{"status":"ok","message-type":"work","message-version":"1.0.0","message":{"indexed":{"date-parts":[[2026,3,15]],"date-time":"2026-03-15T09:55:08Z","timestamp":1773568508705,"version":"3.50.1"},"reference-count":26,"publisher":"Wiley","issue":"1","license":[{"start":{"date-parts":[[2021,5,27]],"date-time":"2021-05-27T00:00:00Z","timestamp":1622073600000},"content-version":"vor","delay-in-days":146,"URL":"http:\/\/creativecommons.org\/licenses\/by\/4.0\/"}],"content-domain":{"domain":["onlinelibrary.wiley.com"],"crossmark-restriction":true},"short-container-title":["Complexity"],"published-print":{"date-parts":[[2021,1]]},"abstract":"<jats:p>In this article, ethylene glycol (EG)\u2009+\u2009waterbased Maxwell nanofluid with radiation and Soret effects within two parallel plates has been investigated. The problem is formulated in the form of partial differential equations. The dimensionless governing equations for concentration, energy, and momentum are generalized by the fractional molecular diffusion, thermal flux, and shear stress defined by the Caputo\u2013Fabrizio time fractional derivatives. The solutions of the problems are obtained via Laplace inversion numerical algorithm, namely, Stehfest\u2019s. Nanoparticles of silver (Ag) are suspended in a mixture of EG\u2009+\u2009water to have a nanofluid. It is observed that the thermal conductivity of fluid is enhanced by increasing the values of time and volume fraction. The temperature and velocity of water\u2010silver nanofluid are higher than those of ethylene glycol (EG)\u2009+\u2009water (H<jats:sub>2<\/jats:sub>O)\u2010silver (Ag) nanofluid. The results are discussed at 2% of volume fraction. The results justified the thermo\u2010physical characteristics of base fluids and nanoparticles shown in the tables. The effects of major physical parameters are illustrated graphically and discussed in detail.<\/jats:p>","DOI":"10.1155\/2021\/5927070","type":"journal-article","created":{"date-parts":[[2021,5,28]],"date-time":"2021-05-28T00:36:58Z","timestamp":1622162218000},"update-policy":"https:\/\/doi.org\/10.1002\/crossmark_policy","source":"Crossref","is-referenced-by-count":50,"title":["Soret and Radiation Effects on Mixture of Ethylene Glycol\u2010Water (50%\u201050%) Based Maxwell Nanofluid Flow in an Upright Channel"],"prefix":"10.1155","volume":"2021","author":[{"given":"Kashif","family":"Sadiq","sequence":"first","affiliation":[]},{"ORCID":"https:\/\/orcid.org\/0000-0002-3303-0623","authenticated-orcid":false,"given":"Fahd","family":"Jarad","sequence":"additional","affiliation":[]},{"given":"Imran","family":"Siddique","sequence":"additional","affiliation":[]},{"given":"Bagh","family":"Ali","sequence":"additional","affiliation":[]}],"member":"311","published-online":{"date-parts":[[2021,5,27]]},"reference":[{"key":"e_1_2_11_1_2","doi-asserted-by":"publisher","DOI":"10.52292\/j.laar.2014.419"},{"key":"e_1_2_11_2_2","doi-asserted-by":"publisher","DOI":"10.1016\/j.jnnms.2015.08.001"},{"key":"e_1_2_11_3_2","doi-asserted-by":"publisher","DOI":"10.1063\/1.4898460"},{"key":"e_1_2_11_4_2","doi-asserted-by":"publisher","DOI":"10.1515\/ijame-2016-0039"},{"key":"e_1_2_11_5_2","doi-asserted-by":"publisher","DOI":"10.1016\/j.mspro.2015.06.007"},{"key":"e_1_2_11_6_2","doi-asserted-by":"publisher","DOI":"10.1063\/1.4898508"},{"key":"e_1_2_11_7_2","doi-asserted-by":"publisher","DOI":"10.1155\/2014\/639159"},{"key":"e_1_2_11_8_2","doi-asserted-by":"publisher","DOI":"10.1016\/j.ijheatmasstransfer.2013.04.032"},{"key":"e_1_2_11_9_2","first-page":"9","article-title":"Radiation and Soret effects of MHD nanofluid flow over a moving vertical moving plate in porous medium","volume":"30","author":"Raju C. 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