillery, the distant booming of cannons or the rumble of thunder.

There may be, also, explosions of inflammable gases occluded in the

crevices of the meteorite which will shatter it into fragments or

the meteorite may be shattered by the resistance and pressure of the

atmosphere or as a result of the extremes of temperature existing

between the interior and its surface. Many meteorites have actually

been seen to burst into fragments in the air with a loud report.

There is practically no foundation for the belief that germs of life

have been brought to our planet on such igneous rocks. No microscopic

examinations of meteorites have yielded any results that could be

interpreted in favor of such a view.

Falls of meteorites are accompanied in nearly every instance by

terrific explosions and sharp reports that can be heard for many

miles around, often causing the ground to shake as in an earthquake.

The meteorite itself has been described as resembling a ball of

fire or the headlight of a locomotive, and is followed frequently

by a trail of light or a cloud of smoke. At the time it enters our

atmosphere a meteorite is moving with planetary velocity ranging from

two to forty-five miles per second. Its interior is intensely cold,

approaching in temperature the absolute zero of interplanetary space,

and it is, therefore, far more brittle than it would be at ordinary

temperatures. As it ploughs its way into the earth's atmosphere its

surface temperature is soon raised by friction to at least 3,000° or

4,000° C., which is sufficient to fuse all surface materials into the

characteristic black crust, with which stony meteorites are coated.

Meteorites are usually first seen at an altitude of fifty or sixty

miles. Although they are moving with a velocity comparable to that of

the planets, when they enter the earth's atmosphere, this velocity is

so rapidly reduced by friction with the atmosphere that they usually

drop to the surface of the earth with a velocity about equal to that

of ordinary falling objects.

The flight of a meteorite often extends over a path several hundred

miles in length and the meteorite may be seen by many observers in

several different States and yet finally fall in some unknown spot

and never be found.

The evidence gathered regarding the actual fall of meteorites is

often contradictory. Some stones are too hot to handle for hours

after they fall, others are merely warm, while still others have been

picked up cool or even intensely cold. Meteorites have been seen to

fall upon dried grass and upon straw without producing even charring

effects. The evidence regarding the depths to which meteorites

penetrate the ground is quite as conflicting. The largest of all

the stony meteorites which fell at Krnyahinya, Hungary, weighed 647

pounds and buried itself to a depth of eleven feet. Yet Peary's Cape

York iron meteorite, weighing 37-1/2 tons, was only partially covered

and showed no signs of abrasions of surface resulting from the fall.

The Willamette iron meteorite, weighing 16-1/2 tons, lay in a forest

when found and was not deeply buried. The Bacubirito iron meteorite,

weighing 20 tons, lay in soft soil, barely beneath the level of the

surface. On the other hand a fragment of a stony-iron meteorite,

weighing 437 pounds, that fell at Estherville, Iowa, buried itself

eight feet in stiff clay.

Geologists in charge of the meteoric collections of various museums

quite frequently have stones sent to them for analysis that are

reputed to be of celestial origin. More often than not such stones

are found to be purely terrestrial in their origin. The composition

of a meteorite is so characteristic and unique that such a stone can

never be mistaken. Finds of bona-fide meteorites are on the whole

extremely rare.

It is also a peculiar fact that meteorites are usually observed in

the months when ordinary meteors or periodic swarms of meteors are

least prevalent, that is in the months of May, June and July.

XXIV

THE EARTH AS A MAGNET

If a small, freely suspended compass needle is moved over a highly

magnetized steel sphere, it will be seen that it constantly changes

its position both horizontally and vertically so as to lie always

along the "lines of force" of the sphere.

There will be one point on the sphere which we will call the _North

Magnetic Pole_, where the _north-seeking_ end of the needle will

point vertically downward or make a "dip" of 90° with the tangent

plane. At the diametrically opposite point on the sphere, called

the South Magnetic Pole, the opposite end of the compass, the

south-seeking end, will point vertically downward; while at a point

midway between the magnetic poles of the sphere the needle will lie

parallel to the diameter connecting the two poles and there will be

no dip.

The total intensity of the magnetic field surrounding the sphere will

be found to be greatest in the vicinity of the magnetic poles and

least, midway between the poles.

Now, a freely suspended compass needle carried to all parts of the

earth will behave very much in the same manner as the needle moved

over the magnetized steel sphere. There are two points on the earth's

surface, known as the North and South Magnetic Poles, where the

needle points vertically downward and approximately midway between is

the _Magnetic Equator_ where the compass needle places itself in a

perfectly horizontal position and the "dip" of the needle is zero. In

other words, the earth acts as a huge magnet and possesses a magnetic

field with lines of force converging towards its poles similar to the

lines of force of the steel sphere.

There are, however, some very important differences between the

sphere of steel and our earth. The matter of which the earth is

composed is not homogeneous. It is believed to possess an iron core

of considerable size, it is true, but its outer shell is composed of

heterogeneous masses that in certain regions cause very appreciable

local deflections of the needle. It is surrounded, moreover, by an

atmosphere permeated by electrified particles of matter shot forth

from the sun, which we now know is a still greater magnet surrounded

by a magnetic field that is of the order of 50 gausses at the poles

and about eighty times more powerful than that of the earth.

It is now a well-established fact that the sun's magnetic field

exerts a powerful influence over the condition of the earth's

magnetic field, and that vast solar disturbances affect very

materially the direction and intensity of the lines of force.

It is thus little wonder that this non-homogeneous and rapidly

rotating terrestrial globe, surrounded by an electrified atmosphere

and subject to the action of a still more powerful magnet, the sun,

should not behave in a manner exactly analogous to a uniformly

magnetized steel sphere.

The earth's magnetic poles are neither symmetrically placed nor

absolutely fixed in position. There is every reason to suspect

that they shift about from year to year, and possibly fluctuate

irregularly in position in the course of a few days or hours under

the influence of disturbing forces. The position of the earth's

North Magnetic Pole, last visited by Amundsen in 1903, now lies

approximately in Latitude 70° N. Longitude 97° W. The position of

the South Magnetic Pole, according to the latest determinations,

is, in round numbers, in Latitude 73° S. and Longitude 156° E. of

Greenwich. It is evident, therefore, that the magnetic poles of the

earth are not symmetrically placed and that they lie fully 30° from

the _geographical_ poles. The chord connecting the magnetic poles

passes 750 miles from the earth's center, and it is about 1,200 miles

from the geographic pole to the nearest magnetic pole. There exist,

moreover, in high latitudes local magnetic poles, due possibly to

heavy local deposits of ore. One such pole was discovered at Cape

Treadwell, near Juneau, Alaska, during Dr. L. A. Bauer's observations

there in 1900 and 1907. In the center of the observing tent at

this point the needle pointed vertically downward and the compass

_reversed_ its direction when carried from one side of the tent to

the other.

It is a well-known fact that there are very few points on the

earth's surface where the compass needle points either to the true

geographical pole or to the magnetic pole, and if it does chance to

do so, it is a transient happening. The "variation of the compass"

or the declination of the needle, as it is called, is the angle that

the compass needle makes with the true north and south line or the

meridian. It is an angle of greatest importance to navigators and

explorers, for it gives them their bearings, yet it is unfortunately

subject to ceaseless variations of a most complicated nature, since

it depends on the constantly pulsating and never ceasing magnetic

changes that sweep over the surface of the earth and through its

crust. It is affected by long period or secular changes, as they

are called, progressing more or less regularly in obscure cycles of

unknown period. It is subject to a diurnal change that depends on the

position of the sun relative to the meridian, and that varies with

the seasons and with the hour of the day. It is affected by the sun

spot cycle of 11.3 years which has a direct effect upon the intensity

of the earth's magnetic field. The intensity of the magnetic field in

sun spots is, according to Abbot, sometimes as high as 4,500 gausses

or 9,000 times the intensity of the earth's field. At times of

maximum spottedness of the sun the intensity of the earth's magnetic

field is reduced.

Moreover, when great and rapidly changing spots appear upon the

sun, electrified particles are shot forth from the sun with great

velocity and in great numbers, and are drawn in towards the magnetic

poles of the earth. Meeting the rarefied gases of the earth's upper

atmosphere, they illuminate them as electric discharges illuminate

a vacuum tube. Some of these electrons are absorbed by gases at

high elevations, other descend to lower levels. The most penetrating

rays have been known to descend to an altitude of twenty-five miles

which is about the lowest limit yet found for auroral displays. It

is the passage of these rays through the atmosphere that cause the

magnetic disturbances known as _magnetic storms_, that are associated

with the appearance of great sun spots and auroral displays. At such

times sudden changes take place in the intensity of the earth's

magnetic field that cause the compass needle to shiver and tremble

and temporarily lose its directive value. These _magnetic storms_

have been known to produce great temporal changes in the intensity

of the earth's field. According to Dr. L. A. Bauer, Director of the

Department of Terrestrial Magnetism of the Carnegie Institute of

Washington, the earth's intensity of magnetization was altered by

about one-twentieth or one-thirtieth part by the magnetic storm of

September 25, 1909, which was one of the most remarkable on record,

and the earth's magnetic condition was below par for fully three

months afterwards as a result.

In addition to these various regular and irregular changes in the

variation of the compass, or declination of the needle, due to

changes in the earth's magnetic field _as a whole_, there are local

effects due to restricted regional disturbances of the earth's

magnetic field or to local deposits of ore, or to volcanoes or

other local causes. The effect of all these disturbances upon the

declination of the needle must be determined by continual magnetic

surveys of all portions of the earth's surface.

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