CHAPTER III

Declination and Right Ascension

Owing to the important place that declination holds in nautical

astronomy, a detailed explanation will appropriately follow closely

in the wake of the preceding remarks. It must be made clear, before

getting under way, that declination is the distance, in degrees,

minutes and seconds, of a body north (+) or south (-) of the celestial

equator measured on the hour circle passing through the body. This

distance is identical with the latitude of the place in the zenith of

which the body happens to be. What declination is to a body in the

heavens, latitude is to the place on the earth directly beneath it.

The declination of fixed stars changes very slowly from month to month,

but the planets meander about on the celestial sphere in a way that

is liable to puzzle anyone other than an astronomer. This element,

however, is worked out in the observatory and given in the nautical

almanac in a way that relieves the navigator of worry concerning the

complex movements of these latter bodies. The same may be said of the

moon, but the subject will be treated, somewhat superficially though

sufficiently for the needs and desires of the practical mariner, in

a special talk on the moon. This eliminates all the celestial bodies

except the sun, the most important; and for this reason the facts

relative to its declination will be considered at some length.

As has already been stated, the sun is stationary, but our movements

around it to the right causes it to appear to move to the left;

precisely as you see, when under way, an anchored vessel’s masts move

to the left along the land behind her, while you move on to the right.

We have no landmarks behind the sun by which to observe his apparent

movements, so in lieu of such ranges, we resort to the fixed stars,

which serve as excellent marks to get a bearing on Old Sol and keep tab

on him as he moves eastward among them. This movement must in no way be

confounded with his apparent daily motion westward. As an illustration,

we may see Orion--a familiar friend--swinging high in the western sky

in the early evening; some weeks later he is riding low, and yet a

little later still, he is swallowed up in the brilliancy of the setting

sun. In other words, the sun and Orion have approached and passed each

other. We know Orion does not move, for he is composed of fixed stars,

and this seeming westward movement of his is in reality the apparent

eastward marching of the sun, which is due to the earth’s movement of

revolution. The sun in this apparent movement eastward follows a course

at a rate equal to that of the earth, along a great circle of the

celestial sphere called the ecliptic, a circle that plays an important

part in the explanation of declination, particularly that of the sun.

The ecliptic is marked by the extension of the earth’s orbit to the

celestial sphere.

A few more words concerning great circles will be introduced here,

and the following statements, while they apply to great circles

in general, especially fit the relationship of the equinoctial or

celestial equator to the ecliptic. These two great circles cut each

other at an angle of 23° 28´. Great circles always bisect each other,

and hence any two great circles of the celestial sphere, regardless

of the angle they may take with the celestial equator, must intersect

each other at exactly opposite points, 180° apart. What is true in this

regard of the celestial sphere is equally true of the great circles of

the earth. A vertex of a great circle is the point which departs the

greatest distance from the equator--the highest point of the circle

reached in declination. There are two vertices 180° apart with the two

points of intersection 90° in either direction. The declination or

latitude of either vertex is equal to the angle at which the circles

intersect each other. The intersections are called the equinoxes, and

it may be well to say here that the word equinox has several meanings

in navigation, often rendering it necessary to judge by the text which

is intended. The vernal equinox, for instance, refers to a certain

time of year--March 21st. The sun is that day directly overhead at

the intersection of the equator and the terrestrial ecliptic and this

_point_ is sometimes called the vernal equinox. Again, the sun at the

same time occupies a point on the heavens also known as the vernal

equinox, which is at the intersection of the celestial equator and the

ecliptic. The point in the orbit occupied by the earth at this time is

also spoken of as the vernal equinox.

The reader is now asked to arouse his imagination and if possible

to conceive himself a passenger in an aeroplane equipped with some

remarkable power capable of carrying him to a position in space,

above, yet a little outside, the earth’s orbit, near the Perihelion,

and there to heave to and view awhile an astronomical picture. Spread

out before his unrestricted vision will be the earth, its orbit, and

the sun. It is to be hoped that the imagination of the reader is

still sufficiently supple to suppose the plane of the orbit to be the

surface of an infinite ocean stretching away beyond human conception of

distance and “breaking” against the celestial sphere; the “surfline”

there marks the ecliptic; the “ocean’s” surface representing the great

plane of the ecliptic. The sun will be seen as if at anchor in his

proper place within the orbit. The earth is “underway,” half submerged,

and listed 23° 28´ _toward our point of vantage_. This inclination, or

direction of the axis, is in a general way toward the perihelion, and

within a few degrees of being parallel with the long diameter of the

orbit. The earth maintains this nearly parallel position of its axis

with the long diameter throughout the period of its revolution; a fact

of importance to remember.

It will be readily seen that during the encircling of the sun there

must be one position where the northern axis is inclined directly

toward that body, another opposite where it is headed away from him,

and two positions midway where the bearing of the axis (projected on

the plane of the orbit) is at right angles to the bearing of the sun

from the earth; another feature to be “salted down” in the memory.

If the earth revolved on an even keel, the equator and the “waterline”

would be coincident, but fortunately this is not the case, and owing

to the inclination of the axis another great circle is defined by the

“waterline,” called the terrestrial ecliptic, being directly beneath

its celestial namesake. The inclination of the northern pole being

in a general way toward the perihelion, correspondingly depresses or

“submerges” that half of the equator below the plane of the ecliptic,

represented by the “water surface,” and at the same time the opposite

side rolls the equator above it. At two points (the equinoxes) on

opposite sides of the earth, and at right angles to the direction of

its inclination, the equator and terrestrial ecliptic cross each other

at the “water’s edge.”

The sun is always exactly overhead for that point of the earth which

is nearest to it. This is an essential fact to remember in navigation.

Bearing in mind that the sun is stationary and ignoring for a time the

rotation of the earth, each advance in its orbit brings about a change

of bearing of the sun and a new position becomes the nearest point,

and thereby directly beneath the sun. The constant changing of the

sun’s bearing continues throughout the year, or one revolution, and a

circle of these overhead positions is marked upon the earth, which is

coincident with the terrestrial ecliptic--the visionary “waterline.”

It is obvious that the vertical rays of the sun must apparently follow

this line, for it can only be overhead for places that are in the same

plane, and this again is the level of the “ocean.”

This circle of overhead positions projected on the celestial sphere

marks the ecliptic--the “margin” of the infinite ocean, and the path

that the sun seems to follow eastward among the stars.

The above paragraphs show us that the sun in following this line

around the earth crosses the equator twice, and twice he attains a

distance of 23° 28´ from it, and so must be on the equator twice and

reach a declination of 23° 28´ north and 23° 28´ south in the course of

one year.

Returning to our imaginary illustration, we will now follow the

peregrinations of the earth for a year and note the effect of its

inclination in the different parts of the orbit upon the declination of

the sun.

It will be assumed that it is the 21st of March and from our airy

position we see the earth away on our right nearly 90° from the

Perihelion. As this is the vernal equinox, there are a number of

interesting points to be considered: The direction of the earth’s axis,

projected on the plane of the orbit, is at right angles to the bearing

of the sun from the earth; the sun is directly over the intersection

of the equator and terrestrial ecliptic, and being overhead for

this point on the equator, the declination must be 0°. Moreover, a

line drawn from this intersection, or terrestrial vernal equinox,

through the center of the sun and extended to the celestial sphere

would strike the corresponding intersection of the ecliptic and the

equinoctial or celestial equator--the celestial vernal equinox. The

arrival of the earth at this position is the signal of spring for the

northern hemisphere, likewise it announces the advent of autumn to our

southern neighbors below the “Line.” The sun this day rises in the east

(approximately) and passing through the zenith, sets in the west for

those living on the equator. The explorer at the north pole is cheered

by the first light as the sun appears in the horizon, while the south

pole becomes enshrouded in the long Antarctic night. Without lingering

for ceremonies over the change of seasons, the earth continues steadily

on its way toward the aphelion; the sun’s vertical rays leave the

intersection of the equator and the terrestrial ecliptic, and follow

along the latter, thus widening its distance from the equator as the

earth proceeds. As the ecliptic in this half of the orbit is above,

or north, of the equator the former is in north latitude and the sun,

following along it, is thereby also in north declination. A line from

any place having the vertical rays, through the sun to the celestial

sphere, always terminates on the celestial ecliptic, all being in the

same plane, and shows the corresponding celestial position of the sun

on it. Its declination distance from the celestial equator, in degrees,

minutes and seconds, is identical with that of the place on the earth

directly beneath it relative to our equator. So by showing the course

of the sun’s overhead positions on the earth its celestial positions

are, at the same time, indicated. The overhead position of the sun on

the terrestrial ecliptic gradually departs from the equator culminating

about June 21st, the summer solstice, in a declination of 23° 28´ at

a point near the aphelion in the orbit, 90° (approximately) from the

equinox.

The positions in the orbit of the summer and winter solstices are

reached by the earth several days before the points of the aphelion and

perihelion. These respective positions would be in conjunction were it

not for a slow and remarkable motion of the earth’s axis before spoken

of, and later to be described, called the precession of the equinoxes.

The summer solstice is the great half-way point of the earth’s annual

circumnavigation of the sun; it is a matter of moment all over the

world, and another great change of seasons is at hand. The sun is

overhead for places along the parallel of 23° 28´ N. and bears north

23° 28´ from the zenith at noon from places on the equator.

At the north pole, since its appearance on the horizon on March 21st,

the sun has mounted to an altitude of 23° 28´ and to nearly 67° at

places on the Arctic circle. The earth’s northern axis is, in this

position, inclined 23° 28´ directly toward the sun, which pours its

rays continuously upon the northern regions, uninterrupted even by

the earth’s daily rotation. It is on this day that the whole Arctic

zone enjoys the full glory of the midnight sun. The earth’s continuous

movement of revolution does not allow a delay of this favorable season

in northern latitudes, but continues to make the sun’s vertical rays

follow the terrestrial ecliptic as before on its way toward the

intersection with the equator 90° away. On this leg of the journey, the

sun is traveling on the upper one of two converging lines and thereby

gradually lessening its distance from the other--the equator--or, in

other words, reducing its declination. This continues until September

21st when the autumnal equinox is reached and the sun’s declination

becomes 0°. The sun now being overhead at the intersection of the

equator and the terrestrial ecliptic, is on the opposite side of the

earth from the intersection of March 21st. In fact the conditions are

similar, but now the earth is on the opposite side of the sun, and

the change of seasons is the entrance of spring for the dwellers in

southern latitudes.

The sun has dropped lower and lower in the sky at the north pole since

June, until on this day it is in the horizon and it is time for the

Esquimos to seek their igloos and prepare to hibernate during the long

Arctic night now ushered in.

The sunshine at the time of the equinoxes is equally distributed over

the northern and southern zones, and the zenith distance of the sun

at noon at any place is, theoretically, equal to the latitude of the

place (except a small error due to change of declination accumulated

subsequent, or previous, to the instant of the equinox).

The conditions during the next six months are reversed as the earth

proceeds into that half of the orbit containing the perihelion. Now the

sun following the terrestrial ecliptic enters southern latitudes or

south declination, for in this part of the orbit the equator is above

(or north) the plane of the ecliptic. The sun’s diverging course from

the equator leads it farther and farther southward until on or about

December 21st it arrives at the winter solstice with a culmination of

23° 28´ south declination. At this point the earth is but a few degrees

from the perihelion as it was from the aphelion at the summer solstice.

The earth’s north pole is now inclined directly away from the sun and

its rays have entirely forsaken the Arctic for the Antarctic zone;

notwithstanding the earth’s daily rotation, which brings alternating

light and darkness to the greater part of the world, the northern polar

regions are in a continuous shadow, and no sunlight reaches these

remote parts. At this time of the year the northern hemisphere above

the tropic of Cancer, is in an unfavorable position relative to the

sun, and as a result places situated on parallels less remote than the

Arctic are having long nights and short days in proportion to their

latitude north. On the other hand, in the southern hemisphere the days

are longer and the nights shorter, as the southern latitude increases

until at the Antarctic circle night disappears and the sunshine is

uninterrupted. It is seen that this is an exact reversal of the

conditions at the summer solstice.

The earth enters the last quadrant of the great ellipse of its orbit,

the sun now approaches the equator as the earth nears the vernal

equinox. The south declination diminishes until on March 21st it

becomes 0° and the earth has completed its revolution. We will now

go on another tack and instead of considering only the effects of

declination due to the earth’s revolution, will assume that the earth

has been halted in its onward course of revolution and is making its

daily rotation in the same position. The earth turning from west to

east causes the sun to appear to proceed from east to west in its

diurnal motion. Each rotation, requiring 24 hours, marks upon the

earth a circle of overhead positions parallel to the equator and

hence without change of declination. The result of such a remarkable

condition would be, no change of seasons and no change in the length

of the days and nights. In reality, however, we are saved from such

monotony, for both the motion of rotation and revolution of the earth

are acting together and giving a compound effect on the apparent

movements of the sun. This alters the daily circles just mentioned to

a fine spiral of overhead positions, ever changing in declination. The

daily difference of the sun’s declination shown in the Nautical Almanac

is equivalent to the distance between two threads of this spiral.

The change of declination is most directly seen and felt in the polar

regions, where the activities of the denizens are mostly limited to

the favorable phases of this change. At the north pole, after the sun

has appeared above the horizon, this spiral of declination can be

continuously followed. The sextant will disclose a constant increase

in altitude as the sun circles round and round the sky, winding itself

up and finally culminating at 23° 28´. The process is then immediately

reversed. The stars here make daily circles of _equal_ altitudes as

their change of declination is insignificant; but the circles of the

planets and the moon are converted into spirals, the fineness of which

is in proportion to the rate of their change of declination.

The fact that the sun reaches an altitude of 23° 28´ at the pole at

the summer solstice with its declination of a like amount and that on

March 21st, when the sun is in the horizon with the altitude 0°, it is

directly over the equator with 0° declination, shows that at this place

(the pole) the altitude is equal to the declination. Should an explorer

travel southward 1°, his sextant would show an altitude 1° greater

than at the pole, yet moving about does not affect the declination at

a given time. It follows by taking his altitude at noon the explorer

in the polar regions may readily learn his distance from the pole by

subtracting the declination in the Nautical Almanac from his sextant

reading.

It may not generally be known that the southern summer is shorter

than the summer of the northern hemisphere, but such is the case by

approximately eight days. The reason of this inequality lies in the

fact that the sun is nearer one end of the orbital ellipse, and the

short diameter passing through this body divides the orbit into unequal

parts. The smaller part being that traveled by the earth during the

_southern_ summer. Furthermore the nearer proximity of the sun causes

an accelerated motion which further tends to lessen the time spent by

the earth in this part of the orbit.

RIGHT ASCENSION

Declination and right ascension being used together as coordinates,

we will not separate them. It will be remembered that the equator

and the terrestrial ecliptic cross each other on opposite sides of

the earth; that on or about March 21, the sun is overhead at the

intersection that is the vernal equinox. Now if at this intersection

on this day a plumb-line were carried upward, it would at length reach

the sun, and continued to infinity and projected on the celestial

sphere would locate a point called the celestial vernal equinox, known

by many as the First Point of Aries. This point is one of the most

important celestial “landmarks” used in astronomy and navigation,

but, unfortunately, no heavenly body marks its place. However, as its

relative position among the neighboring stars is well known, its exact

location is easily ascertained.

The hour circle which passes through this point is known as the

equinoctial colure, and may be considered the prime meridian of the

heavens, for from it is measured the right ascension of all bodies.

Right ascension of a body is the angle at the celestial pole between

this meridian of reference and the hour circle passing through the

body. It is always measured eastward through 24 hours of sidereal time

(360°). The angle is measured by the arc intercepted on the celestial

equator. For example, a star 15° east of the equinoctial colure has a

right ascension of 1 hour or 15°, but, if the star is 15° west, its

right ascension is 23 hours or 345°.

The positions of heavenly bodies are defined by right ascension and

declination exactly as positions upon the earth are expressed by

longitude and latitude, right ascension corresponding to longitude and

declination to latitude.

In the discussion of Time, to follow, more facts concerning right

ascension will be found.

PRECESSION OF THE EQUINOXES

A comparison of the present positions of the fixed stars with their

places as recorded in ancient times shows a great discrepancy. The

celestial latitudes, which were reckoned from the ecliptic, show no

appreciable change; but in the declinations and right ascensions

there is a great departure from the old positions. The error of right

ascension was found by the old Greek astronomer, Hipparchus, to appear

as a uniform eastward movement of all the stars, which led him to

reason that, instead of the stars themselves changing, their point of

reference was moving westward, thus lengthening all right ascensions.

The famous astronomer after further reasoning decided that the

position of the celestial pole was changing, in fact that the line of

the earth’s axis was describing a circle on the heavens, which was

left-handed or against the hands of a watch as viewed from the north

pole of the earth. This movement was found to be extremely slow,

requiring 25,800 years to complete the circle which has as its radius

the amount of the inclination of the earth’s axis--23° 28´.

If a match is put through a piece of cardboard about the size of a half

dollar to the distance of ¼ inch, and spun, the motion of the cardboard

just as it staggers through loss of speed, gives some idea, although

exaggerated, of the precession movement of the plane of the equator,

which is of course infinitely slower. The movement of the top of the

match is a semblance of the corresponding motion of the vanishing point

of the axis on the celestial sphere.

The earth, as already explained, points its axis at practically the

same spot in the heavens throughout the year, and if it were not for

this annual precession of 50´´ it would for all intents and purposes

hold a permanent direction. About December 21, the winter solstice,

while the earth is still some degrees from the perihelion, its northern

axis, is inclined directly away from the sun. Each year this distance

from the perihelion is becoming greater, widening this angle between

the direction of the axis, projected on the plane of the orbit, and

the major diameter of the orbit, until in time the north pole will be

headed directly away from the sun in that part of the orbit which the

earth now occupies in September, and so on.

[Illustration: This diagram shows the successive positions of the earth

at the Vernal Equinox (March 21st) due to the revolution of the axis

and the consequent westward movement of the First Point of Aries.

FIG. 1.]

In the year A.D. 1250 the winter solstice occurred at perihelion and in

the year 6400 A.D. the vernal equinox will occur at this point of the

orbit. That is, the axis of the earth was inclined directly away from

the sun at perihelion in the former year but in the latter year the

inclination will have changed about 90° backward against the earth’s

course about the sun, and it will be the beginning of spring (the

vernal equinox) when the earth is at perihelion instead of the first of

winter as in 1250 A.D. Since 1250 A.D. the inclination has changed an

equivalent of about 11 days for now the earth is at perihelion about

January 1st, and the solstice occurring about December 21st, shows the

present relative situation.

In other words, the vernal equinox is slipping back in the orbit

towards the perihelion, and as the solstices maintain their positions

at 90° from the equinoxes they must likewise be “slipping a cog” each

year.

The vernal equinox was situated many centuries ago in the first part of

the constellation of Aries, and was known as the First Point of Aries,

but owing to the movement of precession it has dropped back or westward

(as we face our southern horizon) 50´´ a year until it has left that

constellation entirely and is now about leaving the constellation

of Pisces, some 30° from the position used by Hipparchus in his

calculations. The majority of navigators still call this point of the

celestial vernal equinox the First Point of Aries.

Holding these facts in mind, it may be clear that as the earth

approaches that part of the orbit where the vernal equinox occurs it

has turned its pole, and correspondingly points on the equator, 50´´

to the right or west during the year; thus causing the point of the

terrestrial equinox to meet (or come under) the sun that much sooner.

In other words, referring to the effect as seen on the heavens, the

celestial equinox was advanced to the westward that much to meet

the sun in its eastward movement among the stars and will become the

nearest point to the sun, 50´´ before the position of the equinox

of last year. As the points in the orbit where the vernal equinox

occurs year by year works back toward the perihelion, the range line

through the sun to the heavens beyond must each year correspondingly

edge its way westward along the celestial ecliptic through different

constellations. This is what is known as the precession of the

equinoxes.

The course of the celestial pole in the heavens is shown by a circle

drawn about the pole of the ecliptic using 23° 28´ as a radius. This

path will pass 1¼° from our pole star and this position marks the

present termination of our extended axis; half way around the circle it

passes the first magnitude star Vega close aboard, thus making this the

future pole star some 12,000 years hence. If there be such creatures as

navigators in those far-away days, latitude by Vega will no doubt be a

popular sight among them.

The cause of this remarkable movement of the earth is due to the fact

that the earth is not a true sphere, and the influence of the sun is

not exerted equally upon its mass. Its flattening at the poles is

attended by a corresponding bulging along the equatorial belt. When

the earth is in the vicinity of the perihelion, leaning away from the

sun, the half of this ring of extra matter on the side towards the

sun is above the plane of the ecliptic or orbit. The tendency of the

added attraction exerted upon it, is to draw the earth to an upright

position, or in other words, at this time the sun is pulling stronger

on the northern or upper side than on the lower. Again, when near the

aphelion and summer solstice, leaning towards the sun, that part of the

ring of extra matter on the side towards the sun is below the level of

the orbit, and the attraction is again tending as before to pull the

earth upright. At the equinoxes there is an equal amount of this extra

matter above and below the plane of the orbit evenly distributing the

attraction.

The effect of this influence would in time bring the earth’s equator

and the plane of the ecliptic into coincidence and the earth’s pole

would be directly beneath the pole of the ecliptic, were it not for

its rotation. The two forces acting upon the earth result in the slow

revolution of the axis. The exact effect of these forces is rather

complex but it is a demonstration of the principle of the gyroscope.

The movement of the axis is affected very slightly by other influences

than that of the sun, the most notable of which is the moon, whose

monthly revolutions around the earth produce a similar influence in the

bulging mass within the tropics, but as its revolutions are so rapid,

it has but a slight effect on the precession movement of the earth.

It is sufficient, however, to cause the extended axis to nod slightly

and make a waved circle of precession on the heavens. This is called

“Nutation,” from the Latin word _nuto_, meaning to nod.

The whys and wherefores of navigation · 第 3 / 11 章