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Numerical investigation on global dynamics for nonlinear stochastic heat conduction via global random attractors theory


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Fig. 1

Supports of invariant measure and random attractors for φNGM3 with case I
Supports of invariant measure and random attractors for φNGM3 with case I

Fig. 2

Section of global random basic attractors for φNGM3 with case II
Section of global random basic attractors for φNGM3 with case II

Fig. 3

Section of global random point attractors for φNGM3 with case II
Section of global random point attractors for φNGM3 with case II

Fig. 4

Section of global random attractors for φNGM3 with case II
Section of global random attractors for φNGM3 with case II

Fig. 5

Section of global point/basic attractors for S(τ,τ–t,ω) with case II
Section of global point/basic attractors for S(τ,τ–t,ω) with case II

Fig. 6

Section of global random basic attractors for φNGM3 with case III
Section of global random basic attractors for φNGM3 with case III

Fig. 7

Section of global random point attractors for φNGM3 with case III
Section of global random point attractors for φNGM3 with case III

Fig. 8

Section of boundary of global random attractors for φNGM3 with case III
Section of boundary of global random attractors for φNGM3 with case III

Fig. 9

Section of global random basic attractors for φNGM3 with case IV
Section of global random basic attractors for φNGM3 with case IV

Fig. 10

Section of global random point attractors for φNGM3 with case IV
Section of global random point attractors for φNGM3 with case IV

Fig. 11

Section of boundary of global random attractors for φNGM3 with case IV
Section of boundary of global random attractors for φNGM3 with case IV

The values of α and corresponding Hasudorff dimension

Case ICase IICase IIICase IV
α12.446
Hausdorff dimenison0123

The one to for order eigenvalues for A

λ1λ2λ3λ4
1.02704.10819.243116.4329
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Life Sciences, other, Mathematics, Applied Mathematics, General Mathematics, Physics