Finite Difference Heat Exchanger Model: Flow Maldistribution with Thermal Coupling
Document Type
Article
Publication Date
1-1-2020
Department
Department of Materials Science and Engineering; Department of Electrical and Computer Engineering
Abstract
Channels not receiving the same amount of flow (flow maldistribution) is an important effectiveness loss for high effectiveness heat exchangers. This paper develops a finite difference model of a counter flow heat exchanger. It reproduced the simple NTU result for two channels exactly. For more than two channels, there is an edge effect, and the model agreed within 0.1% of the literature. Perfect agreement was achieved for a simple flow maldistribution case. For independent pairs of hot and cold channels, as flow rate is reduced, the effectiveness asymptotically approaches the irregularity parameter (a measure of channel flow maldistribution). With thermal coupling between pairs of channels (measured by an equivalent Peclet number), effectiveness continues to increase with decreasing flow rate. These results hold for uncorrelated flow maldistribution on both sides or no flow maldistribution on one side. However, when flow maldistribution is positively correlated, effectiveness is higher; and, when it is negatively correlated, effectiveness is lower. A number of resulting graphs illustrate the effectiveness for each channel with different flow rate and correlation. While one exemplary application is a polymer expanded microchannel heat exchanger, the model could be used for other heat exchangers.
Publication Title
Heat Transfer Engineering
Recommended Citation
Denkenberger, D.,
Brandemuehl, M.,
Zhai, J.,
&
Pearce, J. M.
(2020).
Finite Difference Heat Exchanger Model: Flow Maldistribution with Thermal Coupling.
Heat Transfer Engineering.
http://doi.org/10.1080/01457632.2020.1756060
Retrieved from: https://digitalcommons.mtu.edu/michigantech-p/2078
Publisher's Statement
© 2020 Taylor & Francis Group, LLC. Publisher’s version of record: https://doi.org/10.1080/01457632.2020.1756060