By Freese R.W.
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Extra info for A 2-metric characterization of the euclidean plane
A RAM L J --1 vi a II>MA f 3. - T'OCH~NIQUES of multi-image cor~,esl,onclcnccs, by spatial intersect~ion of honiologol~s rays losing information of t,he system caliblatioll. This is esplairled in detail in Maas  and L:Ians ct al. The releva,nt txpics for the esl’~\riment,Hlist, will be esplaincd hcrc. te system used in fluid mechanic-3. The l,liotogra,Ilimet,ric x-conrl,onrnt is always in ciuncra~ viewing direction. For t,he detection of the particles iu 2D sl)ilce, 8. segmentation Of tllc?
Follow closely the fluid pxticlc t#hey mark. 0ljufi. 4) where pr, is the particle clciisit~y. pf is t;he densit>- of’ the fluid arid 11the ltirrcrrra,tic viscosity of the fluid. 1Vlien measuring in licpiids it, is convenient to choose pxt~icles which liavic a density /‘I, close or eqiial to the flnicl dellsit>- /),f. HerekXftjeKZllld th~Oll~llout t,ho stwly WC assume that Eq. 4) applie,y and w will not distinguish further between fiuicl velocity x1(1 particle velocity. The maximum numbc~r of particles A$ for the dct-e~rnination of pa,rticle coordinat~es is limited by the spatial resoliitioii of the C’C‘D sei1sors.
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A 2-metric characterization of the euclidean plane by Freese R.W.