By Gleb L. Kotkin, V. G. Serbo
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Additional resources for Collection of Problems in Classical Mechanics
Springer-Verlag, Berlin, 1998.  H. Vollmers: "Detection of vortices and quantitative evaluation oftheir main parameters fixmi experimental velocity data". Meas. Sci. Technol. 12,2001, pp. 1-9. Analysis of PIV Flow Field Measurements » 21 : Figure 1 The mapping of a pair of dewarped calibration images from both stereo cameras into one image (left side) demonstrates perfect agreement. The upper vector fields (right side) show the view of both cameras. In the lower part the fields are combined and the vectors are within the plane of the light sheet while the gray values indicate the component normal to the light sheet.
This was unavoidable because spraying sensitive parts like pressure hole and moving parts with black paint was not permitted. Due to this bright background no particles could be distinguished by the cameras in certain areas. The excluded areas reduced information considerably. As both cameras suffer from the reflections, the omitted areas in the combined stereo results are the union of both regions. The thrust with Njsa = 11 050/min was found as a limit for application of PIV because the jet produced condensation in the tuimel for higher thrust.
Further analysis was applied to investigate the location and strength of vortices by methods described in . Examples are given in Figs 3 and 9. The vortex roll-up is continuing and not only one vortex but also strong vorticity layers are generated by the wing and are observed in the velocity fields. The discrepancies between both applied methods for evaluation of vortex parameters become apparent While for the method MOV the distribution of vorticity within the observation area is used, the approximation FAM represents the best fit for the velocity field.
Collection of Problems in Classical Mechanics by Gleb L. Kotkin, V. G. Serbo