Fabri, Honoré, Tractatus physicus de motu locali, 1646

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              uis rarum, & tenue, quod aliquantulum non reſiſtat, vt clarum eſt; </s>
              <s id="N1FA26">tunc
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              quoque eſt reſiſtentia ſine ceſſione, ſeu tota reſiſtentia, cum ipſum cor­
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              pus reſiſtens nullo modo cedit; </s>
              <s id="N1FA2E">id eſt nullo modo mouetur ab ictu; </s>
              <s id="N1FA32">neque
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              enim excogitari poteſt maior reſiſtentia; </s>
              <s id="N1FA38">denique tunc eſt æqualis ceſ­
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              ſio reſiſtentiæ, cum ipſum corpus, in quod aliud impingitur (vocetur re­
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              flectens) tantùm cedit quantum reſiſtit; </s>
              <s id="N1FA40">cedit autem per motum; </s>
              <s id="N1FA44">igitur
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              ſi reflectenti imprimitur æqualis motus ab impacto reflectens æqualiter
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              cedit, & reſiſtit, ſi minor minùs cedit, & plùs reſiſtit, ſi nullus nullo mo­
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              do cedit, ſed tantùm reſiſtit; ſi maior plùs cedit, & minùs reſiſtit, ſcili­
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              cet in infinitum, donec tandem in vacuo ſit tantum ceſſio, nulla reſi­
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              ſtentia. </s>
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              <s id="N1FA54">Tertiò, tunc impactum motum æqualem imprimit reflectenti, cum
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              impactum æquale eſt reflectenti, tùm mole, tùm pondere v.g. globus A
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              impactus in globum B eiuſdem materiæ, & diametri, modo nullus fiat
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              attritus partium, ſeu compreſſio, ſitque linea directionis connectens
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              centra per punctum contactus, quod in primo libro iam demonſtratum
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              eſt; </s>
              <s id="N1FA64">cum enim totus impetus globi A agat, & quantum poteſt; </s>
              <s id="N1FA68">certè pro­
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              ducit æqualem; </s>
              <s id="N1FA6E">nec enim aliunde determinari poteſt æqualitas effectus
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              quàm ab æqualitate cauſæ poſitis iiſdem circumſtantiis, & cum impetus
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              in B impreſſus diſtribuatur tot partibus quot producens æqualis in A,
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              vterque impetus eſt æquè intenſus; </s>
              <s id="N1FA78">igitur æquè velox motus per ſe; </s>
              <s id="N1FA7C">cum
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              per accidens aliquando ſecus accidat; </s>
              <s id="N1FA82">ſi verò reflectens ſit minor, idem
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              impetus paucioribus partibus diſtribuitur; </s>
              <s id="N1FA88">igitur intenſior eſt; </s>
              <s id="N1FA8C">igitur
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              velocior motus, ſecus verò cum maior eſt, donec tandem tanta ſit moles,
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              vt plura ſint puncta in reflectente, quàm ſint in impacto puncta impe­
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              tus; tunc enim nullus imprimitur impetus, vt conſtat ex dictis lib. 1. </s>
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            <p id="N1FA97" type="main">
              <s id="N1FA99">Quartò, quod autem ſit æqualis reſiſtentia, & ceſſio globi B æqualis
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              globo A etiam certum eſt; </s>
              <s id="N1FA9F">tùm quia, ſi æqualiter mouetur, æqualiter ce­
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              dit, vt iam dixi ſi æqualiter cedit, æqualiter reſiſtit; </s>
              <s id="N1FAA5">nam quâ proportio­
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              ne minùs cedit, plùs reſiſtit; </s>
              <s id="N1FAAB">igitur qua proportione ceſſio augetur, reſi­
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              ſtentia imminuitur: præterea cum reſiſtat per ſuam entitatem impene­
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              trabilem, duram &c. </s>
              <s id="N1FAB3">certè ſi eſt æqualis entitas, eſt æqualis reſiſtentia; </s>
              <s id="N1FAB7">
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              quod etiam videmus in corporibus immerſis eiuſdem grauitatis cum
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              medio, ita vt tot ſint partes impellentes, quot impulſæ; </s>
              <s id="N1FABE">denique illud
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              experimentum quo videmus globum A impactum in B æqualem per li­
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              neam connectentem centra immobilem ſiſtere, rem iſtam euincit; </s>
              <s id="N1FAC6">nam
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              ideo ſiſtit, quia eſt æqualis determinatio noua priori; </s>
              <s id="N1FACC">nam vt ſe habet
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              reſiſtentia reflectentis, ita ſe habet noua determinatio, quam ſuo modo
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              confert impacto, vt ſuprà demonſtratum eſt: </s>
              <s id="N1FAD4">& cùm ſint ad lineas op­
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              poſitas ex diametro hæ duæ determinationes, neutra præualere poteſt;
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              igitur neceſſe eſt ſiſtere globum impactum. </s>
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            <p id="N1FADC" type="main">
              <s id="N1FADE">Quintò, certum eſt determinationem nouam eſſe iuxta proportionem
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              reſiſtentiæ, & hanc iuxta proportionem minoris ceſſionis; </s>
              <s id="N1FAE4">vnde cum
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              nulla eſt reſiſtentia, ſed tantùm ceſsio, nulla prorſus eſt noua determina­
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              tio igitur à termino nullius reſiſtentiæ, & totius ceſsionis ad terminum </s>
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          </chap>
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