Phuong M. Le, Ph.D. - Publications
Affiliations: | 2009 | School of Chemical Engineering and Materials Science | University of Oklahoma, Norman, OK, United States |
Area:
Chemical EngineeringYear | Citation | Score | |||
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2021 | Shimizu K, Gilmour S, Mase H, Le PM, Teshima A, Sakamoto H, Nomura S. COVID-19 and Heat Illness in Tokyo, Japan: Implications for the Summer Olympic and Paralympic Games in 2021. International Journal of Environmental Research and Public Health. 18. PMID 33807268 DOI: 10.3390/ijerph18073620 | 0.3 | |||
2009 | Le PM, Papavassiliou DV. A physical picture of the mechanism of turbulent heat transfer from the wall International Journal of Heat and Mass Transfer. 52: 4873-4882. DOI: 10.1016/J.Ijheatmasstransfer.2009.05.024 | 0.707 | |||
2008 | Le PM, Papavassiliou DV. On the scaling of heat transfer using thermal flux gradients for fully developed turbulent channel and Couette flows International Communications in Heat and Mass Transfer. 35: 404-412. DOI: 10.1016/J.Icheatmasstransfer.2007.09.006 | 0.688 | |||
2008 | Le PM, Papavassiliou DV. Mechanism of heat transfer away from the wall and turbulent prandtl numbers for plane channel and plane couette flow Aiche Annual Meeting, Conference Proceedings. | 0.707 | |||
2006 | Le PM, Papavassiliou DV. Turbulent heat transfer in plane Couette flow Journal of Heat Transfer. 128: 53-62. DOI: 10.1115/1.2130404 | 0.715 | |||
2006 | Le PM, Papavassiliou DV. On temperature prediction at low Re turbulent flows using the Churchill turbulent heat flux correlation International Journal of Heat and Mass Transfer. 49: 3681-3690. DOI: 10.1016/J.Ijheatmasstransfer.2006.02.022 | 0.691 | |||
2005 | Le PM, Papavassiliou DV. Turbulent dispersion from elevated line sources in channel and couette flow Aiche Journal. 51: 2402-2414. DOI: 10.1002/Aic.10507 | 0.668 | |||
2004 | Mitrovic BM, Le PM, Papavassiliou DV. On the Prandtl or Schmidt number dependence of the turbulent heat or mass transfer coefficient Chemical Engineering Science. 59: 543-555. DOI: 10.1016/J.Ces.2003.09.039 | 0.685 | |||
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