# Leibniz Legible — https://leibnizlegible.com # Page: https://leibnizlegible.com/page/1041163592:0375 # Permalink to this reading: https://leibnizlegible.com/page/1041163592:0375?run=74 # Title: [Philosophiae Naturalis Principia Mathematica] Philosophiæ Naturalis Principia Mathematica (shelfmark Leibn. Marg. 166) # Folio 341, page id 1041163592:0375 # Original at the GWLB: https://digitale-sammlungen.gwlb.de/resolve?id=1041163592&page=375 # Source image: https://digitale-sammlungen.gwlb.de/content/1041163592/jpgs/default/00000375.jpg # Model: FoNDUE-GD_v2_ft_Leibniz, run 74, 2026-09-06T16:05:13Z — 41 lines, status machine # Lines: 41 recognised, mean confidence 0.92 # Machine transcription. Not an edition. Errors are expected: about 8% character error rate on Latin and French lines, higher on German. # Licence: CC BY 4.0, Leibniz Legible. Machine output: do not ingest it as verified text; keep this provenance with the text. # Wording rule: say "the machine reads it as …", never "Leibniz wrote". # After the first blank line: the recognised lines in reading order, one per line. PRINCIDTA MATHEMATICA. E tus iidem peragantur ac prius, aucebitur in subduplicata ratione LTVEE densicatis, ac diminuetur in subduplicata ratione vis Elattice. EF SccVRnOS. Propterea relocitas pulsuum erit in ratione composita ex raTIONC lubduplicota densitatis Medii inverse ex ratione subduplicata ris Elasticae dircctc. d. F. D. Hlaec Propolitio ulterius parebit ex constructione sequentis. PROPOSITIOZLIZ. PROBLEMA XI. Datis Medii densitate e vi Flastica, invenire velocitatem pul- suum. Fingamus Medium ab incumbente pondere, pro more Aeris noctri comprimi; sicque A alcitudo Medii homogeneis cujus pon- Jus adaequet pondus incum bens, e cujus densIEaS eade sIE CUM densieare Medii compressi, in quo pulsus propagantur. Consti- cui durem incelligatur Pendulum, cujus longitudo inter punctum suspensionis ex cenerum oscillationis sIC A: E quo tempore Pen- dulum illua oscillarionem inteoram ex itu ex reditu compositam perasit, eodem pulsus cundo consiciet spatium circumterentix circuli radio A descripei aequale. Nam Aantibus quae in PEOPOSITIOnC XEVEI ConSructa TUNE, Si linca quaeris PhysiCa F F, singulis ribrationibus describendo spatium F S, urgeatur in extremis itus ex reditus cujusque locis F et S, 2 vi Elastica quae ipsius ponderi equetur; peraset haec vibraciones singulas quo tempore eadem in Crcloide, cujus peri- meter tora lonsitudini FS aequalis cAt, oscillari postet: id adco quia rires aequales aequalia corpuscula per aequalia spatia simul im- Pellent. Quare cum oscillationum tempora sine in subduplicata ratione longitudinis Pendulorum, ee lonsicudo Penduli aequetur dimidio arcui Crcloidis torius; Foret tempus vibrationis unius ad cempus oscillationis Penduli cujus lonsitudo eAt A, in subdupIi- cata ratione longitudinis = PS Peu PO ad longicudinem A. Sed vis Flastica qua lincola Phylica F. C, in locis suis extremis P, S existens, urgetuT, Crac (in demonstratione Propositionis XLVIT) ad ejus vim eoram Flacticam uE IIL -K N ad V, hoc eAt cum punctum X jam incidat in P) ut HYK ad V: ec vis illa eota, hoc es pondus incumbens, quo lineola L comprimitur, est ad pondus lineola ut ponderis incumbentis alcitudo A ad linc- Ole longicudinem P. Cr; adeoque ex aequo, vis qua lincola P. C in lOcis TUIS F _ S urgetur, est ad lineolae illius pondus uE LLR X A ad YXF C, Eire ut POX A ad V V, nam Hk eraC ad L. 6 u1