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<title>Lecture I</title>
<author xml:id="tt"><persName key="nameid_53" sort="Telescope, Tom" ref="nameid_53" xml:base="http://www.newtonproject.sussex.ac.uk/catalogue/xml/persNames.xml">Tom Telescope</persName></author>

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<date>2009</date>
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<note type="metadataLine">1761, <hi rend="italic">c.</hi> 2,135 words.</note>
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<linkGrp n="document_relations" xml:base="http://www.newtonproject.sussex.ac.uk/view/normalized/"><ptr type="next_part" target="OTHE00118">Lecture II [<hi rend="italic">The Newtonian System ... familiarized</hi> (1761)]</ptr><ptr type="parent" target="OTHE00114"><hi rend="italic">The Newtonian System ... familiarized</hi> (1761)</ptr><ptr type="previous_part" target="OTHE00116">Introduction, Being the Substance of A Letter to the Hon. **** [<hi rend="italic">The Newtonian System ... familiarized</hi> (1761)]</ptr></linkGrp>
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<title>The Newtonian System of Philosophy Adapted to the Capacities of young Gentlemen and Ladies, and familiarized and made entertaining by Objects with which they are intimately acquainted</title>
<title type="short">The Newtonian System ... familiarized</title>
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<pb xml:id="p5" n="5"/><fw type="pag" place="topCenter">[ 5 ]</fw><fw type="sig" place="bottomCenter">B 3</fw>

<p rend="center" xml:id="par1"><hi rend="large">LECTURE I.</hi></p>
<p rend="center" xml:id="par2"><hi rend="italic">Of</hi> <hi rend="smallCaps">Matter</hi> <hi rend="italic">and</hi> <hi rend="smallCaps">Motion.</hi></p>
<p xml:id="par3"><hi rend="dropCap">B</hi>y <hi rend="italic">Matter</hi>, my dear friends, <hi rend="italic">we mean <lb xml:id="l1"/>the substance of all things</hi>, or <hi rend="italic">that</hi> of <lb xml:id="l2"/>which all bodies are composed, in what<lb type="hyphenated" xml:id="l3"/>ever form or manner they may present <lb xml:id="l4"/>themselves to our senses: for this top, <lb xml:id="l5"/><hi rend="italic">Tom Wilson</hi>'s ivory ball, the hill before us, <lb xml:id="l6"/>that orange on the table, and all <lb xml:id="l7"/>things you see, are made of matter differently <lb xml:id="l8"/>formed.</p>
<p rend="indent5" xml:id="par4">As to <hi rend="italic">Motion</hi>, I may save myself and <lb xml:id="l9"/>you the trouble of explaining that; for <lb xml:id="l10"/>every boy who can whip his top knows what <lb xml:id="l11"/>motion is as well as his master.</p>
<p rend="indent5" xml:id="par5"><hi rend="italic">Matter</hi>, or <hi rend="italic">Body, is indifferent to motion <lb xml:id="l12"/>or rest</hi>. As for example, now I whip my <lb xml:id="l13"/>top, and it runs round, or is in motion; <lb xml:id="l14"/>but when I no longer whip it, the top <lb xml:id="l15"/>falls down, as you see, and is at rest.</p>
<p rend="indent5" xml:id="par6"><hi rend="italic">When a body is in motion, as much <lb xml:id="l16"/>force is required to make it rest, as was</hi> <lb xml:id="l17"/><fw type="catch" place="bottomRight"><hi rend="italic">required</hi></fw><pb xml:id="p6" n="6"/><fw type="pag" place="topCenter">[ 6 ]</fw> <hi rend="italic">required, while it was at rest, to put it in <lb xml:id="l18"/>motion.</hi> Thus, suppose a boy strikes a <lb xml:id="l19"/>trap-ball with one hand, and another stands <lb xml:id="l20"/>close by to catch it with one of his hands, <lb xml:id="l21"/>it will require as much strength or force <lb xml:id="l22"/>to stop that ball, or put it in a state of rest, <lb xml:id="l23"/>as the other gave to put it in motion; <lb xml:id="l24"/>allowing for the distance the two boys <lb xml:id="l25"/>stand apart.</p>
<p rend="indent5" xml:id="par7"><hi rend="italic">No body or part of matter can give it<lb type="hyphenated" xml:id="l26"/>self either motion or rest:</hi> and therefore a <lb xml:id="l27"/>body at rest will remain so for ever, unless <lb xml:id="l28"/>it be put in motion by some external cause; <lb xml:id="l29"/>and a body in motion will move for ever, <lb xml:id="l30"/>unless some external cause stops it.</p>
<p rend="indent5" xml:id="par8">This seemed so absurd to Master <hi rend="italic">Wilson</hi>, <lb xml:id="l31"/>that he burst into a loud laugh. What, <lb xml:id="l32"/>says he, shall any body tell me that my <lb xml:id="l33"/>hoop or my top will run for ever, when I <lb xml:id="l34"/>know by daily experience that they drop <lb xml:id="l35"/>of themselves, without being touched by <lb xml:id="l36"/>any body? At which our little Philosopher <lb xml:id="l37"/>was angry, and having commanded silence, <lb xml:id="l38"/>Don't expose your ignorance, <hi rend="italic">Tom Wilson</hi>, <lb xml:id="l39"/>for the sake of a laugh, says he: if you <lb xml:id="l40"/>intend to go through my Course of Phi<lb type="hyphenated" xml:id="l41"/>losophy, and to make yourself acquainted <lb xml:id="l42"/>with the nature of things, you must pre<lb type="hyphenated" xml:id="l43"/><fw type="catch" place="bottomRight">pare</fw><pb xml:id="p7" n="7"/><fw type="pag" place="topCenter">[ 7 ]</fw>pare to hear what is more extraordinary <lb xml:id="l44"/>than this. When you say that nothing <lb xml:id="l45"/>touched the top or the hoop, you forget <lb xml:id="l46"/>their friction or rubbing against the ground <lb xml:id="l47"/>they run upon, and the resistance they <lb xml:id="l48"/>meet with from the air in their course, <lb xml:id="l49"/>which is very considerable though it has <lb xml:id="l50"/>escaped your notice. Somewhat too might <lb xml:id="l51"/>be said on the gravity and attraction be<lb type="hyphenated" xml:id="l52"/>tween the top or the hoop, and the earth; <lb xml:id="l53"/>but <hi rend="italic">that</hi> you are not yet able to compre<lb type="hyphenated" xml:id="l54"/>hend, and therefore we shall proceed in <lb xml:id="l55"/>our Lecture.</p>
<p rend="indent5" xml:id="par9"><hi rend="italic">A body in motion will always move on <lb xml:id="l56"/>in a strait line, unless it be turned out of it <lb xml:id="l57"/>by some external cause.</hi> Thus we see <lb xml:id="l58"/>that a marble shot upon the ice, if the <lb xml:id="l59"/>surface be very smooth, will continue its <lb xml:id="l60"/>motion in a strait line, till it is put to rest <lb xml:id="l61"/>by the friction of the ice and air, and the <lb xml:id="l62"/>force of attraction and gravitation.</p>
<p rend="indent5" xml:id="par10"><hi rend="italic">The swiftness of motion is measured by <lb xml:id="l63"/>distance of place, and the length of time <lb xml:id="l64"/>in which it is performed.</hi> Thus if a <lb xml:id="l65"/>cricket-ball and a fives-ball move each of <lb xml:id="l66"/>them twenty yards in the same time, their <lb xml:id="l67"/>motions are equally swift; but if the fives-<lb type="hyphenated" xml:id="l68"/>ball moves two yards while the cricket-ball <lb xml:id="l69"/><fw type="catch" place="bottomRight">is</fw><pb xml:id="p8" n="8"/><fw type="pag" place="topCenter">[ 8 ]</fw>is moving one, then is the motion of the <lb xml:id="l70"/>fives-ball twice as swift as the other.</p>
<p rend="indent5" xml:id="par11"><hi rend="italic">But the quantity of motion is measured <lb xml:id="l71"/>by the swiftness of motion, as above de<lb type="hyphenated" xml:id="l72"/>scribed, and the quantity of matter moved <lb xml:id="l73"/>considered together.</hi> For instance, if the <lb xml:id="l74"/>cricket-ball be equal in bulk and weight <lb xml:id="l75"/>to the fives-ball, and move as swift, then <lb xml:id="l76"/>it hath an equal quantity of motion. But <lb xml:id="l77"/>if the cricket-ball be twice as big and as <lb xml:id="l78"/>heavy as the fives-ball, and yet moves <lb xml:id="l79"/>equally swift, it hath double the quantity <lb xml:id="l80"/>of motion; and so in proportion.</p>
<p rend="indent5" xml:id="par12"><hi rend="italic">All bodies have a natural tendency, at<lb type="hyphenated" xml:id="l81"/>tractions, or gravitation towards each other.</hi> <lb xml:id="l82"/>Here <hi rend="italic">Tom Wilson,</hi> again laughing, told the <lb xml:id="l83"/>Company that Philosophy was made up of <lb xml:id="l84"/>nothing but hard words. That is because <lb xml:id="l85"/>you have not sense enough to enquire into, <lb xml:id="l86"/>and retain the signification of words, says <lb xml:id="l87"/>our Philosopher. All words, continued <lb xml:id="l88"/>he, are difficult till they are explained; <lb xml:id="l89"/>and when that is done, we shall find that <lb xml:id="l90"/>gravity or gravitation will be as easily <lb xml:id="l91"/>understood as praise or commendation, <lb xml:id="l92"/>and attraction as easily as correction; <lb xml:id="l93"/>which you deserve, Tom Wilson, for your <lb xml:id="l94"/>impertinence.</p>
<fw type="catch" place="bottomRight"><hi rend="italic">Gravity,</hi></fw><pb xml:id="p9" n="9"/>
<fw type="pag" place="topCenter">[ 9 ]</fw>
<p rend="indent5" xml:id="par13"><hi rend="italic">Gravity,</hi> my dear friends,<hi rend="italic"> is that uni<lb type="hyphenated" xml:id="l95"/>versal disposition of matter which inclines <lb xml:id="l96"/>or carries the lesser part towards the <lb xml:id="l97"/>centre of the greater part; which is called</hi> weight <lb xml:id="l98"/><hi rend="italic">or gravitation in the lesser body, but</hi> at<lb type="hyphenated" xml:id="l99"/>traction <hi rend="italic">in the greater, because it draws, <lb xml:id="l100"/>as it were, the lesser body to it.</hi> Thus all bodies on or near the earth's surface have <lb xml:id="l101"/>a tendency, or seeming inclination, to des<lb type="hyphenated" xml:id="l102"/>cend towards it middle or centre; <lb xml:id="l103"/>and but for this principle in nature, the <lb xml:id="l104"/>earth (considering its form and situation <lb xml:id="l105"/>in the universe) could not subsist as it is: <lb xml:id="l106"/>for we all suppose the earth to be nearly <lb xml:id="l107"/>round, (nay we are sure it is so, for my <lb xml:id="l108"/>Lord <hi rend="italic">Anson</hi> and many other gentlemen, <lb xml:id="l109"/>you know, have sailed around it) and as it <lb xml:id="l110"/>is suspended in such a mighty void or <lb xml:id="l111"/>space and always in motion, what should <lb xml:id="l112"/>hinder the stones, water, and other parts <lb xml:id="l113"/>of matter falling from the surface, but the <lb xml:id="l114"/>almighty arm of God, or this principle or <lb xml:id="l115"/>universal law of nature, of attraction and <lb xml:id="l116"/>gravitation, which he has established to <lb xml:id="l117"/>keep the universe in order. To illustrate <lb xml:id="l118"/>and explain what I have said, let us sup<lb type="hyphenated" xml:id="l119"/>pose the following figure to be the earth <lb xml:id="l120"/>and seas. Let <hi rend="italic">Tom Wilson</hi> stand at this <lb xml:id="l121"/>point of the globe or earth where we are, <lb xml:id="l122"/><fw type="catch" place="bottomRight">and</fw><pb xml:id="p10" n="10"/><fw type="pag" place="topCenter">[ 10 ]</fw> and <hi rend="italic">Hal Thompson</hi> at the opposite part of <lb xml:id="l123"/>the earth, with his feet (as they must be) <lb xml:id="l124"/>towards us: if <hi rend="italic">Tom</hi> drop an orange out of <lb xml:id="l125"/>his hand, it will fall down towards <hi rend="italic">Hal</hi>; <lb xml:id="l126"/>and if <hi rend="italic">Hal</hi> drop an orange, it will fall <lb xml:id="l127"/>seemingly upwards (if I may so express <lb xml:id="l128"/>myself) towards <hi rend="italic">Tom:</hi> and if these oranges <lb xml:id="l129"/>had weight and power sufficient to displace <lb xml:id="l130"/>the other particles of matter of which the <lb xml:id="l131"/>earth is composed, so as to make way to <lb xml:id="l132"/>the centre, they would there unite toge<lb type="hyphenated" xml:id="l133"/>ther and remain fixed; and they would <lb xml:id="l134"/>then lose their power of gravitation, as be<lb type="hyphenated" xml:id="l135"/>ing at the center of gravity and unable to <lb xml:id="l136"/><fw type="catch" place="bottomRight">fall,</fw><pb xml:id="p11" n="11"/><fw type="pag" place="topCenter">[ 11 ]</fw>fall, and only retain in themselves the power of attraction.</p>
<p rend="indent5" xml:id="par14">This occasioned a general laugh; and <lb xml:id="l137"/><hi rend="italic">Tom Wilson</hi> starting up, asked how Master <lb xml:id="l138"/><hi rend="italic">Thompson</hi> was to stand with his feet up<lb type="hyphenated" xml:id="l139"/>wards, as here represented, without hav<lb type="hyphenated" xml:id="l140"/>ing anything to support his head? Have <lb xml:id="l141"/>patience, says the little Philosopher, and I <lb xml:id="l142"/>will tell you; but pray behave with good <lb xml:id="l143"/>manners, Master <hi rend="italic">Wilson</hi>, and don't laugh <lb xml:id="l144"/>at every thing you cannot comprehend. <lb xml:id="l145"/>This difficulty is solved, and all the seem<lb type="hyphenated" xml:id="l146"/>ing confusion which you apprehend of bo<lb type="hyphenated" xml:id="l147"/>dies flying off from each other is removed,<lb xml:id="l148"/> by means of this attraction and gravita<lb type="hyphenated" xml:id="l149"/>tion. Ask any of the sailors who have <lb xml:id="l150"/>been around the world, and they will tell <lb xml:id="l151"/>you that the people on the part of the <lb xml:id="l152"/>globe over-against us do not walk upon <lb xml:id="l153"/>their heads, though the earth is round; <lb xml:id="l154"/>and though their heels are opposite ours, <lb xml:id="l155"/>they are in no more danger of falling into <lb xml:id="l156"/>the mighty space beneath them, than we <lb xml:id="l157"/>are of falling (or rather rising I must call <lb xml:id="l158"/>it here) up to the moon or the stars.</p>
<p rend="indent5" xml:id="par15">But besides this general law of attraction <lb xml:id="l159"/>and gravitation, which affects all bodies <lb xml:id="l160"/>equally and universally, there are parti<lb type="hyphenated" xml:id="l161"/>cular bodies that attract and repel <lb xml:id="l162"/><fw type="catch" place="bottomRight">other,</fw><pb xml:id="p12" n="12"/><fw type="pag" place="topCenter">[ 12 ]</fw>each other, as may be seen by the <hi rend="italic">Magnet</hi> or <lb xml:id="l163"/><hi rend="italic">Loadstone</hi>, which has not only the property <lb xml:id="l164"/>of directing the nedle of the mariner's <lb xml:id="l165"/>compass when touched with it to the north, <lb xml:id="l166"/>but also of attracting or bringing <lb xml:id="l167"/>iron to it with one end, and repelling or <lb xml:id="l168"/>forcing it away with the other end: and <lb xml:id="l169"/><hi rend="italic">Sam Jones</hi>'s knife, which was whet on a <lb xml:id="l170"/>Loadstone some years ago, still retains the <lb xml:id="l171"/>power you see of picking up needles and <lb xml:id="l172"/>small pieces of iron.</p>
<p rend="indent5" xml:id="par16"><hi rend="italic">Glass, Sealing-Wax, Amber,</hi> and <hi rend="italic">Precious <lb xml:id="l173"/>Stones,</hi> when chafed or rubbed till they <lb xml:id="l174"/>are warm, will likewise both attract and <lb xml:id="l175"/>repel feathers, hairs, straw &amp;<hi rend="italic">c.</hi> which is <lb xml:id="l176"/>sufficient to prove that each of these bodies <lb xml:id="l177"/>has a sphere of arractiuopm assined it, be<lb type="hyphenated" xml:id="l178"/>yond which it will repel the same body it <lb xml:id="l179"/>would otherwise attract.</p>
<p rend="indent5" xml:id="par17">When bodies are so attracted by each <lb xml:id="l180"/>other as to be united or brought into close <lb xml:id="l181"/>contact, they then adhere or cohere toge<lb type="hyphenated" xml:id="l182"/>ther so as not to be easily separated, and <lb xml:id="l183"/>this is called in Philosophy the <hi rend="italic">Power of <lb xml:id="l184"/>Cohesion,</hi> and is undoubtedly that principle <lb xml:id="l185"/>which binds large bodies together; for all <lb xml:id="l186"/>large bodies are made up of atoms or par<lb type="hyphenated" xml:id="l187"/>ticles inconceivably small. And this co<lb type="hyphenated" xml:id="l188"/>hesion will always be proportioned to the <lb xml:id="l189"/><fw type="catch" place="bottomRight">number</fw><pb xml:id="p13" n="13"/><fw type="pag" place="topCenter">[ 13 ]</fw><fw type="sig" place="bottomCenter">C</fw>number of particles or quantity of the sur<lb type="hyphenated" xml:id="l190"/>face of bodies that come into contact or <lb xml:id="l191"/>touch each other: for those bodies that <lb xml:id="l192"/>are of spherical form will not adhere so <lb xml:id="l193"/>strongly as those that are flat or square; <lb xml:id="l194"/>because they can only touch each other <lb xml:id="l195"/>at a certain point; and this is the reason why <lb xml:id="l196"/>the particles of water and quicksilver, <lb xml:id="l197"/>which are globular or round, are so easily <lb xml:id="l198"/>separated with a touch, while those <lb xml:id="l199"/>of metals and some other bodies are not to be <lb xml:id="l200"/>parted but with great force. To give us <lb xml:id="l201"/>a familiar instance of this cohesion of mat<lb type="hyphenated" xml:id="l202"/>ter, our Philosopher took two leaden balls, <lb xml:id="l203"/>and filing a part off each so that the two <lb xml:id="l204"/>flat parts might come into close contact, <lb xml:id="l205"/>he gently pressed them together and they <lb xml:id="l206"/>united so firmly that it required consider<lb type="hyphenated" xml:id="l207"/>able force to get them asunder.</p>
<p rend="indent5" xml:id="par18">One thing I must tell you of magnetism, <lb xml:id="l208"/>which seems pretty extraordinary. Master <lb xml:id="l209"/><hi rend="italic">Brown</hi> took his uncle's sword, and sup<lb type="hyphenated" xml:id="l210"/>ported it with the point downwards, by <lb xml:id="l211"/>resting the shell of the hilt on the top of <lb xml:id="l212"/>his two forefingers; and Master <hi rend="italic">Smith</hi> was <lb xml:id="l213"/>placed with his father's amber-headed <lb xml:id="l214"/>cane at about three or four feet distance, <lb xml:id="l215"/>where he kept rubbing the amber head <lb xml:id="l216"/>round on his waistcoat. After some little <lb xml:id="l217"/><fw type="catch" place="bottomRight">time</fw><pb xml:id="p14" n="14"/><fw type="pag" place="topCenter">[ 14 ]</fw>time the sword began to move, tho' at that <lb xml:id="l218"/>distance; and some time after that it turn<lb type="hyphenated" xml:id="l219"/>ed quite round; but was soon turned back <lb xml:id="l220"/>again by master <hi rend="italic"/>'s rubbing the am<lb type="hyphenated" xml:id="l221"/>ber head backwards, or in a contrary di<lb type="hyphenated" xml:id="l222"/>rection</p>
<p rend="indent5" xml:id="par19">But what seems most worthy of our ad<lb type="hyphenated" xml:id="l223"/>miration is the Electrical Fire, which so <lb xml:id="l224"/>plentifully abounds in the universe, and <lb xml:id="l225"/>which is excited, or made visible, by the <lb xml:id="l226"/>friction or rubbing of a glass globe. This <lb xml:id="l227"/>fire, by a very simple machine, may be con<lb type="hyphenated" xml:id="l228"/>veyed into the human body, every part <lb xml:id="l229"/>of which it pervades in an instant, and is <lb xml:id="l230"/>said to have been very serviceable in the <lb xml:id="l231"/>cure of some disorders. It may be drawn <lb xml:id="l232"/>from the ladies eyes, yet it leaves them no <lb xml:id="l233"/>less brilliant than they were before. It <lb xml:id="l234"/>may be drawn from under thunder-clouds, and <lb xml:id="l235"/>is probably the same species of fire with <lb xml:id="l236"/>the lightening; for Professor <hi rend="italic">Richmann</hi> of <lb xml:id="l237"/><hi rend="italic">Hamburgh&gt;</hi>, who fixed a machine to bring it <lb xml:id="l238"/>down from the clouds in large quantities, <lb xml:id="l239"/>was killed by the stroke it gave him.</p>
<p rend="indent5" xml:id="par20"><hi rend="italic">The same force aplied to two different <lb xml:id="l240"/>bodies will always produce the same quantity <lb xml:id="l241"/>of motion in each of them.</hi> To prove this, <lb xml:id="l242"/>we put Master <hi rend="italic">Jones</hi> into a boat, which <lb xml:id="l243"/>(including his own weight) weighed ten <lb xml:id="l244"/><fw type="catch" place="bottomRight">hundred,</fw><pb xml:id="p15" n="15"/><fw type="pag" place="topCenter">[ 15 ]</fw><fw type="sig" place="bottomCenter">C 2</fw>hundred, on the <hi rend="italic">Thames</hi> by the <hi rend="italic">Mill-bank</hi>; <lb xml:id="l245"/>and on the <hi rend="italic">Lambeth</hi> side, just opposite, we <lb xml:id="l246"/>placed another boat (of one hundred <lb xml:id="l247"/>weight) with a string tied to it. This <lb xml:id="l248"/>string Master <hi rend="italic">Jones</hi> pulled in the other <lb xml:id="l249"/>boat; and we observed that as the boats <lb xml:id="l250"/>approached each other, the small boat <lb xml:id="l251"/>moved ten feet for every foot the other <lb xml:id="l252"/>moved: which proves what we have before <lb xml:id="l253"/>observed as to the quantity of motion.</p>
<p rend="indent5" xml:id="par21"><hi rend="italic">Attraction is the stronger, the nearer the <lb xml:id="l254"/>attracting bodies are to each other; and in <lb xml:id="l255"/>different distances of the same bodies it de<lb type="hyphenated" xml:id="l256"/>creases as the squares of the distances be<lb type="hyphenated" xml:id="l257"/>tween the centres of those bodies increase.</hi> <lb xml:id="l258"/>For if two bodies at a given distance at<lb type="hyphenated" xml:id="l259"/>tract each other with a certain force, at <lb xml:id="l260"/>half the distance they will attract each <lb xml:id="l261"/>other with four times that force. But this <lb xml:id="l262"/>I shall further explain in my next course of Lectures.</p>
<p rend="indent5" xml:id="par22"><hi rend="italic">Two bodies at a distance will put each <lb xml:id="l263"/>other into motion by the force of Attrac<lb type="hyphenated" xml:id="l264"/>tion or Gravitation.</hi> This we know to <lb xml:id="l265"/>be true by experience, though we cannot <lb xml:id="l266"/>account for it; and therefore it is to be <lb xml:id="l267"/>received as a principle in Natural Phi<lb type="hyphenated" xml:id="l268"/>losophy.</p>
<fw type="catch" place="bottomRight">Here</fw>
<pb xml:id="p16" n="16"/>
<fw type="pag" place="topCenter">[ 16 ]</fw>

<fw type="catch" place="bottomRight">LECTURE</fw>
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