2018
DOI: 10.1007/s00161-018-0629-7
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Stochastic many-particle model for LFP electrodes

Abstract: In the framework of non-equilibrium thermodynamics we derive a new model for many-particle electrodes. The model is applied to LiFePO 4 (LFP) electrodes consisting of many LFP particles of nanometer size. The phase transition from a lithium-poor to a lithium-rich phase within LFP electrodes is controlled by both different particle sizes and surface fluctuations leading to a system of stochastic differential equations.An explicit relation between battery voltage and current controlled by the thermodynamic state… Show more

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Cited by 23 publications
(20 citation statements)
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“…Tanaka: As already mentioned, in the context of battery modelling with additive noise [23], no rough path machinery is necessary, leave alone some formidable difficulties for rough differential equations to deal with reflecting boundaries [1,18]. This was the initial motivation for our pathwise study, which soon turned out informative and rather pleasing in the generality displayed here.…”
Section: Introductionmentioning
confidence: 82%
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“…Tanaka: As already mentioned, in the context of battery modelling with additive noise [23], no rough path machinery is necessary, leave alone some formidable difficulties for rough differential equations to deal with reflecting boundaries [1,18]. This was the initial motivation for our pathwise study, which soon turned out informative and rather pleasing in the generality displayed here.…”
Section: Introductionmentioning
confidence: 82%
“…Last not least, our motivation comes from a recent battery model, cf. (1.6) below, taken from [23], which is of the form (1.1) but with reflecting boundary as given in (1.5).…”
Section: Introductionmentioning
confidence: 99%
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“…A more detailed derivation of this reduction of a triple phase line into a 1D model can be found in the context of intercalation electrodes in [20].…”
Section: Surface-triple Phase Boundarymentioning
confidence: 99%
“…In this work, we focus on the class of MV-SDE with drifts of super-linear growth in their spatial components [4,18,19,33,45], encapsulated in the function v, where b, σ are uniformly Lipschitz (in space and measure), and σ is non-constant. This class of MV-SDEs appears in several practical models in science, for example, in neuroscience [3,12] introduce the mean-field FitzHugh-Nagumo model for a neurons networks in the brain; [11] discuss individual-based and swarming Cucker-Smale interaction models; and models of battery electrodes [21,26]. These equation do not have explicit or closed form solutions and numerical approximations are needed.…”
Section: Introductionmentioning
confidence: 99%