SECTION XII.

Mean and Apparent Sidereal Time—Mean and Apparent Solar Time—Equation of

Time—English and French Subdivisions of Time—Leap Year—Christian

Era—Equinoctial Time—Remarkable Eras depending upon the Position of

the Solar Perigee—Inequality of the Lengths of the Seasons in the two

Hemispheres—Application of Astronomy to Chronology—English and French

Standards of Weights and Measures.

ASTRONOMY has been of immediate and essential use in affording

invariable standards for measuring duration, distance, magnitude, and

velocity. The mean sidereal day measured by the time elapsed between two

consecutive transits of any star at the same meridian (N. 148), and the

mean sidereal year which is the time included between two consecutive

returns of the sun to the same star, are immutable units with which all

great periods of time are compared; the oscillations of the isochronous

pendulum measure its smaller portions. By these invariable standards

alone we can judge of the slow changes that other elements of the system

may have undergone. Apparent sidereal time, which is measured by the

transit of the equinoctial point at the meridian of any place, is a

variable quantity, from the effects of precession and nutation. Clocks

showing apparent sidereal time are employed for observation, and are so

regulated that they indicate 0^h 0^m 0^s at the instant the

equinoctial point passes the meridian of the observatory. And as time is

a measure of angular motion, the clock gives the distances of the

heavenly bodies from the equinox by observing the instant at which each

passes the meridian, and converting the interval into arcs at the rate

of 15° to an hour.

The returns of the sun to the meridian and to the same equinox or

solstice have been universally adopted as the measure of our civil days

and years. The solar or astronomical day is the time that elapses

between two consecutive noons or midnights. It is consequently longer

than the sidereal day, on account of the proper motion of the sun during

a revolution of the celestial sphere. But, as the sun moves with greater

rapidity at the winter than at the summer solstice, the astronomical day

is more nearly equal to the sidereal day in summer than in winter. The

obliquity of the ecliptic also affects its duration; for near the

equinoxes the arc of the equator is less than the corresponding arc of

the ecliptic, and in the solstices it is greater (N. 149). The

astronomical day is therefore diminished in the first case, and

increased in the second. If the sun moved uniformly in the equator at

the rate of 59ʹ 8ʺ·33 every day, the solar days would be all equal. The

time therefore which is reckoned by the arrival of an imaginary sun at

the meridian, or of one which is supposed to move uniformly in the

equator, is denominated mean solar time, and is given by clocks and

watches in common life. When it is reckoned by the arrival of the real

sun at the meridian, it is true or apparent time, and is given by dials.

The difference between the time shown by a clock and a dial is the

equation of time given in the Nautical Almanac, sometimes amounting to

as much as sixteen minutes. The apparent and mean time coincide four

times in the year; when the sun’s daily motion in right ascension is

equal to 59ʹ 8ʺ·33 in a mean solar day, which happens about the 16th of

April, the 16th of June, the 1st of September, and the 25th of December.

The astronomical day begins at noon, but in common reckoning the day

begins at midnight. In England it is divided into twenty-four hours,

which are counted by twelve and twelve; but in France astronomers,

adopting the decimal division, divide the day into ten hours, the hour

into one hundred minutes, and the minute into a hundred seconds, because

of the facility in computation, and in conformity with their decimal

system of weights and measures. This subdivision is not now used in

common life, nor has it been adopted in any other country; and although

some scientific writers in France still employ that division of time,

the custom is beginning to wear out. At one period during the French

Revolution, the clock in the gardens of the Tuileries was regulated to

show decimal time. The mean length of the day, though accurately

determined, is not sufficient for the purposes either of astronomy or

civil life. The tropical or civil year of 365^d 5^h 48^m 49^s·7,

which is the time elapsed between the consecutive returns of the sun to

the mean equinoxes or solstices, including all the changes of the

seasons, is a natural cycle peculiarly suited for a measure of duration.

It is estimated from the winter solstice, the middle of the long annual

night under the north pole. But although the length of the civil year is

pointed out by nature as a measure of long periods, the

incommensurability that exists between the length of the day and the

revolution of the sun renders it difficult to adjust the estimation of

both in whole numbers. If the revolution of the sun were accomplished in

365 days, all the years would be of precisely the same number of days,

and would begin and end with the sun at the same point of the ecliptic.

But as the sun’s revolution includes the fraction of a day, a civil year

and a revolution of the sun have not the same duration. Since the

fraction is nearly the fourth of a day, in four years it is nearly equal

to a revolution of the sun, so that the addition of a supernumerary day

every fourth year nearly compensates the difference. But in process of

time further correction will be necessary, because the fraction is less

than the fourth of a day. In fact, if a bissextile be suppressed at the

end of three out of four centuries, the year so determined will only

exceed the true year by an extremely small fraction of a day; and if in

addition to this a bissextile be suppressed every 4000 years, the length

of the year will be nearly equal to that given by observation. Were the

fraction neglected, the beginning of the year would precede that of the

tropical year, so that it would retrograde through the different seasons

in a period of about 1507 years. The Egyptian year began with the

heliacal rising of Sirius (N. 150), and contained only 365 days, by

which they lost one year in every 1461 years, their Sothaic period, or

that cycle in which the heliacal rising of Sirius passes through the

whole year and takes place again on the same day. The division of the

year into months is very old and almost universal. But the period of

seven days, by far the most permanent division of time, and the most

ancient monument of astronomical knowledge, was used by the Brahmins in

India with the same denominations employed by us, and was alike found in

the calendars of the Jews, Egyptians, Arabs, and Assyrians. It has

survived the fall of empires, and has existed among all successive

generations, a proof of their common origin.

The day of the new moon immediately following the winter solstice in the

707th year of Rome was made the 1st of January of the first year of

Julius Cæsar. The 25th of December of his forty-fifth year is considered

as the date of Christ’s nativity; and the forty-sixth year of the Julian

Calendar is assumed to be the first of our era. The preceding year is

called the first year before Christ by chronologists, but by astronomers

it is called the year 0. The astronomical year begins on the 31st of

December at noon; and the date of an observation expresses the days and

hours which have actually elapsed since that time.

Since solar and sidereal time are estimated from the passage of the sun

and the equinoctial point across the meridian of each place, the hours

are different at different places: while it is one o’clock at one place,

it is two at another, three at another, &c.; for it is obvious that it

is noon at one part of the globe at the same moment that it is midnight

at another diametrically opposite to it: consequently an event which

happens at one and the same instant of absolute time is recorded at

different places as having happened at different times. Therefore, when

observations made at different places are to be compared, they must be

reduced by computation to what they would have been had they been made

under the same meridian. To obviate this it was proposed by Sir John

Herschel to employ mean equinoctial time, which is the same for all the

world, and independent alike of local circumstances and inequalities in

the sun’s motion. It is the time elapsed from the instant the mean sun

enters the mean vernal equinox, and is reckoned in mean solar days and

parts of a day.

Some remarkable astronomical eras are determined by the position of the

major axis of the solar ellipse, which depends upon the direct motion of

the perigee (N. 102) and the precession of the equinoxes conjointly, the

annual motion of the one being 11ʺ·8, and that of the other 50ʺ·1. Hence

the axis, moving at the rate of 61ʺ·9 annually, accomplishes a tropical

revolution in 209·84 years. It coincided with the line of the equinoxes

4000 or 4089 years before the Christian era, much about the time

chronologists assign for the creation of man. In 6483 the major axis

will again coincide with the line of the equinoxes; but then the solar

perigee will coincide with the equinox of autumn, whereas at the

creation of man it coincided with the vernal equinox. In the year 1246

the major axis was perpendicular to the line of the equinoxes; then the

solar perigee coincided with the solstice of summer, and the apogee with

the solstice of winter. According to La Place, who computed these

periods from different data, the last coincidence happened in the year

1250 of our era, which induced him to propose that year as a universal

epoch, the vernal equinox of the year 1250 to be the first day of the

first year. These eras can only be regarded as approximate, since

ancient observations are too inaccurate, and modern observations too

recent, to afford data for their precise determination.

The variation in the position of the solar ellipse occasions

corresponding changes in the length of the seasons. In its present

position spring is shorter than summer, and autumn longer than winter;

and while the solar perigee continues as it now is, between the solstice

of winter and the equinox of spring, the period including spring and

summer will be longer than that including autumn and winter. In this

century the difference is between seven and eight days. The intervals

will be equal towards the year 6483, when the perigee will coincide with

the equinox of spring; but, when it passes that point, the spring and

summer taken together will be shorter than the period including the

autumn and winter (N. 151). These changes will be accomplished in a

tropical revolution of the major axis of the earth’s orbit, which

includes an interval of 20,984 years. Were the orbit circular, the

seasons would be equal; their difference arises from the excentricity of

the orbit, small as it is; but the changes are so trifling as to be

imperceptible in the short span of human life.

No circumstance in the whole science of astronomy excites a deeper

interest than its application to chronology. “Whole nations,” says La

Place, “have been swept from the earth, with their languages, arts, and

sciences, leaving but confused masses of ruins to mark the place where

mighty cities stood; their history, with the exception of a few doubtful

traditions, has perished; but the perfection of their astronomical

observations marks their high antiquity, fixes the periods of their

existence, and proves that, even at that early time, they must have made

considerable progress in science.” The ancient state of the heavens may

now be computed with great accuracy; and, by comparing the results of

calculation with ancient observations, the exact period at which they

were made may be verified if true, or, if false, their error may be

detected. If the date be accurate and the observation good, it will

verify the accuracy of modern tables, and will show to how many

centuries they may be extended without the fear of error. A few examples

will show the importance of the subject.

At the solstices the sun is at his greatest distance from the equator;

consequently his declination at these times is equal to the obliquity of

the ecliptic (N. 152), which was formerly determined from the meridian

length of the shadow of the stile of a dial on the day of a solstice.

The lengths of the meridian shadow at the summer and winter solstices

are recorded to have been observed at the city of Layang, in China, 1100

years before the Christian era. From these the distances of the sun from

the zenith (N. 153) of the city of Layang are known. Half the sum of

these zenith distances determines the latitude, and half their

difference gives the obliquity of the ecliptic at the period of the

observation; and, as the law of the variation of the obliquity is known,

both the time and place of the observations have been verified by

computations from modern tables. Thus the Chinese had made some advances

in the science of astronomy at that early period. Their whole chronology

is founded on the observations of eclipses, which prove the existence of

that empire for more than 4700 years. The epoch of the lunar tables of

the Indians, supposed by Bailly to be 3000 years before the Christian

era, was proved by La Place, from the acceleration of the moon, not to

be more ancient than the time of Ptolemy, who lived in the second

century after it. The great inequality of Jupiter and Saturn, whose

cycle embraces 918 years, is peculiarly fitted for marking the

civilization of a people. The Indians had determined the mean motions of

these two planets in that part of their periods when the apparent mean

motion of Saturn was at the slowest, and that of Jupiter the most rapid.

The periods in which that happened were 3102 years before the Christian

era, and the year 1491 after it. The returns of comets to their

perihelia may possibly mark the present state of astronomy to future

ages.

The places of the fixed stars are affected by the precession of the

equinoxes; and, as the law of that variation is known, their positions

at any time may be computed. Now Eudoxus, a contemporary of Plato,

mentions a star situate in the pole of the equator, and it appears from

computation that χ Draconis was not very far from that place about 3000

years ago; but, as it is only about 2150 years since Eudoxus lived, he

must have described an anterior state of the heavens, supposed to be the

same that was mentioned by Chiron about the time of the siege of Troy.

Thus every circumstance concurs in showing that astronomy was cultivated

in the highest ages of antiquity.

It is possible that a knowledge of astronomy may lead to the

interpretation of hieroglyphical characters. Astronomical signs are

often found on the ancient Egyptian monuments, probably employed by the

priests to record dates. The author had occasion to witness an instance

of this most interesting application of astronomy, in ascertaining the

date of a papyrus, sent from Egypt by Mr. Salt, in the hieroglyphical

researches of the late Dr. Thomas Young, whose profound and varied

acquirements do honour to his country, and to the age in which he lived.

The manuscript was found in a mummy case; it proved to be a horoscope of

the age of Ptolemy, and its date was determined from the configuration

of the heavens at the time of its construction.

The form of the earth furnishes a standard of weights and measures for

the ordinary purposes of life, as well as for the determination of the

masses and distances of the heavenly bodies. The length of the pendulum

vibrating seconds of mean solar time, in the latitude of London, forms

the standard of the British measure of extension. Its approximate length

oscillating in vacuo at the temperature of 62° of Fahrenheit, and

reduced to the level of the sea (N. 154), was determined by Captain

Kater to be 39·1393 inches. The weight of a cubic inch of water at the

temperature of 62° of Fahrenheit, barometer 30 inches, was also

determined in parts of the imperial troy pound, whence a standard both

of weight and capacity was deduced. The French have adopted the mètre,

equal to 3·2808992 English feet, for their unit of linear measure, which

is the ten-millionth part of the arc of the meridian which extends from

the equator to the pole, as deduced from the measures of the separate

arc extending from Formentera, the most southern of the Balearic

Islands, to Dunkirk. Should the national standards of the two countries

ever be lost, both may be recovered, since they are derived from natural

and invariable ones. The length of the measure deduced from that of the

pendulum would be found again with more facility than the mètre. But, as

no measure is mathematically exact, an error in the original standard

may at length become sensible in measuring a great extent, whereas the

error that must necessarily arise in measuring the quadrant of the

meridian (N. 155) is rendered totally insensible by subdivision in

taking its ten-millionth part. The French have adopted the decimal

division, not only in time, but also in their degrees, weights, and

measures, on account of the very great facility it affords in

computation. It has not been adopted by any other country, though

nothing is more desirable than that all nations should concur in using

the same standards, not only on account of convenience, but as affording

a more definite idea of quantity. It is singular that the decimal

division of the day, of space, weights, and measures, was employed in

China 4000 years ago; and that at the time Ibn Junis made his

observations at Cairo, about the year 1000 of the Christian era, the

Arabs were in the habit of employing the vibrations of the pendulum in

their astronomical observations as a measure of time.

On the Connexion of the Physical Sciences · 第 12 / 39 章