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. 2022 Dec 13;14(24):6143. doi: 10.3390/cancers14246143

Table A5.

A report of different experiments using uniform initial condition and no-flux boundary condition.

Source Location, Max Magnitude C at t=200, (Relative Difference in C) V, (Relative Difference in Relevant Xi), and Others
Gaussian for M, (case Section 3.4) In the middle, 0.1 Profile I, (20%) V=6.70V0, (300%)
Gaussian for C In the middle, 0.1 - Nonlinear solver collapsed at t=7.5
Gaussian for C In the middle, 0.01 - Nonlinear solver collapsed at t=27.5
Gaussian for Tc, (case Section 3.5) In the middle, 10 C[1.1,1.4], profile II V=4.87V0, (20%), profile I
Gaussian for Mn In the middle, 4 - Nonlinear solver collapsed at t=70
Step function for Tc On the boundary, 1 Profile I, (<5%) V=5.29V0, Tc[1.3,1.4], more on the boundary
Step function for Tc, (case Section 3.6) On the boundary, 4 Profile I, (10%) V=4.75V0, Tc[1.3,1.7], more on the boundary
Step function for Th On the boundary, 1 C=1.573, (<1%) V=5.57V0, Th is more on the boundary, (8%)
Step function for M On the boundary, 1 C[0.88,1.1], profile II V=34.4V0, M[5.5,25], more on the boundary
Step function for M,       (case Section 3.7) On the boundary, 0.1 C[0.23,0.27], profile II V=8.88V0, M[1.3,3.3], more on the boundary