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willingly. 21. Willing or not willing, he shall go away. 22. Will you keep my secret ? 23. I will keep it. 24. He changes his opinion with every event.

EXERCISE 170 (Vol. III., page 221).

1. Se mariera-t-il contre le gré de son père? 2. Il ne se mariera pas contre le gré de ses parents. 3. Pourquoi me savez-vous mauvais gré ? 4. Je ne vous sais point mauvais gré. 5. La chevelure de votre petite fille est-elle nouée ? 6. Elle n'est pas nouée, elle flotte au gré du vent. 7. Que pensez-vous de mon livre ? 8. C'est à mon gré le meilleur livre que j'aie lu. 9. Ne me saurez-vous pas mauvais gré, si je ne viens pas aujourd'hui ? 10. Je ne vous en saurai pas mauvais gré. 11. Ne lirez-vous pas cette lettre ? 12. Quelque bien écrite qu'elle soit, je ne la lirai pas. 13. Ces dames sont-elles belles? 14. Quelque belles et bonnes qu'elles soient, elles ne sont pas à mon gré. 15. Etes-vous faché contre mon frère ? 16. Non, Monsieur; je lui sais bon gré de ses intentions, quelles que soient les suites de sa conduite. 17. Me garderez-vous le secret ? 18. Je vous le garderai de bon gré. 19. Votre sœur garde-t-elle le lit de bon gré ? 20. Elle ne garde pas la chambre de bon gré. 21. Bon gré, mal gré, il faut qu'elle garde la chambre quand elle est malade. 22. Garderez-vous le secret sur ce point? 23. Je le garderai de bon gré. 24. Je vous sais bon gré de vos bonnes intentions. 25. Lui savez-vous bon gré de cela ? 26. Je lui en sais bon gré. 27. Le juge gardera-t-il son domestique ? 28. Il le gardera. 29. Fait-il son travail à son gré? 30. Il le fait à son gré. 31. M. votre frère est-il obligé de garder la maison? 32. Il est obligé de garder le lit. 33. N'a-t-il pas quitté sa chambre? 34. Il n'a pas encore quitté sa chambre; il est trop malade pour la quitter. 35. Je vous saurais le meilleur gré du monde, si vous

vouliez le faire.

EXERCISE 171 (Vol. III., page 221).

1. Sir, to what shall I have the pleasure of helping you? 2. I wiH ask you for a slice of that ham. 3. Have the goodness to help those gentlemen. 4. I will thank you for a slice of that boiled meat. 5. Shall I offer you a slice of that roast meat? 6. I am much obliged to you, Sir; I have enough. 7. Miss, shall I have the honour of would helping you to a wing of this partridge? 8. I thank you, Sir; prefer one of those ortolans. 9. Sir, shall I send you soup? Madam, have the goodness to help this young lady. 11. I will ask you for a little afterwards. 12. John, present this cutlet to that gentleman. 13. These vegetables are delicious. 14. Sir, I am very glad that you find them good. 15. Sir, will you not sit down? 16. I am exceedingly obliged to you, Sir, my father is waiting for me at home. 17. Have you not wished them good morning? 18. I have wished them good evening. 19. Have you bid them adieu ? 20. I have bid my brother adieu. 21. I have taken leave of them. Have you desired them to walk in ? 23. I have. 24. Gentlemen, the dinner is on the table. 25. Have the goodness to sit here,

EXERCISE 172 (Vol. III., page 221).

of a father towards you? 21. He has been to me a father and mother. 22. Will you look more closely into this affair? 23. No, Sir; I will be satisfied with what I know of it. 24. Is not that physician tenacious of his opinion? 25. He cares more about it than about the life of his patients.

PLANE TRIGONOMETRY.-III.

SOLUTION OF RIGHT-ANGLED TRIANGLES-FUNDAMENTAL

PRINCIPLES, ETC.

X. Solution of Right-angled Triangles.-Every triangle con sists of six "elements," three sides and three angles. Any three of these being given, including at least one side (this is necessary, because triangles merely equiangular can be con structed in infinite number), Trigonometry enables us to calcu late the remaining elements. The formulæ evolved as yet only enable us to do this for right-angled triangles, and as these involve one known quantity (the right angle), it is sufficient if any two of the other elements (including one side) be given. We may have (referring to Fig. 3), besides the right angle(1.) Given two sides.

(2.) Given one side and one angle.

Either of these cases may be solved by the ratios given in Section II., and by a table of natural sines and cosines, tangents and cotangents, such as that given at the end of Galbraith and Haughton's "Trigonometry." The following examples may all be solved by the annexed table of ratios for a few angles only, purposely restricted to three places of decimals:

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0.485

0.554

61°

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22.

1. Madame, que vous servirai-je ? 2. Je vous demanderai une tranche de ce jambon. 3. Vous enverrai-je une aile de cette volaille ? 4. Non, je vous remercie, Monsieur. 5. S'il vous plait, Monsieur. 6. Monsieur, aurai-je le plaisir de vous servir une tranche de ce jambon ? 7. Je vous remercie, Monsieur, je prendrai de préférence un morceau de la perdrix. 8. Vous offrirai-je un petit morceau de ce bouilli ? Je vous remercie, Monsieur; j'en ai suffisamment. 10. Madame, vous enverrai-je un peu de potage ? 11. Mille remerciments, Monsieur. 12. Monsieur, oserai-je vous prier de servir mademoiselle ? 13. Avec beaucoup de plaisir, Monsieur. 14. Jean, présentez cette soupe à

9.

monsieur. 15. Ces ortolans sont délicieux. 16. Je suis bien aise

que vous les trouviez bons. 17. A-t-on servi? 18. Non, Monsieur; on n'a pas encore servi. 19. Il est trop tôt. 20. Vous plait-il d'y aller? 21. Il ne me plait pas d'aller chez lui, mais j'irai si vous le désirez. 22. Irai-je avec vous? 23. Comme il vous plaira. 24. Votre ami ne veut-il pas s'asseoir ? 25. Il vous est fort obligé; il n'a pas le temps aujourd'hui. 26. Avez-vous souhaité le bonjour à votre ami ? 27. Je lui ai souhaité le bonsoir. 28. Ne lui avez-vous pas dit adieu ? 29. Je lui ai dit adieu. 30. Ayez la complaisance de vous mettre ici. 31. J'ai pris congé d'eux. 32. J'ai pris congé de tous mes amis.

EXERCISE 173 (Vol. III., page 270).

......

of Angles in Column IL

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a tan. B=100 x 727=72·7;

A 90° B = 54°.

b

Since tan. B:

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1. What hotel does your brother keep? 2. He keeps the hotel of Europe, street. 3. Does your little boy keep himself very clean? 4. He keeps himself very clean. 5. What will be your decision ? 6. I will abide by what I have told you. 7. Do you not know what to decide ? 8. I know perfectly what to decide. 9. Why do you remain standing? 10. Because we have no time to sit down. 11. Have you not forbidden those young men to use such language? 12. 15°. Find B, a and b. I have forbidden them. 13. Has not your coachman used very tusolent language? 14. Are you not afraid of getting a cold, by keeping the doors open? 15. We would prefer keeping them shut. 16. Does your master recommend you to keep your head upright? 17. He recommends me to keep my feet outwards. 18. Why does not your friend keep your company? 19. His sister is indisposed; he is obliged to remain with her. 20. Has not your uncle filled the place

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10. A house 50 feet high abuts upon a street found to measure 33.7 feet in width. Find the length of ladder required to reach the top from the opposite side of the street, and the angle the ladder will make with the wall of the house.

11. Two trains travelling, one at 20 miles an hour, the other faster, come into collision at a level crossing, where the two lines (both being free from curves) cross each other at an angle of 36°. Some time before the collision, a passenger in the slower train observes the other exactly abreast of him on the other line of railway, and judges the trains to be a quarter of a mile apart. How far from the crossing were both trains at that moment, and what was the speed of the faster train?

12. One of two boys, flying a kite in a level field, observes that he has let out the whole of his string-60 yards-just as his companion, looking up, cries out that the kite flies perpendicularly over his head. The boys found afterwards they were standing 30 yards apart. How high was the kite, and what angle did the string make with the ground? 13. The rope holding the "captive balloon "at Chelsea against a strong wind, when 400 yards were paid out, was found to incline 15° from the perpendicular. How high was the balloon, and how far from the foot of the rope would a piece of iron ballast have fallen, if dropped from the balloon ?

XI. The Fundamental Formula.-We have hitherto examined only the relations between ratios of the same angle; we proceed now to trace the relations between ratios of two or more different angles. The number of formulæ expressing these relations may be extended almost at will, but they are all derived from the following formulæ for the sines and cosines of the sum and difference of two angles, known, therefore, as the four fundamental formulæ :—

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Sin. (A + B) = sin. A cos. B + cos. A sin. B...... (33) Sin. (AB): sin. A cos. B cos. A sin. B. (34) Cos. (A+B) = cos. A cos. B sin. A sin. B...... (35) Cos. (AB) = cos. A cos. B + sin. A sin. B...... (36)

where A and B are any angles whatever.

These formulæ may be thus expressed in words :

(33) The sine of the sum of two angles is equal to the sine of the first into the cosine of the second plus the cosine of the first into the sine of the second.

(34) The sine of the difference of two angles is equal to the sine of the first into the cosine of the second minus the cosine of the first into the sine of the second.

(35) The cosine of the sum of two angles is equal to the product of their cosines minus the product of their sines.

(36) The cosine of the difference of two angles is equal to the product of their cosines plus the product of their sines.

To prove (33).-In Fig. 8 let A O B = A, and BOC B; then

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To prove (34).-Let A O B (Fig. 9)= A, and BOC B; then AOC A B.

In o c take any point P, and draw the perpendiculars PQ, P R, and R 8, RT, as before (RT to P Q produced).

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Fig. 9.

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Again, prove (34), where A is a trigonometrical angle in the fourth quadrant, B an angle in the second quadrant, and their difference an angle in the third quadrant.

=

Let A O B in Fig. 11 = A, and BOC B; .'. A o c (A - B). Construct as before

=

S

Fig. 11.

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EXERCISE 3.

1. Prove (33), where A is an angle in the third, and B an angle in Angles.-Dividing (33) by (35), we have—

XIV. Relations between Sines, Cosines, and Tangents of two

the first quadrant, but where A + B reaches to the fourth quadrant.
2. Prove the same where both A and A + B are in the third quad-
rant (which, of course, implies that B is less than a right angle).

3. Prove (34), when A exceeds 180°, but is less than 270°, and
when B exceeds 90°, but is less than 180°.
on the supposition that A is so near 270°, and
180°, that AB falls in the second quadrant.
that AB shall be less than 90°.

Construct the figure
B so much less than
Also construct it so

4. Prove (34), when A is an angle in the fifth quadrant, and when B=180°. In this example AO в must, of course, be drawn as an angle in the first quadrant, and since Boc= 180°, BO and oc are in line with each other. PQ is therefore the only other line in the construction before given which it is possible to draw. A-B the (trigonometrical) angle A D C in the third quadrant.

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Tan. (A+B) =

sin. A cos. B + cos. A sin. B
cos. A cos. B

sin. A sin. B

Dividing both numerator and denominator on the right-hand side by cos. A cos. B, we have

Tan. (A+B)=

sin. A Cos. A

sin. B

+

cos. B

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Similarly, dividing (34) by (36), and again dividing the nume rator and denominator by cos. A cos. B, we obtaintan. A tan. B Tan. (AB) = 1+tan. A tan. B

=

(46)

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Again, dividing (41) by (42), we obtain-
Sin. Asin. B 2 sin. (A+B)

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To prove (36) :

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tan. (A + B) cot. (AB);

.. since cot. (A B)

tan. (A B)'

sin. Asin. B tan. (A+B)
sin. A

Or, the sum of the sines of two angles is to the difference of their sines as the tangent of half their sum is to the tangent of half their difference.

Similarly, by dividing (43) by (44)——

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XV. Formula for the Ratios of the Sum of three Angles may be obtained simply by splitting up the three into two, which can then be dealt with by formulæ already given; thusSin. (A+B+C) = sin. (A + (B+C))

= sin. A. cos. (B+ C) + cos. A. sin. (B+ C)

sin. A (cos. B cos. C sin. B sin. C) + cos. A (sin. B cos. C +cos. B sin. C).

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=

2 sin. A sin. B... (40)

Cos. (A+B) + cos. (AB) = 2 cos. A cos. B...... (39) Cos. (A+B+ C) = cos. A cos. B cos. C cos. A sin. B)
(50)
sin. C- cos. B sin. A sin. C cos. C sin. A sin. B
Dividing (49) by (50), and the numerator and denominator of
the fraction thus obtained by cos. A cos. B cos. C, we obtain

(51

Cos. (A+B) cos. (AB)

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XVI. Formula for the Ratios of the Multiples of an Angle.Substituting A for B in (33), we have

Sin. (AA) sin. A cos. A + cos. A sin. A ; .. sin. 2A = 2 sin. A cos. A.

Adding these results together, we get

Sin. Asin. B = 2 sin.

Or, subtracting one from the other

Similarly, by adding and subtracting like expressions for

By (7), 1 sin. A+ cos.2 A; adding this to (53)-
Cos. 2A 2 cos. A 1.......

=

(52

Similarly, by (35), cos.

(A+A) = cos. A cos. A sin. A .. cos. 2A= cos.2 A

sin. A sin. A

(53

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Subtracting (7) from (53)—

Cos. 2A 1 2 sin. A..... Again, substituting A for B in (45), we have2 tan. A

cos. A and cos. B, we get

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(57)

3 cos. A...... (58)
3 tan. A tan.3 A
1-3 tan. A

perceive that the field of view is covered with points of light, and the number of these telescopic stars is found to be immensely greater than that of those visible to the naked eye. These stars are classed into magnitudes down to the fifteenth and sixteenth, or even lower, according to the power of the telescope required to show them. The total number down to the fourteenth magnitude is estimated at 20,000,000. The question now suggests itself whether these different degrees of brightness result from differences in the size of the stars, or in their distances. To this we cannot give an answer with absolute certainty, as there are only a few stars whose distances have been measured. There appears, however, to be little doubt that the difference is chiefly in their distances. The stars, instead of being ranged in a sphere around us, as at first sight they seem to be, are scattered through boundless space, and placed at varying distances from us and from one another. They (60) are all likewise in motion round the centre of gravity of the whole cluster.

(59) XVII. Formula for the Ratios of an Angle in terms of the Ratios of the Sub-multiples of that Angle.-Substituting A for 2A on the left-hand side of (52) to (56), and therefore for A on the right-hand side, we have

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A

(61)

(62)

(63)

From (57), (58), and (59), like formulæ may be obtained, by like means, for sin. A, cos. A, tan. A, in terms of the same ratios ofa. The student should do this for himself.

3

The distances of the stars are ascertained in the same manner as those of the Sun and planets-that is, by parallax. Instead, however, of taking two stations at different parts of the Earth's surface, and laying down a base line between them, we take the diameter of the Earth's orbit, or 183,000,000 miles, as the base, the observations being taken at intervals of six months.

Even with this immense line, however, the parallax is so small that it can only be detected by the most careful observa(64) tions and accurate instruments. In no case has it been found to be greater than 1"; and if this be its value, the distance of the star must be 206,000 times as great as that of the Sun. The parallax of about a dozen stars has now been ascertained, and is found to vary between 0.919" and 0.046". The star a Centauri is the nearest to the Earth, and its distance is estimated at 20,496,000,000,000, or more than 20 billions of miles; while the average distance of stars of the first magnitude is probably three or four times as great as this. These figures, however, fail to convey to the mind any definite idea as to the real distance; perhaps the best mode of expressing it is by stating that light, with its speed of 184,000 miles a second, takes 34 years to travel from that star to us; while the smaller telescopic stars are so remote that it must require upwards of 5,000 years for their light to reach us.

In this lesson have been given those formulæ most likely to occur in after-practice. The student should not be content with reading the demonstrations, but should in every case write them out as he follows the proof, inserting any intermediate steps which, from their simple character, may have been omitted to save space. He should also arrange new formula for himself, as may be done to any extent by simple substitutions, or by additions, subtractions, and divisions of formulæ already given.

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WE must now turn our attention from the planets to the fixed tars which so thickly stud the sky. It is very difficult by mere pection to form any estimate of the number of these bodies; it appears, however, from catalogues which have been compiled, at the total number visible to the naked eye is about 6,000. Only half of the sky, however, can be seen at one time, and the aber visible on a clear night may therefore be set down ghly at 3,000. These stars vary very greatly in brilliancy ad apparent size, and have accordingly been divided into six classes, the brightest being said to be of the first magnitude, la the faintest visible to the naked eye are classed as the ith, the rest being divided into the remaining four magnitudes. As a general rule, it is computed that stars of the first magniare about 100 times as brilliant as those of the sixth. The ht of Sirius, the brightest star in the sky, is, however, estimated to be equal to that of 324 of the latter.

If

Though the number of stars seen by the naked eye is thus hmited, we must not suppose that these are all that exist. We direct a telescope to any part of the sky, we shall at once

The rays by which we now see these stars must have left them soon after the creation of Adam; and, for aught we know, At the some of them may for ages have ceased to exist. contemplation of these things, however, the mind is altogether lost in wonder; we are verging on the infinite, and are led to feel that this planet is indeed but a minute speck in the immensity of creation.

In studying the stars we need some mode of identifying them, and in this there is some little difficulty. Special names have been assigned to many of the more brilliant ones, but these have a tendency to confuse. At a very early period they were divided into constellations; many new ones have since been added, so as to make in all 109. Several of these, however, are very small and unimportant, and hence are rejected by some astronomers. In 1604, a German astronomer, named Bayer, published a celestial atlas in which he designated the stars in each constellation by the letters of the Greek alphabet, the brightest being called a, the next B, and so on. This plan was found to answer so well that it has been continued to the present time. In some constellations, however, the number of stars now catalogued is so great that more letters are required to denote them; the English alphabet therefore follows the Greek, and if both prove insufficient, the remaining stars are denoted by numbers.

In a few instances the stars are not arranged quite in the order of brightness, either from want of accuracy in Bayer's observations, or from a change in the light of the star since his time; it is considered better, however, not to attempt to amend this, as it would only produce confusion.

The best plan for the student to become practically familiar
with the different constellations is to study the sky itself, with the
aid of some maps or of a globe. Several of the constellations-
as, for instance, the Pleiades, the V-shaped cluster of the
Hyades, and Orion (Fig. 43), with the three stars in the !
commonly known as the Yard Measure-are familiar t
every one; these will serve as a guide in determining

The stars are all of them bright, self-luminous bodic
Sun, which in all probability appears to other worlds t

of the stars. Delicate observations show us that they have proper motions, but it is very ifficult to determine these. We can, however, ascertain the motion of the Sun by observing the relative distances of the stars. We find that in one part of the sky the stars seem to be very gradually opening out, and getting further apart, while in the opposite quarter they are as gradually closing up, evidently showing that we are moving towards the former part, just as when we are travelling in a wood the trees in front seem opening out, while those we have passed appear to be getting closer together.

Astronomers have naturally been anxious to ascertain something of the shape of the whole cluster of stars which constitutes our

system, and have employed the telescope as a sounding-line to learn the depth in different directions. If the stars are scattered at all uniformly in space, they will, of course, appear more sparse in those parts where we look through the thinnest layer of them. Now when we observe the sky on a clear night, we at once notice a pale belt passing round it, commonly known as the Milky Way. In one part of its course it divides into two branches, which, after separating a little way, and passing about a third round the sky, again unite into Powerful telescopes show us that this consists of a dense mass of minute stars. The greater portion, indeed, of those visible are clustered along this line, while in those parts of the sky removed from it the number of telescopic stars is comparatively small; hence we may reasonably assume that this belt indicates to us the direction in which the greatest number of the stars lie, and in which our cluster extends furthest.

one.

From this we may form an idea of our system, and it seems that the best representation of it may be obtained by taking a flat circular body-as, for example, a cheese and splitting it by passing a knife about one-third of the way through, the two parts being made to diverge a little, as shown at a, b (Fig. 44). The Sun, (s) is situated somewhere near the centre, and the split side causes the divided appearance of the Milky Way. One of the nebulæ, when seen through a powerful telescope, is found to present a somewhat similar appearance, and is considered to be a cluster closely resembling our own.

they happened to lie in a straight line directed almost towards the Earth; that they were, in fact, merely optical couples, one being an immense distance behind the other. After many

observations, Herschel found that their distances and relative positions did vary, but instead of it being, as he expected, an annual fluctuation caused by the Earth's motion, it was a progressive change. He thus found that in some cases the two stars were revolving round one another in elliptical orbits, and that they were physical couples, the two forming one system. These he called binary stars or couples, to distinguish them from optical pairs. Other observers have followed up these investiga tions, and there are now upwards of 600 binary stars known and noted, and in many cases their times of revolution have been calculated. One of the best examples of this class is afforded by e Lyra, which is sometimes called the Double-double Star. To the naked

eye it appears a somewhat faint star, but a telescope of very little power will show it to be double. When, however, a more powerful instrument is employed, each of tl.ese components is in turn found to consist of two smaller ones, as shown in Fig. 45. The lower pair revolves in about 2,000 years, and the upper in about half that time, while the two couples take a very long period to revolve around their common centre of gravity.

One remarkable feature in connection with the double stars is the fact that in some instances the component stars are of different colours. In R Leporis, for instance, one is white, while the other is a deep red; in 8 Cygni again, the colours are yellow and blue; and in y Andromeda, they are orange and green.

When we come to note the colour of different stars, and compare it with former records, we find that in a few instances a change has taken place. Thus Sirius, which now shines with a pure white light, is spoken of by old observers as a ruddy star. There are also many others which exhibit changes in brilliancy, and these changes seem, in most cases, to be periodical. The star on which this discovery was made is o Ceti, called also Mira, or the Wonderful Star, a name it well deserves. At the time of its greatest brightness it is usually of the first or second magnitude, it then decreases for two or three months,

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Fig. 43. THE CONSTELLATION ORION.

When we look at the heavens on a clear night, we observe here and there two stars in very close proximity: the telescope further reveals to us that very many of these which appear to the naked eye as single stars, consist in reality of two or more so close together that they ap. pear as one. Sir W. Herschel was the first to direct specialattention to these objects, of which he compiled a list. He hoped that by very accurate measurements of the apparent distances between them, he might be able in some instances to detect a variation, and thus ascertain their parallax, and by that their distances. The idea then was that these stars merely appeared close together because

till it becomes invisible, and remains so for about five months, its minimum brightness being about equal to that of a twelfth magnitude star. It then again appears, and the whole period occupied by these changes is about 331 days.

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Algol, or B Persei, is another variable star, remarkable for its short period and rapid changes. It ordinarily appears as a star of the second magnitude, but in a period of three and a half hours it diminishes in brightness to the fourth magnitude, and after a few minutes begins again to increase, attaining its former brilliancy in another period of three and a half hours. At this it remains two days thirteen hours, and then the same series of changes recurs.

Fig. 44.-SECTION OF THE MILKY WAY.

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