CHAPTER II. TESTIMONY OF THE ATMOSPHERE.—Concluded.
Religion and Chemistry | ||
2. CHAPTER II.
TESTIMONY OF THE ATMOSPHERE.—Concluded.
DURING a recent journey in Switzerland, at the close of a delightful summer's day, in the early part of July, I arrived at Interlachen, in company with a number of fellow-travellers. We had been sailing on the beautiful lake of Brienz, and some minutes before we reached our destination the sun had set, and the mountains had already cast their long shadows across the lake. Early in the afternoon the clouds had settled on the nearer hills, and we had been disappointed at not obtaining a view of the distant summits of the Bernese Oberland; but suddenly, as the boat neared the shore, the magnificent peak of the Jungfrau appeared from behind the veil of clouds, clothed in her white mantle of everlasting snow, and bathed with a flood of rosy light. The effect thus heightened by the contrast was grand beyond description, and as beautiful as it was grand. It seemed like a vision of the Heavenly Kingdom,—as if the glory of God had rested on the mountain. The scene completely filled the soul, and the heart overflowed with gratitude for the blessing it enjoyed. It was felt to be one of the
It may not be permitted to many to behold the Jungfrau blushing before her retiring lord, but all have witnessed the same effect on even a grander scale, when the white clouds, piled up on the western horizon like vast mountain chains, become, at evening, resplendent with the rays of the setting sun; and many have watched their varying tints of gold and purple, until at last their ghostly forms vanished in the dusk of the evening, and the stars came out to take up with their measured twinkling the silent song of praise. Perhaps, also, there may be some who, after anxious watching through the night, have felt their hearts strengthened and their hopes revived when the blush of morning reassured them of their Father's providence, and all nature smiled in the floods of returning light.
All these glorious visions, all this beauty, and all the pure emotions of our hearts which they excite, we owe, my friends, to the skill with which the physical qualities of the atmosphere have been adjusted to the wants of our physical and moral natures, and they all thus become the silent witnesses not only of the wisdom, but also of the goodness of our God.
We have already, in the first lecture, discussed some of the adaptations of the physical condition of the atmosphere to the purposes which it subserves on the globe, and I wish this evening to develop still further the same subject, by considering a few additional examples; and first I will ask your attention to those evidences of design which are to be found in the relations of the atmosphere to light and heat. Here, however, I am met by a difficulty. In order to explain fully these relations it would be necessary to develop from first principles the sciences of optics and thermotics, and to do this in a popular manner would require several lectures. These sciences furnish some of the most wonderful evidences of design which are to be found in nature and I have no doubt will be given their appropriate place in this series of lectures. Without, therefore, attempting any detailed explanations, I will merely bring before you a few facts, drawn from these departments of knowledge, which illustrate the adaptations of the atmosphere to its appointed ends.
The atmosphere, although very much more pervious to light than any kind of solid or liquid matter, is far from being perfectly transparent. Indeed, the reverse is sufficiently evident from our daily experience. Every one has noticed that distant objects appear less distinct in proportion as they are removed, their colors become fainter, the contrast between light and shade less marked, and that they seem as if covered with a pale blue veil. This effect, always noticed on distant mountains, is owing to a partial absorption of the light while passing through
The transparency of the atmosphere differs very greatly under different circumstances, but it has been estimated that, under the most favorable conditions, at least thirty per cent. of all the light coming from the heavenly bodies is absorbed before reaching the surface of the earth, and in our latitude, at this season, even when the sun is on the meridian and the sky clear, fully one-half of his rays are thus spent. Do not suppose, however, that all the light so expended is lost. Quite the contrary, for every particle of the atmosphere, illuminated by the sunbeam, becomes itself a new centre of emission, radiating the light in every direction.
This diffusion of the sun's rays is the cause of that wonderful effect which we term daylight. I say wonderful effect, for, although so familiar, it is one of the most remarkable results of skilful adaptation and infinite wisdom. The very daylight which streams in at the open windows of our houses, filling them with cheerfulness, and penetrating to their inmost recesses, which enlivens the whole landscape, and which bars and bolts cannot wholly exclude even from the prisoner's dungeon, is another evidence of the adaptation of the atmosphere to the constitution of man. Indeed, the atmosphere is as much an essential condition of our seeing as of our breathing, and the immeasurable pleasure which we derive from our sense of vision depends upon its
I have thus far spoken only of the influence of the atmosphere in softening the intensity of the rays of
In regard to the precise means which are employed by nature to produce these results, scientific men are not agreed. It has been proved that the blue color of the sky is seen by reflected light, and it is probable that the color is caused by repeated reflections of the sun's rays from the surfaces of the innumerable small water-bubbles which are constantly floating in the atmosphere. You have all noticed the blue color of the soap-bubble shortly before it breaks. This color is caused by the action of the very thin film of water in decomposing the light reflected from its surface, and it is supposed to be an action of the same sort, only very much increased by repeated reflections, which gives to the sky its azure hue.
While the blue color of the sky appears to result from changes in the white light of the sun caused by reflection, it is equally probable that the sunset tints arise from changes in the same white light caused by an unequal absorption of its different colored rays during their transmission through the atmosphere. Here, again, the vapor in the air is supposed to be the active agent; and the theory is, that the tints are produced while the vapor is condensing into clouds,—a change which naturally occurs at sunset. But this is a mere theory, and
So far, however, as our present argument is concerned, it is not essential that we should understand exactly how these glorious results are obtained. It is enough that we are constantly enjoying their beauty, and that we know they are owing to the peculiar constitution of the atmosphere. When future discoveries shall bring to light the methods, at present secret, by which nature gilds the sunset clouds and covers our beautiful dwelling-place with its canopy of blue, we shall unquestionably find fresh evidences of God's wisdom; but even now, when ignorant, perhaps, of these hidden causes, we have that which is far more excellent, the most conclusive evidence of His goodness and love. Our Father has not only adapted the atmosphere to the wants of our bodies, and made it conducive to our physical enjoyment, but He has also made it the scene of the highest beauty,—a beauty which satisfies the longings of our souls and calls forth their noblest and purest aspirations. Man, sinful as he is, cannot look up into the pure blue of heaven without a sense of reproach, and the feeling that it is a fit emblem of the kingdom of purity and peace. And when the setting sun lights up the evening altar in the West, who can repress the rising prayer of devotion, and hesitate to believe, with the child, that his Heavenly Father is smiling behind the clouds? There is a depth to the beauty of nature which man cannot fathom. Poetry cannot describe it, and the highest art only displays
Such are some of the evidences of design which we discover in the relations of the atmosphere to light. Let us now examine some of its relations to heat, which we shall find not less instructive. It was formerly supposed that the rays of heat, although accompanying the luminous rays in the sunbeam, were essentially different from those of light. But it is now almost universally believed that the rays of heat differ from those of light only, at most, as one color differs from another, and that even the same rays, which, falling on the retina of the eye, excite the sensation of light, when falling on the nerves of feeling may excite heat. But what, you may ask, is the difference between the different colors? The subject is somewhat abstruse, but if you will follow me attentively for a few minutes I will try to make it intelligible.
Every one who has dropped a stone into the water of a still lake has noticed the system of waves which, with its ever-increasing circles, spreads in every direction from the stone; but all may not
Our ears are so constituted that they can hear a musical note only when within certain fixed limits of pitch, differing to a slight extent with different individuals. The deepest bass note, which can be heard, as such, by a good ear, is produced by about
Notes | Length of waves in feet. |
Number of waves striking the ear in one second. |
C-3 | 70 | 16 |
C-2 | 35 | 32 |
C-1 | 17.5 | 64 |
C1 | 8.75 | 128 |
C2 | 4.375 | 256 |
C3 | 2.178 | 512 |
C4 | 1.093 | 1,024 |
Name of Note, | C1 | D1 | E1 | F1 | G1 | A1 | B1 | C2 |
Number of Waves, | 128 | 144 | 160 | 170 2/3 | 192 | 213 1/3 | 240 | 256 |
Ratio of each number to that of Note C,} |
1 | 9/8 | 5/4 | 4/3 | 3/2 | 5/3 | 15/8 | 2 |
Sounds of the highest pitch, like the cry of some insects, become disagreeable, and by some persons cannot even be distinguished. It is quite possible to produce a sound, which, though painfully shrill to one person, shall be entirely unheard by another.
"I once crossed a Swiss mountain in company with a friend; a donkey was in advance of us, and the dull tramp of the animal was plainly heard by my companion; but to me this sound was almost masked by the shrill chirruping of innumerable insects, which thronged the adjacent grass; my friend heard nothing of this, it lay quite beyond his range of hearing.''
There may, therefore, be innumerable sounds in nature to which our ears are perfectly deaf, although they are the sweetest melody to more refined senses. Nay, more, the very air around us may be resounding with the hallelujahs of the heavenly host, when our dull ears hear nothing but the feeble accents of our broken prayers.
We have been studying, my friends, the nature of sound, in order to comprehend more readily the nature of light and heat, for the phenomena included under these names are produced, like the phenomena of sound, by waves; not, however, by waves in the air, but by waves in a medium which is as much more subtile than air as air is more subtile than water,—indeed, a medium so exceedingly thin that it eludes all our powers of chemical analysis; but which, as we assume, pervades all space, and this, too, whether the space be filled or not, at the same time, by other forms of matter. We call this medium "ether,'' and through it the waves of
Yet great as is the difference of velocity, the analogy between sound on the one side, and light or heat on the other, is complete. Every luminiferous body, like this candle-flame, excites in the tenuous ether a system of waves, which spread, in ever-enlarging spheres, with the immense velocity just described; and it is these little billows which, passing through the humors of the eye, and breaking on the retina, produce the sensation we call light, or, falling on the skin, excite the less delicate nerves of feeling, and cause the sensation of heat.
Moreover, the difference between colors is of precisely the same kind as the difference between notes. Red, yellow, green, blue, violet, etc., are names we give to sensations caused by waves of ether breaking at regular intervals on the retina. Color corresponds to pitch, and—what may seem to you incredible—we are able to calculate from actual measurements the number of waves of ether which must break on the retina in a second in order to produce the sensation of a given color. Here are some of the numbers, and, extravagant as they appear, they are the sober results of science, and have been as accurately determined as the magnitudes and distances of astronomy.
Colors. | Number of waves in an inch.[*] | Number of waves in a second. | ||
Red | 39,000 | 447 million million. | ||
Orange | 42,000 | 506 | '' | '' |
Yellow | 44,000 | 535 | '' | '' |
Green | 47,000 | 577 | '' | '' |
Blue | 51,000 | 622 | '' | '' |
Indigo | 54,000 | 658 | '' | '' |
Violet | 57,000 | 699 | '' | '' |
It is actually true, that when we are receiving the sensation of red there are no less than 477 million millions of ether waves breaking on the retina of our eyes every second. And more than this, we have measured the length of these waves, and we know that the length of a wave of red light from crest to crest is 1/39000 of an inch. By examining the table you will also discover that the sensation of red, as compared with other colors, results from the smallest number of waves, and that these waves are comparatively large. On the other hand, the sensation of violet is caused by the largest number of waves, which, however, are proportionally small in size. The red light, therefore, corresponds to low,
Waves of all the dimensions given in the table, together with waves of every possible length between certain extremes,—which are far wider than those indicated above,—move together in the sunbeam, and their combined impression produces the sensation of white light. We have a very simple way of analyzing the sunbeam and separating its different color-producing waves. The method consists in passing the sunbeam through a glass prism. The prism has the power of bending the beam from its rectilinear direction; but it does not change the direction of the motion of all the waves to the same extent. The longer waves, which give the sensation of red, are bent from their course much less than the shorter waves, which produce the sensation of violet, while waves of an intermediate length take a course between the two. Hence, after emerging from the prism the directions of the different waves diverge, and if we receive the beam of light thus analyzed, on a screen, the various color-producing waves strike the screen at different points of a continuous line. A more or less narrow band on the screen will thus be illuminated with lights of different colors in the following order—Red, Orange, Yellow, Green, Blue, Indigo, Violet—and this beautiful phenomenon is familiar to almost every one under the name of the solar spectrum.
Here, where we have the whole scale of colors spread out before us, the analogy of light to sound
I hope that I have been able to make clear two points,—first, that light and heat are forms of motion; second, that the differences in the phenomena which have been referred to these two agents are
From the principles stated, it is evident that the atmosphere must act in diffusing heat, just as we have seen that it acts in diffusing light. Indeed, this effect is one of the thousand conditions on which the existence of organic life depends. Were it not for the influence of the atmosphere, the greatest extremes of temperature would be produced by the alternation of day and night, and even were the
But not only does the atmosphere diffuse the heat of the sun's rays, it also acts, and even more effectually, in retaining on the surface the heat which the earth is constantly receiving from that great central luminary. The atmosphere has been compared to a mantle, and the comparison is just; for, like a huge cloak, it envelops the earth in its folds, and protects it from the chill of the celestial spaces through which we are rushing with such frightful velocity. In order to understand how a thin and transparent medium like air can thus act to keep the earth warm, we must recur to some of the facts established above.
As the ether-waves, breaking on the eye more or less rapidly, produce the different sensations of color, so when breaking on the skin they occasion analogous differences in the sensation of heat, which, although not so accurately distinguished, because the sense is less delicate, nevertheless are as real as the difference between a low and sweet musical note, and one that is high and shrill. There are waves of heat which break upon our nerves of feeling like the shrill cry of the cricket on the ear, and seem to penetrate to the very brain, while there are others which fall like the low tones of an organ, diffusing throughout the system a genial glow. Such, for example, is the difference between the heat from a hard-coal fire and that from a steam radiator. The waves of the
Now it is found that the sunbeam is chiefly made up of waves of the first class, which are therefore able readily to penetrate the atmosphere and warm the surface of the earth. The earth thus warmed becomes itself a hot body, surrounded by an intensely cold space, and, like any other hot body, tends to lose its heat by radiation. But the waves of heat which the earth [*] sets in motion are of the second class, long and slow undulations, and these are in great measure arrested by the atmosphere; indeed, as experiments have proved, they are chiefly absorbed by the lower strata, [*] in which we live and move.
Thus it is that the atmosphere keeps us warm; and if you desire further proof of the correctness of these experimental deductions, ascend any high mountain, and, as the thickness of the aerial covering above you is diminished by the elevation, you will find that the chill increases, vegetation slowly disappears, and before long you will reach a region of eternal snow and ice. It is true that there are other causes acting to lower the temperature at high
The atmosphere not only thus acts in diffusing the sun's rays, and retaining the heat which they bring to us, but it also subserves an equally important end in distributing their genial warmth over the whole surface of the earth, thus moderating the climate of the temperate zone, and mitigating the intense heat of the tropics. Air, like all gases, is expanded by heat, and thus rendered specifically lighter, and on this simple principle all our methods of warming and ventilating are based. When now it is remembered that the atmosphere under the tropics must become more intensely heated by the vertical rays of the sun than it is in the temperate zones, the result will be obvious. The heated air rises, and the cold air rushes in from the North and South to take its place. Thus, two general currents are excited in the aerial ocean of each hemisphere, one on the surface of the earth, tending towards the
In the first place, the rotation of the globe on its axis imparts to objects on the surface a motion from West to East, varying in velocity from nothing, at the poles, to the speed of a cannon-ball, at the equator. In consequence of this, a mass of air moving towards the equator is constantly arriving at a point on the surface of the earth, which is moving towards the East more rapidly than the point it has just left; and as, in virtue of the law of inertia, the moving mass cannot accommodate itself instantaneously to the increased velocity, it is left a little behind,—that is, a little to the West, at every step. Hence, the lower or polar currents bend more and more towards the West as they approach the equator, acquiring in the northern hemisphere a south-westerly, and in the southern hemisphere a north-westerly direction; and the currents of the two hemispheres, meeting at the equator, combine to produce the great trade-wind, which, in the Pacific Ocean, blows constantly from the East to the West, and would blow regularly in this direction all round the globe if the continents did not intervene to disturb its course at various points.
The effect of the earth's rotation on the current of warm air which flows from the equator in the upper atmosphere, must evidently be the reverse of that just described, bending it constantly to the
Again, the unequal heating effect of the sun's rays on the earth, as compared with the sea, combined with the irregular distribution of land and water over the surface of the globe, tends to complicate still further the motion of the aerial currents. For reasons which will hereafter appear, the land is more quickly heated by the sun's rays than the sea when under the same conditions, and, on the other hand, as soon as the sun is withdrawn, it cools more rapidly. Hence, on an island in a warm climate we generally have, during the daytime, a current of heated air rising from the surface of the earth, and a current of cooler air flowing in on all sides from the ocean to take its place, while after sunset the land soon cools below the temperature of the surrounding ocean, and the current is reversed. Thus is produced the daily alternation of land and sea breezes, so familiar to every one who has visited the tropics, where the phenomena are most strongly marked.
Quite a similar reciprocal action between the continents and the great ocean is caused by the alternation of seasons, and of this the monsoons of the Indian Ocean are a remarkable illustration. This mediterranean ocean, shut off from the influence of the general trade-winds by the great continental masses which surround it, has a system of aerial currents, peculiar to itself, blowing six months of the year in one direction and six months in the other. These are set in motion by the unequal heating of the continents of Asia and Africa during the extreme seasons. In the months of December, January, and February, the part of Africa south of the equator is exposed to the vertical rays of a summer's sun, while the countries of southern Asia are feeling the comparative cold of their winter. The natural consequence is, that a stream of cold air rushes across the Indian Ocean to feed the intensely-heated current which is rising over the burning plains of Africa, and produces a strong north-easterly breeze, which is the winter monsoon of India. When, however, the sun comes north of the equator, all these conditions are reversed. The ocean air now rushes to the more heated plains of India, and the summer monsoon sets in, which blows from the south-west, the change from one to the other being always attended by variable winds and furious storms. Lastly, the position of mountain chains and the configuration of the continents, which break and turn the winds, or open to them a freer channel, have an important influence in determining the direction of the aerial currents on the earth.
But we have not time for further details; they are given in all works on physical geography, [*] and the student of natural theology will find that subject rich in illustrations of God's wisdom and power. We have already become sufficiently acquainted with the general plan to understand how the atmosphere acts in equalizing the climate of the globe. The aerial currents which come to us from the South bring with them the heat of the tropics, and distribute it over the temperate zone. As they blow from the south-west, they naturally exert the greatest heating power on the western coasts of the continents, and this is one great cause of the well-known fact that the climate of western Europe is so much milder than our own, and the climate of California and Oregon so much warmer than that of the corresponding latitudes on the eastern coast of Asia. Moreover, the sea-breezes on islands and along seacoasts, the monsoons of the Indian Ocean, and other local currents, all combine, as our theory shows, to produce the same general result, cooling such regions of the earth as from any cause have become overheated, and transferring the warmth to places where it is more needed. Just as the heat of burning fuel is diffused over a whole building from the furnace by the currents of air it sets in motion, so the sun's heat is diffused over the earth from the tropics by the great terrestrial currents we have so briefly described. Indeed, as already stated, in all our methods of heating, we merely apply, on
But, although the heat of the sun might set in motion these aerial currents, they would have but little effect in warming our northern climate, were it not that the air has been endowed with a certain capacity for holding heat. All substances possess this capacity to a greater or less degree, but the differences between them are very large. Thus the amount of heat required to warm a pound of water is ten times greater than would be required to raise the temperature of a pound of iron, and thirty times greater than would be required to raise the temperature of a pound of mercury to an equal extent. Hence, under the same conditions, a pound of water may be said to contain ten times as much heat as a pound of iron, and thirty times as much as a pound of mercury; or, again, in other words, the capacity of water for heat is ten times greater than that of iron, and thirty times greater than that of mercury. The capacity of air for heat is, weight for weight, about twice as great as that of iron, and although only one-fifth as great as the capacity of water, it is yet greater than that of most other substances. The point, however, to which I wish to direct your attention, is the fact that this capacity is exactly adjusted to the office which the air has been appointed to fill. Were the capacity of the air less, the hot air from the tropics would bring to us proportionally less heat; were it greater, the reverse would be the case; and in either event, the distribution of temperature on the earth would be changed. To what extent
Such are a few of the more obvious marks of design, which may be discovered by studying the relations of the atmosphere to light and heat. I might here close one division of my subject; but I should fail to give you an adequate idea of the wonderful play of physical forces in the atmosphere, were I to leave out of view that mighty agent which charges the artillery of heaven and feeds the flaming torches in the northern sky. It is true that the atmospheric relations of electricity are very imperfectly understood, and the important ends which it undoubtedly subserves in the economy of nature almost entirely unknown. We cannot, therefore, expect them to furnish us with many additional illustrations of the Divine attributes; but since electrical phenomena play so conspicuous a part in the atmosphere, and must have been included in its plan, they certainly should not be overlooked if we
Of all the assumed agents of nature there is hardly one which is so little understood, and yet has been so carefully studied, as electricity. To the uneducated it affords the convenient explanation of most obscure phenomena, while with men of science it is the object of much laborious investigation and careful theorizing. The study of its phenomena has been fruitful in the discovery of facts; but it has as yet led to but few general principles, and has furnished only a meagre explanation of those grand displays of nature in which it seems to be such an important agent.
In regard to the nature of electricity, we are entirely ignorant. The phenomena of light and heat [*] admit, to say the least, of an intelligible explanation, and can be referred to a dynamical origin; but in the case of electricity we are obliged to be content with collecting facts, and must await the further progress of science to reveal the now hidden cause. I am well aware that electricity has been regarded as a very rare and subtile "fluid,'' and that this theory has not only afforded a plausible explanation of most of the phenomena of statical electricity, but also that the numerical results based upon it have been most remarkably verified by experiment. Yet nevertheless, although the theory may still be used as a convenient frame in which to exhibit the facts, there are but few investigators of the present day
The fundamental facts of electricity were known to the ancients, and are familiar to every one. If a stick of sealing-wax or a glass tube be rubbed with a warm silk handkerchief, it becomes, as we say electrified, and in this condition has the power of attracting pieces of paper or any light particles of matter. When the scientific men of the last century came to examine these phenomena more carefully, they found that the handkerchief was also electrified, and thrown into a state differing from that of the glass in the one case, and that of the resin in the other, very much as the north pole of a magnet differs from its south pole. They found, also, that the resin was electrified oppositely to the glass, and they hence concluded that there were two kinds of electricity, which they distinguished by the names resinous and vitreous, or positive and negative. They also discovered that this agent could readily be drawn off from electrified bodies by the metals, but only with difficulty, if at all, by such materials as india-rubber, glass, resin, or silk, and they were hence led to divide substances into conductors and non-conductors of electricity. A good conductor, when insulated by non-conductors, was found to retain for a short time the electricity it had received from the electrified glass or resin, although the charge was soon dissipated by the surrounding air, especially when moist. By bringing in the aid of machinery, and thus increasing the surface of friction,
More recently it has been discovered that friction is by no means the only source of electricity, and it seems probable that no change, either chemical or physical, takes place in nature without some manifestation of this agent. It was at first supposed that there were several kinds of electricity, which were named thermo-electricity, magneto-electricity, voltaic electricity, and animal electricity, according to the nature of the process in which the electrical action was developed; but it is now universally conceded that all are only different manifestations of the same agent, and most investigators believe that electricity will in time be shown to be a form of molecular motion analogous to that which produces the phenomena of light and heat, although it has not as yet been found possible to frame a comprehensive and intelligible theory based upon this hypothesis. Again, it has been found that friction is a far more general source of electricity than was at first believed. In fact, electrical phenomena appear to be a constant result of friction, whatever may be the nature of the substances rubbed. Thus it is developed by blowing air over glass, and the hydro-electric machine, one of the most effective means of generating electricity we possess, owes its surprising energy to the friction of globules of water against the sides of the vent-cock of a steam-boiler. [*]
When, now, we consider that the air is always
Since the atmosphere is, at best, a very poor conductor, the electricity developed by the processes just considered tends to accumulate; and under peculiar conditions the clouds may become so highly charged, that at length the pent-up power acquires sufficient force to break through all barriers, and the lightning dashes to the earth, crashing, rending, and burning on its way. To guard his roof from its destructive action, man erects the lightning-rod, whose bristling points quietly drain the clouds, or, failing to do this, receive the charge, and bear it harmlessly to the earth. But ages before Franklin pointed the first rod to the storm, the Merciful Parent of mankind had surrounded the dwellings of his children with a protection far more effectual than this; for, since the creation of organic life, every pointed leaf, every twig, and every blade of grass
I am indebted for many of the above illustrations to an admirable paper on atmospheric electricity, in the American Almanac for 1854, by my friend and colleague Prof. Joseph Lovering.
I must here conclude this very imperfect sketch of the physical adaptations of the atmosphere to the ends it subserves on the earth. We studied in the first place its aeriform condition, and found that its density not only formed an essential part of the scheme of organic nature, but also was closely related to the dimensions of the solar system. In this Lecture we have studied the relations of the atmosphere to light, heat, and electricity; and although we have been able only to glance at some of the more prominent features in these wonderful displays of creative energy, we have found, wherever we turned, abundant illustrations of the wisdom, power, and goodness of our God. I trust that you have been impressed by the vastness, the complexity, and yet
Paley has compared the mechanism of nature to a watch, and, so far as the argument for design is
How different it is with the mechanism of nature! Here, also, it is true, the more we study, the more we understand the workmanship; but then we never reach the limit. The more our powers of thought and observation are developed, and the more our experience is enlarged, the more the field of possible knowledge expands before us. The larger our attainments, the less we seem to know.
We still recognize the unmistakable marks of intelligence
By most men these heights of knowledge are unattainable. Why, then, should we hesitate to receive the evidence of a philosopher like Newton, who,
We can all recognize the marks of design in nature, and when we add to this evidence of our senses the testimony of a man like Newton, who assures us that the more our powers are enlarged, and the wider our knowledge becomes, the grander and vaster the design will appear, until it surpasses all our powers of thought or imagination, we begin to feel the full depth of the truth I have been endeavoring to enforce. If our minds are incapable of comprehending the plan, who could have been equal to the design? "Whence, then, cometh wisdom, and where is the place of understanding, seeing it is hid from the eyes of all living, and kept close from the fowls of the air? * * * God understandeth the way thereof, and he knoweth the place thereof. For he looketh to the ends of the earth, and seeth under the whole heaven, to make the weight for the winds * * * and a way for the lightning of
A given wave-length corresponds to each point on the line of the solar spectrum, to be described further on. The numbers given in the table are to be regarded merely as the mean values for each color, measured at points on the spectrum, marked by certain prominent dark lines called Frauenhofer's lines. The solar spectrum, as seen with a powerful spectroscope, is crossed by thousands of these lines, which have a fixed position, and therefore serve to mark definite points on this otherwise continuous band of blending colors.
The effects of expansion, melting, evaporation, the permanent elasticity of gases and vapors, and many other phenomena, formerly referred to the action of a peculiar agent called heat, are now supposed to be the result of the motion which the ether-waves communicate to the material particles of the bodies on which they strike or through which they are transmitted. To understand this, we must remember that the molecules, even of the densest solids, are supposed to be separated from each other by comparatively large spaces filled with ether, through which the waves of heat and light may move more or less freely, just as the waves of air pass between the branches in a forest. Moreover, as the waves of air impart motion to the branches of the trees, and afterwards are kept in motion by the waving boughs, so also the material particles of a body may set in motion the waves of ether, or receive motion from them in return.
The pitch, if we may so speak, and penetrating power of the heat-waves depend on the temperature of the body by which they are set in motion, and in proportion as the temperature rises the pitch is higher and the penetrating power greater.
Professor Tyndall has shown that this effect is due almost entirely to the aqueous vapor in the atmosphere, which is present in greatest quantity in the strata nearest to the earth.
In the sunbeam, as it passes through space, there are undoubtedly waves of low pitch in abundance, but these are almost entirely arrested by the atmosphere before reaching the surface of the earth. It has been estimated that of the heat the earth receives from the sun about one third is thus absorbed.
This machine consists simply of a small steam-boiler insulated on glass pillars, having a peculiarly-constructed vent-cock and provided with suitable metallic conductors for receiving the electricity. The steam, as it escapes under high pressure, becomes filled with globules of water which rub against the sides of the vent-tube, and this is so shaped as to facilitate their formation.
CHAPTER II. TESTIMONY OF THE ATMOSPHERE.—Concluded.
Religion and Chemistry | ||