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Civil-Comp Conferences
ISSN 2753-3239 CCC: 1
PROCEEDINGS OF THE FIFTH INTERNATIONAL CONFERENCE ON RAILWAY TECHNOLOGY: RESEARCH, DEVELOPMENT AND MAINTENANCE Edited by: J. Pombo
Paper 28.2
Dynamic coupling between convective cooling and power losses: Application to train electronic systems C. Montsarrat, C. O'Reilly and
C. Casanueva
KTH Royal Institute of Technology, Centre for ECO2 Vehicle Design, Stockholm, Sweden C. Montsarrat, C. O'Reilly and
C. Casanueva, "Dynamic coupling between convective cooling and power
losses: Application to train electronic systems", in J. Pombo, (Editor), "Proceedings of the Fifth International Conference on Railway Technology: Research, Development and Maintenance",
Civil-Comp Press, Edinburgh, UK,
Online volume: CCC 1, Paper 28.2, 2022, doi:10.4203/ccc.1.28.2
Keywords: passive cooling, power electronics, losses, coupling, CFD, integral
method.
Abstract
The recent progress obtained with silicon carbide on the performance of electronic
systems has opened possible improvements on the cooling system. Instead of using
forced cooling, the possibility of passive cooling is investigated, which would reduce
the size and weight of the cooling system on trains. This study focuses on the unsteady
coupling between the flow past a flat plate and the flux input heating the flat plate.
This coupling impacts the temperature response at the interface and is of significant
interest regarding the cooling of electronic systems on trains. With the use of two
driving behaviours corresponding to two classical phases of train in operation, the
interaction between the heat flux and the flow is investigated via two methods. These
two driving behaviours are simplified versions of a constant speed phase, with
constant losses, and an acceleration phase. An integral method is applied for a laminar
incompressible flow to get the temperature evolution over time at different locations
on the flat plate for these two cases. CFD simulations for a laminar flow are carried
out and compared with the results of the first method. For the first driving behaviour,
the agreement is good in the first half of the flat plate considered between the two
methods. The differences are more important in the second half. This could be
explained by the assumptions made on the boundary layer development. Regarding
the acceleration phase, the peaks are well captured, and the match is very good in the
temperature evolutions in the first half of the plate.
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