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. 2024 Mar 27;17(7):1527. doi: 10.3390/ma17071527

Table A1.

The elements αN, βN, GeN and τrN of the FMM parameter vector gN solving identification task (25) for real relaxation modulus (36) of the material described by the unimodal Gauss-like distribution, the mean-square identification indices QNgN, Equation (24), the mean relative square model approximation index QNrelgN, Equation (38), the sampling points-independent integral indices QgN defined by the optimization task (26), and the relative errors ERR (37) of the FMM parameter g approximation for N relaxation modulus measurements independently disturbed by additive, zero mean, normally distributed noises with standard deviation σ=2 kPa.

N QNgN kPa2 QNrelgN QgN kPa2 ERR [%] αN βN GeN kPa τrNs
50 9.295186 × 10−5 2.102093 × 10−3 2.863765 × 10−3 0.527 0.963788 8.644275 × 10−2 2.862573 15.170858
100 5.614324 × 10−4 5.907274 × 10−5 1.350707 × 10−3 1.224 0.965614 7.207174 × 10−2 2.745219 16.225154
200 2.185904 × 10−4 1.109724 × 10−4 4.959376 × 10−3 4.537 × 10−3 0.954725 8.815551 × 10−2 3.065976 14.289093
500 5.559271 × 10−4 5.053629 × 10−5 5.262647 × 10−4 7.740 × 10−3 0.915232 1.261495 × 10−2 3.113879 12.68090
1000 4.594139 × 10−4 1.476206 × 10−4 5.268387 × 10−4 3.104 × 10−4 0.920937 1.341017 × 10−2 3.081285 12.926718
2000 4.668059 × 10−4 3.243456 × 10−6 5.396114 × 10−4 5.315 × 10−2 0.929099 2.375304 × 10−2 3.015563 13.557098
5000 5.289533 × 10−4 3.282759 × 10−7 5.213213 × 10−4 2.876 × 10−4 0.920502 1.445854 × 10−2 3.081489 12.984136
7000 5.224292 × 10−4 3.978418 × 10−6 5.215398 × 10−4 1.654 × 10−4 0.920364 1.419721 × 10−2 3.082754 12.979817
10,000 5.082251 × 10−4 3.739909 × 10−6 5.219846 × 10−4 9.301 × 10−5 0.920327 1.391317 × 10−2 3.083746 12.942422
12,000 5.150186 × 10−4 1.363350 × 10−5 5.208965 × 10−4 1.689 × 10−5 0.920187 1.504288 × 10−2 3.085455 12.942422
15,000 5.247854 × 10−4 3.687418 × 10−6 5.205439 × 10−4 1.938 × 10−8 0.920014 1.472034 × 10−2 3.086680 12.949456