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<title xml:id="main_title">Original letter from Isaac Newton to Richard Bentley, dated 17 January 1692/3</title>
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<extent><hi rend="italic">c.</hi> <num n="word_count" value="1313">1,313</num> words</extent>

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<date>2007</date>
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<note type="metadataLine">17 January 1692/3, in English, <hi rend="italic">c.</hi> 1,331 words.</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_follow_up_to" target="THEM00254">Original letter from Isaac Newton to Richard Bentley, dated 10 December 1692 [189.R.4.47, ff. 4A-5]</ptr><ptr type="is_followed_up_by" target="THEM00256">Original letter from Isaac Newton to Richard Bentley, dated 11 February 1692/3 [189.R.4.47, f. 6]</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="p005r" n="5"/><fw type="pag">5</fw>
<p xml:id="par1"><choice><abbr>S<hi rend="superscript">r</hi></abbr><expan>Sir</expan></choice></p>
<p xml:id="par2">I agree with you that if matter eavenly diffused through a finite space <lb xml:id="l1"/>not spherical, should fall into a solid mass, this mass would affect <choice><abbr>y<hi rend="superscript">e</hi></abbr><expan>the</expan></choice> figure <lb xml:id="l2"/>of <choice><abbr>y<hi rend="superscript">e</hi></abbr><expan>the</expan></choice> whole space, provided it were not soft like <choice><abbr>y<hi rend="superscript">e</hi></abbr><expan>the</expan></choice> old Chaos, but so hard &amp; <lb xml:id="l3"/>solid from <choice><abbr>y<hi rend="superscript">e</hi></abbr><expan>the</expan></choice> beginning, that <choice><abbr>y<hi rend="superscript">e</hi></abbr><expan>the</expan></choice> weight of its protuberant parts could not make <lb xml:id="l4"/>it yeild to their pressure. Yet by earthquakes loosing <choice><abbr>y<hi rend="superscript">e</hi></abbr><expan>the</expan></choice> parts of this solid, <choice><abbr>y<hi rend="superscript">e</hi></abbr><expan>the</expan></choice> pro<lb type="hyphenated" xml:id="l5"/>tuberances might sometimes sink alittle by their Weight, &amp; thereby <choice><abbr>y<hi rend="superscript">e</hi></abbr><expan>the</expan></choice> mass might <lb xml:id="l6"/>by degrees approach a spherical figure.</p>
<p xml:id="par3">The reason why matter <add place="supralinear" indicator="yes">eavenly</add> scattered through a finite space would convene in <lb xml:id="l7"/><choice><abbr>y<hi rend="superscript">e</hi></abbr><expan>the</expan></choice> midst you conceive <choice><abbr>y<hi rend="superscript">e</hi></abbr><expan>the</expan></choice> same with me: but that there should be a Central par<lb type="hyphenated" xml:id="l8"/>ticle so accurately placed in <choice><abbr>y<hi rend="superscript">e</hi></abbr><expan>the</expan></choice> middle as to be always equally attracted on all <lb xml:id="l9"/>sides &amp; thereby continue without motion, seems to me a supposition fully as hard <lb xml:id="l10"/>as to make <choice><abbr>y<hi rend="superscript">e</hi></abbr><expan>the</expan></choice> sharpest needle stand upright on its point upon a lookingglass. <lb xml:id="l11"/><unclear reason="copy" cert="high">ffor</unclear> if <choice><abbr>y<hi rend="superscript">e</hi></abbr><expan>the</expan></choice> very mathematical center of <choice><abbr>y<hi rend="superscript">e</hi></abbr><expan>the</expan></choice> central particle be not accurately in <lb xml:id="l12"/><choice><abbr>y<hi rend="superscript">e</hi></abbr><expan>the</expan></choice> very mathematical center of <choice><abbr>y<hi rend="superscript">e</hi></abbr><expan>the</expan></choice> attractive power of <choice><abbr>y<hi rend="superscript">e</hi></abbr><expan>the</expan></choice> whole mass, <choice><abbr>y<hi rend="superscript">e</hi></abbr><expan>the</expan></choice> particle <lb xml:id="l13"/>will not be attracted equally on all sides<supplied reason="omitted">.</supplied></p>
<p xml:id="par4">And much harder it is to suppose that all <choice><abbr>y<hi rend="superscript">e</hi></abbr><expan>the</expan></choice> particles in an infinite <lb xml:id="l14"/>space should be so accurately poised one among another as to stand still in a <lb xml:id="l15"/>perfect equilibrium. ffor I reccon this as hard as to make not one needle only <lb xml:id="l16"/>but an infinite number of them (so many as there are particles in an infinite <lb xml:id="l17"/>space) stand accurately poised upon their points. Yet I grant it possible, at least <lb xml:id="l18"/>by a divine power; &amp; if they were once so placed I agree with you that <lb xml:id="l19"/>they would continue in that posture without motion for ever, unless put into <lb xml:id="l20"/>new motion by the same power. When therefore I said that matter eavenly <lb xml:id="l21"/>spread through all spaces would convene by its gravity into one or more great <lb xml:id="l22"/>masses<choice><sic>.</sic><corr>,</corr></choice> I understand it of matter not resting in an accurate poise.</p>
<p xml:id="par5">But you argue in <choice><abbr>y<hi rend="superscript">e</hi></abbr><expan>the</expan></choice> next paragraph of your letter that every particle <lb xml:id="l23"/>of matter in an infinite space has an infinite quantity of matter on all sides <lb xml:id="l24"/>&amp; by consequence an infinite attraction every way &amp; therefore must rest <foreign xml:lang="lat">in <lb xml:id="l25"/>equilibrio</foreign> because all infinites are equal. Yet you suspect a parallogism in <lb xml:id="l26"/>this <choice><abbr>argum<hi rend="superscript">t</hi></abbr><expan>argument</expan></choice>, &amp; I conceive <choice><abbr>y<hi rend="superscript">e</hi></abbr><expan>the</expan></choice> parallogism lies in <choice><abbr>y<hi rend="superscript">e</hi></abbr><expan>the</expan></choice> position that all infinites are <lb xml:id="l27"/>Equal. The generality of mankind consider infinites no other ways then <lb xml:id="l28"/>definitely, &amp; in this sense they say all infinites are equal, though they <unclear reason="copy" cert="high">would</unclear> <lb xml:id="l29"/>speak more truly if they should say they are neither equal nor unequal nor <lb xml:id="l30"/>have any certain difference or proportion one to another. In this sense there<lb xml:id="l31"/>fore no conclusions can be drawn fr<choice><orig>ō</orig><reg>om</reg></choice> them about <choice><abbr>y<hi rend="superscript">e</hi></abbr><expan>the</expan></choice> equality, proportions or <lb xml:id="l32"/>differences of things, &amp; they that attempt to do it, usually fall into parallogism. <lb xml:id="l33"/>So when men argue against <choice><abbr>y<hi rend="superscript">e</hi></abbr><expan>the</expan></choice> infinite divisibility of magnitude by saying <lb xml:id="l34"/>that if an inch may be divided into an infinite number of parts, <choice><abbr>y<hi rend="superscript">e</hi></abbr><expan>the</expan></choice> sum of <lb xml:id="l35"/>those parts will be an inch, &amp; if a foot may be divided into an infinite number <lb xml:id="l36"/>of parts <choice><abbr>y<hi rend="superscript">e</hi></abbr><expan>the</expan></choice> sum of those parts must be a foot, &amp; therefore since all infinites <lb xml:id="l37"/>are equal those summs must be equal, that is an inch equal to a foot. The <lb xml:id="l38"/>falsness of <choice><abbr>y<hi rend="superscript">e</hi></abbr><expan>the</expan></choice> conclusion shews an error in <choice><abbr>y<hi rend="superscript">e</hi></abbr><expan>the</expan></choice> premisses, &amp; <choice><abbr>y<hi rend="superscript">e</hi></abbr><expan>the</expan></choice> error lies in <choice><abbr>y<hi rend="superscript">e</hi></abbr><expan>the</expan></choice> <lb xml:id="l39"/>position that all infinites are equal. There is therefore another way of con<lb type="hyphenated" xml:id="l40"/>sidering infinites used by Mathematicians, &amp; that is under certain definite re<lb type="hyphenated" xml:id="l41"/>strictions &amp; limitations whereby infinites are determined to have certain differen<lb type="hyphenated" xml:id="l42"/>ces or proportions to one another. Thus D<hi rend="superscript">r</hi> Wallis considers <add place="supralinear" indicator="yes">them</add> in his <foreign xml:lang="lat">Arithmetica <lb xml:id="l43"/>Infinitorum</foreign>, where by <choice><abbr>y<hi rend="superscript">e</hi></abbr><expan>the</expan></choice> various proportions of infinite summs he gathers <choice><abbr>y<hi rend="superscript">e</hi></abbr><expan>the</expan></choice> <fw type="catch" place="bottomRight">various</fw><pb xml:id="p005v" n="5v"/> various proportions of infinite magnitudes: which way of arguing is generally <lb xml:id="l44"/>allowed by Mathematicians &amp; yet would not be good were all infinites equall. <lb xml:id="l45"/>According to <choice><abbr>y<hi rend="superscript">e</hi></abbr><expan>the</expan></choice> same way of Considering infinites, a Mathematician would tell <lb xml:id="l46"/>you that though there be an infinite number of infinitely little parts in an inch <lb xml:id="l47"/>yet there is twelve times that number of such parts in a foot; that is, <choice><abbr>y<hi rend="superscript">e</hi></abbr><expan>the</expan></choice> in<lb type="hyphenated" xml:id="l48"/>finite number of those parts in a foot is not equall to, but twelve times big<lb type="hyphenated" xml:id="l49"/>ger then <choice><abbr>y<hi rend="superscript">e</hi></abbr><expan>the</expan></choice> infinite number of them in an inch. And so a Mathematician <lb xml:id="l50"/>will tell you that if a body stood <foreign xml:lang="lat">in equilibrio</foreign> between any two equal and <lb xml:id="l51"/>contrary attracting infinite forces, &amp; if to either of those forces you add any <lb xml:id="l52"/>new finite attracting force: that new force how little so ever will destr<supplied reason="copy" cert="high">oy</supplied> <lb xml:id="l53"/><choice><abbr>y<hi rend="superscript">e</hi></abbr><expan>the</expan></choice> equilibrium &amp; put <choice><abbr>y<hi rend="superscript">e</hi></abbr><expan>the</expan></choice> body into <choice><abbr>y<hi rend="superscript">e</hi></abbr><expan>the</expan></choice> same motion into which it would pu<supplied reason="copy" cert="high">t</supplied> it were those two contrary <add place="supralinear" indicator="yes">equal</add> forces but finite or even none at all: so tha<supplied reason="copy" cert="high">t</supplied> <lb xml:id="l54"/>in this case two equal infinites by <choice><abbr>y<hi rend="superscript">e</hi></abbr><expan>the</expan></choice> addition of a finite to either of them <lb xml:id="l55"/>become unequal in our ways of recconning. And after these ways we must <lb xml:id="l56"/>reccon, if from <choice><abbr>y<hi rend="superscript">e</hi></abbr><expan>the</expan></choice> consideration of infinites we would always draw true conclu<lb type="hyphenated" xml:id="l57"/>sions.</p>
<p xml:id="par6">To the last part of your letter I answer <add place="supralinear" indicator="yes">first</add> that if <choice><abbr>y<hi rend="superscript">e</hi></abbr><expan>the</expan></choice> earth (without <choice><abbr>y<hi rend="superscript">e</hi></abbr><expan>the</expan></choice> <lb xml:id="l58"/>moon) were placed any where with its center in <choice><abbr>y<hi rend="superscript">e</hi></abbr><expan>the</expan></choice> <foreign xml:lang="lat">Orbis magnus</foreign> &amp; stood sti<supplied reason="copy" cert="high">ll</supplied> <lb xml:id="l59"/>there without any gravitation or projection &amp; then at once were <del type="cancelled">i<unclear reason="del" cert="high">n</unclear></del> infused into <lb xml:id="l60"/>it both a gravitating energy towards <choice><abbr>y<hi rend="superscript">e</hi></abbr><expan>the</expan></choice> sun &amp; a transverse impulse of a just <lb xml:id="l61"/>quantity moving it directly in a tangent to <choice><abbr>y<hi rend="superscript">e</hi></abbr><expan>the</expan></choice> <foreign xml:lang="lat">Orbis magnus</foreign>: <choice><abbr>y<hi rend="superscript">e</hi></abbr><expan>the</expan></choice> compound of <lb xml:id="l62"/>this attraction &amp; pr<del type="over">p</del><add place="over" indicator="no">o</add>jection would according to my notion cause a circular <lb xml:id="l63"/>revolution of <choice><abbr>y<hi rend="superscript">e</hi></abbr><expan>the</expan></choice> earth about <choice><abbr>y<hi rend="superscript">e</hi></abbr><expan>the</expan></choice> Sun. But <choice><abbr>y<hi rend="superscript">e</hi></abbr><expan>the</expan></choice> transverse impulse must be of a <lb xml:id="l64"/>just quantity, for if it be too big or too little it will cause <choice><abbr>y<hi rend="superscript">e</hi></abbr><expan>the</expan></choice> earth to move <lb xml:id="l65"/>in some other line.</p>
<p xml:id="par7">Secondly I do not know any power in nature <choice><abbr>w<hi rend="superscript">ch</hi></abbr><expan>which</expan></choice> could cause this trans<lb xml:id="l66"/>verse motion without <choice><abbr>y<hi rend="superscript">e</hi></abbr><expan>the</expan></choice> divine arm. Blondel tells us some where in his <lb xml:id="l67"/>book of Bombs that Plato affirms that <choice><abbr>y<hi rend="superscript">e</hi></abbr><expan>the</expan></choice> motion of <choice><abbr>y<hi rend="superscript">e</hi></abbr><expan>the</expan></choice> planets is such as if <lb xml:id="l68"/>they had all of them been created by God in some region very remote from <lb xml:id="l69"/>our Systeme &amp; let fall from thence towards <choice><abbr>y<hi rend="superscript">e</hi></abbr><expan>the</expan></choice> Sun, &amp; so soon as they arrived at <lb xml:id="l70"/>their several orbs their motion of falling turned aside into a transverse one; <lb xml:id="l71"/>&amp; this is true supposing <choice><abbr>y<hi rend="superscript">e</hi></abbr><expan>the</expan></choice> gravitating power of <choice><abbr>y<hi rend="superscript">e</hi></abbr><expan>the</expan></choice> Sun was doubled at that <lb xml:id="l72"/>moment of time in <choice><abbr>w<hi rend="superscript">ch</hi></abbr><expan>which</expan></choice> they all arrive at their several orbs: but then <choice><abbr>y<hi rend="superscript">e</hi></abbr><expan>the</expan></choice> divine <lb xml:id="l73"/><supplied reason="damage">po</supplied>wer is here required in a double respect; namely to turn <choice><abbr>y<hi rend="superscript">e</hi></abbr><expan>the</expan></choice> descending mo<lb type="hyphenated" xml:id="l74"/><supplied reason="damage" cert="high">tion</supplied> of <choice><abbr>y<hi rend="superscript">e</hi></abbr><expan>the</expan></choice> falling planets into a side motion, &amp; at <choice><abbr>y<hi rend="superscript">e</hi></abbr><expan>the</expan></choice> same time to double <choice><abbr>y<hi rend="superscript">e</hi></abbr><expan>the</expan></choice> <lb xml:id="l75"/>attractive power of <choice><abbr>y<hi rend="superscript">e</hi></abbr><expan>the</expan></choice> Sun. So then gravity may put <choice><abbr>y<hi rend="superscript">e</hi></abbr><expan>the</expan></choice> planets into motion <lb xml:id="l76"/>but without <choice><abbr>y<hi rend="superscript">e</hi></abbr><expan>the</expan></choice> divine power it could never put them into such a Circulating <lb xml:id="l77"/>motion as they have about <choice><abbr>y<hi rend="superscript">e</hi></abbr><expan>the</expan></choice> Sun, &amp; therefore for this as well as other reasons <lb xml:id="l78"/>I am compelled to ascribe <choice><abbr>y<hi rend="superscript">e</hi></abbr><expan>the</expan></choice> frame of this Systeme to an intelligent agent.</p>
<p xml:id="par8">You sometimes speak of gravity as essential &amp; inherent to matter: <lb xml:id="l79"/>pray do not ascribe that notion to me, for <choice><abbr>y<hi rend="superscript">e</hi></abbr><expan>the</expan></choice> cause of gravity is what I <lb xml:id="l80"/>do not pretend to know, &amp; therefore would take more time to consider of it <lb xml:id="l81"/>I fear what I have said of infinites will seem obscure to you: but it is enough <lb xml:id="l82"/>if you understand that infinites when considered absolutely without any restric<lb type="hyphenated" xml:id="l83"/>tion or limitation, are neither equal nor unequal nor have any certain <lb xml:id="l84"/>proportion to one another, &amp; therefore <choice><abbr>y<hi rend="superscript">e</hi></abbr><expan>the</expan></choice> principle that all infinites are <lb xml:id="l85"/>equal is a precarious one. <choice><abbr>S<hi rend="superscript">r</hi></abbr><expan>Sir</expan></choice> I am</p> 
<p rend="indent15" xml:id="par9"><choice><abbr>Yo<hi rend="superscript">r</hi></abbr><expan>Your</expan></choice> most humble Servant</p>
<p rend="indent25" xml:id="par10">Is. Newton</p>
<p rend="indent0" xml:id="par11">Trin. Coll. Ian. 17.</p>
<p xml:id="par12">1692/3</p>
<pb xml:id="envelope" n="envelope"/>
<p xml:id="par13">For M<hi rend="superscript">r</hi> Bently at the <lb type="intentional" xml:id="l86"/>Palace in</p>
<p rend="indent15" xml:id="par14">Worcester</p>
<p xml:id="par15"><handShift new="#rb" scribe="Richard_Bentley"/>A 2<hi rend="superscript">d</hi> Letter from M<hi rend="superscript">r</hi> Newton <lb xml:id="l87"/>in answer to some further <lb xml:id="l88"/>Queries</p>
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