Resolution limits of active triangulation systems by defocusing

In active triangulation systems, one side of the triangulation triangle is made up of a spatial light structure of well-known shape and location, causing a pattern on the surface of the target object. The other side of the triangle is embodied by ray bundles, imaging this pattern onto a position sensor. Because nearly all surfaces show scattering characteristics between specular and diffuse reflection, the corresponding image-forming wavefronts are not of uniform amplitude, and so the irradiance of the imaging pupil is also nonuniform. If the imaging is done by an aberrated system, this can cause deviations from the image as predicted by geometric optics. An estimate of deviations resulting from defocusing by treating the imaging process in terms of scalar diffraction theory, using a linear model for nonuniform pupil irradiance is given

Triangulationssensoren für Roboteranwendungen

Viele Meß- und Prüfprobleme in Fertigung und Montage sind durch reine Grauwert-Bildverarbeitung nicht befriedigend zu lösen, weil hier nur ein informationsreduziertes zweidimensionales Abbild der real dreidimensionalen Szene als Informationsbasis zur Verfügung steht. Dreidimensionale Objektinformation bietet hingegen ein wesentlich höheres Informationspotential und ermöglicht neben völlig neuen Lösungsansätzen auch weniger aufwendige Lösungen von Standardproblemen. Zur dreidimensionalen Objekterfassung werden punkt- und flächenhaft arbeitende Verfahren eingesetzt. Punktverfahren gewinnen Abstandsbilder durch zeitsequentielle Meßpunkterfassung, wohingegen flächenhafte Verfahren auf zeitlich paralleler Erfassung von 3-D-Information beruhen. Die folgenden Ausführungen beschränken sich ausschließlich auf punktorientierte Verfahren

3-D-Koordinatenmessung durch optische Triangulation

Das hier vorgestellte Drei-Koordinaten-Meßgerät arbeitet nach dem Prinzip der optischen Triangulation. Einzelne Punkte einer Oberfläche können gezielt angetastet und vermessen werden. Hierbei wurden Meßunsicherheiten von ± 0,1mm bei einer maximalen Meßgeschwindigkeil von 25 Punkten/Sekunde erreicht. Bei einem Meßabstand von 420mm beläuft sich das Antastfeld auf 150 x 150mm. Der optische Aufbau ermöglicht einen Abstandsmeßbereich von ca. 350 mm. Das Gerät eignet sich zur räumlichen Vermessung nichtspiegelnder Werkstückoberflächen. Da das Meßkonzept eine freie Vorgabe der Antastpunkte gestattet, sind Toleranz- und Vollständigkeitsprüfungsaufgaben in der Serienfertigung bevorzugte Anwendungen

Grundlagenuntersuchung, Entwicklung und Erprobung optischer Sensoren für die Qualitätssicherung und zum Einsatz an Montagerobotern in der flexiblen Montage : Teilprojekt A4

Die dreidimensionale berührungslose Objektvermessung ist eine zentrale Sensoraufgabe in der industriellen Montage und Qualitätssicherung. Hierfür geeignet sind optische Triangulationsverfahren, die sich im Vergleich zu anderen Verfahren durch hohe relative Distanz- und Lateralauflösung sowie geringen apparativen Aufwand auszeichnen

Determination of nutrient salts by automatic methods both in seawater and brackish water: the phosphate blank

9 páginas, 2 tablas, 2 figurasThe main inconvenience in determining nutrients in seawater by automatic methods is simply solved: the preparation of a suitable blank which corrects the effect of the refractive index change on the recorded signal. Two procedures are proposed, one physical (a simple equation to estimate the effect) and the other chemical (removal of the dissolved phosphorus with ferric hydroxide).Support for this work came from CICYT (MAR88-0245 project) and Conselleria de Pesca de la Xunta de GaliciaPeer reviewe

Measurement of inclusive π0\pi^{0} production in hadronic Z0Z^{0} decays

An analysis is presented of inclusive \pi^0 production in Z^0 decays measured with the DELPHI detector. At low energies, \pi^0 decays are reconstructed by \linebreak using pairs of converted photons and combinations of converted photons and photons reconstructed in the barrel electromagnetic calorimeter (HPC). At high energies (up to x_p = 2 \cdot p_{\pi}/\sqrt{s} = 0.75) the excellent granularity of the HPC is exploited to search for two-photon substructures in single showers. The inclusive differential cross section is measured as a function of energy for {q\overline q} and {b \bar b} events. The number of \pi^0's per hadronic Z^0 event is N(\pi^0)/ Z_{had}^0 = 9.2 \pm 0.2 \mbox{(stat)} \pm 1.0 \mbox{(syst)} and for {b \bar b}~events the number of \pi^0's is {\mathrm N(\pi^0)/ b \overline b} = 10.1 \pm 0.4 \mbox{(stat)} \pm 1.1 \mbox{(syst)} . The ratio of the number of \pi^0's in b \overline b events to hadronic Z^0 events is less affected by the systematic errors and is found to be 1.09 \pm 0.05 \pm 0.01. The measured \pi^0 cross sections are compared with the predictions of different parton shower models. For hadronic events, the peak position in the \mathrm \xi_p = \ln(1/x_p) distribution is \xi_p^{\star} = 3.90^{+0.24}_{-0.14}. The average number of \pi^0's from the decay of primary \mathrm B hadrons is found to be {\mathrm N} (B \rightarrow \pi^0 \, X)/\mbox{B hadron} = 2.78 \pm 0.15 \mbox{(stat)} \pm 0.60 \mbox{(syst)}

Search for Neutral Heavy Leptons Produced in Z Decays

Weak isosinglet Neutral Heavy Leptons ($\nu_m$) have been searched for using data collected by the DELPHI detector corresponding to $3.3\times 10^{6}$ hadronic~Z$^{0}$ decays at LEP1. Four separate searches have been performed, for short-lived $\nu_m$ production giving monojet or acollinear jet topologies, and for long-lived $\nu_m$ giving detectable secondary vertices or calorimeter clusters. No indication of the existence of these particles has been found, leading to an upper limit for the branching ratio $BR($Z$^0\rightarrow \nu_m \overline{\nu})$ of about $1.3\times10^{-6}$ at 95\% confidence level for $\nu_m$ masses between 3.5 and 50 GeV/$c^2$. Outside this range the limit weakens rapidly with the $\nu_m$ mass. %Special emphasis has been given to the search for monojet--like topologies. One event %has passed the selection, in agreement with the expectation from the reaction: %$e^+e^- \rightarrow\ell \bar\ell \nu\bar\nu$. The results are also interpreted in terms of limits for the single production of excited neutrinos

Measurement of the Quark and Gluon Fragmentation Functions in Z0Z^0 Hadronic Decays

The fragmentation functions and multiplicities in $b\overline{b}$ and light quark events are compared. The measured transverse and longitudinal components of the fragmentation function allow the gluon fragmentation function to be evaluated

Search for new phenomena using single photon events in the DELPHI detector at LEP

Data are presented on the reaction \epem~\into~\gamma + no other detected particle at center-of-mass energies, \sqs = 89.48 GeV, 91.26 GeV and 93.08 GeV. The cross section for this reaction is related directly to the number of light neutrino generations which couple to the \zz boson, and to several other phenomena such as excited neutrinos, the production of an invisible `X' particle, a possible magnetic moment of the tau neutrino, and neutral monojets. Based on the observed number of single photon events, the number of light neutrinos which couple to the \zz is measured to be N_\nu = 3.15 \pm 0.34. No evidence is found for anomalous production of energetic single photons, and upper limits at the 95\% confidence level are determined for excited neutrino production (BR < 4-9 \times 10^{-6}), production of an invisible `X' particle (\sigma < 0.1 pb), and the magnetic moment of the tau neutrino (< 5.2 \times 10^{-6} \mu_B). No event with the topology of a neutral monojet is found, and this corresponds to the limit \sigma < 0.044/\epsilon pb at the 95\% confidence level, where \epsilon is the unknown overall monojet detection efficiency

Measurement of the Bd0^{0}_{d} oscillation frequency using kaons, leptons and jet charge

A measurement of the mass difference, \Delta m_d, between the two physical \mbox{B}^0_d states has been obtained from the analysis of the impact parameter distribution of a lepton emitted at large transverse momentum (p_t) relative to the jet axis and from the analysis of the flight distance distribution of secondary vertices tagged by either a high p_t lepton or an identified kaon. In the opposite hemisphere of the event, the charge of the initial quark has been evaluated using a high p_t lepton, a charged kaon or the mean jet charge. With 1.7 million hadronic Z^0 decays recorded by DELPHI between 1991 and 1993, \Delta m_d is found to be: \Delta m_d = 0.531^{+0.050}_{-0.046} ~(stat.) \pm 0.078 ~(syst.) ~ {\mathrm{ps}}^{-1} \,