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

Table A3.

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 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 parameter g approximation for N measurements independently disturbed by additive, zero mean, normally distributed noises with standard deviation σ=8 kPa.

N QNgN kPa2 QNrelgN QgN kPa2 ERR [%] αN βN GeN kPa τrNs
50 1.823164 × 10−4 4.314509 × 10−3 2.993805 × 10−3 0.504 0.961565 8.769949 × 10−2 2.867641 15.1708579
100 6.647523 × 10−4 0.353591 9.411604 × 10−4 0.517 0.949857 5.428199 × 10−2 2.864822 15.193338
200 2.961081 × 10−4 4.334879 × 10−4 4.686224 × 10−3 4.277 × 10−3 0.954203 8.597868 × 10−2 3.066582 14.289093
500 6.078210 × 10−4 2.946700 × 10−5 5.271033 × 10−4 3.193 × 10−4 0.918084 1.579814 × 10−2 3.092238 12.837417
1000 5.328032 × 10−4 2.789884 × 10−3 5.267889 × 10−4 1.300 × 10−4 0.921325 1.356372 × 10−2 3.083203 12.926718
2000 5.248407 × 10−4 3.026647 × 10−7 5.403471 × 10−4 5.202 × 10−2 0.929297 2.403479 × 10−2 3.016320 13.557098
5000 5.883023 × 10−4 1.431097 × 10−5 5.210845 × 10−4 3.179 × 10−4 0.920442 1.473303 × 10−2 3.081219 12.984135
7000 5.759879 × 10−4 1.780341 × 10−7 5.220610 × 10−4 2.087 × 10−3 0.921658 1.538542 × 10−2 3.072622 13.066791
10,000 5.616302 × 10−4 2.127802 × 10−6 5.220589 × 10−4 5.578 × 10−4 0.920855 1.448935 × 10−2 3.079433 12.979817
12,000 5.739756 × 10−4 2.163690 × 10−4 5.211071 × 10−4 8.574 × 10−4 0.921109 1.594595 × 10−2 3.077685 13.006321
15,000 5.843841 × 10−4 5.116492 × 10−6 5.207537 × 10−4 4.857 × 10−4 0.920823 1.552819 × 10−2 3.079921 13.006321