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dc.contributor.advisorSallam, Khaled A.
dc.contributor.authorOlinger, David Simon
dc.date.accessioned2013-12-10T18:05:21Z
dc.date.available2013-12-10T18:05:21Z
dc.date.issued2012-05
dc.identifier.urihttps://hdl.handle.net/11244/7814
dc.description.abstractScope and Method of Study:
dc.description.abstractThis report has discussed the advantages that holography has over other spray diagnostic approaches; namely, holography is a volumetric measurement as opposed to a point measurement and drops are not limited to a particular shape. This project has advanced holographic spray analysis by automating the image processing algorithms. The program was then applied to sprays in a realistic testing environment. Aerated liquid jets in a high subsonic crossflow were analyzed, including the rarely investigated near injector region (from the injector to the far field, x/d = 0..100). Usable data was presented in a variety of figures. These results demonstrate that practical 3D analysis of sprays has been pushed well into the near injector region, specifically up to x/d ~ 15. Additional data was obtained even closer to the injector, but its confidence drops significantly.
dc.description.abstractFindings and Conclusions:
dc.description.abstractThe hologram image processing algorithm has been validated and its uncertainty quantified. The drop detection false positive rate is 6% and false negative rate is 20%. These detection rates are independent of the drop size, for drop images with a diameter greater than six pixels.
dc.description.abstractThe area near the injector floor in the figures are composed of a high number density, wide span of very small droplets separated from the main, high density core. This region immediately downstream of the injector, under the jet core, features a continuous distribution of drops. Hence, while a wake of relatively large drops forms downstream of the injection site, the near-field wake is not completely empty.
dc.description.abstractThe downstream location is important to the Sauter Mean Diameter in the near field; larger drops break up during secondary atomization. However, even with the near field data, the influence of x is much less than GLR or M for the given data set. SMD is inversely proportional to all three factors.
dc.formatapplication/pdf
dc.languageen_US
dc.rightsCopyright is held by the author who has granted the Oklahoma State University Library the non-exclusive right to share this material in its institutional repository. Contact Digital Library Services at lib-dls@okstate.edu or 405-744-9161 for the permission policy on the use, reproduction or distribution of this material.
dc.titleAutomatic digital holographic analysis of near-field aerated liquid jets in crossflow
dc.contributor.committeeMemberArena, Andrew S.
dc.contributor.committeeMemberCheng, Qi
dc.contributor.committeeMemberHanan, Jay C.
dc.contributor.committeeMemberHoberock, Lawrence L.
osu.filenameOlinger_okstate_0664D_12104.pdf
osu.accesstypeOpen Access
dc.type.genreDissertation
dc.type.materialText
dc.subject.keywordsatomization
dc.subject.keywordsdrop
dc.subject.keywordshologram
dc.subject.keywordsholography
dc.subject.keywordsjet
dc.subject.keywordsspray
thesis.degree.disciplineMechanical and Aerospace Engineering
thesis.degree.grantorOklahoma State University


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