Fabri, Honoré, Dialogi physici in quibus de motu terrae disputatur, 1665

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            <p type="main">
              <s id="s.000769">
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              ſanè omnibus experimentis repugnat, quæ cum ſpatio Galileano prorſus
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              conſentiunt. </s>
            </p>
            <p type="main">
              <s id="s.000770">
                <emph type="italics"/>
              Antim.
                <emph.end type="italics"/>
              </s>
              <s id="s.000771"> Nemo vnquam hujus rei periculum fecit in 4. inſtantibus,
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              ſed tantùm in 4. temporibus ſenſibilibus, nempe inſtantia ſub ſenſum non
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              cadunt; at ſupponuntur hoc loco 4.inſtantia. </s>
              <s id="s.000772">iuxta ſingularem illam tem­
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              poris hypotheſim ; equidem ſi tempus AE ex quatuor partibus temporis
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              ſenſibilibus componas ſecundùm communem, aut etiam Galileanam tem­
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              poris hypotheſim, & dividas AE in 8. tempora æqualia; in progreſſione
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              Galilei, tempore AE, idem ſpatium decurritur; at verò in mea decurritur
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              ſpatium, quod complectitur 18.triangula æqualia ABV; igitur ſpatium in
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              mea decurſum majus erit Galileano, vna octava; & ſi adhuc tempora bi­
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              fariam dividas, majus erit vna decima ſexta; atque ita deinceps decre­
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              ſcent exceſſus iuxta hanc ſeriem 1/4. &c. </s>
              <s id="s.000773">igitur. </s>
              <s id="s.000774">ſi vel in­
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              ſtantia infinita ſunt, vel partes infinitæ, differentia ſpatiorum in mea
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              progreſſione & Galileana decreſcit in infinitum; ac proinde Illa ſpatia
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              æqualia cenſenda ſunt, quorum vnum aliud ſuperat, exceſſu, minore quo­
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              libet aſſignabili: Hæc ſi non nemo paulò attentiùs conſideraſſet, meam
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              progreſſionem tam citò vt falſam & experimentis omnino repugnantem
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              minimè rejeciſſet, nec adeò dubitaſſet de vera hujus accelerationis cauſa,
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              quæ in eo poſita eſt, quod prioribus gradibus impetus novi gradus conti­
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              nuè accedant, idque ſi quodlibet tempus ex infinitis conſter, vel etiam ex
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              finitis, ſed innumerabilibus, in triangulo; ſi verò ex paucis finitis, in
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              rectangulis, iuxta figuram AEF diſpoſitis; nec alia ſuper hoc, meo judi­
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              cio, difficultas reſtat; vnde concludo, meam progreſſionem alteri præfe­
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              rendam eſſe, quia ſcilicet vtrique hypotheſi facit ſatis; quanquam ad vſum.
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              </s>
              <s id="s.000775">Galileana omnino adhibenda eſt, cùm in eam mea reſolvatur, vt verò ad
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              cauſam phyſicam accelerationis res reducatur pro vtraque hypotheſi, mea
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              certè non modò præferenda eſt, verùm etiam neceſſariò tenenda; ſed tam
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              multa de hac re ſcripſimus, vt de his plura ſcribere operæ pretium non ſit. </s>
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            <p type="main">
              <s id="s.000776">
                <emph type="italics"/>
              Chryſocom.
                <emph.end type="italics"/>
              </s>
              <s id="s.000777"> Neſcio, quomodo dicas, nullam ſupereſſe difficultatem,
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              cùm inſuperabilis adhuc reſtet; nempe ſi primo inſtanti mobile acquirit
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              AV, & ſecundo, ſpatium CH, duplum, igitur, cùm mobile eſſet ih ſpa­
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              tio AV tanquam in loco adæquato erit in CH duplo ſcilicet, tanquam
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              in loco adæquato majore. </s>
            </p>
            <p type="main">
              <s id="s.000778">
                <emph type="italics"/>
              Antim.
                <emph.end type="italics"/>
              Hæc maxima eſt difficultas, fateor, & in communi temporis
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                <figure id="id.025.01.072.1.jpg" xlink:href="025/01/072/1.jpg" number="23"/>
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              hypotheſi, ſi rèm ipſam, non verba conſideremus,
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              ferè inſuperabilis; immò & in Galilei opinione, qui
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              vult, tempus ex infinitis inſtantibus Mathematicis
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              componi, inſolubilis nodus eſt; ſi enim in tempore
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              AE accipiantur duo inſtantia, ſcilicet B & C, nem­
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              pe vt linea AE repræſentat tempus, ita quodlibet illius
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              punctum repræſentat vnum inſtans, porrò mobile,
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              quod movetur tempore AE, inſtanti B eſt in ſpa­
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              tio BF, inſtanti C in ſpatio CG duplo prioris;
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              quia vt arca trianguli AEI repræſentat, totum </s>
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