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Articles

Combination of singularly perturbed vector field method and method of directly defining the inverse mapping applied to complex ODE system prostate cancer model

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Pages 961-986 | Received 06 Jun 2018, Accepted 22 Oct 2018, Published online: 01 Nov 2018

Figures & data

Table 1. Parameters used in the model (Equation4)–(Equation9).

Table 2. Parameters used in the model (Equation4)–(Equation9).

Figure 1. The solution profiles of N1(t), the androgen-dependent cancer cells. 1: MDDIM, 2: QSS, Quasi-steady state approximation, 3: numerical simulations for the full model. These cancer cells grow at the beginning of the treatment, then after they decrease very quickly.

Figure 1. The solution profiles of N1(t), the androgen-dependent cancer cells. 1: MDDIM, 2: QSS, Quasi-steady state approximation, 3: numerical simulations for the full model. These cancer cells grow at the beginning of the treatment, then after they decrease very quickly.

Figure 2. The solution profiles of N2(t), the androgen-independent cancer cells. 1: MDDIM, 2: QSS, quasi-steady state approximation, 3: numerical simulations for the full model. These cells decrease rapidly with the onset of immunotherapy.

Figure 2. The solution profiles of N2(t), the androgen-independent cancer cells. 1: MDDIM, 2: QSS, quasi-steady state approximation, 3: numerical simulations for the full model. These cells decrease rapidly with the onset of immunotherapy.

Figure 3. The solutions profiles of the T cells. 1: MDDIM, 2: QSS, quasi-steady state approximation, 3: numerical simulations for the full model. At first treatment, there is a very sharp increase in these cells and then drop to equilibrium point.

Figure 3. The solutions profiles of the T cells. 1: MDDIM, 2: QSS, quasi-steady state approximation, 3: numerical simulations for the full model. At first treatment, there is a very sharp increase in these cells and then drop to equilibrium point.

Figure 4. The solution profiles of IL(t), the concentration of cytokine. 1: MDDIM, 2: QSS, quasi-steady state approximation, 3: numerical simulations for the full model. During the treatment, the concentration of cytokines increases due to the intense activity of the immune system.

Figure 4. The solution profiles of IL(t), the concentration of cytokine. 1: MDDIM, 2: QSS, quasi-steady state approximation, 3: numerical simulations for the full model. During the treatment, the concentration of cytokines increases due to the intense activity of the immune system.

Figure 5. The solution profiles of A(t), the concentration of androgen. 1: MDDIM, 2: QSS, quasi-steady state approximation, 3: numerical simulations for the full model. The androgens corresponding to the dendritic cells stabilize after ≈60 days, to their equilibrium point.

Figure 5. The solution profiles of A(t), the concentration of androgen. 1: MDDIM, 2: QSS, quasi-steady state approximation, 3: numerical simulations for the full model. The androgens corresponding to the dendritic cells stabilize after ≈60 days, to their equilibrium point.

Figure 6. The solution profiles of D, the number of dendritic cells. 1: MDDIM, 2: QSS, quasi-steady state approximation, 3: numerical simulations for the full model. The number of dendritic cells stabilizes after 56 days.

Figure 6. The solution profiles of D, the number of dendritic cells. 1: MDDIM, 2: QSS, quasi-steady state approximation, 3: numerical simulations for the full model. The number of dendritic cells stabilizes after ≈56 days.

Figure 7. The solution profiles of N~1, the new variable in the new coordinates. 1: MDDIM, 2: QSS, quasi-steady state approximation, 3: numerical simulations for the full model in the new coordinates, 4: combination of MDDIM and SPVF, 5: SPVF method.

Figure 7. The solution profiles of N~1, the new variable in the new coordinates. 1: MDDIM, 2: QSS, quasi-steady state approximation, 3: numerical simulations for the full model in the new coordinates, 4: combination of MDDIM and SPVF, 5: SPVF method.

Figure 8. The solution profiles of N~2, the new variable in the new coordinates. 1: MDDIM, 2: QSS, quasi-steady state approximation, 3: numerical simulations for the full model in the new coordinates, 4: combination of MDDIM and SPVF, 5: SPVF method.

Figure 8. The solution profiles of N~2, the new variable in the new coordinates. 1: MDDIM, 2: QSS, quasi-steady state approximation, 3: numerical simulations for the full model in the new coordinates, 4: combination of MDDIM and SPVF, 5: SPVF method.

Figure 9. The solution profiles of T~, the new variable in the new coordinates. 1: MDDIM, 2: QSS, quasi-steady state approximation, 3: numerical simulations for the full model in the new coordinates, 4: combination of MDDIM and SPVF, 5: SPVF method.

Figure 9. The solution profiles of T~, the new variable in the new coordinates. 1: MDDIM, 2: QSS, quasi-steady state approximation, 3: numerical simulations for the full model in the new coordinates, 4: combination of MDDIM and SPVF, 5: SPVF method.

Figure 10. The solution profiles of I~L, the new variable in the new coordinates. 1: MDDIM, 2: QSS, quasi-steady state approximation, 3: numerical simulations for the full model in the new coordinates, 4: combination of MDDIM and SPVF, 5: SPVF method.

Figure 10. The solution profiles of I~L, the new variable in the new coordinates. 1: MDDIM, 2: QSS, quasi-steady state approximation, 3: numerical simulations for the full model in the new coordinates, 4: combination of MDDIM and SPVF, 5: SPVF method.

Figure 11. The solution profiles of A~, the new variable in the new coordinates. 1: MDDIM, 2: QSS, quasi-steady state approximation, 3: numerical simulations for the full model in the new coordinates, 4: combination of MDDIM and SPVF, 5: SPVF method. Since we transfer the model using eigenvectors, we obtain a negative value of A~ which is biologically insignificant. And hence, for sake of biological understanding, we must ignore these negative values.

Figure 11. The solution profiles of A~, the new variable in the new coordinates. 1: MDDIM, 2: QSS, quasi-steady state approximation, 3: numerical simulations for the full model in the new coordinates, 4: combination of MDDIM and SPVF, 5: SPVF method. Since we transfer the model using eigenvectors, we obtain a negative value of A~ which is biologically insignificant. And hence, for sake of biological understanding, we must ignore these negative values.

Figure 12. The solution profiles of D~, the new variable in the new coordinates. 1: MDDIM, 2: QSS, quasi-steady state approximation, 3: numerical simulations for the full model in the new coordinates, 4: combination of MDDIM and SPVF, 5: SPVF method.

Figure 12. The solution profiles of D~, the new variable in the new coordinates. 1: MDDIM, 2: QSS, quasi-steady state approximation, 3: numerical simulations for the full model in the new coordinates, 4: combination of MDDIM and SPVF, 5: SPVF method.

Figure 13. PSA serum level, with an injection rate of 0.078 billion cells for various values of e1, the maximum rate T cells kill cancer cells. A wider range of e1 is able to suppress the growth of cancer and elongate the cycles of IAD.

Figure 13. PSA serum level, with an injection rate of 0.078 billion cells for various values of e1, the maximum rate T cells kill cancer cells. A wider range of e1 is able to suppress the growth of cancer and elongate the cycles of IAD.