Please use this identifier to cite or link to this item: https://dspace.iiti.ac.in/handle/123456789/9992
Title: Topology of flow and heat transfer from prisms in square array
Authors: Shanmugam, Dhinakaran
Keywords: Drag|Heat transfer|Reynolds number|Shear flow|Topology|Vortex flow|Vortex shedding|Wakes|Flow and heat transfer|Fluid forces|Lateral interactions|Multiple columns|Reattachment flow|Recirculation bubbles|Square array|Square cylinders|Square prism|Vortex-shedding|Prisms
Issue Date: 2022
Publisher: Elsevier Ltd
Citation: Zheng, Z., Alam, M. M., Zheng, Q., Dhinakaran, S., & Islam, M. (2022). Topology of flow and heat transfer from prisms in square array. International Journal of Mechanical Sciences, 220 doi:10.1016/j.ijmecsci.2022.107163
Abstract: Structures in an array with multiple rows and columns may undergo both inline and side-by-side interferences. A system of nine square prisms in a 3 × 3 square array is numerically investigated for pitch ratio L/D = 1.2 – 7.0 at a Reynolds number of 150, where L is the spacing between the centers of two adjacent prisms, and D is the side width of a square prism. The focus is given on investigating the effect of L/D on flow topology, fluid forces, heat transfer, vortex shedding, and recirculation bubbles. An increase in L/D from 1.2 to 7.0 leads to evolutions of five distinct flows: single bluff body flow (L/D < 1.6), reattachment flow (1.6 < L/D < 3.3), lateral-interaction-induced coshedding flow (3.3 < L/D < 4.1), mixed flow (4.1 < L/D < 4.6) and free coshedding flow (4.6 < L/D < 7.0). The reattachment flow corresponds to small fluid forces while the lateral-interaction-induced coshedding flow induces large fluid forces. The time-mean drag force coefficient of the center prism drastically increases from 0.09 to 1.0 as the flow evolves from the reattachment flow to the lateral-interaction-induced coshedding flow. The maximum heat transfer from the center prism, 10% higher than that from a standalone prism, occurs for the lateral-interaction-induced coshedding flow where the flow around the center prism resembles creeping flow, no recirculation bubble forming on the front or rear surface of the prism. The coherence between heat transfer and flow patterns is discussed, including the impacts of shear layer reattachment, flow recirculation, and vortex shedding on heat transfer. © 2022
URI: https://dspace.iiti.ac.in/handle/123456789/9992
https://doi.org/10.1016/j.ijmecsci.2022.107163
ISSN: 0020-7403
Type of Material: Journal Article
Appears in Collections:Department of Mechanical Engineering

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