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<v Speaker 1>Section twenty seven of Sun, Moon and Stars Astronomy for Beginners.

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<v Speaker 1>This is a LibriVox recording. All LibriVox recordings are in

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<v Speaker 1>the public domain. For more information or to volunteer, please

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<v Speaker 1>visit LibriVox dot org. Read by Jennifer beckett Wood Sun

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<v Speaker 1>Moon and Stars Astronomy for Beginners by Agnes Giburne, Reading

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<v Speaker 1>the Light, God said let there be light, And there

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<v Speaker 1>was light Genesis one three. Many times in the course

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<v Speaker 1>of this little book, mention has been made of an

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<v Speaker 1>instrument called the spectroscope, to which much of our present

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<v Speaker 1>knowledge of the heavens is due. The subject of spectrum

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<v Speaker 1>analysis is too complex to be fully discussed in a

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<v Speaker 1>volume of this kind, but a few words of explanation

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<v Speaker 1>may be desirable. By means of the spectroscope, we know

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<v Speaker 1>with almost certainty many of the substances which are contained

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<v Speaker 1>in the Sun, in the stars, in nebulae. How large,

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<v Speaker 1>or how far away, or how quickly moving some of

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<v Speaker 1>the heavenly bodies are, could be discovered through the telescope

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<v Speaker 1>without help from the spectroscope. But the actual make of

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<v Speaker 1>them lay, until recent years beyond our grasp, not upon

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<v Speaker 1>Earth alone, but also in the Sun. Exist iron and sodium,

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<v Speaker 1>copper and zinc, magnesium, cobalt, and many other substances with

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<v Speaker 1>which we are familiar, notably hydrogen. Every metal may be

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<v Speaker 1>either in the solid or in the liquid, or in

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<v Speaker 1>the vapor form. Iron, as we commonly see it, is solid.

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<v Speaker 1>In other words, it is frozen like ice. Most metals

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<v Speaker 1>freeze at a much lower temperature than water does. Just

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<v Speaker 1>as a certain increase of heat will turn ice into water,

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<v Speaker 1>so a certain increase of heat will transform solid iron

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<v Speaker 1>into liquid iron. And just as yet greater heat will

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<v Speaker 1>turn water into steam, so very much greater heat will

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<v Speaker 1>transform liquid iron into vapor of iron or iron gas.

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<v Speaker 1>A little heat will do for ice what immense heat

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<v Speaker 1>will do for iron. The intense heat of the Sun

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<v Speaker 1>causes metals which are solid upon Earth to float as

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<v Speaker 1>glowing vapor in the solar atmosphere. Indeed, that dense and

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<v Speaker 1>far reaching atmosphere is largely composed of such metals. Whether

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<v Speaker 1>iron and other earthly metals can be found anywhere in

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<v Speaker 1>or near the sun in anything approaching to a solid

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<v Speaker 1>form is more than doubtful. But in the photosphere they

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<v Speaker 1>probably do exist, in a shape ordering on the liquid form,

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<v Speaker 1>where glowing clouds appear to float formed of condensed and

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<v Speaker 1>radiant metals. This state would answer not to the liquid

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<v Speaker 1>waters of a river, but to the condensed water droplets

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<v Speaker 1>of a fog or cloud. Spectrum analysis, beside teaching us

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<v Speaker 1>what metals may be found in the sun, has also

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<v Speaker 1>a word to say about those which exist in some

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<v Speaker 1>of the stars far distant as those sums of light are.

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<v Speaker 1>We know that in them, too are such earthly materials

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<v Speaker 1>as iron, sodium, magnesium, and a variety of kindred substances,

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<v Speaker 1>while in many of them hydrogen predominates. But how can

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<v Speaker 1>we know all this? How could the wildest guessing grow

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<v Speaker 1>to more than a guess and reveal to us the

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<v Speaker 1>actual presence in even our own particular sun of iron

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<v Speaker 1>or hydrogen, not to speak of more diday distant suns.

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<v Speaker 1>We know it by means of spectrum analysis. The spectroscope

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<v Speaker 1>may be looked upon as twin sister to the telescope.

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<v Speaker 1>A telescope gathers together widely scattered rays of light into

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<v Speaker 1>a spot or focus for our use. The spectroscope separates

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<v Speaker 1>those rays of lights into ribbons, sorts them, and enables

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<v Speaker 1>us to read in them hidden meanings. When a ray

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<v Speaker 1>of light reaches us from the sun, that ray is white,

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<v Speaker 1>but in the whiteness other hues are hidden. A white

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<v Speaker 1>ray is composite in form, made up of many lesser

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<v Speaker 1>rays of diverse colors blended together. Newton was the first

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<v Speaker 1>to discover so much. If a sunlight ray is allowed

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<v Speaker 1>to pass through a small round hole in the wall,

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<v Speaker 1>it will fall upon the opposite wall or upon the ground,

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<v Speaker 1>in a little round patch of light. But if a

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<v Speaker 1>piece of glass cut into the shape of a prism

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<v Speaker 1>is placed in the path of that sunbeam, the round

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<v Speaker 1>patch of light vanishes. In its stead appear several bands

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<v Speaker 1>of soft color, each overlapping and melting into the next. Red, orange, yellow, green, blue, indigo, violet.

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<v Speaker 1>All these become visible. The arrangement of colors is invariably

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<v Speaker 1>the same. Now the prism has done two things. First,

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<v Speaker 1>it has bent the ray out of a straight course,

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<v Speaker 1>causing it to fall in a different place from where

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<v Speaker 1>the round spot lay. Secondly, it has broken up or disintegrated,

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<v Speaker 1>the white ray into those differently tinted rays of which

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<v Speaker 1>it was made. And the manner of breaking it up

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<v Speaker 1>is simply this, that one color is always more or

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<v Speaker 1>less bent than another color in passing through a prism. Therefore,

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<v Speaker 1>all the different tints fall upon different places. The whole

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<v Speaker 1>variegated band, whether of sunlight or of any other light,

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<v Speaker 1>is known as the spectrum of that light, and the

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<v Speaker 1>breaking up of the ray and searching into its make

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<v Speaker 1>is called the analysis of it. Thus the reading of light,

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<v Speaker 1>whether earthly light, moonlight, sunlight, or starlight, is included under

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<v Speaker 1>the head of spectrum analysis. At the so called lowest

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<v Speaker 1>end of the spectrum lies red, the least bent of

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<v Speaker 1>all the colored rays. Of the so called highest end

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<v Speaker 1>lies violet, the most bent. All other hues visible to

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<v Speaker 1>our eyes are placed between light. Beyond the violet and

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<v Speaker 1>below the red. We cannot see. That is, by no

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<v Speaker 1>means to say that it does not exist. We can

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<v Speaker 1>feel the warmth of rays below the red, although we

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<v Speaker 1>cannot see them, and photographs are taken by means of

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<v Speaker 1>rays beyond both the red violet, albeit they are to

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<v Speaker 1>us invisible. By means of those faint rays, photographs can

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<v Speaker 1>actually be taken of countless stars, which no living man

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<v Speaker 1>can see through the most powerful telescopes. For the rays

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<v Speaker 1>are there, however, faint, and they will slowly impress their

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<v Speaker 1>image upon prepared sensitive paper long exposed to their dim shining,

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<v Speaker 1>though human eyes cannot gaze long or steadily enough to

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<v Speaker 1>detect them. Suppose now that for the round hole in

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<v Speaker 1>the wall we substitute a very narrow slit. Then, letting

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<v Speaker 1>the sunshine again stream through, we once more place a

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<v Speaker 1>prism of glass in the path of the ray. When

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<v Speaker 1>it has entered the slit, bright bands of color are

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<v Speaker 1>perceived anew arranged, always in the same order, from red

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<v Speaker 1>to violet. But the different colors no longer overlap as before,

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<v Speaker 1>and in addition to the bright hues, a great many slender,

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<v Speaker 1>dark lines or gaps in the coloring are to be seen.

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<v Speaker 1>These dark lines in the spectrum of sunlight were for

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<v Speaker 1>a long while a great perplexity. At first it was

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<v Speaker 1>thought that they might be caused by something in our

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<v Speaker 1>own atmosphere, but this notion had to be given up.

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<v Speaker 1>It became manifest that the lines were somehow connected with

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<v Speaker 1>the sun, not with the earth. Whenever a ray of

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<v Speaker 1>sunlight was passed through a narrow slit and analyzed there,

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<v Speaker 1>they were always the same in position. More and more

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<v Speaker 1>of them were found through closer observation, but the old

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<v Speaker 1>ones did not change. A ray of moonlight was found

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<v Speaker 1>to contain exactly the same dark lines as a ray

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<v Speaker 1>of sunlight, and most naturally, for a ray of moonlight

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<v Speaker 1>really is nothing more or less than a ray of

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<v Speaker 1>sunlight reflected from the moon. But in a ray of

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<v Speaker 1>starlight the lines were found to be in time different,

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<v Speaker 1>and this alone is enough to do away with the

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<v Speaker 1>idea of the lines being due to something in our air.

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<v Speaker 1>Starlight and sunlight, both alike journey through Earth's atmosphere. Every

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<v Speaker 1>star has its own particular spectrum, sometimes bands of color,

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<v Speaker 1>like our sun's spectrum with fine dark lines. Only the

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<v Speaker 1>arrangement of lines is never the same as those of

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<v Speaker 1>our sun, and it is never the same in any

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<v Speaker 1>two stars. These dark lines in sunlight and starlight tell

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<v Speaker 1>us much and briefly, as follows. If the light of

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<v Speaker 1>a white hot metal, either solid or liquid, is allowed

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<v Speaker 1>to pass through the slit and prism of a spectroscope,

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<v Speaker 1>bands of bright color are seen, one passing into another,

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<v Speaker 1>as with the solar spectrum, but under ordinary conditions of

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<v Speaker 1>bodies in a gaseous state, the spectrum does not consist

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<v Speaker 1>of broad, hazy bands of color, but of sharp bright

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<v Speaker 1>lines and mark this. Each particular gas has its own

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<v Speaker 1>especial lines, always occupying the same position. A chemist knows

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<v Speaker 1>to a certainty how many lines will be seen in

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<v Speaker 1>the case of iron gas, or sodium gas or hydrogen gas,

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<v Speaker 1>and where each line will fall. But suppose mark this again,

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<v Speaker 1>that the light comes either from a solid or a

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<v Speaker 1>liquid or a highly compressed gas, and passes on its

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<v Speaker 1>way through a gas medium at a lower temperature, such

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<v Speaker 1>as a gas flame or glowing gas atmosphere. In such

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<v Speaker 1>a case, when the ray has gone through slit and

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<v Speaker 1>prism and has spread out its spectrum of color bands,

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<v Speaker 1>dark lines will be seen in those bands. These dark

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<v Speaker 1>lines are gas or breaks in the light. They mean

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<v Speaker 1>the absence of part of the sunlight or starlight for

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<v Speaker 1>the gas through which that light has traveled on its way.

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<v Speaker 1>Hitherwood has absorbed or captured part of the light, and

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<v Speaker 1>only part has been free to continue its journey. A

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<v Speaker 1>ray of light from the Sun's photosphere has to pass

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<v Speaker 1>through the Sun's atmosphere of gases, and as it passes,

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<v Speaker 1>each gas in the solar atmosphere takes possession of some

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<v Speaker 1>part of it, producing dark lines which are peculiar to

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<v Speaker 1>that gas. In consequence of this, hundreds of tiny breaks

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<v Speaker 1>are formed in the solar spectrum where the much robbed

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<v Speaker 1>ray falls. If the light of a sodium flame is

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<v Speaker 1>passed through the spectroscope, two bright lines are always seen,

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<v Speaker 1>always in the same position. But in the Sun's coloured spectrum,

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<v Speaker 1>those two lines are dark, for the sodium in the

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<v Speaker 1>Sun's atmosphere has absorbed or stolen exactly that part of

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<v Speaker 1>the sunlight which would have given the two bright sodium lines.

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<v Speaker 1>The spectrum of our means not two, but hundreds of

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<v Speaker 1>bright lines in the solar spectrum. These hundreds of lines

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<v Speaker 1>are dark because the iron gas in the atmosphere of

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<v Speaker 1>the Sun has absorbed all that part of the light

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<v Speaker 1>ray on its journey from the radiant photosphere. Therefore, when

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<v Speaker 1>certain dark lines are apparent in the spectrum of the

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<v Speaker 1>Sun or of a star, we know that the metal

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<v Speaker 1>which always shows exactly corresponding bright lines is present in

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<v Speaker 1>the atmosphere of that sun or star. By the same mode,

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<v Speaker 1>the make of comets, of nebulae, and of other heavenly

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<v Speaker 1>bodies can be tested and examined. This may give just

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<v Speaker 1>a faint idea of the first principles of a new

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<v Speaker 1>grand branch of astronomy, included under the head of spectrum analysis.

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<v Speaker 1>The science is a science of itself, however, and one

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<v Speaker 1>full of complexity. Chemistry and astronomy here walk hand in hand,

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<v Speaker 1>and the spectroscope alone can decide whether any particular star

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<v Speaker 1>is in fact a sun. If the rainbow tinted ribbon

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<v Speaker 1>of light is there crossed by thin dark lines due

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<v Speaker 1>to the stellar atmosphere through which each ray has passed

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<v Speaker 1>after quitting the photosphere, then that star may be counted

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<v Speaker 1>a true sun. Such stars constitute the majority among the

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<v Speaker 1>hosts of Heaven, yet variety without limit is found. In

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<v Speaker 1>one star, the light from the photosphere is almost lost,

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<v Speaker 1>almost absorbed by the surrounding atmosphere. In another, the light

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<v Speaker 1>of the atmosphere so overpowers that of the photosphere that

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<v Speaker 1>only bright gas lines are seen in the spectroscope, the

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<v Speaker 1>continuous color band being comparatively faint. Besides telling us of

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<v Speaker 1>the make of the stars, the spectroscope also speaks to

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<v Speaker 1>us of their motions. A very tiny shift movement of

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<v Speaker 1>the little dark lines or bright lines to right or

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<v Speaker 1>left is sufficient. From this can be calculated with it

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<v Speaker 1>is believed astonishing exactness the rate at which a star

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<v Speaker 1>is rushing towards us or rushing away from us. For

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<v Speaker 1>if the star is nearing our earth, the light waves

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<v Speaker 1>coming from him are pressed together, so to speak, hurrying

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<v Speaker 1>one upon another, while if the star is retreating, the

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<v Speaker 1>light waves are affected in a reverse manner, delayed or

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<v Speaker 1>pulled apart, if such a term may be used. By

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<v Speaker 1>this method, also stars are discovered so dim as to

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<v Speaker 1>be not only utterly invisible to the naked eye, but

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<v Speaker 1>undiscoverable by the telescope. End of Section twenty seven.
