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Pore scale modelling of a cathode catalyst layer in fuel cell environment: agglomerate reconstruction and variables optimization

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Abstract

In this work, a new strategy is adopted to optimize the cathode catalyst layer of a PEM fuel cell and to analyse the impact of three pertinent design variables. A pore scale, three-dimensional model is developed to predict the performance of a single agglomerate of the catalyst layer. The pore scale modelling is implemented as a two-step procedure. First, the microstructure of the catalyst layer is computationally reconstructed and then the governing and constitutive equations can be discretized and numerically solved. The agglomerate reconstruction follows a stochastic approach of the catalyst layer structure, and random routines are added to capture the variability and imperfections of the fabrication methods. From the obtained results, it is concluded that the design variables with the highest impact on performance were the carbon particle diameter and the Nafion volume fraction. In contrast, the agglomerate diameter did not show any impact on performance for the tested operational conditions. Another important finding was related with the influence of the operational pressure on the design variables performance impact. As pressure increased, the design variables contribution to the potential variability vanished. This work also demonstrated that performance was markedly affected by the random nature of the agglomerate structure.

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Abbreviations

a c :

Specific surface area, m2

A m :

Area of the interface porous/Nafion, m2

c :

Concentration, mol m−3

c 0 :

Concentration at the porous/Nafion interface, mol m−3

\( {c}_{O_2}^{ref} \) :

Reference concentration, mol m−3

\( \tilde{D} \) :

Binary diffusivity, m s−1

D m :

Diffusion coefficient in Nafion, m s−1

DOF p :

Degrees of freedom

E :

Activation energy, J

E rev :

Reversible potential, V

F :

Faraday’s constant, C mol−1

F CF :

F-value for each control factor

F critical :

F critical

I :

Current, A

i :

Current density, A m−2

i 0 :

Exchange current density, A m−2

j m :

Mass flux, kg m−2 s−1

j n :

Molar flux, mol m−2 s−1

L :

Number of levels per control factor

L c :

Catalyst loading, kg m−2

N :

Number of simulations

M :

Molecular mass, kg mol−1

n :

Number of electrons

p :

Pressure, Pa

\( {p}_{H_2O} \) :

Water partial pressure, Pa

R :

Gas constant, J K−1 mol−1

\( {S}_{O_2} \) :

Oxygen solubility in Nafion, mol m−3 Pa−1

SS e :

Sum of squared error

SS p :

Sum of squared deviations

SS T :

Sum of squares

T :

Temperature, K

U :

Potential, V

V p :

Variance of each control factor

w :

Mass fraction

x :

Molar fraction

α :

Charge transfer coefficient

γ :

Pressure coefficient or reaction order

η :

Overpotential, V

λ :

Water uptake

ρ :

Species mixture density, kg m−3

i and j :

Chemical species

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Acknowledgments

The present work is financed by FEDER funds through Programa Operacional Factores de Competitividade—COMPETE and by national funds through the Fundação para a Ciência e a Tecnologia (FCT) Project FCOMP-01-0124-FEDER-028580.

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Correspondence to T. Sousa.

Appendices

Appendix A

Table 6 shows the 27 simulations with the corresponded levels of the design variables. These simulations were used to analyse the influence of each design variable level on performance.

Table 6 List of the 27 simulations with the corresponded levels of the design variables

Appendix B. Analysis of variance (ANOVA)

The analysis of variance (ANOVA) is of particular interest to identify the relative importance amongst the analysed control factors on performance, and also to decide, through the F-test, if a specific control factor is significant or not for the performance variability.

In ANOVA, the analysis of variance is achieved by separating the total variability of the S/N ratios into contributions of each control factor and error. The total variability was obtained by the sum of the squared deviations from the total mean S/N ratio:

$$ S{S}_T={\displaystyle {\sum}_{i=1}^N{\left(S/{N}_i-\overline{S/N}\right)}^2} $$
(B1)

where, SS T is the sum of squares, N is the number of simulations in the orthogonal array (N = 18), S/N i is the S/N value for the i th case and \( \overline{S/N} \) is the total mean of the S/N values.

The contribution of each control factor to the sum of squares was calculated as:

$$ S{S}_p={\displaystyle {\sum}_{j=1}^L{\left(\frac{sS/{N}_j}{t}\right)}^2}-\frac{1}{N}{\left[{\displaystyle {\sum}_{i=1}^NS/{N}_i}\right]}^2 $$
(B2)

where, SS p is the sum of squared deviations due to each control factor, j is the level number, L is the number of levels per control factor, t is the repetition per level and sS/N j is the sum of the S/N ratio involving level j. The sum of squared error (SS e ) was then easily derived from the sum of squares and from the sum of the squared deviation of each control factor. The variance of the control factor was simply:

$$ {V}_p=S{S}_p/ DO{F}_p $$
(B3)

where, V p is the variance of each control factor or mean square deviation and DOF p are the degrees of freedom. The F-value for each control factor (F CF ) was simply the ratio of the mean of squares deviations to the mean of the squared error. Finally, the percentage of contribution by each of the control factor in the total sum of squared deviations was the ratio between SS p and SS T . More details about this methodology can be found elsewhere [27].

The F critical (F critical ) was found based on the statistical approach which obeyed f-distribution with L-1 numerator degrees of freedom, N-L denominator degrees of freedom and a significance level of 0.05. Having into account these considerations the F critical was found and the hypothesis for accepting or rejecting the significance of a control factor was given by the following rules: the control factor was not significant if F CF  ≤ F critical ; the control factor was significant if F CF  > F critical .

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Sousa, T., Rangel, C.M. Pore scale modelling of a cathode catalyst layer in fuel cell environment: agglomerate reconstruction and variables optimization. J Solid State Electrochem 20, 541–554 (2016). https://doi.org/10.1007/s10008-015-3076-4

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  • DOI: https://doi.org/10.1007/s10008-015-3076-4

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