Please use this identifier to cite or link to this item: http://gukir.inflibnet.ac.in:8080/jspui/handle/123456789/4944
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dc.contributor.authorBiradar D.S
dc.contributor.authorThipperudrappa J
dc.contributor.authorHanagodimath S.M.
dc.date.accessioned2020-06-12T15:05:44Z-
dc.date.available2020-06-12T15:05:44Z-
dc.date.issued2007
dc.identifier.citationSpectroscopy Letters , Vol. 40 , 4 , p. 559 - 571en_US
dc.identifier.uri10.1080/00387010701301147
dc.identifier.urihttp://gukir.inflibnet.ac.in:8080/jspui/handle/123456789/4944-
dc.description.abstractFluorescence quenching of 1,3-diphenyl benzene (m-terphenyl) by carbon tetrachloride (CCl4) at steady state in different solvents, namely n-hexane, n-heptane, cyclohexane, toluene, benzene acetonitrile, 1,4-dioxane, and with a transient method in benzene has been done at room temperature to understand the role of quenching mechanisms. The Stern-Volmer plot was found to be linear for all the solvents studied. The probability of quenching per encounter p was determined in all the solvents and was found to be less than unity. Further, from the studies of rate parameters and lifetime measurements in benzene at different temperatures (30-60°C), it was shown that the phenomenon of quenching is generally governed by the well-known Stern-Volmer (S-V) plot. The activation energy Ea (E?a) of quenching was determined using literature values of activation energy of diffusion Ed, and it was found to be greater than Ed, which confirms the fact that the quenching mechanism is not solely due to material diffusion but there is also contribution from activation energy. Copyright © Taylor & Francis Group, LLC.en_US
dc.subjectActivation energy
dc.subjectm-terphenyl
dc.subjectMaterial diffusion
dc.subjectS-V plot
dc.subjectSteady state
dc.subjectTransient fluorescence quenching
dc.titleFluorescence quenching studies of 1,3-diphenyl benzeneen_US
dc.typeArticle
Appears in Collections:1. Journal Articles

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