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Abstract

Automotive industry is in the process of changing from conventional propulsion to electric drive. Introduction of high voltage circuits, voltage above 48V, brings new challenges to the design of the vehicle. One of those is the need to protect the harness from harmful ingress of moisture or particulates that would cause is to fail prematurely or cause a hazard for the end user. The usage of various materials for protection against foreign material intrusions can cause unforeseen issues, depending on the choice of materials for encapsulation and the level of protection required, be it over-moulding, potting or enclosure. In this article a case study of incorrect material choice will be presented with possible implications and what to do to avoid the problem from occurring in future endeavours. Incorrect choice of materials for enclosure can cause it to fail in its function due to differences in thermal expansions factors and the possibility can cause the destruction of the assembly.

Keywords

thermal expansion; encapsulation; ingress protection; material incompatibility; high voltage; material bonding.

Introduction

In the development of electric vehicles, there has been a need to develop new ways to route the connections inside the vehicle. High voltage architecture has got its own challenges to overcome in order to be competitive in production. Using new types of connections and the usage of new materials to protect the connection between two lines.[1]

Examples for connections can be placed into the following groups:

  • Direct connection, cannot be disengaged, no terminal or connector required.
  • Terminal connection, can be disengaged, terminal and or connector required.

Both connection types have their advantages and disadvantages. The direct connection is preferred in situations that require resistance to forces that might be transferred threw it during assembly of the system. The connection is done with the use of a type of a screw joint or Direct connection of two lines.[2] The negative of this type of connection is that it is hard to disassemble after the component has been installed and the insulation of both parts of the conductor have to be extended. Terminal connection offers a quick disassembly possibility but is more prone to damage coming from forces in the system, for example during assembly of the component. Also in case of high voltage systems it must be protected against sparking that could destroy the connector during disassembly. The need to protect the route of the connection especially their joints against the ingress of the elements be in particle pollutants or fluids that can either damage the conductor causing an increase of contact resistance or disrupt the connection completely [1]. Insufficient ingress protection can also cause water to travel along the conductor and cause damage to the devices that are interconnected by the line.  Various method have been employed to try to prevent the phenomenon from occurring. One was to use of gaskets to prevent the ingress of pollutants into the system. The other that will be looked in more detail in this article will be encapsulation of a material with other material. This can be done in a multitude of methods. Over-moulding is the process in which a high temperature plastic is used to encapsulate the instance of interest by the means of injection of the plastic. For this method the same material or similar can be used for encapsulation. The drawback of the method is the requirement of using tooling for the injection moulding process this has a significant impact on the piece price, especially in case of low volume production. Potting [3] is a similar method to over-moulding. However in the case of potting the material is fed into the assembly under gravity or by the use of low pressure system. Hot melt is a form of using a low pressure and low temperature material for over-moulding, in comparison to pressures and temperatures in case of standard over-moulding. [4],[5] For all the above mentioned cases depending on the material used a phenomenon can be observed that leads to the systems ingress protection being compromised and in some cases the whole assembly being destroyed. [6] In this study we will try to explain the reason for the occurrence of the phenomenon and what can be done to prevent the failure mechanism from occurring.  The case has been observed during a thermal shock test [7]. Test sample encapsulated in an over-moulded [8] material has been destroyed by a cable pushing threw the material after a series of cycles of the thermal shock. Simulation of thermal behaviour [9] of the materials and an explanation of what led to the destruction of the sample will be described further in this article.

2. Materials and Methods

The phenomenon has been observed during the thermal shock testing [7] of the sample. The sample has been constructed in order to test ingress protection for an encapsulation solution and it’s resistance to mechanical stress coming from sudden temperature changes. Sample has been constructed out of two conductors ultrasonically welded together to represent a joint. Conductive material is CuETP and insulation material is made of PA material. Encapsulant is made of modified PA6 material. Diagram of the sample’s construction has been illustrated in figure 1.

Figure 1. Test Sample.

This has been tested using thermal shock test according to DIN EN60068-2-14. Schematic of a thermal chamber with two chambers, one set to [Tmax] the second to [Tmin] can be seen in Figure 2.

Figure 2. Test Chamber Schematic.

Maximum temperature has been selected to be 180 degrees, minimum temperature has been set to minus 40 degrees. The change time is less than 30 seconds and the dwell time was 15 minutes per temperature after the temperature stabilised. Number of test samples was set to 6, this is a standard amount in automotive industry testing n=6.

Figure 3. Thermal shock test graph.

3 Data preparation (Finite Element Method)                 

For the purpose of the simulation part of the model was used due to its symmetry. The part of the sample that was modelled can be seen in figure 4.

Figure 4. Part of sample used for FEM simulation.

In order to be able to properly model the phenomenon the following data had to be prepared. For example the following method can be used [10]

  • Material properties for the specific material in question.[11],[12], [13],[14],[15]

? Encapsulant:                                     PA6                                        

 ? Conductor insulator:                        PE                                          

  ? Conductor:                                  Copper                           

Sample length has been set to 100mm length for the conductor and insulator and the over-moulding material were set to 50mm in length. This was done to represent a sufficient encapsulation to prevent capillary pull of water into the uninsulated part of the conductor.[8]

  • Testing procedure.
  • Sample had been heated to 180°C
  • Boundary conditions.
  • Boundary conditions can be seen in figure 5

Figure 5. Boundary conditions

? Frictionless support at the connection planes between the different bodies.

• Element size has been set to 0.5mm as illustrated in figure 5. The complete amount of calculation nodes is 332318 and 72823 elements.

Figure 6. Mesh element size 0,5mm

• Sample has been heated up to 180 degrees in order to illustrate the relative increase in dimensions for the different materials.

4 Model results & verification

Calculation model has been prepared as a 3D section of the sample tested. This has been done in order to better visualise the phenomenon. Relative sizes had been kept. [17],[18],[19] Setup of the model described in section 3 has been used to simulate the behaviour of materials during the test. The model has been prepared, as mentioned, with a frictionless support to be able to visualise the difference in expansion coefficients of the different materials.

Figures 7,8,9 depict distortion of material in the 3 principal axis.

Figure 7. Thermal expansion rate, differences between bodies.

Figure 8. Thermal deformation in X-axis.

Figure 9. Thermal deformation in Y-axis.

Figure 10. Thermal deformation in Z-axis.

The model depicts that the biggest expansion is for the insulation material.  The next is the environmental protection material, conductor material is the one that expands the least. In the model it was possible to observe that the insulator has extended by approximately 2mm, next in regards to thermal expansion was the over-moulding material. It has expanded by approximately 1,2mm last was the conductor that had expanded by only 0,2mm. As can be seen in figure 10. This does confirm the laboratory observations.

5 Results & Discussion

It was observed that after 100 to 150 cycles samples were being destroyed. The failure occurred when a cable has been pushed through the encapsulating material. In the case study the material was a modified PA material used for the process of hot-melt over-moulding. Encapsulation has been done by over moulding a cable assembly with the aforementioned hot-melt material. Failure mechanism was found out to be caused by a specific order of thermal expansion and contraction during testing. In the heat up phase the material to heat up first was the conductor of the cable, due to good thermal conductivity of copper. Next was cable insulator, last to expand was the encapsulating material. Big role in the phenomenon was also the thermal expansion factor difference of the materials. This made the insulator expand significantly more than metallic conductor. During the cooling phase the same order caused the conductor to be pressed into the enclosure, initially be the insulator while contracting pressed the conductor in and next material of the casing further pressed it into the sample and prevented it from moving in the initial stages of heat up part of the cycle.

Figure 11. Failure mechanism 0-50 cycles.

Each cycle had caused the conductor to be pressed a bit more into the material, forcing it through the enclosure in the end. Figure 11 shows the initial status of the sample the conductor is being pressed inside the encapsulation.

Figure 12. Failure mechanism 50-100 cycles.

In the middle of the testing process the weld knot had become distorted and depending on where friction was greater that side will act as the anchor point. Opposite side will start to press on the weld knot and start to distort it. This will in turn start to move one end of the knot towards the edge of the encapsulating moulding. This was represented in schematic in figure 12.

Figure 13. Failure mechanism 100-150 cycles.

After about 100 to 150 cycles the weld knot will be forced through the samples moulding material. As can be seen in figure 13. Break occurs in gradual steps as was presented in figure 14. It is possible to observe a gradual breaking line as the weld knot is gradually pushed through the plastic material. It has been established that the event occurred because the materials are all chemically inert and will not react with each other during processing. Chemical bond would ensure good protection against incursion of elements. The material used for case moulding did not bond chemically to the insulation material. Only method of ensuring contact between the two materials was a mechanical bond. Coming from pressure from shrinkage of materials after moulding process. During the thermal shock the material is being pressed in little by little. The conductor breakout occurred and the laboratory samples have had a beachhead break fracture of the over mould material.

From the observation of the phenomenon, it was possible to establish that the choice of material for ingress protection needs to be done with significant thought behind it. This phenomenon was not observed in the industry until now as the usage of high voltage systems became widespread with the introduction of electric vehicles. In case of low voltage circuits the operating temperatures were lower and this behaviour was not observed. The case of high voltage makes this even more important as the temperatures and implications of incorrect choice are more severe than in case of low voltage (below 48V) systems. Protecting material has to either be able to bond chemically with the insulation or have a similar thermal expansion coefficient to allow for both the materials to retain a mechanical bond during the life cycle of the component. Second possibility is to select a material that is more flexile so that it can accommodate the thermal distortions coming form the rapid change of temperature. This way bond between the materials can be retained as well as protection against elements. Failure to correctly select material can result as in case of this study in not only loss of intended function by the component but also in destruction of the component

Figure 14. Break out of the conductor threw encapsulant.

What can be seen in figure14 is that the breakout had occurred in gradual steps. The beachhead lines of the gradual progression of the break out created by the conductor, slowly, in each cycle, cracking the encapsulating over-mould and gradually pushing threw the material.

6 Conclusions

It is important to choose correct materials when choosing protective material. If materials are not chosen in a correct way it may cause an unforeseen behaviour of the system like the phenomenon that had occurred. Materials chosen should have similar thermal expansion in order to expand and contract in a similar way, that will decrease the mechanical stress on the components. Alternatively, materials should have sufficient flexibility to be able to accommodate for the relative movement. Ideally material pairs should be chosen that they form a chemical bond or adhere to each other. 

Lack of the above-mentioned conditions might lead to thermo-mechanical stress that in turn might lead breakage of mechanical bond between material parts and damage components causing loss of function or destruction of component like in the presented case. [17],[18],[19],[20] In the preparation of this article no GenAI tool have been used.

Author Contributions: Conceptualization, investigation, data validation, writing—original draft preparation Rafal Krawczyk; formal analysis Marcin ??cki and Grzegorz Górecki; data curation, Marcin ??cki and Grzegorz Górecki.; writing—review and editing, Marcin ??cki and Grzegorz Górecki.; supervision, ?ukasz Kaczmarek. All authors have read and agreed to the published version of the manuscript.”

Funding: This research received no external funding

Data Availability Statement: Exact laboratory data are the property of the SEI Automotive Europe GmbH.

Acknowledgments: The Authors would like to thank SEI Automotive Europe GmbH for their support.

Conflicts of Interest: Declare conflicts of interest or state “The authors declare no conflicts of interest.” Authors must identify and declare any personal circumstances or interest that may be perceived as inappropriately influencing the representation or interpretation of reported research results. Any role of the funders in the design of the study; in the collection, analyses or interpretation of data; in the writing of the manuscript; or in the decision to publish the results must be declared in this section. If there is no role, please state “The funders had no role in the design of the study; in the collection, analyses, or interpretation of data; in the writing of the manuscript; or in the decision to publish the results”.

Abbreviations

The following abbreviations are used in this manuscript.

REFERENCES

  1. Aptiv WhitePaper Busbar Technology. Randy Sumner ,Director, Global High Voltage Wiring Product Line & Tom Drummond Manager, Global High Voltage Product Engineering.
  2. Effects of cable insulations’ physical and geometrical parameters on sheath transients and insulation losses Natheer Alatawneh Cysca Technologies Inc., 275A Pierre-Le Gardeur blvd., Repentigny, Quebec, Canada Polytechnique Montreal, 2900 boul. Edouard-Montpetit, Quebec, Canada.
  3. https://www.sciencedirect.com/science/article/pii/S0026271418303007
  4. Influence of injection temperature and pressure on the properties of alumina parts fabricated by low pressure injection molding (LPIM) M. Sardarian, O. Mirzaee, A. Habibolahzadeh Faculty of Materials and Metallurgical Engineering, Semnan University, Semnan, Iran.
  5. Numerical and experimental study of injection step, separation, and imbalance filling in low pressure injection molding of ceramic components Rezvan Yavari, Hamid Khorsand Faculty of Materials Science and Engineering, K. N. Toosi University of Technology, Vanak Sq., Pardis St., 19991-43344, Tehran, Iran
  6. A study on the coefficients of thermal expansion of periodic unidirectional fiber reinforced composites. Proceedings of the XLI Ibero-Latin-American Congress on Computational Methods in Engineering, ABMEC Foz do Iguaçu/PR, Brazil, November 16-19, 2020
  7. https://www.sciencedirect.com/science/article/pii/S0026271425000514
  8. Experimental study of thermal shrinkage and melt dripping properties of expanded polystyrene under various heat fluxes Manman Zhang, Mi Li, Yu Wang, Jinhua Sun, State Key Laboratory of Fire Science, University of Science and Technology of China, Huangshan Road 443, Hefei, 230026, Anhui, China.
  9. Calculation of the loading capacity of high voltage cables laid in close proximity to heat pipelines using iterative finite-element method. Jovan Nahmana, Miladin Tanaskovicb. Faculty of Electrical Engineering, University of Belgrade, Bul. K. Aleksandra 73, 11000 Belgrade, Serbia Electricity Board Serbia, Masarikova 1-3, 11000 Belgrade, Serbia.
  10. Measurement of Thermal expansion coefficient of solid Materials by double slit Interferometric method. IOP Conf. Series: Materials Science and Engineering 768 (2020) 022024 doi:10.1088/1757-899X/768/2/022024
  11. Finite element analysis of electric field distribution in water treed XLPE cable insulation (1): The influence of geometrical configuration of water electrode for accelerated water treeing test Chonung Kima, Jongbok Jangc, Xingyi Huanga, Pingkai Jianga, Hyeil Ki
  12. Resin Transfer molding of High-Fluidity Polyamide-6 with modified Glass-Fabric preforms Colin Gomez, Damiano Salvatori, Baris Caglar, Robin Trigueira, Gilles Orange, V´eronique Michaud.
  13. Polyamide (PA) 66 molding defect studied with optical coherence tomography (OCT) and near-infrared (NIR) spectroscopy Hideyuki Shinzawa, Maito Koga. Research Institute for Sustainable Chemistry, National Institute of Advanced Industrial Science and Technology (AIST), Tsukuba, Japan.
  14. Degradation mechanisms of cable insulation materials durin gradiation thermal ageingin radiation environment Tadao Seguchi, KiyotoshiTamura, TakeshiOhshima, AkihikoShimada, HisaakiKudoh. Japan Atomic Energy Agency, Tokai 319-1195,Japan. University of Tokyo,Tokai319-1195,Japan.
  15. Crystalline properties of injection molded polyamide-6 and polyamide-6/montmorillonite nanocomposites Africa Yebra-Rodríguez, Pedro Alvarez-Lloret, Carolina Cardell, Alejandro B. Rodríguez-Navarro. Department of Geology, Faculty of Experimental Science, University of Jaen, Campus Las Lagunillas, s/n, 23071 Jaén, Spain. Department of Mineralogy and Petrology, Faculty of Science, University of Granada, Campus Fuentenueva s/n, 18071 Granada, Spain
  16. Kui Liu, Renato Zagorš?ak, Richard J. Sandford, Oliver N. Cwikowski, Alexander Yanushkevich and Hywel R. Thomas. Insights into the Thermal Performance of Underground High Voltage Electricity Transmission Lines through Thermo-Hydraulic Modelling. Energies 2022, 15, 8897. https://doi.org/10.3390/en15238897, www.mdpi.com/journal/energies
  17. Peng-yu Wang, Hui Ma, Gang Liu1, Zhuo-zhan Han, De-ming Guo, Tao Xu, Long-yun Kang Dynamic Thermal Analysis of High-voltage Power Cable Insulation for Cable Dynamic Thermal Rating DOI 10.1109/ACCESS.2019.2913704, IEEE Access
  18. Boguslaw Wiecek, Gilbert De Mey, Vasilis Chatziathanasiou, Antonis Papagiannakis, Ioanna Theodosoglou, Harmonic analysis of dynamic thermal problems in high voltage overhead transmission lines and buried cables, International Journal of Electrical Power & Energy Systems, Volume 58, 2014, Pages 199-205, ISSN 0142-0615, https://doi.org/10.1016/j.ijepes.2014.01.031.
  19. Sergio Daniel Montana Salas, Andrea Michiorri. Long-Term Dynamic Thermal Ratings of Underground Cables Integrating Soil Dynamics and Climate Projections. 2024. hal-04453943Author 1, A.B.; Author 2, C.D. Title of the article. Abbreviated Journal Name Year, Volume, page range.

Reference

  1. Aptiv WhitePaper Busbar Technology. Randy Sumner ,Director, Global High Voltage Wiring Product Line & Tom Drummond Manager, Global High Voltage Product Engineering.
  2. Effects of cable insulations’ physical and geometrical parameters on sheath transients and insulation losses Natheer Alatawneh Cysca Technologies Inc., 275A Pierre-Le Gardeur blvd., Repentigny, Quebec, Canada Polytechnique Montreal, 2900 boul. Edouard-Montpetit, Quebec, Canada.
  3. https://www.sciencedirect.com/science/article/pii/S0026271418303007
  4. Influence of injection temperature and pressure on the properties of alumina parts fabricated by low pressure injection molding (LPIM) M. Sardarian, O. Mirzaee, A. Habibolahzadeh Faculty of Materials and Metallurgical Engineering, Semnan University, Semnan, Iran.
  5. Numerical and experimental study of injection step, separation, and imbalance filling in low pressure injection molding of ceramic components Rezvan Yavari, Hamid Khorsand Faculty of Materials Science and Engineering, K. N. Toosi University of Technology, Vanak Sq., Pardis St., 19991-43344, Tehran, Iran
  6. A study on the coefficients of thermal expansion of periodic unidirectional fiber reinforced composites. Proceedings of the XLI Ibero-Latin-American Congress on Computational Methods in Engineering, ABMEC Foz do Iguaçu/PR, Brazil, November 16-19, 2020
  7. https://www.sciencedirect.com/science/article/pii/S0026271425000514
  8. Experimental study of thermal shrinkage and melt dripping properties of expanded polystyrene under various heat fluxes Manman Zhang, Mi Li, Yu Wang, Jinhua Sun, State Key Laboratory of Fire Science, University of Science and Technology of China, Huangshan Road 443, Hefei, 230026, Anhui, China.
  9. Calculation of the loading capacity of high voltage cables laid in close proximity to heat pipelines using iterative finite-element method. Jovan Nahmana, Miladin Tanaskovicb. Faculty of Electrical Engineering, University of Belgrade, Bul. K. Aleksandra 73, 11000 Belgrade, Serbia Electricity Board Serbia, Masarikova 1-3, 11000 Belgrade, Serbia.
  10. Measurement of Thermal expansion coefficient of solid Materials by double slit Interferometric method. IOP Conf. Series: Materials Science and Engineering 768 (2020) 022024 doi:10.1088/1757-899X/768/2/022024
  11. Finite element analysis of electric field distribution in water treed XLPE cable insulation (1): The influence of geometrical configuration of water electrode for accelerated water treeing test Chonung Kima, Jongbok Jangc, Xingyi Huanga, Pingkai Jianga, Hyeil Ki
  12. Resin Transfer molding of High-Fluidity Polyamide-6 with modified Glass-Fabric preforms Colin Gomez, Damiano Salvatori, Baris Caglar, Robin Trigueira, Gilles Orange, V´eronique Michaud.
  13. Polyamide (PA) 66 molding defect studied with optical coherence tomography (OCT) and near-infrared (NIR) spectroscopy Hideyuki Shinzawa, Maito Koga. Research Institute for Sustainable Chemistry, National Institute of Advanced Industrial Science and Technology (AIST), Tsukuba, Japan.
  14. Degradation mechanisms of cable insulation materials durin gradiation thermal ageingin radiation environment Tadao Seguchi, KiyotoshiTamura, TakeshiOhshima, AkihikoShimada, HisaakiKudoh. Japan Atomic Energy Agency, Tokai 319-1195,Japan. University of Tokyo,Tokai319-1195,Japan.
  15. Crystalline properties of injection molded polyamide-6 and polyamide-6/montmorillonite nanocomposites Africa Yebra-Rodríguez, Pedro Alvarez-Lloret, Carolina Cardell, Alejandro B. Rodríguez-Navarro. Department of Geology, Faculty of Experimental Science, University of Jaen, Campus Las Lagunillas, s/n, 23071 Jaén, Spain. Department of Mineralogy and Petrology, Faculty of Science, University of Granada, Campus Fuentenueva s/n, 18071 Granada, Spain
  16. Kui Liu, Renato Zagorš?ak, Richard J. Sandford, Oliver N. Cwikowski, Alexander Yanushkevich and Hywel R. Thomas. Insights into the Thermal Performance of Underground High Voltage Electricity Transmission Lines through Thermo-Hydraulic Modelling. Energies 2022, 15, 8897. https://doi.org/10.3390/en15238897, www.mdpi.com/journal/energies
  17. Peng-yu Wang, Hui Ma, Gang Liu1, Zhuo-zhan Han, De-ming Guo, Tao Xu, Long-yun Kang Dynamic Thermal Analysis of High-voltage Power Cable Insulation for Cable Dynamic Thermal Rating DOI 10.1109/ACCESS.2019.2913704, IEEE Access
  18. Boguslaw Wiecek, Gilbert De Mey, Vasilis Chatziathanasiou, Antonis Papagiannakis, Ioanna Theodosoglou, Harmonic analysis of dynamic thermal problems in high voltage overhead transmission lines and buried cables, International Journal of Electrical Power & Energy Systems, Volume 58, 2014, Pages 199-205, ISSN 0142-0615, https://doi.org/10.1016/j.ijepes.2014.01.031.
  19. Sergio Daniel Montana Salas, Andrea Michiorri. Long-Term Dynamic Thermal Ratings of Underground Cables Integrating Soil Dynamics and Climate Projections. 2024. hal-04453943Author 1, A.B.; Author 2, C.D. Title of the article. Abbreviated Journal Name Year, Volume, page range.

Photo
Rafal Krawczyk
Corresponding author

SEI Automotive Europe GmbH

Photo
Lukasz Kaczmarek
Co-author

Technical University of Lodz

Photo
Grzegorz Gorecki
Co-author

Technical University of Lodz

Photo
Marcin Lecki
Co-author

Technical University of Lodz

Rafa? Krawczyk*, Marcin ??cki, Grzegorz Górecki, ?ukasz Kaczmarek, Thermal expansion of materials in High Voltage applications and possible failures coming from incorrect choice, Int. J. in Engi. Sci., 2025, Vol 2, Issue 12, 12-21. https://doi.org/10.5281/zenodo.18844351

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