Method and system for predicting electrochemical alternating-current impedance spectrum changing along with fuel cell attenuation
A technology of AC impedance spectroscopy and fuel cells, which is applied in prediction, design optimization/simulation, electrical digital data processing, etc. It can solve the problems of irreversible damage and consumption of fuel cells, and achieve the reduction of required time, high reliability and high precision Effect
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Embodiment 1
[0067] In the fuel cell attenuation experiment, take 50h as the time period T, record the high-frequency internal resistance data r ohm Variation with decay time t.
[0068] Take a quadratic polynomial: r=a 2 x 2 +a 1 x+a 0 , where r is the high-frequency internal resistance of the fuel cell, x is the decay test time, and a is the coefficient.
[0069] Considering the measurement noise of the instrument, the above-mentioned quadratic polynomial is corrected as r=a 2 x 2 +a 1 x+a 0 +ε, where ε is the noise mean square error.
[0070] Take the 0-300h high-frequency internal resistance measured data, and calculate r=a 2 x 2 +a 1 x+a 0 The actual function of +ε.
[0071] According to the calculation, the parameter a T estimated value of Estimated High Frequency Internal Resistance Vary with test time t;
[0072] During the attenuation test, as mentioned above, the high-frequency internal resistance in the subsequent attenuation experiment is estimated based on t...
Embodiment 2
[0075] In the fuel cell attenuation experiment, take 50h as the time period T, record the high-frequency impedance arc radius R hf Variation with decay time t.
[0076] Take a quadratic polynomial: r=a 2 x 2 +a 1 x+a 0 , where r is the high frequency impedance arc radius R hf , x is the time of the decay test, and a is the coefficient.
[0077] Considering the measurement noise of the instrument, the above-mentioned quadratic polynomial is corrected as r=a 2 x 2 +a 1 x+a 0 +ε, where ε is the noise mean square error.
[0078] Take 0-300h high frequency impedance arc radius R hf Measured data, calculated to get r=a 2 x 2 +a 1 x+a 0 The actual function of +ε.
[0079] According to the calculation, the parameter a T estimated value of Estimated high-frequency impedance arc radius R hf Vary with test time t;
[0080] During the attenuation test, as mentioned above, the radius R of the high-frequency impedance arc in the subsequent attenuation experiment is estim...
Embodiment 3
[0083] In the fuel cell attenuation experiment, take 50h as the time period T, record the low-frequency impedance arc radius R lf Variation with decay time t.
[0084] Take a quadratic polynomial: r=a 2 x 2 +a 1 x+a 0 , where r is the low-frequency impedance arc radius R lf , x is the time of the decay test, and a is the coefficient.
[0085] Considering the measurement noise of the instrument, the above-mentioned quadratic polynomial is corrected as r=a 2 x 2 +a 1 x+a 0 +ε, where ε is the noise mean square error.
[0086] Take 0-300h low frequency impedance arc radius R lf Measured data, calculated to get r=a 2 x 2 +a 1 x+a 0 The actual function of +ε.
[0087] According to the calculation, the parameter a T estimated value of Estimated low frequency impedance arc radius R lf Vary with test time t;
[0088] During the attenuation test, as mentioned above, the radius R of the low-frequency impedance arc in the subsequent attenuation experiment is estimated ...
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