Research Article

Spectral Classification of Non-Coaxiality for Two-Dimensional Incremental Stress-Strain Response

Table 3

(a) Model parameters for stable INC ( 𝐶 𝑑 𝑖 𝑗 𝑘 𝑙 𝛿 𝑘 𝑙 = 0 , 𝜆 1 = 𝜆 1 = 0 )

Classification Domains in Figure 6 𝐶 𝑖 𝑗 𝑘 𝑙 coefficientsSpectral propertiesComputation results in Figure 7

I 1 . 5 0 . 5 0 0 . 5 1 . 5 0 0 0 0 . 1 𝜆 2 = 2 . 0 , 𝜆 3 = 0 . 2 ,(a)
( 𝐵 = 𝐵 ) 𝜆 2 = 2 . 0 , 𝜆 3 = 0 . 2

𝑎 + 𝐴 + 1 . 0 0 . 5 1 . 5 1 . 0 1 . 5 1 . 5 0 0 1 . 0 𝜆 2 = 3 . 5 , 𝜆 3 = 0 . 5 ,(b)
( 𝐵 > 𝐵 ) 𝜆 2 = 𝜆 3 = 2 . 0

𝑜 𝐴 + 1 . 5 0 . 5 0 0 . 5 1 . 5 0 0 0 1 . 0 𝜆 2 = 𝜆 3 = 𝜆 2 = 𝜆 3 = 2 . 0 (c)
( 𝐵 = 𝐵 )

VI 1 . 0 0 . 5 1 . 0 1 . 0 1 . 5 1 . 0 2 . 0 2 . 0 1 . 0 𝜆 2 = 3 . 0 , 𝜆 3 = 1 . 0 (d)
( 𝐵 > 𝐵 ) 𝜆 2 = 2 . 0 + 2 . 8 𝑖 (complex) 𝜆 3 = 2 . 0 2 . 8 𝑖 (complex)

(b) Model parameters for instable INC ( 𝐶 𝑑 𝑖 𝑗 𝑘 𝑙 𝛿 𝑘 𝑙 = 0 , 𝜆 1 = 𝜆 1 = 0 )

Classification Domains in Figure 6 𝐶 𝑖 𝑗 𝑘 𝑙 coefficientsSpectral propertiesComputation results in Figure 8

II 0 . 5 1 . 5 0 1 . 5 0 . 5 0 0 0 0 . 1 𝜆 2 = 0 . 2 , 𝜆 3 = 1 . 0 ,(a)
( 𝐵 = 𝐵 ) 𝜆 2 = 0 . 2 , 𝜆 3 = 1 . 0

𝑎 𝐴 0 . 5 2 . 0 0 1 . 5 1 . 0 0 0 . 5 0 . 5 0 . 5 𝜆 2 = 0 . 5 , 𝜆 3 = 1 . 5 ,(b)
( 𝐵 > 𝐵 ) 𝜆 2 = 𝜆 3 = 1 . 0

𝑜 𝐴 0 . 5 1 . 5 0 1 . 5 0 . 5 0 0 0 0 . 5 𝜆 2 = 𝜆 3 = 𝜆 2 = (c)
( 𝐵 = 𝐵 ) 𝜆 3 = 1 . 0

VII 0 . 5 2 . 0 1 . 0 1 . 5 1 . 0 1 . 0 1 . 5 1 . 5 0 . 5 𝜆 2 = 0 . 5 , 𝜆 3 = 1 . 5 (d)
𝜆 2 = 1 . 0 + 2 . 4 5 𝑖 (complex)
( 𝐵 > 𝐵 ) 𝜆 3 = 1 . 0 2 . 4 5 𝑖 (complex)

(c) Model parameters for stable-instable INC transition ( 𝐶 𝑑 𝑖 𝑗 𝑘 𝑙 𝛿 𝑘 𝑙 = 0 , 𝜆 1 = 𝜆 1 = 0 )

Classification Domains in Figure 6 𝐶 𝑖 𝑗 𝑘 𝑙 coefficientSpectral propertiesComputation results in Figure 9

Point 𝑜 1 . 0 1 . 5 0 . 1 1 . 0 1 . 5 0 . 1 0 . 1 0 . 1 0 . 0 𝜆 2 = 𝜆 3 = 0
( 𝐵 > 𝐵 ) 𝜆 2 = 0 . 2 𝑖 (complex) 𝜆 3 = 0 . 2 𝑖 (complex)

(d) Model parameters for partially stable INC ( 𝐶 𝑑 𝑖 𝑗 𝑘 𝑙 𝛿 𝑘 𝑙 = 0 , 𝜆 1 = 𝜆 1 = 0 )

Classification Domains in Figure 6 𝐶 𝑖 𝑗 𝑘 𝑙 coefficientsSpectral propertiesComputation results in Figure 10

IV 1 . 0 0 . 5 0 . 6 1 . 0 1 . 5 0 . 6 1 . 5 1 . 5 1 . 0 𝜆 2 = 4 . 1 , 𝜆 3 = 0 . 1 (a)
( 𝐵 > 𝐵 ) 𝜆 2 = 3 . 9 , 𝜆 3 = 0 . 1

𝑜 𝑎 + 1 . 0 0 . 5 4 . 0 1 . 0 1 . 5 4 . 0 0 . 0 0 . 0 1 . 0 𝜆 2 = 6 . 0 , 𝜆 3 = 2 . 0 (b)
( 𝐵 > 𝐵 ) 𝜆 2 = 𝜆 3 = 2 . 0

V 0 . 5 2 . 0 0 . 2 5 1 . 5 1 . 0 0 . 2 5 1 . 0 1 . 0 0 . 6 𝜆 2 = 0 . 1 5 , 𝜆 3 = 2 . 3 5 (c)
( 𝐵 > 𝐵 ) 𝜆 2 = 0 . 0 9 5 , 𝜆 3 = 2 . 1

𝑜 𝑎 0 . 5 2 . 0 0 1 . 5 1 . 0 0 2 . 0 2 . 0 0 . 5 𝜆 2 = 1 . 0 , 𝜆 3 = 3 . 0 (d)
( 𝐵 > 𝐵 ) 𝜆 2 = 𝜆 3 = 1 . 0
III 1 . 5 0 . 5 1 . 0 0 . 5 1 . 5 1 . 0 1 . 0 1 . 0 0 . 6 𝜆 2 = 2 . 9 6 , 𝜆 3 = 2 . 1 6 (e)
( 𝐵 = 𝐵 ) 𝜆 2 = 2 . 9 6 , 𝜆 3 = 2 . 1 6

VIII 1 . 0 0 . 5 0 . 4 1 . 0 1 . 5 0 . 4 5 . 0 5 . 0 0 . 5 𝜆 2 = 6 . 1 3 , 𝜆 3 = 3 . 1 3 (f)
( 𝐵 > 𝐵 ) 𝜆 2 = 1 . 5 + 2 . 7 8 𝑖 (complex) 𝜆 3 = 1 . 5 2 . 7 8 𝑖 (complex)

(e) Model parameters for partially stable INC ( 𝐶 𝑑 𝑖 𝑗 𝑘 𝑙 𝛿 𝑘 𝑙 0 , 𝜆 1 = 0 )

𝐶 𝑖 𝑗 𝑘 𝑙 coefficientSpectral propertiesComputation Results in Figure 11

1 . 0 0 . 5 0 0 . 5 5 . 0 0 0 0 1 . 0 𝜆 2 = 3 . 5 , 𝜆 3 = 2 . 0 (a)
𝜆 1 = 3 . 7 7 , 𝜆 2 = 2 . 0 , 𝜆 3 = 0 . 2 7

1 . 0 0 . 5 1 . 0 1 . 0 2 . 0 1 . 0 1 . 0 1 . 0 0 . 7 5 𝜆 2 = 1 . 1 2 5 + 1 . 9 6 𝑖 (complex)(b)
𝜆 3 = 1 . 1 2 5 1 . 9 6 𝑖 (complex)
𝜆 1 = 1 . 5 , 𝜆 2 = 0 . 9 , 𝜆 3 = 0 . 1 5 5