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. 2007 Apr 22;4(13):283-304.
doi: 10.1098/rsif.2006.0170.

Mathematical models of the VEGF receptor and its role in cancer therapy

Affiliations

Mathematical models of the VEGF receptor and its role in cancer therapy

Tomás Alarcón et al. J R Soc Interface. .

Abstract

We present an analysis of a stochastic model of the vascular endothelial growth factor (VEGF) receptor. This analysis addresses the contribution of ligand-binding-induced oligomerization, activation of src-homology 2 domain-carrying kinases and receptor internalization in the overall behaviour of the VEGF/VEGF receptor (VEGFR) system. The analysis is based upon a generalization of a Wentzel-Kramers-Brillouin (WKB) approximation of the solution of the corresponding master equation. We predict that tumour-mediated overexpression of VEGFRs in the endothelial cells (ECs) of tumour-engulfed vessels leads to an increased sensitivity of the ECs to low concentrations of VEGF, thus endowing the tumour with increased resistance to anti-angiogenic treatment.

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Figures

Figure 1
Figure 1
Schematic of our receptor-binding model (table 1) including ligand-induced dimerization (receptor activation). The black rectangles represent the cytoplasmic kinase domains of the receptors. The asterisks denote that the dimerized receptors have undergone cross-phosphorylation and hence provide high-affinity docking sites for SH2 domain-carrying kinases. See text for a definition of keffx.
Figure 2
Figure 2
Schematic of our receptor-binding model (table 3). The black rectangles represent the cytoplasmic kinase domains of the receptors. The asterisks denote that the dimerized receptors have undergone cross-phosphorylation and hence provide high-affinity docking sites for SH2 domain-carrying kinases. See text for a definition of keffis, i=1, … , 4.
Figure 3
Figure 3
Simulation results corresponding to Model 3 with konx=4.6×103s1 and koffx=103s1, respectively. This plot shows the time course of the proportion of surface dimers for different values of L. Key: solid line corresponds to L=10 nM, dashed line to L=1 nM, dot-dashed line to L=0.1 nM and dotted line to L=0.01 nM. Ligand is introduced at t=0.
Figure 4
Figure 4
(a) Simulation results corresponding to Model 3 with konx=4.6×103s1 and koffx=103s1. The squares in this plot show the maximum value achieved by the proportion of surface dimers (figure 3) as a function of ligand concentration. Solid line corresponds to a Hill curve X=XmaxLn/(Kn+Ln) with n=1.2. (b) Experimental results by Park et al. (2003). Solid line corresponds to a Hill curve X=XmaxLn/(Kn+Ln) with n=1.5. In both panels, dashed lines correspond to a Hill curve with n=1, which has been included for comparison. Ligand is introduced at t=0.
Figure 5
Figure 5
Simulation results corresponding to Model 3. These plots show the time course of the proportion of surface dimers bound to SH2 domains (x1, x2, x3 and x4) for L=10−8 M.
Figure 6
Figure 6
Simulation results corresponding to Model 3. (a) corresponds to results showing the proportion of surface dimers (upper plot) and the proportion of bound SH2 domains (lower plot) without anti-VEGF treatment for L=10 nM. (b) Results from a simulation in which anti-VEGF therapy was implemented by reducing the level of VEGF from L=10 nM to L=0.01 nM at time t=10−2. (c): idem at t=10−3. Parameter values have been taken from table 2.
Figure 7
Figure 7
x* as a function of the dimensionless quantity AL for different values of the dimensionless quantity konx. Parameter values have been taken from table 2. Squares, konx=4.6×103s1; triangles, konx=4.6×102s1; and circles, konx=4.6×101s1.
Figure 8
Figure 8
Numerical solution for the first cumulant equations corresponding to Model 2 (table 3). (a) corresponds to log(AL)=−6, panel (b) to log(AL)=1 and (c) to log(AL)=6. Parameter values have been taken from table 2.
Figure 9
Figure 9
Simulation results corresponding to Model 2. (a) corresponds to results showing the proportion of surface dimers (upper plot) and the proportion of bound SH2 domains (lower plot) without anti-VEGF treatment for L=10 nM. (b) Results from a simulation in which anti-VEGF therapy was implemented by reducing the level of VEGF from L=10 to 0.01 nM at time t=10−3. (c): idem at t=104. Parameter values have been taken from table 2.
Figure 10
Figure 10
Simulation results corresponding to Model 2 where the effect of combining anti-VEGF therapy and reduction of konx is demonstrated. Both therapies have been applied at t=104. VEGF concentration has been reduced from L=10 to 0.01 nM. The dimerization rate has been reduced from konx=4.6×103s1 to konx=4.6×101s1. The rest of the parameter values have been taken from table 2.
Figure 11
Figure 11
Simulation results for Model 4 (equations (5.1)–(5.15)) for a physiological situation. This plot shows the proportion of receptors. Dashed line corresponds to L=10−8 M, solid line to L=10−9 M, dot-dashed line to L=10−10 M and dotted line to L=10−11 M. Parameter values have been taken from table 2.
Figure 12
Figure 12
Simulation results for Model 4 (equations (5.1)–(5.15)) for a physiological situation. This plot shows the number of SH2 domains bound to receptor dimers on the surface of the cell. Solid line corresponds to L=10−8 M, dashed line to L=10−9 M, dot-dashed line to L=10−10 M and dotted line to L=10−18 M. Parameter values have been taken from table 2.
Figure 13
Figure 13
Simulation results for Model 4 (equations (5.1)–(5.15)). This plot shows the proportion of SH2 domains bound to surface receptors dimers. Solid line corresponds to L=10−8 M, dashed line to L=10−9 M, dot-dashed line to L=10−10 M and dotted line L=10−18 M. (a) corresponds to ks=4.5×10−4 and (b) to ks=9×10−4. Other parameter values have been taken from table 2.
Figure 14
Figure 14
Simulation results of the effect of anti-VEGF therapy on Model 4 (equations (5.1)–(5.15)) in a physiological situation. The levels of VEGF have been reduced from L=10 to 0.01 nM. (a) corresponds to drug administration at t=10−4 and (b) to administration time t=10−2. Parameter values have been taken from table 2.
Figure 15
Figure 15
Simulation results of the effect of anti-VEGF therapy on Model 4 (equations (5.1)–(5.15)) in a pathological situation. The value of the rate of receptor synthesis has been increased to ks=4.5×10−4, i.e. fivefold its physiological value. The levels of VEGF have been reduced from L=10 to 0.01 nM. (a) corresponds to an untreated case and (b) to drug administration at t=10−4. Other parameter values have been taken from table 2.
Figure 16
Figure 16
Simulation results of the effect of anti-VEGF therapy on Model 4 (equations (5.1)–(5.15)) in a physiological situation. The levels of VEGF have been reduced from L=10 to 0.01 nM. (a) corresponds to drug administration at t=104 and (b) to a close-up of (a). Parameter values have been taken from table 2.
Figure 17
Figure 17
Variance of x for Model 1 (table 1) calculated at the steady state shown on a logarithmic scale. Circles correspond to konx=4.6×102s1 and triangles to konx=4.6×102s1. Parameter values have been taken from table 2.
Figure 18
Figure 18
(a) Simulation results corresponding to Models 3 and 4 (with ks=9×10−5 s−1). The squares (Model 3) and triangles (Model 4) in this plot show the maximum values achieved by the proportion of surface dimers (figure 3) as a function of ligand concentration when the models were simulated until t=1.2, i.e. 20 min in dimensional terms. (b) Experimental results by Cai et al. (2006).

References

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