The faculæ are very unstable, and are constantly changing: t

THE

TROUVELOT

ASTRONOMICAL DRAWINGS

MANUAL

BY

E. L. TROUVELOT,

FORMERLY CONNECTED WITH THE OBSERVATORY OF HARVARD COLLEGE; FELLOW OF THE

AMERICAN ACADEMY OF ARTS AND SCIENCES, AND MEMBER OF THE SELENO-GRAPHICAL

SOCIETY OF GREAT BRITAIN; IN CHARGE OF A

GOVERNMENT EXPEDITION TO OBSERVE THE

TOTAL SOLAR ECLIPSE OF 1878.

NEW YORK

CHARLES SCRIBNER'S SONS

1882

INTRODUCTION

During a study of the heavens, which has now been continued for more

than fifteen years, I have made a large number of observations

pertaining to physical astronomy, together with many original drawings

representing the most interesting celestial objects and phenomena.

With a view to making these observations more generally useful, I was

led, some years ago, to prepare, from this collection of drawings, a

series of astronomical pictures, which were intended to represent the

celestial phenomena as they appear to a trained eye and to an

experienced draughtsman through the great modern telescopes, provided

with the most delicate instrumental appliances. Over two years were

spent in the preparation of this series, which consisted of a number of

large drawings executed in pastel. In 1876, these drawings were

displayed at the United States Centennial Exhibition at Philadelphia,

forming a part of the Massachusetts exhibit, in the Department of

Education and Science.

The drawings forming the present series comprise only a part of those

exhibited at Philadelphia; but, although fewer in number, they are quite

sufficient to illustrate the principal classes of celestial objects and

phenomena.

While my aim in this work has been to combine scrupulous fidelity and

accuracy in the details, I have also endeavored to preserve the natural

elegance and the delicate outlines peculiar to the objects depicted; but

in this, only a little more than a suggestion is possible, since no

human skill can reproduce upon paper the majestic beauty and radiance of

the celestial objects.

The plates were prepared under my supervision, from the original pastel

drawings, and great care has been taken to make the reproduction exact.

The instruments employed in the observations, and in the delineation of

the heavenly bodies represented in the series, have varied in aperture

from 6 to 26 inches, according to circumstances, and to the nature of

the object to be studied. The great Washington refractor, kindly placed

at my disposal by the late Admiral C. H. Davis, has contributed to this

work, as has also the 26 inch telescope of the University of Virginia,

while in the hands of its celebrated constructors, Alvan Clark & Sons.

The spectroscope used was made by Alvan Clark & Sons. Attached to it is

an excellent diffraction grating, by Mr. L. M. Rutherfurd, to whose

kindness I am indebted for it.

Those unacquainted with the use of optical instruments generally suppose

that all astronomical drawings are obtained by the photographic process,

and are, therefore, comparatively easy to procure; but this is not true.

Although photography renders valuable assistance to the astronomer in

the case of the Sun and Moon, as proved by the fine photographs of these

objects taken by M. Janssen and Mr. Rutherfurd; yet, for other subjects,

its products are in general so blurred and indistinct that no details of

any great value can be secured. A well-trained eye alone is capable of

seizing the delicate details of structure and of configuration of the

heavenly bodies, which are liable to be affected, and even rendered

invisible, by the slightest changes in our atmosphere.

The method employed to secure correctness in the proportions of the

original drawings is simple, but well adapted to the purpose in view. It

consists in placing a fine reticule, cut on glass, at the common focus

of the objective and the eye-piece, so that in viewing an object, its

telescopic image, appearing projected on the reticule, can be drawn very

accurately on a sheet of paper ruled with corresponding squares. For a

series of such reticules I am indebted to the kindness of Professor

William A. Rogers, of the Harvard College Observatory.

The drawings representing telescopic views are inverted, as they appear

in a refracting telescope--the South being upward, the North downward,

the East on the right, and the West on the left. The Comet, the

Milky-Way, the Eclipse of the Moon, the Aurora Borealis, the Zodiacal

Light and the Meteors are represented as seen directly in the sky with

the naked eye. The Comet was, however, drawn with the aid of the

telescope, without which the delicate structure shown in the drawing

would not have been visible.

The plate representing the November Meteors, or so-called "Leonids," may

be called an ideal view, since the shooting stars delineated, were not

observed at the same moment of time, but during the same night. Over

three thousand Meteors were observed between midnight and five o'clock

in the morning of the day on which this shower occurred; a dozen being

sometimes in sight at the same instant. The paths of the Meteors,

whether curved, wavy, or crooked, and also their delicate colors, are in

all cases depicted as they were actually observed.

In the Manual, I have endeavored to present a general outline of what is

known, or supposed, on the different subjects and phenomena illustrated

in the series. The statements made are derived either from the best

authorities on physical astronomy, or from my original observations,

which are, for the most part, yet unpublished.

The figures in the Manual relating to distance, size, volume, mass,

etc., are not intended to be strictly exact, being only round numbers,

which can, therefore, be more easily remembered.

It gives me pleasure to acknowledge that the experience acquired in

making the astronomical drawings published in Volume VIII. of the Annals

of the Harvard College Observatory, while I was connected with that

institution, has been of considerable assistance to me in preparing this

work; although no drawings made while I was so connected have been used

for this series.

E. L. TROUVELOT.

_Cambridge, March, 1882._

CONTENTS

INTRODUCTION

LIST OF PLATES

_THE SUN_

GENERAL REMARKS ON THE SUN

SUN-SPOTS AND VEILED SPOTS

SOLAR PROTUBERANCES

TOTAL ECLIPSE OF THE SUN

_THE AURORAL AND ZODIACAL LIGHTS_

THE AURORA BOREALIS

THE ZODIACAL LIGHT

_THE MOON_

THE MOON

ECLIPSES OF THE MOON

_THE PLANETS_

THE PLANETS

THE PLANET MARS

THE PLANET JUPITER

THE PLANET SATURN

_COMETS AND METEORS_

COMETS

SHOOTING-STARS AND METEORS

_THE STELLAR SYSTEMS_

THE MILKY-WAY OR GALAXY

THE STAR-CLUSTERS

THE NEBULÆ

APPENDIX

LIST OF PLATES[1]

PLATE

I. GROUP OF SUN-SPOTS AND VEILED SPOTS.

_Observed June 17, 1875, at 7 h. 30m. A. M._

II. SOLAR PROTUBERANCES.

_Observed May 5, 1873, at 9h. 40m. A. M._

III. TOTAL ECLIPSE OF THE SUN.

_Observed July 29, 1878, at Creston, Wyoming Territory._

IV. AURORA BOREALIS.

_As observed March 1, 1872, at 9h. 25m. P. M._

V. THE ZODIACAL LIGHT.

_Observed February 20, 1876._

VI. MARE HUMORUM.

_From a study made in 1875._

VII. PARTIAL ECLIPSE OF THE MOON.

_Observed October 24, 1874._

VIII. THE PLANET MARS.

_Observed September 3, 1877, at 11h. 55m. P. M._

IX. THE PLANET JUPITER.

_Observed November 1, 1880, at 9h. 30m. P. M._

X. THE PLANET SATURN.

_Observed November 30, 1874, at 5th. 50m. P. M._

XI. THE GREAT COMET OF 1881.

_Observed on the night of June 25-26, at 1h. 30m. A. M._

XII. THE NOVEMBER METEORS.

_As observed between midnight and 3 o'clock A. M., on the night

of November 13-14, 1868._

XIII. PART OF THE MILKY-WAY.

_From a study made during the years 1874, 1875 and 1876._

XIV. STAR-CLUSTER IN HERCULES.

_From a study made in June, 1877._

XV. THE GREAT NEBULA IN ORION.

_From a study made in the years 1873-76._

[Footnote 1: For Key to the Plates, see Appendix.]

_Reproduced from the Original Drawings, by Armstrong & Company,

Riverside Press, Cambridge, Mass._

GENERAL REMARKS ON THE SUN

The Sun, the centre of the system which bears its name, is a

self-luminous sphere, constantly radiating heat and light.

Its apparent diameter, as seen at its mean from the Earth, subtends an

angle of 32', or a little over half a degree. A dime, placed about six

feet from the eye, would appear of the same proportions, and cover the

Sun's disk, if projected upon it.

That the diameter of the Sun does not appear larger, is due to the great

distance which separates us from that body. Its distance from the Earth

is no less than 92,000,000 miles. To bridge this immense gap, would

require 11,623 globes like the Earth, placed side by side, like beads on

a string.

The Sun is an enormous sphere whose diameter is over 108 times the

diameter of our globe, or very nearly 860,000 miles. Its radius is

nearly double the distance from the Earth to the Moon. If we suppose,

for a moment, the Sun to be hollow, and our globe to be placed at the

centre of this immense spherical shell, not only could our satellite

revolve around us at its mean distance of 238,800 miles, as now, but

another satellite, placed 190,000 miles farther than the Moon, could

freely revolve likewise, without ever coming in contact with the solar

envelope.

The circumference of this immense sphere measures 2,800,000 miles. While

a steamer, going at the rate of 300 miles a day, would circumnavigate

the Earth in 83 days, it would take, at the same rate, nearly 25 years

to travel around the Sun.

The surface of the Sun is nearly 12,000 times the surface of the Earth,

and its volume is equal to 1,300,000 globes like our own. If all the

known planets and satellites were united in a single mass, 600 such

compound masses would be needed to equal the volume of our luminary.

Although the density of the Sun is only one-quarter that of the Earth,

yet the bulk of this body is so enormous that, to counterpoise it, no

less than 314,760 globes like our Earth would be required.

The Sun uniformly revolves around its axis in about 25½ days. Its

equator is inclined 7° 15' to the plane of the ecliptic, the axis of

rotation forming, therefore, an angle of 82° 45' with the same plane.

As the Earth revolves about the Sun in the same direction as that of the

Sun's rotation, the apparent time of this rotation, as seen by a

terrestrial spectator, is prolonged from 25½ days to about 27 days and

7 hours.

The rotation of the Sun on its axis, like that of the Earth and the

other planets, is direct, or accomplished from West to East. To an

observer on the Earth, looking directly at the Sun, the rotation of this

body is from left to right, or from East to West.

The general appearance of the Sun is that of an intensely luminous disk,

whose limb, or border, is sharply defined on the heavens. When its

telescopic image is projected on a screen, or fixed on paper by

photography, it is noticed that its disk is not uniformly bright

throughout, but is notably more luminous in its central parts. This

phenomenon is not accidental, but permanent, and is due in reality to a

very rare but extensive atmosphere which surrounds the Sun, and absorbs

the light which that body radiates, proportionally to its thickness,

which, of course, increases towards the limb, to an observer on the

Earth.

THE ENVELOPING LAYERS OF THE SUN

The luminous surface of the Sun, or that part visible at all times, and

which forms its disk, is called the _Photosphere_, from the property it

is supposed to possess of generating light. The photosphere does not

extend to a great depth below the luminous surface, but forms a

comparatively thin shell, 3,000 or 4,000 miles thick, which is distinct

from the interior parts, above which it seems to be kept in suspense by

internal forces. From the observations of some astronomers it would

appear that the diameter of the photosphere is subject to slight

variations, and, therefore, that the solar diameter is not a constant

quantity. From the nature of this envelope, such a result does not seem

at all impossible, but rather probable.

Immediately above the photosphere lies a comparatively thin stratum,

less than a thousand miles in thickness, called the _Reversing Layer_.

This stratum is composed of metallic vapors, which, by absorbing the

light of particular refrangibilities emanating from the photosphere

below, produces the dark Fraunhofer lines of the solar spectrum.

Above the reversing layer, and resting immediately upon it, is a

shallow, semi-transparent gaseous layer, which has been called the

_Chromosphere_, from the fine tints which it exhibits during total

eclipses of the Sun, in contrast with the colorless white light radiated

by the photosphere below. Although visible to a certain extent on the

disk, the chromosphere is totally invisible on the limb, except with the

spectroscope, and during eclipses, on account of the nature of its

light, which is mainly monochromatic, and too feeble, compared with that

emitted by the photosphere, to be seen.

The chromospheric layer, which has a thickness of from 3,000 to 4,000

miles, is uneven, and is usually upheaved in certain regions, its matter

being transported to considerable elevations above its general surface,

apparently by some internal forces. The portions of the chromosphere

thus lifted up, form curious and complicated figures, which are known

under the names of _Solar Protuberances, or Solar Flames_.

Above the chromosphere, and rising to an immense but unknown height, is

the solar atmosphere proper, which is only visible during total eclipses

of the Sun, and which then surrounds the dark body of the Moon with the

beautiful rays and glorious nimbus, called the _Corona_.

These four envelopes: the photosphere, the reversing layer, the

chromosphere, and the corona, constitute the outer portions of our

luminary.

Below the photosphere little can be seen, although it is known, as will

appear below, that at certain depths cloud-like forms exist, and freely

float in an interior atmosphere of invisible gases. Beyond this all is

mystery, and belongs to the domain of hypothesis.

STRUCTURE OF THE PHOTOSPHERE AND CHROMOSPHERE

The apparent uniformity of the solar surface disappears when it is

examined with a telescope of sufficient aperture and magnifying powers.

Seen under good atmospheric conditions, the greater part of the solar

surface appears mottled with an infinite number of small, bright

granules, irregularly distributed, and separated from each other by a

gray-tinted background.

These objects are known under different names. The terms granules and

granulations answer very well for the purpose, as they do not imply

anything positive as to their form and true nature. They have also been

called _Luculœ_, _Rice Grains_, _Willow Leaves_, etc., by different

observers.

Although having different shapes, the granulations partake more or less

of the circular or slightly elongated form. Their diameter, which varies

considerably, has been estimated at from 0".5 to 3", or from 224 to

1,344 miles. The granulations which attain the largest size appear,

under good atmospheric conditions, to be composed of several granules,

closely united and forming an irregular mass, from which short

appendages protrude in various directions.

The number of granulations on the surface of the Sun varies considerably

under the action of unknown causes. Sometimes they are small and very

numerous, while at other times they are larger, less numerous, and more

widely separated. Other things being equal, the granulations are better

seen in the central regions of the Sun than they are near the limb.

Usually the granulations are very unstable; their relative position,

form, and size undergoing continual changes. Sometimes they are seen to

congregate or to disperse in an instant, as if acting under the

influence of attractive and repulsive forces; assembling in groups or

files, and oftentimes forming capricious figures which are very

remarkable, but usually of short duration. In an area of great solar

disturbances, the granulations are often stretched to great distances,

and form into parallel lines, either straight, wavy, or curved, and they

have then some resemblance to the flowing of viscous liquids.

The granulations are usually terminated either by rounded or sharply

pointed summits, but they do not all rise to the same height, as can be

ascertained with the spectroscope when they are seen sidewise on the

limb. In the regions where they are most abundant, they usually attain

greater elevations, and when observed on the limb with the spectroscope,

they appear as slender acute flames.

The granulations terminated by sharply-pointed crests, although observed

in all latitudes, seem to be characteristic of certain regions. A daily

study of the chromosphere, extending over a period of ten years, has

shown me that the polar regions are rarely ever free from these objects,

which are less frequent in other parts of the Sun. In the polar regions

they are sometimes so abundant that they completely form the solar limb.

These forms of granulation are comparatively rare in the equatorial

zones, and when seen there, they never have the permanency which they

exhibit in the polar regions. When observed in the equatorial regions,

they usually appear in small groups, in the vicinity of sun spots, or

they are at least enclosed in areas of disturbances where such spots are

in process of formation. In these regions they often attain greater

elevations than those seen in high latitudes.

As we are certain that in the equatorial zones these slender flames (_i.

e._, granulations) are a sure sign of local disturbance, it may be

reasonably supposed that the same kind of energy producing them nearly

always prevails in the polar regions, although it is there much weaker,

and never reaches beyond certain narrow limits.

Studied with the spectroscope, the granulations are found to be composed

in the main of incandescent hydrogen gas, and of an unknown substance

provisionally called "helium." Among the most brilliant of them are

found traces of incandescent metallic vapors, belonging to various

substances found on our globe.

The chromosphere is not fixed, but varies considerably in thickness in

its different parts, from day to day. Its thickness is usually greater

in the polar regions, where it sometimes exceeds 6,700 miles. In the

equatorial regions the chromosphere very rarely attains this height, and

when it does, the rising is local and occupies only a small area. In

these regions it is sometimes so shallow that its depth is only a few

seconds, and is then quite difficult to measure. These numbers give, of

course, the extreme limits of the variations of the chromosphere; but,

nearly always, it is more shallow in the equatorial regions; and, as far

as my observations go, the difference in thickness between the polar and

equatorial zones is greater in years of calm than it is in years of

great solar activity. But ten years of observation are not sufficient to

warrant any definite conclusions on this subject.

There is undoubtedly some relation between the greater thickness of the

chromosphere in the polar regions, and the abundance and permanence of

the sharply-pointed granulations observed in the same regions. This

becomes more evident when we know that the appearance of

similarly-pointed flames in the equatorial zones is always accompanied

with a local thickening of the chromosphere. The thickening in the polar

regions may be only apparent, and not due to a greater accumulation of

chromospheric gases there; but may be caused by some kind of repulsive

action or polarity, which lifts up and extends the summit of the

granulations in a manner similar to the well-known mode of electric

repulsion and polarity.

As it seems very probable that the heat and light emanating from the Sun

are mainly generated at the base of the granulations, in the filamentary

elements composing the chromosphere and photosphere, it would follow

that, as the size and number of these objects constantly vary, the

amount of heat and light emitted by the Sun should also vary in the same

proportion.

The granulations of the solar surface are represented on Plate I., and

form the general background to the group of Sun-spots forming the

picture.

THE FACULÆ

Although the solar surface is mainly covered with the luminous

granulations and the grayish background above described, it is very rare

that its appearance is so simple and uniform as already represented. For

the most part, on the contrary, it is diversified by larger, brighter,

and more complicated forms, which are especially visible towards the

border of the Sun. Owing to their extraordinary brilliancy, these

objects have been called _Faculœ_ (torches).

Although the faculæ are very seldom seen well beyond 50 heliocentric

degrees from the limb, yet they exist, and are as numerous in the

central parts of the disk as they are towards the border; since they

form a part of the solar surface, and participate in its movement of

rotation. Their appearance near the limb has been attributed to the

effect of absorption produced by the solar atmosphere on the

light from the photosphere; but this explanation seems inadequate,

and does not solve the problem. The well-known fact that the solar

protuberances--which are in a great measure identical with the

faculæ--are much brighter at the base than they are at the summit,

perhaps gives a clue to the explanation of the phenomenon; especially

since we know that, in general, the summit of the protuberances is

considerably broader than their base. When these objects are observed in

the vicinity of the limb, they present their brightest parts to the

observer, since, in this position, they are seen more or less sidewise;

and, therefore, they appear bright and distinct. But as the faculæ

recede from the limb, their sides, being seen under a constantly

decreasing angle, appear more and more foreshortened; and, therefore,

these objects grow less bright and less distinct, until they finally

become invisible, when their bases are covered over by the broad, dusky

summit generally terminating the protuberances.

The faculæ appear as bright and luminous masses or streaks on the

granular surface of the Sun, but they differ considerably in form and

size. Two types at least are distinguishable. In their simplest form

they appear either as isolated white spots, or as groups of such spots

covering large surfaces, and somewhat resembling large flakes of snow.

In their most characteristic types they appear as intensely luminous,

heavy masses, from which, in most cases, issue intricate ramifications,

sometimes extending to great distances. Generally, the ramifications

issuing from the masses of faculæ have their largest branches directed

in the main towards the eastern limb of the Sun. Some of these branches

have gigantic proportions. Occasionally they extend over 60° and even

80° of the solar surface, and, therefore, attain a length of from

450,000 to 600,000 miles.

Although the faculæ may be said to be seen everywhere on the surface of

the Sun, there is a vast difference in different regions, with regard to

their size, number, and brilliancy. They are largest, most abundant, and

brightest on two intermediate zones parallel to the solar equator, and

extending 35° or 40° to the north and to the south of this line. The

breadth of these zones varies considerably with the activity of the

solar forces. When they are most active, the faculæ spread on either

side, but especially towards the equator, where they sometimes nearly

meet those of the other zone. In years of little solar activity the

belts formed by the faculæ are very narrow--the elements composing them

being very few and small, although they never entirely disappear.

The faculæ are very unstable, and are constantly changing: those of the

small types sometimes form and vanish in a few minutes. When an area of

disturbance of the solar surface is observed for some time, all seems in

confusion; the movements of the granulations become unusually violent;

they congregate in all sorts of ways, and thus frequently form temporary

faculæ. Action of this kind is, for the most part, peculiar to the

polar regions of the Sun.

The larger faculæ have undoubtedly another origin, as they seem to be

mainly formed by the ejection of incandescent gases and metallic vapors

from the interior of the photosphere. In their process of development

some of the heavy masses of faculæ are swollen up to great heights,

being torn in all sorts of ways, showing large rents and fissures

through which the sight can penetrate.

Very few faculæ are represented in Plate I.; several streaks are shown

at the upper left-hand corner, some appearing as whitish ramifications

among the granulations representing the general solar surface.

SUN-SPOTS AND VEILED SPOTS

PLATE I

Besides the brilliant faculæ already described, much more conspicuous

markings, though of a totally different character, are very frequently

observed on the Sun. On account of their darkish appearance, which is in

strong contrast with the white envelope of our luminary, these markings

were called _Maculæ_, or Sun-spots, by their earlier observers.

The Sun-spots are not equally distributed on the solar surface; but like

the faculæ, to which they are closely related, they occupy two

zones--one on each side of the equator. These zones are comprised

between 10° and 35° of north latitude, and 10° and 35° of south

latitude. Between these two zones is a belt 20° in width, where the

Sun-spots are rarely seen.

Above the latitudes 35° north and south, the Sun-spots are rare, and it

is only occasionally, and during years of great solar activity, that

they appear in these regions; in only a few cases have spots of

considerable size been seen there. A few observers, however, have seen

spots as far as 40° and 50 from the equator; and La Hire even observed

one in 70° of north latitude; but these cases are exceedingly rare. It

is not uncommon, however, to see very small spots, or groups of such

spots, within 8° or 10° from the poles.

The activity of the Sun is subject to considerable fluctuation, and

accordingly the Sun-spots vary in size and number in different years.

During some years they are large, complicated, and very numerous; while

in others they are small and scarce, and are sometimes totally absent

for weeks and months together. The fluctuations in the frequency of

Sun-spots are supposed to be periodical in their character, although

their periods do not always appear to recur at exactly regular

intervals. Sometimes the period is found to be only nine years, while at

other times it extends to twelve years. The period generally adopted now

is 11⅒ years, nearly; but further investigations are needed to

understand the true nature of the phenomenon.

The number of Sun-spots does not symmetrically augment and diminish, but

the increase is more rapid than the diminution.

The period of increase is only about four years, while that of decrease

is over seven years; each period of Sun-spot maximum being nearer the

preceding period of Sun-spot minimum than it is to that next following.

The cause of these fluctuations in the solar energy is at present wholly

unknown. Some astronomers, however, have attributed it to the influence

of the planets Venus and Jupiter, the period of revolution of the latter

planet being not much longer than the Sun-spot period; but this

supposition lacks confirmation from direct observations, which, so far,

do not seem to be in favor of the hypothesis. At the present time the

solar activity is on the increase, and the Sun-spots will probably reach

their maximum in 1883. The last minimum occurred in 1879, when only

sixteen small groups of spots were observed during the whole year.

Sun-spots vary in size and appearance; but, unless they are very small,

in which case they appear as simple black dots, they generally consist

of two distinct and well-characterized parts, nearly always present.

There is first, a central part, much darker than the other, and sharply

divided from it, called the "_Umbra_;" second, a broad, irregular

radiated fringe of lighter shade, completely surrounding the first, and

called the "_Penumbra_."

Reduced to its simplest expression, a Sun-spot is a funnel-shaped

opening through the chromosphere and the photosphere. The inner end of

the funnel, or opening, gives the form to the umbra, while its sloping

sides form the penumbra.

The umbra of Sun-spots, whose outlines approximately follow the

irregularities of the penumbral fringe, has a diameter which generally

exceeds the width of the penumbral ring. Sometimes it appears uniformly

black throughout; but it is only so by contrast, as is proved when

either Mercury or Venus passes near a spot during a transit over the

Sun's disk. The umbra then appears grayish, when compared with the

jet-black disk of the planet.

The umbra of spots is rarely so simple as just described; but it is

frequently occupied, either partly or wholly, by grayish and rosy forms,

somewhat resembling loosely-entangled muscular fibres. These forms have

been called the _Gray and Rosy Veils_. Frequently these veils appear as

if perforated by roundish black holes, improperly called _Nuclei_, which

permit the sight to penetrate deeper into the interior. To all

appearance the gray and rosy veils are of the same nature as the

chromosphere and the faculæ, and are therefore mainly composed of

hydrogen gas.

Whatever can be known about the interior of the Sun, must be learned

from the observations of these openings, which are comparatively small.

But whatever this interior may be, we certainly know that it is not

homogeneous. Apparently, the Sun is a gigantic bubble, limited by a very

thin shell. Below this shell exists a large open space filled with

invisible gases, in which, through the openings constituting the

Sun-spots, the gray and rosy veils described above are occasionally seen

floating.

The fringe forming the penumbra of spots is much more complicated than

the umbra. In its simpler form, it is composed of a multitude of bright,

independent filaments of different forms and sizes, partly projecting

one above the other, on the sloping wall of the penumbra, from which

they seem to proceed. Seen from the Earth, these filaments have somewhat

the appearance of thatched straw, converging towards the centre of the

umbra. It is very rare, however, that the convergence of the penumbral

filaments is regular, and great confusion sometimes arises from the

entanglement of these filaments. Some of these elements appear straight,

others are curved or loop-shaped; while still others, much larger and

brighter than the rest, give a final touch to this chaos of filaments,

from which results the general thatched and radiating appearance of the

penumbra.

The extremities of the penumbral filaments, especially of those forming

the border of the umbra, are usually club-shaped and appear very

brilliant, as if these elements had been superheated by some forces

escaping through the opening of the spots.

Besides these characteristics, the Sun-spots have others, which,

although not always present, properly belong to them. Comparatively few

spots are so simple as the form just described. Very frequently a spot

is accompanied by brilliant faculæ, covering part of its umbra and

penumbra, and appearing to form a part of the spot itself.

When seen projected over Sun-spots, the faculæ appear intensely bright,

and from these peculiarities they have been called _Luminous Bridges_.

They are, in fact, bridges, but in most cases they are at considerable

heights above the spots, kept there by invisible forces. When such spots

with luminous bridges approach the Sun's limb, it is easy to see, by the

rapid apparent displacement which they undergo, that they are above the

general level.

When the spots are closing up, the inverse effect is sometimes observed.

On several occasions, I have seen huge masses of faculæ advance slowly

over the penumbra of a spot and fall into the depths of the umbra,

resembling gigantic cataracts. I have seen narrow branches of faculæ,

which, after having fallen to great depths in the umbra, floated across

it and disappeared under the photosphere on the opposite side. I have

also seen luminous bridges, resembling cables, tightly stretched across

the spots, slackening slowly, as if loosened at one end, and gently

curving into the umbra, where they formed immense loops, large enough to

receive our globe.

It is to be remarked that, in descending under the photospheric shell,

the bright faculæ and the luminous bridges gradually lose their

brilliancy. At first they appear grayish, but in descending farther they

assume more and more the pink color peculiar to the rosy veils. The

pinkish color acquired by the faculæ when they reach a certain depth

under the photosphere, is precisely the color of the chromosphere and of

the solar protuberances, as seen during total eclipses of the Sun--a

fact which furnishes another proof that the faculæ are of the same

nature as the protuberances.

I record here an observation which, at first sight, may appear

paradoxical; but which seems, however, to be of considerable importance,

as it shows unmistakably that the solar light is mainly, if not

entirely, generated on its surface, or at least very near to it. On May

26, 1878, I observed a large group of Sun-spots at a little distance

from the east limb of the Sun. The spot nearest to the limb was partly

covered over on its eastern and western sides by bright and massive

faculæ which concealed about two-thirds of the whole spot, only a

narrow opening, running from north to south, being left across the

middle of the spot. Owing to the rotundity of the Sun, the penumbra of

this spot, although partly covered by the faculæ, could, however, be

seen on its eastern side, since the sight of the observer could there

penetrate sidewise under the faculæ. Upon that part of the penumbra

appeared a strong shadow, representing perfectly the outline of the

facular mass situated above it. The phenomenon was so apparent that no

error of observation was possible, and a good drawing of it was secured.

If this faculæ had been as bright beneath as it was above, it is

evident that no shadow could have been produced; hence the light of

these faculæ must have been mainly generated on or very near their

exterior surfaces. This, with the well-proved fact that the bright

faculæ lose their light in falling into the interior of the Sun, seems

to suggest the idea that the bright light emitted by the faculæ, and

very probably all the solar light, can be generated only on its surface;

the presence of the coronal atmosphere being perhaps necessary to

produce it. Several times before this observation, I had suspected that

some faculæ were casting a shadow, but as this seemed so improbable, my

attention was not awakened until the phenomenon became so prominent that

it could not escape notice.

With due attention, some glimpses of the phenomenon can frequently be

observed through the openings of some of the faculæ projecting over the

penumbra of Sun-spots. It is very seldom that the structure of the

penumbra is seen through such openings, which usually appear as dark as

the umbra of the large spots, although they do not penetrate through the

photosphere like the latter. It is only when the rents in the faculæ

are numerous and quite large, that the penumbral structure is recognized

through them. Since these superficial rents in the faculæ do not extend

through the photosphere, and appear black, it seems evident that the

penumbra seen through them cannot be as bright as it is when no faculæ

are projected upon it, and therefore that the faculæ intercept light

from the exterior surface, which would otherwise reach the penumbra.

While the matter forming the faculæ sometimes falls into the interior

of the Sun, the same kind of matter is frequently ejected in enormous

quantities, and with great force, from the interior, through the visible

and invisible openings of the photosphere, and form the protuberances

described in the following section of this manual (Solar protuberances)

It is not only the incandescent hydrogen gas or the metallic vapors

which are thus ejected, but also cooler hydrogen gas, which sometimes

appears as dark clouds on the solar surface. On December 12, 1875, I

observed such a cloud of hydrogen issuing from the corner of a small

Sun-spot. It traveled several thousand miles on the solar surface, in a

north-easterly direction, before it became invisible.

Solar spots are formed in various ways; but, for the most part, the

apparition of a spot is announced beforehand, by a great commotion of

the solar surface at the place of its appearance, and by the formation

of large and bright masses of faculæ, which are usually swollen into

enormous bubbles by the pressure of the internal gases. These bubbles

become visible in the spectroscope while they are traversing the solar

limb, as they are then presented to us sidewise. Under the action of the

increasing pressure, the base of the faculæ is considerably stretched,

and, its weakest side finally giving way, the facular mass is torn in

many places from the solar surface, and is perforated by holes of

different sizes and forms. The holes thus made along the border of the

faculæ appear as small black spots, separated more or less by the

remaining portion of the lacerated faculæ, and they enlarge more and

more at the expense of the intervening portions, which thus become very

narrow. This perforated side of the faculæ, offering less resistance,

is gradually lifted up, as would be the cover of a box, for example,

while its opposite side remains attached to the surface. The facular

matter separating the small black holes is greatly stretched during this

action, and forms long columns and filaments. These appear as luminous

bridges upon the large and perfectly-formed spot, which is then seen

under the lifted facular masses. The spots thus made visible are soon

freed from the facular masses, which are gradually shifted towards the

opposite side.

In such cases the spots are undoubtedly formed under the faculæ before

they can be seen. This becomes evident when such spots, not yet cleared

from the faculæ covering them, are observed near the east limb; since

in this position the observer can see through the side-openings of the

faculæ, and sometimes recognize the spots under their cover.

It frequently occurs that the spots thus formed under the faculæ

continue to be partly covered by the facular clouds, the forces at work

in them being apparently too feeble to shift them aside. In such cases

these spots are visible when they are in the vicinity of the limb, where

they are seen sidewise; but when observed in the east, in being carried

forward by the solar rotation towards the centre of the disk, they

gradually diminish in size, and finally become invisible. The

disappearance of these spots, however, is only apparent, being due to

the fact that, as they advance towards the centre of the disk, our

lateral view of them is gradually lost, and they are finally hidden from

sight by the overhanging faculæ which then serve as a screen between

the observer and the spot. This class of spots may be called _Lateral

Spots_, from the fact that they can only be seen laterally, and near the

Sun's limb.

Solar spots are also formed in various other ways. Some, like those

represented in Plate I., appearing without being announced by any

apparent disturbance of the surface, or by the formation of any faculæ,

form and develop in a very short time. Others, appearing at first as

very small spots having an umbra and a penumbra, slowly and gradually

develop into very large spots. This mode of formation, which would seem

to be the most natural, is, however, quite rare. Spots of this class

have a duration and permanence not observed in those of any other type.

These spots of slow and regular development are never accompanied by

faculæ or luminous bridges, nor have they any gray or rosy veils in

their interior; a fact which may, perhaps, account for their permanent

character.

Another class of spots, which is also rare, appear as long and narrow

crevasses showing the penumbral structure of the ordinary spots; but

these rarely have any umbra. These long, and sometimes exceedingly

narrow fissures of the solar envelopes, with their radiated penumbral

structure, strongly suggest the idea that the photosphere is composed of

a multitude of filamentary elements having the granulations for summits.

Such a crevasse is represented on Plate I., and unites the two spots

which form the group.

The duration of Sun-spots varies greatly. Some last only for a few

hours; while others continue for weeks and even months at a time, but

not without undergoing changes.

The modes of disappearance of Sun-spots are as various as those of their

apparition. The spots rarely close up by a gradual diminution or

contraction of their umbra and penumbra. This mode of disappearance

belongs exclusively to the spots deprived of faculæ and veils. One of

the most common modes of the disappearance of a spot is its invasion by

large facular masses, which slowly advance upon its penumbra and umbra

and finally cover it entirely. It is a process precisely the reverse of

that in which spots are formed by the shifting aside of the faculæ, as

above described. In other types, the spots close up by the gradual

enlargement of the luminous bridges traversing them, which are slowly

transformed into branches of the photosphere, all of the characteristics

of which they have acquired. In many cases, the spots covered over by

the faculæ continue to exist for some time, hidden under these masses,

as is often proved, either by the appearance of small spots on the

facular mass left at the place they occupied, or even by the

reappearance of the same spot.

Apart from the general movement of rotation of the solar surface, some

of the spots seem to be endowed with a proper motion of their own, which

becomes greater the nearer the spots are to the solar equator. According

to the observations of Mr. Carrington, the period of rotation of the

Sun, as deduced from the observations of the solar spots during a period

of seven years, is 25 days at the equator; while at 50° of heliocentric

latitude it is 27 days. But the period of rotation, as derived from the

observations of spots occupying the same latitude, is far from being

constant, as it varies at different times, with the frequency of the

spots and with the solar activity, so that at present the law of these

variations is not well known. From the character of the solar envelope,

it seems very natural that the rotation should differ in the different

zones and at different times, since this envelope is not rigid, but very

movable, and governed by forces which are themselves very variable.

Although it is a general law that the spots near the equator have a more

rapid motion than those situated in higher latitudes, yet, in many

cases, the proper motion of the spots is more apparent than real. For

the most part, the changes of form and the rapid displacements observed

in some spots are only apparent, and due to the fact that the large

masses of faculæ which are kept in suspense above them are very

unstable, and change position with the slightest change in the forces

holding them in suspension. Since in these cases we view the spots

through the openings of the faculæ situated above them, the slightest

motion of these objects produces an apparent motion in the spots,

although they have remained motionless. Accordingly, it has been

remarked that of all the spots, those which have the greater proper

motion are precisely those which have the most faculæ and luminous

bridges; while the other spots in the same regions, but not attended by

similar phenomena, are comparatively steady in their movement. These

last spots are undoubtedly better adapted than any others to exhibit the

rotation of the Sun; but it is probable that this period of rotation

will never be known with accuracy, simply because the solar surface is

unstable, and does not rotate uniformly.

The Sun-spots have a remarkable tendency to form into groups of various

sizes, but whatever may be the number of spots thus assembled, the group

is nearly always composed of two principal spots, to which the others

are only accessories. The tendency of the Sun-spots to assemble in pairs

is general, and is observed in all latitudes, even among the minute

temporary groups formed in the polar regions. Whenever several are

situated quite close together, those belonging to the same group can be

easily recognized by this character. Whatever may be the position of the

axis of the two principal spots of a group when it is first formed, this

axis has a decided tendency to place itself parallel to the solar

equator, no matter to what latitude the group belongs; and if it is

disturbed from this position, it soon returns to it when the disturbance

has ceased.

It is also remarkable that the spots observed at the same time remain in

nearly the same parallel of latitude for a greater or less period of

time; but they keep changing their position from year to year, their

latitude decreasing with the activity of the solar forces.

Among the Sun-spots, those associated with faculæ form the groups which

attain the largest proportions. When such groups acquire an apparent

diameter of 1' or more, they are plainly visible to the naked eye, since

for a spot to be visible to the naked eye on the Sun, it need only

subtend an angle of 50". I have sometimes seen such groups through a

smoky atmosphere, when the solar light was so much reduced that the disk

could be observed directly and without injury to the sight.

The largest spot which ever came under my observation was seen during

the period from the 13th to the 19th of November, 1870. This spot, which

was on the northern hemisphere of the Sun, was conspicuous among the

smaller spots constituting the group to which it belonged, and followed

them on the east. On November 16th, when it attained its largest size,

the diameter of its penumbra occupied fully one-fifth of the diameter of

the Sun; its real diameter being, therefore, not less than 172,000

miles, or nearly 22 times the diameter of the Earth. As the umbra of

this spot occupied a little more than one-third of its whole diameter,

seven globes like our own, placed side by side on a straight line, could

easily have passed through this immense gap. To fill the area of this

opening, about 45 such globes would have been needed. This spot was, of

course, very easily seen with the naked eye, its diameter being almost

eight times that required for a spot to be visible without a telescope.

Ancient historians often speak of obscurations of the Sun, and it has

been supposed by some astronomers that this phenomenon might have been

due in some cases to the apparition of large spots. A few spots on the

surface of the Sun, like that just described, would sensibly reduce its

light.

Besides the ordinary Sun-spots already described, others are at times

observed on the surface of the Sun, which show some of the same

characteristics, but never attain so large proportions. They always

appear as if seen through a fog, or veil, between the granulations of

the solar surface. On account of their vagueness and ill-defined

contours, I have proposed for these objects the term, "_Veiled Spots_."

Veiled spots have a shorter duration than the ordinary spots, the

smaller types sometimes forming and vanishing in a few minutes. Some of

the larger veiled spots, however, remain visible for several days in

succession, and show the characteristics of other spots in regard to the

arrangement of their parts.

The Trouvelot astronomical drawings manual · 第 1 / 17 段