Modeling the temperature distribution and performance of a PEM fuel cell with thermal contact resistance

Author(s):  
Tao-Feng Cao ◽  
Yu-Tong Mu ◽  
Jing Ding ◽  
Hong Lin ◽  
Ya-Ling He ◽  
...  
Author(s):  
Ehsan Sadeghi ◽  
Ned Djilali ◽  
Majid Bahrami

Heat transfer through the gas diffusion layer (GDL) of a PEM fuel cell is a key process in the design and operation a PEM fuel cell. The analysis of this process requires determination of the effective thermal conductivity as well as the thermal contact resistance between the GDL and adjacent surfaces/layers. In the present study, a guarded-hot-plate apparatus has been designed and built to measure the effective thermal conductivity and thermal contact resistance in GDLs under vacuum and atmospheric pressure. Toray carbon papers with the porosity of 78% and different thicknesses are used in the experiments under a wide range of compressive loads. Moreover, novel analytical models are developed for the effective thermal conductivity and thermal contact resistance and compared against the present experimental data. Results show good agreements between the experimental data and the analytical models. It is observed that the thermal contact resistance is the dominant component of the total thermal resistance and neglecting this phenomenon may result in enormous errors.


Author(s):  
Adam S. Hollinger ◽  
Stefan T. Thynell

Localized temperature gradients in a polymer electrolyte fuel cell (PEFC) are known to decrease the durability of the polymer membrane. The most important factor in controlling these temperature gradients is the thermal contact resistance at the interface of the gas diffusion layer (GDL) and the bipolar plate. Here, we present thermal contact resistance measurements of carbon paper and carbon cloth GDLs over a pressure range of 0.7–14.5 MPa. Contact resistances are highly dependent upon the clamping pressure applied to a fuel cell, and in the present work, contact resistances vary from 3.5 × 10−4 to 2.0 × 10−5 m2 K/W, decreasing nonlinearly over the pressure range for each material tested. The contact resistances of carbon cloth GDLs are two to four times higher than contact resistances of carbon paper GDLs throughout the range of pressures tested. The data presented here also show that the thermal resistance of the sample is negligible in comparison to the thermal contact resistance. Controlling temperature gradients in a fuel cell is desirable, and the measurements presented here can be used to more accurately predict temperature distribution in a polymer electrolyte fuel cell.


2012 ◽  
Vol 538-541 ◽  
pp. 730-734
Author(s):  
Bing Fang ◽  
Lei Zhang ◽  
Jian Fu Zhang ◽  
Ya Hong Li

This paper presented a real-time measuring method of temperature fields and thermal deformations in vertical machining center. And a FEA model including the thermal contact resistance at interface for evaluating the temperature distribution and tools deformation in vertical machining center (VMC) was established. Compared with the experiment results, it is shown that the new model is much more accurate than the traditional model without considering thermal contact resistance at interface.


2019 ◽  
Vol 45 (17) ◽  
pp. 22196-22202 ◽  
Author(s):  
Milad Sakkaki ◽  
Farhad Sadegh Moghanlou ◽  
Mohammad Vajdi ◽  
FatemehZahra Pishgar ◽  
Mohammadreza Shokouhimehr ◽  
...  

Author(s):  
Adam S. Hollinger ◽  
Stefan T. Thynell

Localized temperature gradients in a polymer electrolyte fuel cell are known to decrease the durability of the polymer membrane. The most important factor in controlling these temperature gradients is the thermal contact resistance at the interface of the gas diffusion layer and the bipolar plate. Here we present thermal contact resistance measurements of carbon paper and carbon cloth gas diffusion layers over a pressure range of 0.7–14.5 MPa. Contact resistances are highly dependent upon the clamping pressure applied to a fuel cell, and in the present work, contact resistances vary from 3.5E−4 to 2.0E−5 m2K/W, decreasing non-linearly over the pressure range for each material tested. The data presented here also shows that the thermal resistance of the sample is negligible in comparison to the thermal contact resistance. Thermal uniformity in a fuel cell is desirable, and the measurements presented here can be used to more accurately predict temperature distribution in a polymer electrolyte fuel cell.


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