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dc.contributor.authorPai, Su-Chengen_US
dc.contributor.authorLai, Yee-Hwongen_US
dc.contributor.authorChiao, Ling-Yunen_US
dc.contributor.authorYu, Tiingen_US
dc.date.accessioned2014-12-08T15:14:56Z-
dc.date.available2014-12-08T15:14:56Z-
dc.date.issued2007-01-12en_US
dc.identifier.issn0021-9673en_US
dc.identifier.urihttp://dx.doi.org/10.1016/j.chroma.2006.11.011en_US
dc.identifier.urihttp://hdl.handle.net/11536/11232-
dc.description.abstractA dispersion-convolution model is proposed for simulating peak shapes in a single-line flow injection system. It is based on the assumption that an injected sample plug is expanded due to a "bulk" dispersion mechanism along the length coordinate, and that after traveling over a distance ora period of time. the sample zone will develop into a Gaussian-like distribution. This spatial pattern is further transformed to a temporal coordinate by a convolution process, and finally a temporal peak image is generated. The feasibility of the proposed model has been examined by experiments with various coil lengths, sample sizes and pumping rates. An empirical dispersion coefficient (D*) can be estimated by using the observed peak position. height and area (t(p)(*), h* and A(t)(*)) from a recorder. An empirical temporal shift ((Phi*) can be further approximated by (Phi* = D*/u(2), which becomes an important parameter in the restoration of experimental peaks. Also, the dispersion coefficient can be expressed as a second-order polynomial function of the pumping rate Q, for which D*(Q) =delta(0) + delta(1)Q+delta(2)Q(2). The optimal dispersion occurs at a pumping rate of Q(opt) = root delta(0)/delta(.)(2) This explains the interesting "Nike-swoosh" relationship between the peak height and pumping rate. The excellent coherence of theoretical and experimental peak shapes confirms that the temporal distortion effect is the dominating reason to explain the peak asymmetry in flow injection analysis. (c) 2006 Elsevier B.V. All rights reserved.en_US
dc.language.isoen_USen_US
dc.subjectdispersion-convolution modelen_US
dc.subjectflow injection analysisen_US
dc.subjectpeak simulationen_US
dc.titleDispersion-convolution model for simulating peaks in a flow injection systemen_US
dc.typeArticleen_US
dc.identifier.doi10.1016/j.chroma.2006.11.011en_US
dc.identifier.journalJOURNAL OF CHROMATOGRAPHY Aen_US
dc.citation.volume1139en_US
dc.citation.issue1en_US
dc.citation.spage109en_US
dc.citation.epage120en_US
dc.contributor.department應用化學系zh_TW
dc.contributor.departmentDepartment of Applied Chemistryen_US
dc.identifier.wosnumberWOS:000244060900015-
dc.citation.woscount7-
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