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Kolling S, Haufe A, Feucht M, Bois PD (2006) A constitutive formulation for polymers subjected to high strain rates. In: 9th international LS-Dyna users conference. Detroit, USA 25. Boisse P (2010) Simulations of composite reinforcement forming. In: Dobnik Dubrovski P (ed) Woven fabric engineering. InTech, Rijeka, p 387–414 26. P676: Methodenentwicklung zur Berechnung von höherfesten Stahlklebeverbindungen des Fahrzeugbaus unter Crashbelastung (2008). V. Düsseldorf 27. Chauffray M, Delattre G, Guerin L, Pouvreau C (2013) Prediction of laser welding failure on seat mechanisms simulation.

Transition temperatures of the LFP specimen were noticeably higher than those of both metal/oxide cells (LCO/NMC and NMC). The LFP cell was able to withstand the highest temperature before going into thermal runaway. Both metal oxide cells showed the three stages described above (heat-up, quasi exponential heating, rapid thermal runaway). In contrast, the thermal runaway profile of the LFP cell lacked a distinct quasi-exponential stage. For the LFP cell, it was difficult to find a clear distinction between θo and θr .

Current collectors in the cell and details of a cylindrical cell are shown in Fig. 13). Here, it can be necessary to simplify the actual geometry, since an applicable FE crash net has a mesh size of about 5 mm, as shown for a cylindrical cell in Fig. 7. This can be done if the local deformation effects are understood and taken into account in the subsequent failure assessment. The active material, the jelly roll, contributes to the cell stiffness. Depending on the loading direction, it can be a major load-carrying component with a strong anisotropic deformation behaviour (shown in Fig.

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Automobile Magazine (June 2012)

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