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Particle diffusional layer thickness in a USP dissolution apparatus II: A combined function of particle size and paddle speed

dc.contributor.authorSheng, Jennifer J.en_US
dc.contributor.authorSirois, Paul J.en_US
dc.contributor.authorDressman, Jennifer B.en_US
dc.contributor.authorAmidon, Gordon L.en_US
dc.date.accessioned2008-11-03T18:52:35Z
dc.date.available2010-01-05T16:59:14Zen_US
dc.date.issued2008-11en_US
dc.identifier.citationSheng, Jennifer J.; Sirois, Paul J.; Dressman, Jennifer B.; Amidon, Gordon L. (2008). "Particle diffusional layer thickness in a USP dissolution apparatus II: A combined function of particle size and paddle speed." Journal of Pharmaceutical Sciences 97(11): 4815-4829. <http://hdl.handle.net/2027.42/61209>en_US
dc.identifier.issn0022-3549en_US
dc.identifier.issn1520-6017en_US
dc.identifier.urihttps://hdl.handle.net/2027.42/61209
dc.identifier.urihttp://www.ncbi.nlm.nih.gov/sites/entrez?cmd=retrieve&db=pubmed&list_uids=18314890&dopt=citationen_US
dc.description.abstractThis work was to investigate the effects of particle size and paddle speed on the particle diffuisonal layer thickness h app in a USP dissolution apparatus II. After the determination of the powder dissolution rates of five size fractions of fenofibrate, including <20, 20–32, 32–45, 63–75, and 90–106 µm, the present work shows that the dependence of h app on particle size follows different functions in accordance with the paddle speed. At 50 rpm, the function of h app is best described by a linear plot of $h_{{rm app}} = 9.91sqrt d - 23.31$ ( R 2  = 0.98) throughout the particle diameter, d , from 6.8 to 106 µm. In contrast, at 100 rpm a transitional particle radius, r , of 23.7 µm exists, under which linear relationship h app  = 1.59 r ( R 2  = 0.98) occurs, but above which h app becomes a constant of 43.5 µm. Thus, h app changes not only with particle size, but also with the hydrodynamics under standard USP configurations, which has been overlooked in the past. Further, the effects of particle size and paddle speed on h app were combined using dimensionless analysis. Within certain fluid velocity/particle regime, linear correlation of h app / d with the square-root of Reynolds number $(dvarpi /upsilon )^{1/2} $ , that is, $h_{{rm app}} /d = 1.5207 - 9.25 times 10^{ - 4} (dvarpi /nu )^{1/2} $ ( R 2  = 0.9875), was observed. © 2008 Wiley-Liss, Inc. and the American Pharmacists Association J Pharm Sci 97:4815–4829, 2008en_US
dc.format.extent409196 bytes
dc.format.extent3118 bytes
dc.format.mimetypeapplication/pdf
dc.format.mimetypetext/plain
dc.publisherWiley Subscription Services, Inc., A Wiley Companyen_US
dc.subject.otherChemistryen_US
dc.subject.otherFood Science, Agricultural, Medicinal and Pharmaceutical Chemistryen_US
dc.titleParticle diffusional layer thickness in a USP dissolution apparatus II: A combined function of particle size and paddle speeden_US
dc.typeArticleen_US
dc.rights.robotsIndexNoFollowen_US
dc.subject.hlbsecondlevelPharmacy and Pharmacologyen_US
dc.subject.hlbtoplevelHealth Sciencesen_US
dc.description.peerreviewedPeer Revieweden_US
dc.contributor.affiliationumCollege of Pharmacy, University of Michigan, 428 Church Street, Ann Arbor, Michigan 48109-1065en_US
dc.contributor.affiliationumCollege of Pharmacy, University of Michigan, 428 Church Street, Ann Arbor, Michigan 48109-1065 ; College of Pharmacy, University of Michigan, 428 Church Street, Ann Arbor, Michigan 48109-1065. Telephone: 734-764-2440; Fax: 734-763-6423.en_US
dc.contributor.affiliationotherLilly Research Laboratories, Eli Lilly and Company, Indianapolis, Indiana 46285en_US
dc.contributor.affiliationotherInstitute for Pharmaceutical Technology, Biocenter-Johann Wolfgang Goethe-University, Frankfurt 60439, Germanyen_US
dc.identifier.pmid18314890en_US
dc.description.bitstreamurlhttp://deepblue.lib.umich.edu/bitstream/2027.42/61209/1/21345_ftp.pdf
dc.identifier.doihttp://dx.doi.org/10.1002/jps.21345en_US
dc.identifier.sourceJournal of Pharmaceutical Sciencesen_US
dc.owningcollnameInterdisciplinary and Peer-Reviewed


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