# Leibniz Legible — https://leibnizlegible.com # Page: https://leibnizlegible.com/page/00068208:0128 # Permalink to this reading: https://leibnizlegible.com/page/00068208:0128?run=74 # Title: Leibniz-Handschriften zur Mathematik LH 35, 15, 6 # Folio 63v, page id 00068208:0128 # Scan: One image of two folio pages side by side, registered by the library under both labels (also fol. 53r); this page is its left half. # Original at the GWLB: https://digitale-sammlungen.gwlb.de/resolve?id=00068208&page=128 # Source image: https://digitale-sammlungen.gwlb.de/content/00068208/jpgs/default/00000128.jpg # Model: FoNDUE-GD_v2_ft_Leibniz, run 74, 2026-09-06T16:05:13Z — 66 lines, status machine # Lines: 66 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. ndim interdum guber.aculo quiestente cae- tera circumaguntur interdum media pars navis locuque ubimatus est, interdum ipsa propra prora ABb Eacrpavio den quiesat puppi circum acha, ideo Angulys flexioni, id est quem facium muaelinece moly navis AB AB vi nis eo casu, quano centrum verticitatus navis et magnetis non coincidunt, non est differentia angulorum directionis. Esto enim centrum certicitatis in navi A. in magnete B. tunc si polus esset in c. linea directionis megneticae erit BC aut bc. Sed quia polus est quidem in recta AC. sed non in non est in C. et simlitr sedverum in recta AC. ultra C. producta in tantam longitudinem ut angulus Ae si exfingatur d magneticus seu quem faciunt maelineae ACB. vel ACb (si C. interim polus sitmalleus directionum ex diversis esse fingatur, ceti diictimum centris verticitatutm magneticarum, ft ob niniam exilitatem ha beri possit pro mulo ac proinde lineae di rectio num ex diversis centris verlicitatum magne- ticarum pro parallelis: ideo posito poto longe ultra C. et linea directionis ex centro verticitatis A. posita AC. utcunque producta ad seu feu BD. t et ex centro b. erit bd. prdacta produicta ultra d. saltem ad sensum eruntus parallelae AC. BD. bd Eruntue Eiquatuur duo anguli directionis semper aequales (quamdm ma– gnes non mulat directionem superveniente forte qu declinatione, de quo postea) CABe sie magnes sit in A. nempe duo: CAB. et C Ab. sivi sit in B, nemane B vel b. nempe DBA d b et si linea navigationis sit AB. et duo magnetes alius in A. alius in B. erunt aequa les anguli DBA. et C AB. similiter si linea novigavis sit AB. erunt aequales an- et magnes sit a A. vel b. vel utroque simul. erunt anguli aequales CAb. dbA posito autem magnete extra centrum verticitatis ipsius navis, duorum diversorum situum lineae anguli directionis DBA. et dbA in ter se different. Differentiae quantitas ita computabitur: finge acum verticitate propria carere, seu verti- citate navrs circumagi, id est transfer BD in bDD. et AC. in ACC. ut linea CA. DB. eundem faciunt angulum ad AB. eum faciant ad Ab. Erit angulus DB DD bA aequalis angulo DBA. ac pro inde differentia duorum angulorum directionis anguli DBA et db A erit DDbD. Restat determinare angulum flexionis BAb tatur Id ita fiet e datur linea navigationis D in sctu posterioni aequalus Ab in situ si centrum motuss verticitatis navis seu punctum A vel quantitatem lineae AB habetimus. antqss dtonem in +posita eadem linea navigationis, ubicunque sit ma- gnes, sive etiam si plures sint magnetes +quem