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

Table A2.

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 measurements independently disturbed by additive, zero mean, normally distributed noises with standard deviation σ=5 kPa.

N QNgN kPa2 QNrelgN QgN kPa2 ERR [%] αN βN GeN kPa τrNs
50 1.246174 × 10−4 3.1182072 × 10−3 2.953417 × 10−3 0.501 0.962059 8.720788 × 10−2 2.868287 15.170858
100 6.042548 × 10−4 9.788569 × 10−3 9.505292 × 10−4 0.542 0.950711 5.528005 × 10−2 2.859441 15.193338
200 2.469407 × 10−4 2.622478 × 10−4 4.888504 × 10−3 3.999 × 10−3 0.954563 8.747687 × 10−2 3.067250 14.289093
500 5.754599 × 10−4 1.136117 × 10−7 5.288353 × 10−4 1.1543 × 10−4 0.917799 1.594113 × 10−2 3.090037 12.837417
1000 4.8724914 × 10−4 6.769619 × 10−4 5.261736 × 10−4 2.129 × 10−4 0.921142 1.374989 × 10−2 3.082219 12.926718
2000 4.8687842 × 10−4 3.040833 × 10−7 5.400918 × 10−4 5.345 × 10−2 0.929234 2.394509 × 10−2 3.015365 13.557098
5000 5.4973567 × 10−4 3.940686 × 10−6 5.211862 × 10−4 3.026 × 10−4 0.920472 1.459525 × 10−2 3.081354 12.984135
7000 5.401956 × 10−4 1.559930 × 10−6 5.214093 × 10−4 1.573 × 10−4 0.920350 1.428889 × 10−2 3.082852 12.979817
10,000 5.261243 × 10−4 2.744246 × 10−6 5.221499 × 10−4 5.516 × 10−4 0.920905 1.446157 × 10−2 3.079473 12.979817
12,000 5.356062 × 10−4 5.782985 × 10−5 5.208668 × 10−4 2.386 × 10−5 0.920122 1.495904 × 10−2 3.085216 12.942422
15,000 5.457918 × 10−4 4.535517 × 10−6 5.205517 × 10−4 2.513 × 10−7 0.919980 1.477095 × 10−2 3.086569 12.949456