Abstract

Today, poor long-term performance and durability combined with high production and maintenance costs remain the main obstacles for the commercialization of the polymer electrolyte membrane (PEM) fuel cells (PEMFCs). While on-line diagnosis and operating condition optimization play an important role in addressing the durability issue of the fuel cell, health-monitoring and prognosis (or PHM) techniques are of equally great significance in terms of scheduling condition-based maintenance (CBM) to minimize repair and maintenance costs, the associated operational disruptions, and also the risk of unscheduled downtime for the fuel cell systems.The two essential components of a PHM scheme for a general engineering system are 1) an accurate aging model that is capable of capturing the system’s gradual health deterioration, and 2) an algorithm for damage estimation and prognostics. In this paper, a physics-based, prognostic-oriented fuel cell catalyst degradation model is developed to characterize the relationship between the operating conditions and the degradation rate of the electro-chemical surface area (ECSA). The model complexity is kept minimal for on-line prognostic purpose. An unscented Kalman filter (UKF) approach is then proposed for the purpose of damage tracking and remaining useful life prediction of a PEMFC.

Highlights

  • To date long-term performance and durability of the fuel cells are difficult to quantify because not all degradation mechanisms of the various fuel cell components are completely understood

  • The rest of the paper is organized as follows: Section 2 presents the derivation process of a prognostic-oriented fuel cell catalyst degradation model; Section 3 gives a brief introduction to the unscented Kalman filter (UKF) framework; and in Section 4, we apply the UKF approach to the damage tracking and RUL prediction of the fuel cell, and discuss the results obtained from the simulation tests

  • Various filtering techniques can be implemented in this general recursive estimation framework, including the most widely used extended Kalman filter (EKF), particle filtering (PF), and unscented Kalman filter (UKF)

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Summary

INTRODUCTION

To date long-term performance and durability of the fuel cells are difficult to quantify because not all degradation mechanisms of the various fuel cell components are completely understood. The fuel cell’s performance degrades irreversibly throughout its lifetime mainly due to the following components’ degradations: (1) catalyst degradation (catalyst particle coarsening); (2) carbon support degradation (carbon corrosion); and (3) membrane degradation (chemical deterioration and dehydration) (Okada, 2003; Schmittinger & Vahidi, 2008) Factors affecting these degradation processes include temperature, high potentials, heat cycle but most of all water management, contaminants, and impurities. Sheng, Shao-Horn, & Morgan, 2009) investigated the influence of particle size distribution (PSD) and crossover hydrogen on the Pt nanoparticle stability in PEM fuel cells by extending the previous degradation model of Darling and Meyers The rest of the paper is organized as follows: Section 2 presents the derivation process of a prognostic-oriented fuel cell catalyst degradation model; Section 3 gives a brief introduction to the UKF framework; and, we apply the UKF approach to the damage tracking and RUL prediction of the fuel cell, and discuss the results obtained from the simulation tests The rest of the paper is organized as follows: Section 2 presents the derivation process of a prognostic-oriented fuel cell catalyst degradation model; Section 3 gives a brief introduction to the UKF framework; and in Section 4, we apply the UKF approach to the damage tracking and RUL prediction of the fuel cell, and discuss the results obtained from the simulation tests

Catalyst Degradation Mechanisms
N-Group Catalyst Degradation Model
Bayesian framework for joint estimation
UKF implementation
UKF Approach for Prediction
Damage Tracking and Prognostics for Catalyst Degradation
Fault Detection of the Initiation of Massive Hydrogen Crossover
CONCLUSION
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