TY - JOUR
T1 - Plate-fin heat sink forced convective heat transfer augmentation with a fractal insert
AU - Hoi, Su Min
AU - Teh, An Liang
AU - Ooi, Ean Hin
AU - Chew, Irene Mei Leng
AU - Foo, Ji Jinn
N1 - Funding Information:
The authors would like to thank the Malaysia Ministry of Higher Education (MOHE) for the financial support of the present research project (Project Code: FRGS/2/2014/TK05/MUSM/03/1 ). We would also like to thank Monash University Malaysia for supporting the High Performance Computing (HPC) system for the current research study (Research Project No: 25209434-02 ).
Publisher Copyright:
© 2019 Elsevier Masson SAS
Copyright:
Copyright 2019 Elsevier B.V., All rights reserved.
PY - 2019/8
Y1 - 2019/8
N2 - The interaction of fractal grid-induced turbulence on plate-fin heat sink is numerically investigated at flow Reynolds number of ReDh = 7.3 × 104. Three fractal grids of different number of fractal iterations N, namely: The rectangular fractal grid of N = 2 (RFG2), square fractal grid of N = 3 (SFG3), and square fractal grid of N = 4 (SFG4)are employed to perturb the windward fluid flow. For each case, the effects of eight fractal grid first iterative bar thicknesses t0 at five different inter-fin distances δ are investigated. Results show that Nusselt number Nu and pressure drop ΔP increase with t0 for all cases. 57%, 51% and 43% of forced convective heat transfer augmentations are observed using SFG3, RFG2 and SFG4, respectively, than that of the control plate-fin heat sink. The thermal and fluid flow perturbation promoted by SFG3 outperforms the rest with Nu = 7.07 × 103 at δ = 10 and 25 mm, but at a cost of higher ΔP. RFG2's maximum Nu is 6.82 × 103 where wider δ of δ = 50 mm is preferred, and SFG4 is 6.42 × 103 at δ=10 mm. Interestingly, SFG4 enjoys a lower ΔP, which is highly energy sustainable. The strength of SFG3-induced turbulence intensity is able to infiltrate deeper into the fins at a higher flow rate, which may facilitate the continuous restructuring of inter-fin flow boundary layers, thus promoting thermal dissipation. In short, plate-fin heat sink forced convection is strongly dependent on the interaction between the insert configuration and the induced flow structures within fins, of which, the effects of t0 and δ are highly correlated.
AB - The interaction of fractal grid-induced turbulence on plate-fin heat sink is numerically investigated at flow Reynolds number of ReDh = 7.3 × 104. Three fractal grids of different number of fractal iterations N, namely: The rectangular fractal grid of N = 2 (RFG2), square fractal grid of N = 3 (SFG3), and square fractal grid of N = 4 (SFG4)are employed to perturb the windward fluid flow. For each case, the effects of eight fractal grid first iterative bar thicknesses t0 at five different inter-fin distances δ are investigated. Results show that Nusselt number Nu and pressure drop ΔP increase with t0 for all cases. 57%, 51% and 43% of forced convective heat transfer augmentations are observed using SFG3, RFG2 and SFG4, respectively, than that of the control plate-fin heat sink. The thermal and fluid flow perturbation promoted by SFG3 outperforms the rest with Nu = 7.07 × 103 at δ = 10 and 25 mm, but at a cost of higher ΔP. RFG2's maximum Nu is 6.82 × 103 where wider δ of δ = 50 mm is preferred, and SFG4 is 6.42 × 103 at δ=10 mm. Interestingly, SFG4 enjoys a lower ΔP, which is highly energy sustainable. The strength of SFG3-induced turbulence intensity is able to infiltrate deeper into the fins at a higher flow rate, which may facilitate the continuous restructuring of inter-fin flow boundary layers, thus promoting thermal dissipation. In short, plate-fin heat sink forced convection is strongly dependent on the interaction between the insert configuration and the induced flow structures within fins, of which, the effects of t0 and δ are highly correlated.
KW - CFD
KW - Fractal geometry
KW - HVAC
KW - Plate-fin heat sink
KW - Thermal dissipation
KW - Turbulence
UR - http://www.scopus.com/inward/record.url?scp=85065487709&partnerID=8YFLogxK
U2 - 10.1016/j.ijthermalsci.2019.04.035
DO - 10.1016/j.ijthermalsci.2019.04.035
M3 - Article
AN - SCOPUS:85065487709
SN - 1290-0729
VL - 142
SP - 392
EP - 406
JO - International Journal of Thermal Sciences
JF - International Journal of Thermal Sciences
ER -