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<body><section class="pg-boilerplate pgheader" id="pg-header" lang="en"><h2 id="pg-header-heading" title="">The Project Gutenberg eBook of <span lang="en" id="pg-title-no-subtitle">Treatise on light</span></h2>
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<div class="container" id="pg-machine-header"><p><strong>Title</strong>: Treatise on light</p>
<p style="margin-top:0"><span style="padding-left: 7.5ex"> </span>In which are explained the causes of that which occurs in reflexion, & in refraction and particularly in the strange refraction of Iceland crystal</p>
<div id="pg-header-authlist">
<p><strong>Author</strong>: Christiaan Huygens</p>
<p><strong>Translator</strong>: Silvanus P. Thompson</p>
</div>
<p><strong>Release date</strong>: January 18, 2005 [eBook #14725]<br>
Most recently updated: December 19, 2020</p>
<p><strong>Language</strong>: English</p>
<p><strong>Credits</strong>: E-text prepared by Clare Boothby, Stephen Schulze, and the Project Gutenberg Online Distributed Proofreading Team</p>
</div><div id="pg-start-separator">
<span>*** START OF THE PROJECT GUTENBERG EBOOK TREATISE ON LIGHT ***</span>
</div></section><p></p>
<p> </p>
<p>E-text prepared by Clare Boothby, Stephen Schulze,<br>
and the Project Gutenberg Online Distributed Proofreading Team</p>
<p> </p>
<hr class="full">
<p> </p>
<h1> <a id="Page_iii"></a><b>TREATISE ON LIGHT</b></h1>
<p class="center">In which are explained<br>
The causes of that which occurs<br>
<b>In REFLEXION, & in REFRACTION</b></p>
<p class="center">And particularly<br>
<b>In the strange REFRACTION</b><br>
<b>OF ICELAND CRYSTAL</b></p>
<h3>By</h3>
<h2> <b>CHRISTIAAN HUYGENS</b></h2>
<p class="center">Rendered into English</p>
<p class="center">By</p>
<p class="center"><b>SILVANUS P. THOMPSON</b></p>
<p> </p>
<p> </p>
<h6>University of Chicago Press</h6>
<p><a id="Page_iv"></a></p>
<p> </p>
<p> </p>
<p> </p>
<div class="pagenum">[Pg v]<a id="Page_v"></a></div>
<div class="figcenter" style="width: 600px;">
<img alt="" height="150" src="./The Project Gutenberg eBook of Treatise on Light, by Christiaan Huygens_files/prefhead.png" title="" width="600" id="id-8802152595684315141">
</div>
<h2>PREFACE</h2>
<div style="width: 147px; float: left; margin-right: .2em;">
<img alt="I" height="150" src="./The Project Gutenberg eBook of Treatise on Light, by Christiaan Huygens_files/pref.png" title="I" width="147" id="id-139463754583909775">
</div><p> wrote this Treatise during my sojourn in France twelve years ago,
and I communicated it in the year 1678 to the learned persons who then
composed the Royal Academy of Science, to the membership of which the
King had done me the honour of calling, me. Several of that body who
are still alive will remember having been present when I read it, and
above the rest those amongst them who applied themselves particularly
to the study of Mathematics; of whom I cannot cite more than the
celebrated gentlemen Cassini, Römer, and De la Hire. And, although I
have since corrected and changed some parts, the copies which I had
made of it at that time may serve for proof that I have yet added
nothing to it save some conjectures touching the formation of Iceland
Crystal, and a novel observation on the refraction of Rock Crystal. I
have desired to relate these particulars to make known how long I have
meditated the things which now I publish, and not for the purpose of
detracting from the merit of those who, without having seen anything
that I have written, may be found to have treated <span class="pagenum">[Pg vi]</span><a id="Page_vi"></a>of like matters: as
has in fact occurred to two eminent Geometricians, Messieurs Newton
and Leibnitz, with respect to the Problem of the figure of glasses for
collecting rays when one of the surfaces is given.</p>
<p>One may ask why I have so long delayed to bring this work to the
light. The reason is that I wrote it rather carelessly in the Language
in which it appears, with the intention of translating it into Latin,
so doing in order to obtain greater attention to the thing. After
which I proposed to myself to give it out along with another Treatise
on Dioptrics, in which I explain the effects of Telescopes and those
things which belong more to that Science. But the pleasure of novelty
being past, I have put off from time to time the execution of this
design, and I know not when I shall ever come to an end if it, being
often turned aside either by business or by some new study.
Considering which I have finally judged that it was better worth while
to publish this writing, such as it is, than to let it run the risk,
by waiting longer, of remaining lost.</p>
<p>There will be seen in it demonstrations of those kinds which do not
produce as great a certitude as those of Geometry, and which even
differ much therefrom, since whereas the Geometers prove their
Propositions by fixed and incontestable Principles, here the
Principles are verified by the conclusions to be drawn from them; the
nature of these things not allowing of this being done otherwise.</p>
<p>It is always possible to attain thereby to a degree of probability
which very often is scarcely less than complete proof. To wit, when
things which have been demonstrated by the Principles that have been
assumed correspond perfectly to the phenomena which experiment has
brought under observation; especially when there are a great number of
<span class="pagenum">[Pg vii]</span><a id="Page_vii"></a>them, and further, principally, when one can imagine and foresee new
phenomena which ought to follow from the hypotheses which one employs,
and when one finds that therein the fact corresponds to our prevision.
But if all these proofs of probability are met with in that which I
propose to discuss, as it seems to me they are, this ought to be a
very strong confirmation of the success of my inquiry; and it must be
ill if the facts are not pretty much as I represent them. I would
believe then that those who love to know the Causes of things and who
are able to admire the marvels of Light, will find some satisfaction
in these various speculations regarding it, and in the new explanation
of its famous property which is the main foundation of the
construction of our eyes and of those great inventions which extend so
vastly the use of them.</p>
<p>I hope also that there will be some who by following these beginnings
will penetrate much further into this question than I have been able
to do, since the subject must be far from being exhausted. This
appears from the passages which I have indicated where I leave certain
difficulties without having resolved them, and still more from matters
which I have not touched at all, such as Luminous Bodies of several
sorts, and all that concerns Colours; in which no one until now can
boast of having succeeded. Finally, there remains much more to be
investigated touching the nature of Light which I do not pretend to
have disclosed, and I shall owe much in return to him who shall be
able to supplement that which is here lacking to me in knowledge. The
Hague. The 8 January 1690.<span class="pagenum">[Pg viii]</span><a id="Page_viii"></a></p>
<div class="pagenum">[Pg ix]<a id="Page_ix"></a></div>
<div class="figcenter" style="width: 600px;">
<img alt="." height="151" src="./The Project Gutenberg eBook of Treatise on Light, by Christiaan Huygens_files/tranhead.png" title="" width="600" id="id-8628891925490331551">
</div>
<h2><a id="NOTE_BY_THE_TRANSLATOR"></a>NOTE BY THE TRANSLATOR</h2>
<div style="width: 150px; float: left; margin-right: .2em;">
<img alt="C" height="150" src="./The Project Gutenberg eBook of Treatise on Light, by Christiaan Huygens_files/trans.png" title="C" width="150" id="id-2389313070812496619">
</div><p>onsidering the great influence which this Treatise has exercised in
the development of the Science of Optics, it seems strange that two
centuries should have passed before an English edition of the work
appeared. Perhaps the circumstance is due to the mistaken zeal with
which formerly everything that conflicted with the cherished ideas of
Newton was denounced by his followers. The Treatise on Light of
Huygens has, however, withstood the test of time: and even now the
exquisite skill with which he applied his conception of the
propagation of waves of light to unravel the intricacies of the
phenomena of the double refraction of crystals, and of the refraction
of the atmosphere, will excite the admiration of the student of
Optics. It is true that his wave theory was far from the complete
doctrine as subsequently developed by Thomas Young and Augustin
Fresnel, and belonged rather to geometrical than to physical Optics.
If Huygens had no conception of transverse vibrations, of the
principle of interference, or of the existence of the ordered sequence
of waves in trains, he nevertheless attained to a remarkably clear
understanding of the prin<span class="pagenum">[Pg x]</span><a id="Page_x"></a>ciples of wave-propagation; and his
exposition of the subject marks an epoch in the treatment of Optical
problems. It has been needful in preparing this translation to
exercise care lest one should import into the author's text ideas of
subsequent date, by using words that have come to imply modern
conceptions. Hence the adoption of as literal a rendering as possible.
A few of the author's terms need explanation. He uses the word
"refraction," for example, both for the phenomenon or process usually
so denoted, and for the result of that process: thus the refracted ray
he habitually terms "the refraction" of the incident ray. When a
wave-front, or, as he terms it, a "wave," has passed from some initial
position to a subsequent one, he terms the wave-front in its
subsequent position "the continuation" of the wave. He also speaks of
the envelope of a set of elementary waves, formed by coalescence of
those elementary wave-fronts, as "the termination" of the wave; and
the elementary wave-fronts he terms "particular" waves. Owing to the
circumstance that the French word <i>rayon</i> possesses the double
signification of ray of light and radius of a circle, he avoids its
use in the latter sense and speaks always of the semi-diameter, not of
the radius. His speculations as to the ether, his suggestive views of
the structure of crystalline bodies, and his explanation of opacity,
slight as they are, will possibly surprise the reader by their seeming
modernness. And none can read his investigation of the phenomena found
in Iceland spar without marvelling at his insight and sagacity.</p>
<div style="margin-left: 80%;"><p>S.P.T.</p>
<p><i>June</i>, 1912.</p></div>
<hr style="width: 65%;">
<div class="pagenum">[Pg xi]<a id="Page_xi"></a></div>
<h2><a id="TABLE_OF_MATTERS"></a>TABLE OF MATTERS</h2>
<h3> <i>Contained in this Treatise</i></h3>
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<tbody><tr><td><a href="https://www.gutenberg.org/cache/epub/14725/pg14725-images.html#CHAPTER_I" class="pginternal"><b>CHAP. I. On Rays Propagated in Straight Lines.</b></a>
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<tbody><tr><td style="text-align: left;"><i>That Light is produced by a certain movement.</i></td><td style="text-align: left;"><a href="https://www.gutenberg.org/cache/epub/14725/pg14725-images.html#Page_3" class="pginternal">p. 3</a></td></tr>
<tr><td style="text-align: left;"><i>That no substance passes from the luminous object to the eyes.</i></td><td style="text-align: left;"><a href="https://www.gutenberg.org/cache/epub/14725/pg14725-images.html#Page_3" class="pginternal">p. 3</a></td></tr>
<tr><td style="text-align: left;"><i>That Light spreads spherically, almost as Sound does.</i></td><td style="text-align: left;"><a href="https://www.gutenberg.org/cache/epub/14725/pg14725-images.html#Page_4" class="pginternal">p. 4</a></td></tr>
<tr><td style="text-align: left;"><i>Whether Light takes time to spread.</i></td><td style="text-align: left;"><a href="https://www.gutenberg.org/cache/epub/14725/pg14725-images.html#Page_4" class="pginternal">p. 4</a></td></tr>
<tr><td style="text-align: left;"><i>Experience seeming to prove that it passes instantaneously.</i></td><td style="text-align: left;"><a href="https://www.gutenberg.org/cache/epub/14725/pg14725-images.html#Page_5" class="pginternal">p. 5</a></td></tr>
<tr><td style="text-align: left;"><i>Experience proving that it takes time.</i></td><td style="text-align: left;"><a href="https://www.gutenberg.org/cache/epub/14725/pg14725-images.html#Page_8" class="pginternal">p. 8</a></td></tr>
<tr><td style="text-align: left;"><i>How much its speed is greater than that of Sound.</i></td><td style="text-align: left;"><a href="https://www.gutenberg.org/cache/epub/14725/pg14725-images.html#Page_10" class="pginternal">p. 10</a></td></tr>
<tr><td style="text-align: left;"><i>In what the emission of Light differs from that of Sound.</i></td><td style="text-align: left;"><a href="https://www.gutenberg.org/cache/epub/14725/pg14725-images.html#Page_10" class="pginternal">p. 10</a></td></tr>
<tr><td style="text-align: left;"><i>That it is not the same medium which serves for Light and Sound.</i></td><td style="text-align: left;"><a href="https://www.gutenberg.org/cache/epub/14725/pg14725-images.html#Page_11" class="pginternal">p. 11</a></td></tr>
<tr><td style="text-align: left;"><i>How Sound is propagated.</i></td><td style="text-align: left;"><a href="https://www.gutenberg.org/cache/epub/14725/pg14725-images.html#Page_12" class="pginternal">p. 12</a></td></tr>
<tr><td style="text-align: left;"><i>How Light is propagated.</i></td><td style="text-align: left;"><a href="https://www.gutenberg.org/cache/epub/14725/pg14725-images.html#Page_14" class="pginternal">p. 14</a></td></tr>
<tr><td style="text-align: left;"><i>Detailed Remarks on the propagation of Light.</i></td><td style="text-align: left;"><a href="https://www.gutenberg.org/cache/epub/14725/pg14725-images.html#Page_15" class="pginternal">p. 15</a></td></tr>
<tr><td style="text-align: left;"><i>Why Rays are propagated only in straight lines.</i></td><td style="text-align: left;"><a href="https://www.gutenberg.org/cache/epub/14725/pg14725-images.html#Page_20" class="pginternal">p. 20</a></td></tr>
<tr><td style="text-align: left;"><i>How Light coming in different directions can cross itself.</i></td><td style="text-align: left;"><a href="https://www.gutenberg.org/cache/epub/14725/pg14725-images.html#Page_22" class="pginternal">p. 22</a></td></tr>
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<tr><td>
<a href="https://www.gutenberg.org/cache/epub/14725/pg14725-images.html#CHAPTER_II" class="pginternal"><b>CHAP. II. On Reflexion.</b></a>
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<tbody><tr><td style="text-align: left;"><i>Demonstration of equality of angles of incidence and reflexion.</i></td><td style="text-align: left;"><a href="https://www.gutenberg.org/cache/epub/14725/pg14725-images.html#Page_23" class="pginternal">p. 23</a> </td></tr>
<tr><td style="text-align: left;"><i>Why the incident and reflected rays are in the same plane perpendicular to the reflecting surface.</i></td><td style="text-align: left;"><a href="https://www.gutenberg.org/cache/epub/14725/pg14725-images.html#Page_25" class="pginternal">p. 25</a></td></tr>
<tr><td style="text-align: left;"><i>That it is not needful for the reflecting surface to be perfectly flat to attain equality of the angles of incidence and reflexion.</i></td><td style="text-align: left;"><a href="https://www.gutenberg.org/cache/epub/14725/pg14725-images.html#Page_27" class="pginternal">p. 27</a></td></tr>
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<a href="https://www.gutenberg.org/cache/epub/14725/pg14725-images.html#CHAPTER_III" class="pginternal"><b>CHAP. III. On Refraction.</b></a>
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<tbody><tr><td style="text-align: left;"><i>That bodies may be transparent without any substance passing through them.</i></td><td style="text-align: left;"><a href="https://www.gutenberg.org/cache/epub/14725/pg14725-images.html#Page_29" class="pginternal">p. 29</a></td></tr>
<tr><td style="text-align: left;"><i>Proof that the ethereal matter passes through transparent bodies.</i></td><td style="text-align: left;"><a href="https://www.gutenberg.org/cache/epub/14725/pg14725-images.html#Page_30" class="pginternal">p. 30</a></td></tr>
<tr><td style="text-align: left;"><i>How this matter passing through can render them transparent.</i></td><td style="text-align: left;"><a href="https://www.gutenberg.org/cache/epub/14725/pg14725-images.html#Page_31" class="pginternal">p. 31</a></td></tr>
<tr><td style="text-align: left;"><i>That the most solid bodies in appearance are of a very loose texture.</i></td><td style="text-align: left;"><a href="https://www.gutenberg.org/cache/epub/14725/pg14725-images.html#Page_31" class="pginternal">p. 31</a></td></tr>
<tr><td style="text-align: left;"><i>That Light spreads more slowly in water and in glass than in air.</i></td><td style="text-align: left;"><a href="https://www.gutenberg.org/cache/epub/14725/pg14725-images.html#Page_32" class="pginternal">p. 32</a></td></tr>
<tr><td style="text-align: left;"><i>Third hypothesis to explain transparency, and the retardation which Light suffers.</i></td><td style="text-align: left;"><a href="https://www.gutenberg.org/cache/epub/14725/pg14725-images.html#Page_32" class="pginternal">p. 32</a></td></tr>
<tr><td style="text-align: left;"><i>On that which makes bodies opaque.</i></td><td style="text-align: left;"><a href="https://www.gutenberg.org/cache/epub/14725/pg14725-images.html#Page_34" class="pginternal">p. 34</a></td></tr>
<tr><td style="text-align: left;"><i>Demonstration why Refraction obeys the known proportion of Sines.</i></td><td style="text-align: left;"><a href="https://www.gutenberg.org/cache/epub/14725/pg14725-images.html#Page_35" class="pginternal">p. 35</a></td></tr>
<tr><td style="text-align: left;"><i>Why the incident and refracted Rays produce one another reciprocally.</i></td><td style="text-align: left;"><a href="https://www.gutenberg.org/cache/epub/14725/pg14725-images.html#Page_39" class="pginternal">p. 39</a></td></tr>
<tr><td style="text-align: left;"><i>Why Reflexion within a triangular glass prism is suddenly augmented when the Light can no longer penetrate.</i></td><td style="text-align: left;"><a href="https://www.gutenberg.org/cache/epub/14725/pg14725-images.html#Page_40" class="pginternal">p. 40</a></td></tr>
<tr><td style="text-align: left;"><i>That bodies which cause greater Refraction also cause stronger Reflexion.</i></td><td style="text-align: left;"><a href="https://www.gutenberg.org/cache/epub/14725/pg14725-images.html#Page_42" class="pginternal">p. 42</a></td></tr>
<tr><td style="text-align: left;"><i>Demonstration of the Theorem of Mr. Fermat.</i></td><td style="text-align: left;"><a href="https://www.gutenberg.org/cache/epub/14725/pg14725-images.html#Page_43" class="pginternal">p. 43</a></td></tr>
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<a href="https://www.gutenberg.org/cache/epub/14725/pg14725-images.html#CHAPTER_IV" class="pginternal"><b>CHAP. IV. On the Refraction of the Air.</b></a>
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<tbody><tr><td style="text-align: left;"><i>That the emanations of Light in the air are not spherical.</i></td><td style="text-align: left;"><a href="https://www.gutenberg.org/cache/epub/14725/pg14725-images.html#Page_45" class="pginternal">p. 45</a></td></tr>
<tr><td style="text-align: left;"><i>How consequently some objects appear higher than they are.</i></td><td style="text-align: left;"><a href="https://www.gutenberg.org/cache/epub/14725/pg14725-images.html#Page_47" class="pginternal">p. 47</a></td></tr>
<tr><td style="text-align: left;"><i>How the Sun may appear on the Horizon before he has risen.</i></td><td style="text-align: left;"><a href="https://www.gutenberg.org/cache/epub/14725/pg14725-images.html#Page_49" class="pginternal">p. 49</a></td></tr>
<tr><td style="text-align: left;"><i>That the rays of light become curved in the Air of the Atmosphere, and what effects this produces.</i></td><td style="text-align: left;"><a href="https://www.gutenberg.org/cache/epub/14725/pg14725-images.html#Page_50" class="pginternal">p. 50</a></td></tr>
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<a href="https://www.gutenberg.org/cache/epub/14725/pg14725-images.html#CHAPTER_V" class="pginternal"><b>CHAP. V. On the Strange Refraction of Iceland Crystal.</b></a>
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<tbody><tr><td style="text-align: left;"><i>That this Crystal grows also in other countries.</i></td><td style="text-align: left;"><a href="https://www.gutenberg.org/cache/epub/14725/pg14725-images.html#Page_52" class="pginternal">p. 52</a></td></tr>
<tr><td style="text-align: left;"><i>Who first-wrote about it.</i></td><td style="text-align: left;"><a href="https://www.gutenberg.org/cache/epub/14725/pg14725-images.html#Page_53" class="pginternal">p. 53</a></td></tr>
<tr><td style="text-align: left;"><i>Description of Iceland Crystal; its substance, shape, and properties.</i></td><td style="text-align: left;"><a href="https://www.gutenberg.org/cache/epub/14725/pg14725-images.html#Page_53" class="pginternal">p. 53</a></td></tr>
<tr><td style="text-align: left;"><i>That it has two different Refractions.</i></td><td style="text-align: left;"><a href="https://www.gutenberg.org/cache/epub/14725/pg14725-images.html#Page_54" class="pginternal">p. 54</a></td></tr>
<tr><td style="text-align: left;"><i>That the ray perpendicular to the surface suffers refraction, and that some rays inclined to the surface pass without suffering refraction.</i></td><td style="text-align: left;"><a href="https://www.gutenberg.org/cache/epub/14725/pg14725-images.html#Page_55" class="pginternal">p. 55</a></td></tr>
<tr><td style="text-align: left;"><i>Observation of the refractions in this Crystal.</i></td><td style="text-align: left;"><a href="https://www.gutenberg.org/cache/epub/14725/pg14725-images.html#Page_56" class="pginternal">p. 56</a></td></tr>
<tr><td style="text-align: left;"><i>That there is a Regular and an Irregular Refraction.</i></td><td style="text-align: left;"><a href="https://www.gutenberg.org/cache/epub/14725/pg14725-images.html#Page_57" class="pginternal">p. 57</a></td></tr>
<tr><td style="text-align: left;"><i>The way of measuring the two Refractions of Iceland Crystal.</i></td><td style="text-align: left;"><a href="https://www.gutenberg.org/cache/epub/14725/pg14725-images.html#Page_57" class="pginternal">p. 57</a></td></tr>
<tr><td style="text-align: left;"><i>Remarkable properties of the Irregular Refraction.</i></td><td style="text-align: left;"><a href="https://www.gutenberg.org/cache/epub/14725/pg14725-images.html#Page_60" class="pginternal">p. 60</a></td></tr>
<tr><td style="text-align: left;"><i>Hypothesis to explain the double Refraction.</i></td><td style="text-align: left;"><a href="https://www.gutenberg.org/cache/epub/14725/pg14725-images.html#Page_61" class="pginternal">p. 61</a></td></tr>
<tr><td style="text-align: left;"><i>That Rock Crystal has also a double Refraction.</i></td><td style="text-align: left;"><a href="https://www.gutenberg.org/cache/epub/14725/pg14725-images.html#Page_62" class="pginternal">p. 62</a></td></tr>
<tr><td style="text-align: left;"><i>Hypothesis of emanations of Light, within Iceland Crystal, of spheroidal form, for the Irregular Refraction.</i></td><td style="text-align: left;"><a href="https://www.gutenberg.org/cache/epub/14725/pg14725-images.html#Page_63" class="pginternal">p. 63</a></td></tr>
<tr><td style="text-align: left;"><i>How a perpendicular ray can suffer Refraction.</i></td><td style="text-align: left;"><a href="https://www.gutenberg.org/cache/epub/14725/pg14725-images.html#Page_64" class="pginternal">p. 64</a></td></tr>
<tr><td style="text-align: left;"><i>How the position and form of the spheroidal emanations in this Crystal can be defined.</i></td><td style="text-align: left;"><a href="https://www.gutenberg.org/cache/epub/14725/pg14725-images.html#Page_65" class="pginternal">p. 65</a></td></tr>
<tr><td style="text-align: left;"><i>Explanation of the Irregular Refraction by these spheroidal emanations.</i></td><td style="text-align: left;"><a href="https://www.gutenberg.org/cache/epub/14725/pg14725-images.html#Page_67" class="pginternal">p. 67</a></td></tr>
<tr><td style="text-align: left;"><i>Easy way to find the Irregular Refraction of each incident ray.</i></td><td style="text-align: left;"><a href="https://www.gutenberg.org/cache/epub/14725/pg14725-images.html#Page_70" class="pginternal">p. 70</a></td></tr>
<tr><td style="text-align: left;"><i>Demonstration of the oblique ray which traverses the Crystal without being refracted.</i></td><td style="text-align: left;"><a href="https://www.gutenberg.org/cache/epub/14725/pg14725-images.html#Page_73" class="pginternal">p. 73</a></td></tr>
<tr><td style="text-align: left;"><i>Other irregularities of Refraction explained.</i></td><td style="text-align: left;"><a href="https://www.gutenberg.org/cache/epub/14725/pg14725-images.html#Page_76" class="pginternal">p. 76</a></td></tr>
<tr><td style="text-align: left;"><i>That an object placed beneath the Crystal appears double, in two images of different heights.</i></td><td style="text-align: left;"><a href="https://www.gutenberg.org/cache/epub/14725/pg14725-images.html#Page_81" class="pginternal">p. 81</a></td></tr>
<tr><td style="text-align: left;"><i>Why the apparent heights of one of the images change on changing the position of the eyes above the Crystal.</i></td><td style="text-align: left;"><a href="https://www.gutenberg.org/cache/epub/14725/pg14725-images.html#Page_85" class="pginternal">p. 85</a></td></tr>
<tr><td style="text-align: left;"><i>Of the different sections of this Crystal which produce yet other refractions, and confirm all this Theory.</i></td><td style="text-align: left;"><a href="https://www.gutenberg.org/cache/epub/14725/pg14725-images.html#Page_88" class="pginternal">p. 88</a></td></tr>
<tr><td style="text-align: left;"><i>Particular way of polishing the surfaces after it has been cut.</i></td><td style="text-align: left;"><a href="https://www.gutenberg.org/cache/epub/14725/pg14725-images.html#Page_91" class="pginternal">p. 91</a></td></tr>
<tr><td style="text-align: left;"><i>Surprising phenomenon touching the rays which pass through two separated pieces; the cause of which is not explained.</i></td><td style="text-align: left;"><a href="https://www.gutenberg.org/cache/epub/14725/pg14725-images.html#Page_92" class="pginternal">p. 92</a></td></tr>
<tr><td style="text-align: left;"><i>Probable conjecture on the internal composition of Iceland Crystal, and of what figure its particles are.</i></td><td style="text-align: left;"><a href="https://www.gutenberg.org/cache/epub/14725/pg14725-images.html#Page_95" class="pginternal">p. 95</a></td></tr>
<tr><td style="text-align: left;"><i>Tests to confirm this conjecture.</i></td><td style="text-align: left;"><a href="https://www.gutenberg.org/cache/epub/14725/pg14725-images.html#Page_97" class="pginternal">p. 97</a></td></tr>
<tr><td style="text-align: left;"><i>Calculations which have been supposed in this Chapter.</i></td><td style="text-align: left;"><a href="https://www.gutenberg.org/cache/epub/14725/pg14725-images.html#Page_99" class="pginternal">p. 99</a></td></tr>
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<a href="https://www.gutenberg.org/cache/epub/14725/pg14725-images.html#CHAPTER_VI" class="pginternal"><b>CHAP. VI. On the Figures of transparent bodies which serve for Refraction and for Reflexion.</b></a>
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<tbody><tr><td style="text-align: left;"><i>General and easy rule to find these Figures.</i></td><td style="text-align: left;"><a href="https://www.gutenberg.org/cache/epub/14725/pg14725-images.html#Page_106" class="pginternal">p. 106</a></td></tr>
<tr><td style="text-align: left;"><i>Invention of the Ovals of Mr. Des Cartes for Dioptrics.</i></td><td style="text-align: left;"><a href="https://www.gutenberg.org/cache/epub/14725/pg14725-images.html#Page_109" class="pginternal">p. 109</a></td></tr>
<tr><td style="text-align: left;"><i>How he was able to find these Lines.</i></td><td style="text-align: left;"><a href="https://www.gutenberg.org/cache/epub/14725/pg14725-images.html#Page_114" class="pginternal">p. 114</a></td></tr>
<tr><td style="text-align: left;"><i>Way of finding the surface of a glass for perfect refraction, when the other surface is given.</i></td><td style="text-align: left;"><a href="https://www.gutenberg.org/cache/epub/14725/pg14725-images.html#Page_116" class="pginternal">p. 116</a></td></tr>
<tr><td style="text-align: left;"><i>Remark on what happens to rays refracted at a spherical surface.</i></td><td style="text-align: left;"><a href="https://www.gutenberg.org/cache/epub/14725/pg14725-images.html#Page_123" class="pginternal">p. 123</a></td></tr>
<tr><td style="text-align: left;"><i>Remark on the curved line which is formed by reflexion in a spherical concave mirror.</i></td><td style="text-align: left;"><a href="https://www.gutenberg.org/cache/epub/14725/pg14725-images.html#Page_126" class="pginternal">p. 126</a></td></tr>
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<div><span class="pagenum">[Pg 1]</span><a id="Page_1"></a></div>
<div class="figcenter" style="width: 600px;">
<img alt="" height="137" src="./The Project Gutenberg eBook of Treatise on Light, by Christiaan Huygens_files/ch01head.png" title="" width="600" id="id-5061221996984011727">
</div>
<h1>TREATISE ON LIGHT</h1>
<h2><a id="CHAPTER_I"></a>CHAPTER I</h2>
<h3>ON RAYS PROPAGATED IN STRAIGHT LINES</h3>
<div style="width: 154px; float: left; margin-right: .2em;">
<img alt="A" height="150" src="./The Project Gutenberg eBook of Treatise on Light, by Christiaan Huygens_files/ch01.png" title="A" width="154" id="id-6947915879938039392">
</div><p>s happens in all the sciences in which Geometry is applied to matter,
the demonstrations concerning Optics are founded on truths drawn from
experience. Such are that the rays of light are propagated in straight
lines; that the angles of reflexion and of incidence are equal; and
that in refraction the ray is bent according to the law of sines, now
so well known, and which is no less certain than the preceding laws.</p>
<p>The majority of those who have written touching the various parts of
Optics have contented themselves with presuming these truths. But
some, more inquiring, have desired to investigate the origin and the
causes, considering these to be in themselves wonderful effects of
Nature. In which they advanced some ingenious things, but not however
such that the most intelligent folk do not wish for better and more
satisfactory explanations. Wherefore I here desire to propound what I
have meditated on the sub<span class="pagenum">[Pg 2]</span><a id="Page_2"></a>ject, so as to contribute as much as I can
to the explanation of this department of Natural Science, which, not
without reason, is reputed to be one of its most difficult parts. I
recognize myself to be much indebted to those who were the first to
begin to dissipate the strange obscurity in which these things were
enveloped, and to give us hope that they might be explained by
intelligible reasoning. But, on the other hand I am astonished also
that even here these have often been willing to offer, as assured and
demonstrative, reasonings which were far from conclusive. For I do not
find that any one has yet given a probable explanation of the first
and most notable phenomena of light, namely why it is not propagated
except in straight lines, and how visible rays, coming from an
infinitude of diverse places, cross one another without hindering one
another in any way.</p>
<p>I shall therefore essay in this book, to give, in accordance with the
principles accepted in the Philosophy of the present day, some clearer
and more probable reasons, firstly of these properties of light
propagated rectilinearly; secondly of light which is reflected on
meeting other bodies. Then I shall explain the phenomena of those rays
which are said to suffer refraction on passing through transparent
bodies of different sorts; and in this part I shall also explain the
effects of the refraction of the air by the different densities of the
Atmosphere.</p>
<p>Thereafter I shall examine the causes of the strange refraction of a
certain kind of Crystal which is brought from Iceland. And finally I
shall treat of the various shapes of transparent and reflecting bodies
by which rays are collected at a point or are turned aside in various
ways. From this it will be seen with what facility, following our new
Theory, we find not only the Ellipses, Hyperbolas, and <span class="pagenum">[Pg 3]</span><a id="Page_3"></a>other curves
which Mr. Des Cartes has ingeniously invented for this purpose; but
also those which the surface of a glass lens ought to possess when its
other surface is given as spherical or plane, or of any other figure
that may be.</p>
<p>It is inconceivable to doubt that light consists in the motion of some
sort of matter. For whether one considers its production, one sees
that here upon the Earth it is chiefly engendered by fire and flame
which contain without doubt bodies that are in rapid motion, since
they dissolve and melt many other bodies, even the most solid; or
whether one considers its effects, one sees that when light is
collected, as by concave mirrors, it has the property of burning as a
fire does, that is to say it disunites the particles of bodies. This
is assuredly the mark of motion, at least in the true Philosophy, in
which one conceives the causes of all natural effects in terms of
mechanical motions. This, in my opinion, we must necessarily do, or
else renounce all hopes of ever comprehending anything in Physics.</p>
<p>And as, according to this Philosophy, one holds as certain that the
sensation of sight is excited only by the impression of some movement
of a kind of matter which acts on the nerves at the back of our eyes,
there is here yet one reason more for believing that light consists in
a movement of the matter which exists between us and the luminous
body.</p>
<p>Further, when one considers the extreme speed with which light spreads
on every side, and how, when it comes from different regions, even
from those directly opposite, the rays traverse one another without
hindrance, one may well understand that when we see a luminous object,
it cannot be by any transport of matter coming to us from this object,
<span class="pagenum">[Pg 4]</span><a id="Page_4"></a>in the way in which a shot or an arrow traverses the air; for
assuredly that would too greatly impugn these two properties of light,
especially the second of them. It is then in some other way that light
spreads; and that which can lead us to comprehend it is the knowledge
which we have of the spreading of Sound in the air.</p>
<p>We know that by means of the air, which is an invisible and impalpable
body, Sound spreads around the spot where it has been produced, by a
movement which is passed on successively from one part of the air to
another; and that the spreading of this movement, taking place equally
rapidly on all sides, ought to form spherical surfaces ever enlarging
and which strike our ears. Now there is no doubt at all that light
also comes from the luminous body to our eyes by some movement
impressed on the matter which is between the two; since, as we have
already seen, it cannot be by the transport of a body which passes
from one to the other. If, in addition, light takes time for its
passage—which we are now going to examine—it will follow that this
movement, impressed on the intervening matter, is successive; and
consequently it spreads, as Sound does, by spherical surfaces and
waves: for I call them waves from their resemblance to those which are
seen to be formed in water when a stone is thrown into it, and which
present a successive spreading as circles, though these arise from
another cause, and are only in a flat surface.</p>
<p>To see then whether the spreading of light takes time, let us consider
first whether there are any facts of experience which can convince us
to the contrary. As to those which can be made here on the Earth, by
striking lights at great distances, although they prove that light
takes no sensible time to pass over these distances, one may say with
good <span class="pagenum">[Pg 5]</span><a id="Page_5"></a>reason that they are too small, and that the only conclusion to
be drawn from them is that the passage of light is extremely rapid.
Mr. Des Cartes, who was of opinion that it is instantaneous, founded
his views, not without reason, upon a better basis of experience,
drawn from the Eclipses of the Moon; which, nevertheless, as I shall
show, is not at all convincing. I will set it forth, in a way a little
different from his, in order to make the conclusion more
comprehensible.</p>
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<p>Let A be the place of the sun, BD a part of the orbit or annual path
of the Earth: ABC a straight line which I suppose to meet the orbit of
the Moon, which is represented by the circle CD, at C.</p>
<p>Now if light requires time, for example one hour, to traverse the
space which is between the Earth and the Moon, it will follow that the
Earth having arrived at B, the shadow which it casts, or the
interruption of the light, will not yet have arrived at the point C,
but will only arrive there an hour after. It will then be one hour
after, reckoning from the moment when the Earth was at B, <span class="pagenum">[Pg 6]</span><a id="Page_6"></a>that the
Moon, arriving at C, will be obscured: but this obscuration or
interruption of the light will not reach the Earth till after another
hour. Let us suppose that the Earth in these two hours will have
arrived at E. The Earth then, being at E, will see the Eclipsed Moon
at C, which it left an hour before, and at the same time will see the
sun at A. For it being immovable, as I suppose with Copernicus, and
the light moving always in straight lines, it must always appear where
it is. But one has always observed, we are told, that the eclipsed
Moon appears at the point of the Ecliptic opposite to the Sun; and yet
here it would appear in arrear of that point by an amount equal to the
angle GEC, the supplement of AEC. This, however, is contrary to
experience, since the angle GEC would be very sensible, and about 33
degrees. Now according to our computation, which is given in the
Treatise on the causes of the phenomena of Saturn, the distance BA
between the Earth and the Sun is about twelve thousand diameters of
the Earth, and hence four hundred times greater than BC the distance
of the Moon, which is 30 diameters. Then the angle ECB will be nearly
four hundred times greater than BAE, which is five minutes; namely,
the path which the earth travels in two hours along its orbit; and
thus the angle BCE will be nearly 33 degrees; and likewise the angle
CEG, which is greater by five minutes.</p>
<p>But it must be noted that the speed of light in this argument has been
assumed such that it takes a time of one hour to make the passage from
here to the Moon. If one supposes that for this it requires only one
minute of time, then it is manifest that the angle CEG will only be 33
minutes; and if it requires only ten seconds of time, <span class="pagenum">[Pg 7]</span><a id="Page_7"></a>the angle will
be less than six minutes. And then it will not be easy to perceive
anything of it in observations of the Eclipse; nor, consequently, will
it be permissible to deduce from it that the movement of light is
instantaneous.</p>
<p>It is true that we are here supposing a strange velocity that would be
a hundred thousand times greater than that of Sound. For Sound,
according to what I have observed, travels about 180 Toises in the
time of one Second, or in about one beat of the pulse. But this
supposition ought not to seem to be an impossibility; since it is not
a question of the transport of a body with so great a speed, but of a
successive movement which is passed on from some bodies to others. I
have then made no difficulty, in meditating on these things, in
supposing that the emanation of light is accomplished with time,
seeing that in this way all its phenomena can be explained, and that
in following the contrary opinion everything is incomprehensible. For
it has always seemed tome that even Mr. Des Cartes, whose aim has been
to treat all the subjects of Physics intelligibly, and who assuredly
has succeeded in this better than any one before him, has said nothing
that is not full of difficulties, or even inconceivable, in dealing
with Light and its properties.</p>
<p>But that which I employed only as a hypothesis, has recently received
great seemingness as an established truth by the ingenious proof of
Mr. Römer which I am going here to relate, expecting him himself to
give all that is needed for its confirmation. It is founded as is the
preceding argument upon celestial observations, and proves not only
that Light takes time for its passage, but also demonstrates how much
time it takes, and that its velocity is even at least six times
greater than that which I have just stated.</p>
<p><span class="pagenum">[Pg 8]</span><a id="Page_8"></a>For this he makes use of the Eclipses suffered by the little planets
which revolve around Jupiter, and which often enter his shadow: and
see what is his reasoning. Let A be the Sun, BCDE the annual orbit of
the Earth, F Jupiter, GN the orbit of the nearest of his Satellites,
for it is this one which is more apt for this investigation than any
of the other three, because of the quickness of its revolution. Let G
be this Satellite entering into the shadow of Jupiter, H the same
Satellite emerging from the shadow.</p>
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<p>Let it be then supposed, the Earth being at B some time before the
last quadrature, that one has seen the said Satellite emerge from the
shadow; it must needs be, if the Earth remains at the same place,
that, after 42-1/2 hours, one would again see a similar emergence,
because that is the time in which it makes the round of its orbit, and
when it would come again into opposition to the Sun. And if the Earth,
for instance, were to remain always at B during 30 revolutions of this
Satellite, one would see it again emerge from the shadow after 30
times 42-1/2 hours. But the Earth having been carried along during
this time to C, increasing thus its distance from Jupiter, it follows
that if Light requires time for its passage the illumination of the
little planet will be perceived later at <span class="pagenum">[Pg 9]</span><a id="Page_9"></a>C than it would have been at
B, and that there must be added to this time of 30 times 42-1/2 hours
that which the Light has required to traverse the space MC, the
difference of the spaces CH, BH. Similarly at the other quadrature
when the earth has come to E from D while approaching toward Jupiter,
the immersions of the Satellite ought to be observed at E earlier than
they would have been seen if the Earth had remained at D.</p>
<p>Now in quantities of observations of these Eclipses, made during ten
consecutive years, these differences have been found to be very
considerable, such as ten minutes and more; and from them it has been
concluded that in order to traverse the whole diameter of the annual
orbit KL, which is double the distance from here to the sun, Light
requires about 22 minutes of time.</p>
<p>The movement of Jupiter in his orbit while the Earth passed from B to
C, or from D to E, is included in this calculation; and this makes it
evident that one cannot attribute the retardation of these
illuminations or the anticipation of the eclipses, either to any
irregularity occurring in the movement of the little planet or to its
eccentricity.</p>
<p>If one considers the vast size of the diameter KL, which according to
me is some 24 thousand diameters of the Earth, one will acknowledge
the extreme velocity of Light. For, supposing that KL is no more than
22 thousand of these diameters, it appears that being traversed in 22
minutes this makes the speed a thousand diameters in one minute, that
is 16-2/3 diameters in one second or in one beat of the pulse, which
makes more than 11 hundred times a hundred thousand toises; since the
diameter of the Earth contains 2,865 leagues, reckoned at 25 to the
degree, and each <span class="pagenum">[Pg 10]</span><a id="Page_10"></a>each league is 2,282 Toises, according to the exact
measurement which Mr. Picard made by order of the King in 1669. But
Sound, as I have said above, only travels 180 toises in the same time
of one second: hence the velocity of Light is more than six hundred
thousand times greater than that of Sound. This, however, is quite
another thing from being instantaneous, since there is all the
difference between a finite thing and an infinite. Now the successive
movement of Light being confirmed in this way, it follows, as I have
said, that it spreads by spherical waves, like the movement of Sound.</p>
<p>But if the one resembles the other in this respect, they differ in
many other things; to wit, in the first production of the movement
which causes them; in the matter in which the movement spreads; and in
the manner in which it is propagated. As to that which occurs in the
production of Sound, one knows that it is occasioned by the agitation
undergone by an entire body, or by a considerable part of one, which
shakes all the contiguous air. But the movement of the Light must
originate as from each point of the luminous object, else we should
not be able to perceive all the different parts of that object, as
will be more evident in that which follows. And I do not believe that
this movement can be better explained than by supposing that all those
of the luminous bodies which are liquid, such as flames, and
apparently the sun and the stars, are composed of particles which
float in a much more subtle medium which agitates them with great
rapidity, and makes them strike against the particles of the ether
which surrounds them, and which are much smaller than they. But I hold
also that in luminous solids such as charcoal or metal made red hot in
the fire, this same movement is caused by the violent <span class="pagenum">[Pg 11]</span><a id="Page_11"></a>agitation of
the particles of the metal or of the wood; those of them which are on
the surface striking similarly against the ethereal matter. The
agitation, moreover, of the particles which engender the light ought
to be much more prompt and more rapid than is that of the bodies which
cause sound, since we do not see that the tremors of a body which is
giving out a sound are capable of giving rise to Light, even as the
movement of the hand in the air is not capable of producing Sound.</p>
<p>Now if one examines what this matter may be in which the movement
coming from the luminous body is propagated, which I call Ethereal
matter, one will see that it is not the same that serves for the
propagation of Sound. For one finds that the latter is really that
which we feel and which we breathe, and which being removed from any
place still leaves there the other kind of matter that serves to
convey Light. This may be proved by shutting up a sounding body in a
glass vessel from which the air is withdrawn by the machine which Mr.
Boyle has given us, and with which he has performed so many beautiful
experiments. But in doing this of which I speak, care must be taken to
place the sounding body on cotton or on feathers, in such a way that
it cannot communicate its tremors either to the glass vessel which
encloses it, or to the machine; a precaution which has hitherto been
neglected. For then after having exhausted all the air one hears no
Sound from the metal, though it is struck.</p>
<p>One sees here not only that our air, which does not penetrate through
glass, is the matter by which Sound spreads; but also that it is not
the same air but another kind of matter in which Light spreads; since
if the air is <span class="pagenum">[Pg 12]</span><a id="Page_12"></a>removed from the vessel the Light does not cease to
traverse it as before.</p>
<p>And this last point is demonstrated even more clearly by the
celebrated experiment of Torricelli, in which the tube of glass from
which the quicksilver has withdrawn itself, remaining void of air,
transmits Light just the same as when air is in it. For this proves
that a matter different from air exists in this tube, and that this
matter must have penetrated the glass or the quicksilver, either one
or the other, though they are both impenetrable to the air. And when,
in the same experiment, one makes the vacuum after putting a little
water above the quicksilver, one concludes equally that the said
matter passes through glass or water, or through both.</p>
<p>As regards the different modes in which I have said the movements of
Sound and of Light are communicated, one may sufficiently comprehend
how this occurs in the case of Sound if one considers that the air is
of such a nature that it can be compressed and reduced to a much
smaller space than that which it ordinarily occupies. And in
proportion as it is compressed the more does it exert an effort to
regain its volume; for this property along with its penetrability,
which remains notwithstanding its compression, seems to prove that it
is made up of small bodies which float about and which are agitated
very rapidly in the ethereal matter composed of much smaller parts. So
that the cause of the spreading of Sound is the effort which these
little bodies make in collisions with one another, to regain freedom
when they are a little more squeezed together in the circuit of these
waves than elsewhere.</p>
<p>But the extreme velocity of Light, and other properties which it has,
cannot admit of such a propagation of motion, <span class="pagenum">[Pg 13]</span><a id="Page_13"></a>and I am about to show
here the way in which I conceive it must occur. For this, it is
needful to explain the property which hard bodies must possess to
transmit movement from one to another.</p>
<p>When one takes a number of spheres of equal size, made of some very
hard substance, and arranges them in a straight line, so that they
touch one another, one finds, on striking with a similar sphere
against the first of these spheres, that the motion passes as in an
instant to the last of them, which separates itself from the row,
without one's being able to perceive that the others have been
stirred. And even that one which was used to strike remains motionless
with them. Whence one sees that the movement passes with an extreme
velocity which is the greater, the greater the hardness of the
substance of the spheres.</p>
<p>But it is still certain that this progression of motion is not
instantaneous, but successive, and therefore must take time. For if
the movement, or the disposition to movement, if you will have it so,
did not pass successively through all these spheres, they would all
acquire the movement at the same time, and hence would all advance
together; which does not happen. For the last one leaves the whole row
and acquires the speed of the one which was pushed. Moreover there are
experiments which demonstrate that all the bodies which we reckon of
the hardest kind, such as quenched steel, glass, and agate, act as
springs and bend somehow, not only when extended as rods but also when
they are in the form of spheres or of other shapes. That is to say
they yield a little in themselves at the place where they are struck,
and immediately regain their former figure. For I have found that on
striking with a ball of glass or of agate against a large and quite
thick <span class="pagenum">[Pg 14]</span><a id="Page_14"></a>thick piece of the same substance which had a flat surface,
slightly soiled with breath or in some other way, there remained round
marks, of smaller or larger size according as the blow had been weak
or strong. This makes it evident that these substances yield where
they meet, and spring back: and for this time must be required.</p>
<p>Now in applying this kind of movement to that which produces Light
there is nothing to hinder us from estimating the particles of the
ether to be of a substance as nearly approaching to perfect hardness
and possessing a springiness as prompt as we choose. It is not
necessary to examine here the causes of this hardness, or of that
springiness, the consideration of which would lead us too far from our
subject. I will say, however, in passing that we may conceive that the
particles of the ether, notwithstanding their smallness, are in turn
composed of other parts and that their springiness consists in the
very rapid movement of a subtle matter which penetrates them from
every side and constrains their structure to assume such a disposition
as to give to this fluid matter the most overt and easy passage
possible. This accords with the explanation which Mr. Des Cartes gives
for the spring, though I do not, like him, suppose the pores to be in
the form of round hollow canals. And it must not be thought that in
this there is anything absurd or impossible, it being on the contrary
quite credible that it is this infinite series of different sizes of
corpuscles, having different degrees of velocity, of which Nature
makes use to produce so many marvellous effects.</p>
<p>But though we shall ignore the true cause of springiness we still see
that there are many bodies which possess this property; and thus there
is nothing strange in supposing <span class="pagenum">[Pg 15]</span><a id="Page_15"></a>that it exists also in little
invisible bodies like the particles of the Ether. Also if one wishes
to seek for any other way in which the movement of Light is
successively communicated, one will find none which agrees better,
with uniform progression, as seems to be necessary, than the property
of springiness; because if this movement should grow slower in
proportion as it is shared over a greater quantity of matter, in
moving away from the source of the light, it could not conserve this
great velocity over great distances. But by supposing springiness in
the ethereal matter, its particles will have the property of equally
rapid restitution whether they are pushed strongly or feebly; and thus
the propagation of Light will always go on with an equal velocity.</p>
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<p>And it must be known that although the particles of the ether are not
ranged thus in straight lines, as in our row of spheres, but
confusedly, so that one of them touches several others, this does not
hinder them from transmitting their movement and from spreading it
always forward. As to this it is to be remarked that there is a law of
motion serving for this propagation, and verifiable by experiment. It
is that when a sphere, such as A here, touches several other similar
spheres CCC, if it is struck by another sphere B in such a way as to
exert an impulse against all the spheres CCC which touch it, it
transmits to them the whole of its movement, and remains after that
motionless like the sphere B. And without supposing that the ethereal
particles are of spherical form (for I see indeed no need to suppose
them so) one may well understand that this property of communicating
an impulse <span class="pagenum">[Pg 16]</span><a id="Page_16"></a>does not fail to contribute to the aforesaid propagation
of movement.</p>
<p>Equality of size seems to be more necessary, because otherwise there
ought to be some reflexion of movement backwards when it passes from a
smaller particle to a larger one, according to the Laws of Percussion
which I published some years ago.</p>
<p>However, one will see hereafter that we have to suppose such an
equality not so much as a necessity for the propagation of light as
for rendering that propagation easier and more powerful; for it is not
beyond the limits of probability that the particles of the ether have
been made equal for a purpose so important as that of light, at least
in that vast space which is beyond the region of atmosphere and which
seems to serve only to transmit the light of the Sun and the Stars.</p>
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<p>I have then shown in what manner one may conceive Light to spread
successively, by spherical waves, and how it is possible that this
spreading is accomplished with as great a velocity as that which
experiments and celestial observations demand. Whence it may be
further remarked that although the particles are supposed to be in
continual movement (for there are many reasons for this) the
successive propagation of the waves cannot be hindered by this;
because the propagation consists nowise in the transport of those
particles but merely in a small agitation which they cannot help
communicating to those surrounding, notwithstanding any movement which
may act on them causing them to be changing positions amongst
themselves.</p>
<p>But we must consider still more particularly the origin of these
waves, and the manner in which they spread. And, first, it follows
from what has been said on the production <span class="pagenum">[Pg 17]</span><a id="Page_17"></a>of Light, that each little
region of a luminous body, such as the Sun, a candle, or a burning
coal, generates its own waves of which that region is the centre. Thus
in the flame of a candle, having distinguished the points A, B, C,
concentric circles described about each of these points represent the
waves which come from them. And one must imagine the same about every
point of the surface and of the part within the flame.</p>
<p>But as the percussions at the centres of these waves possess no
regular succession, it must not be supposed that the waves themselves
follow one another at equal distances: and if the distances marked in
the figure appear to be such, it is rather to mark the progression of
one and the same wave at equal intervals of time than to represent
several of them issuing from one and the same centre.</p>
<p>After all, this prodigious quantity of waves which traverse one
another without confusion and without effacing one another must not be
deemed inconceivable; it being certain that one and the same particle
of matter can serve for many waves coming from different sides or even
from contrary directions, not only if it is struck by blows which
follow one another closely but even for those which act on it at the
same instant. It can do so because the spreading of the movement is
successive. This may be proved by the row of equal spheres of hard
matter, spoken of above. If against this row there are pushed from two
opposite sides at the same time two similar spheres A and <span class="pagenum">[Pg 18]</span><a id="Page_18"></a>D, one will
see each of them rebound with the same velocity which it had in
striking, yet the whole row will remain in its place, although the
movement has passed along its whole length twice over. And if these
contrary movements happen to meet one another at the middle sphere, B,
or at some other such as C, that sphere will yield and act as a spring
at both sides, and so will serve at the same instant to transmit these
two movements.</p>
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<p>But what may at first appear full strange and even incredible is that
the undulations produced by such small movements and corpuscles,
should spread to such immense distances; as for example from the Sun
or from the Stars to us. For the force of these waves must grow feeble
in proportion as they move away from their origin, so that the action
of each one in particular will without doubt become incapable of
making itself felt to our sight. But one will cease to be astonished
by considering how at a great distance from the luminous body an
infinitude of waves, though they have issued from different points of
this body, unite together in such a way that they sensibly compose one
single wave only, which, consequently, ought to have enough force to
make itself felt. Thus this infinite number of waves which originate
at the same instant from all points of a fixed star, big it may be as
the Sun, make practically only one single wave which may well have
force enough to produce an impression on our eyes. Moreover from each
luminous point there may come many thousands of waves in the smallest
imaginable time, by the frequent percussion of the corpuscles which
strike the <span class="pagenum">[Pg 19]</span><a id="Page_19"></a>Ether at these points: which further contributes to
rendering their action more sensible.</p>
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<p>There is the further consideration in the emanation of these waves,
that each particle of matter in which a wave spreads, ought not to
communicate its motion only to the next particle which is in the
straight line drawn from the luminous point, but that it also imparts
some of it necessarily to all the others which touch it and which
oppose themselves to its movement. So it arises that around each
particle there is made a wave of which that particle is the centre.
Thus if DCF is a wave emanating from the luminous point A, which is
its centre, the particle B, one of those comprised within the sphere
DCF, will have made its particular or partial wave KCL, which will
touch the wave DCF at C at the same moment that the principal wave
emanating from the point A has arrived at DCF; and it is clear that it
will be only the region C of the wave KCL which will touch the wave
DCF, to wit, that which is in the straight line drawn through AB.
Similarly the other particles of the sphere DCF, such as <i>bb</i>, <i>dd</i>,
etc., will each make its own wave. But each of these waves can be
infinitely feeble only as compared with the wave DCF, to the
composition of which all the others contribute by the part of their
surface which is most distant from the centre A.</p>
<p><span class="pagenum">[Pg 20]</span><a id="Page_20"></a>One sees, in addition, that the wave DCF is determined by the
distance attained in a certain space of time by the movement which
started from the point A; there being no movement beyond this wave,
though there will be in the space which it encloses, namely in parts
of the particular waves, those parts which do not touch the sphere
DCF. And all this ought not to seem fraught with too much minuteness
or subtlety, since we shall see in the sequel that all the properties
of Light, and everything pertaining to its reflexion and its
refraction, can be explained in principle by this means. This is a
matter which has been quite unknown to those who hitherto have begun
to consider the waves of light, amongst whom are Mr. Hooke in his
<i>Micrographia</i>, and Father Pardies, who, in a treatise of which he let
me see a portion, and which he was unable to complete as he died
shortly afterward, had undertaken to prove by these waves the effects
of reflexion and refraction. But the chief foundation, which consists
in the remark I have just made, was lacking in his demonstrations; and
for the rest he had opinions very different from mine, as may be will
appear some day if his writing has been preserved.</p>
<p>To come to the properties of Light. We remark first that each portion
of a wave ought to spread in such a way that its extremities lie
always between the same straight lines drawn from the luminous point.
Thus the portion BG of the wave, having the luminous point A as its
centre, will spread into the arc CE bounded by the straight lines ABC,
AGE. For although the particular waves produced by the particles
comprised within the space CAE spread also outside this space, they
yet do not concur at the same instant to compose a wave which
terminates the <span class="pagenum">[Pg 21]</span><a id="Page_21"></a>movement, as they do precisely at the circumference
CE, which is their common tangent.</p>
<p>And hence one sees the reason why light, at least if its rays are not