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<title>An Extract of a Letter lately written by an ingenious person from Paris [Christiaan Huygens]</title>
<title type="short">Some Considerations upon <hi rend="italic">Mr. Newton's</hi> Doctrine of <hi rend="italic">Colors</hi></title>
<author xml:id="ch"><persName key="nameid_8" sort="Huygens, Christiaan" ref="nameid_8" xml:base="http://www.newtonproject.sussex.ac.uk/catalogue/xml/persNames.xml">Christiaan Huygens</persName></author>

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<extent><hi rend="italic">c.</hi> <num n="word_count" value="559">559</num> words</extent>

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<note type="metadataLine">21 July 1673, in English, <hi rend="italic">c.</hi> 563 words, 2pp.</note>
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<p>in English</p>
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<linkGrp n="document_relations" xml:base="http://www.newtonproject.sussex.ac.uk/view/normalized/"><ptr type="is_responded_by" target="NATP00017">Mr. Newtons Answer to the foregoing Letter [of Christiaan Huygens] [<hi rend="italic">Philosophical Transactions</hi> 96 (21 July 1673)]</ptr><ptr type="is_responded_by" target="NATP00018">An Extract of Mr Isaac Newton's Letter … concerning the Number of Colors [<hi rend="italic">Philosophical Transactions</hi> 97 (6 October 1673)]</ptr><ptr type="is_responded_by" target="NATP00317">Answer to Huygens' critique of Newton's new theory of light and colours, dated 10 June 1673 [EL/N1/47]</ptr><ptr type="is_response_to" target="NATP00028">Mr Isaac Newtons Answer to some Considerations [of Robert Hooke] upon his doctrine of Light and Colors [<hi rend="italic">Philosophical Transactions</hi> 88 (18 November 1672)]</ptr></linkGrp>
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<change when="2001-01-01" type="metadata">Catalogue information compiled by Rob Iliffe, Peter Spargo &amp; John Young</change>
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<pb xml:id="p6086" n="6086"/><fw type="pag" place="topRight">(6086)</fw>
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<head xml:id="hd1"><hi rend="italic">An Extract of a Letter lately written by an ingenious person from</hi> Paris, <hi rend="italic">containing some Considerations upon</hi> M<hi rend="italic">r</hi>. Newtons <hi rend="italic">Doctrine of</hi> Colors, <hi rend="italic">as also upon the effects of the different Refractions of the Rays in Telescopical Glasses</hi>.</head>
<p rend="indent0" xml:id="par1"><hi rend="dropCap">I</hi> Have seen, how Mr. <hi rend="italic">Newton</hi> endeavours to maintain his new Theory concerning <hi rend="italic">Colours</hi>. Me thinks, that the most im<lb type="hyphenated" xml:id="l1"/>portant Objection, which is made against him by way of <hi rend="italic">Quæ<lb type="hyphenated" xml:id="l2"/>re</hi>, is that, Whether there be more than two sorts of Colours. For my part, I believe, that an <hi rend="italic">Hypothesis</hi>, that should explain mechanically and by the nature of motion the Colours <hi rend="italic"><choice><sic>Jellow</sic><corr>Yellow</corr></choice></hi> and <hi rend="italic">Blew</hi>, would be sufficient for all the rest, in regard that those others, being only more deeply charged (as appears by the Prismes of Mr. <hi rend="italic">Hook</hi>,) do produce the dark or deep-Red and Blew; and that of these four all the other colors may be compounded. Neither do I see, why Mr. <hi rend="italic">Newton</hi> doth not con<lb type="hyphenated" xml:id="l3"/>tent himself with the two Colors, Yellow and Blew; for it will be much more easy to find an <hi rend="italic">Hypothesis</hi> by Motion, that may explicate these two differences, than for so many diversities as there are of <choice><sic>others</sic><corr>other</corr></choice> Colors. And till he hath found this <hi rend="italic">Hypo<lb type="hyphenated" xml:id="l4"/>thesis</hi>, he hath not taught us, what it is wherein consists the na<lb type="hyphenated" xml:id="l5"/>ture and difference of Colours, but only this accident (which certainly is very considerable,) of their <hi rend="italic">different Refrangibi<lb type="hyphenated" xml:id="l6"/>lity</hi>.</p>
<p xml:id="par2">As for the composition of <hi rend="italic">White</hi> made by all the Colors to<lb type="hyphenated" xml:id="l7"/>gether, it may possibly be, that <hi rend="italic">Yellow</hi> and <hi rend="italic">Blew</hi> might also be <lb xml:id="l8"/>sufficient for that: Which is worth while to try; and it may be done by the Experiment, which Mr. <hi rend="italic">Newton</hi> proposeth, by receiving against a wall of a darkn'd room the Colours of the Prisme, and to cast their reflected light upon white pa<lb type="hyphenated" xml:id="l9"/>per. Here you must hinder the Colors of the extremeties, <hi rend="italic">viz</hi>. the Red and Purple, from striking against the wall, and leave only the intermediate Colors; yellow, green and blew, to see, whether the light of these alone would not make the paper appear white, as well as when they all give light. I even doubt, whether the lightest place of the yellow color may not all a<lb type="hyphenated" xml:id="l10"/>lone produce that effect, and I mean to try it at the first con<lb type="hyphenated" xml:id="l11"/>veniency; for this thought never came into my mind but just <fw type="catch" place="bottomRight">now</fw><pb xml:id="p6087" n="6087"/><fw type="pag" place="topRight">(6087)</fw> now. Mean time you may see, that if these Experiments do succeed, it can no more be said, that all the Colors are neccessa<lb type="hyphenated" xml:id="l12"/>ry to compound White, and that 'tis very probable, that all the rest are nothing but degrees of <hi rend="italic">Yellow</hi> and <hi rend="italic">Blew</hi>, more or less <lb xml:id="l13"/>charged.</p>
<p xml:id="par3">Lastly, touching the Effect of the different Refractions of the Rays in Telescopical Glasses, 'tis certain, that Experience agrees not with what Mr. <hi rend="italic">Newton</hi> holds. For to consider only a picture, which is made by an object-glass of 12 feet in a dark room, we see, it is too distinct and too well defined to be produced by rayes, that should stray the 50<hi rend="italic">th</hi>. part*<anchor xml:id="n002-01"/> <note target="#n002-01"><hi rend="italic">Compare herewith what Mr</hi>. Newton <hi rend="italic">saith in</hi> Numb. 80. <hi rend="italic">of these Tracts</hi>, pag. 3079.</note> of the Aperture. So that, (as I believe I have told you heretofore) the difference of the Refrangibility doth not, it may be, alwayes follow the same proportion in the great and small inclinations of the Rayes upon the surface of the Glass.</p>
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