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. 2006 Aug 22;3(9):545-59.
doi: 10.1098/rsif.2006.0116.

Stochastic models of receptor oligomerization by bivalent ligand

Affiliations

Stochastic models of receptor oligomerization by bivalent ligand

Tomás Alarcón et al. J R Soc Interface. .

Abstract

In this paper, we develop stochastic models of receptor binding by a bivalent ligand. A detailed kinetic study allows us to analyse the role of cross-linking in cell activation by receptor oligomerization. We show how oligomer formation could act to buffer intracellular signalling against stochastic fluctuations. In addition, we put forward the hypothesis that formation of long linear oligomers increases the range of ligand concentration to which the cell is responsive, whereas formation of closed oligomers increases ligand concentration specificity. Thus, different physiological functions requiring different degrees of specificity to ligand concentration would favour formation of oligomers with different lengths and geometries. Furthermore, provided that ligand concentration specificity is taken as a design principle, our model enables us to estimate parameters, such as the minimum proportion of receptors, that must engage in oligomer formation in order to trigger a cellular response.

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Figures

Figure 1
Figure 1
Schematic of the cross-linking model with (a) dimer formation, (b) trimer formation and (c) ring formation. The physical meaning of the parameter Δ is illustrated in (d). B, X, X1 and Y are the number of oligomers of type (1), (2), (3) and (4), as shown in panel (e), respectively. In panels (d) and (e), red colour indicates diffusible ligand, whereas black colour denotes membrane-bound receptor.
Figure 2
Figure 2
Simulation results from a single realization for (a) N=10 000, (b) N=1000, (c) N=100, (d) N=50. Black lines correspond to x, red lines to b, and green lines to u. L=107 mol l−1. See appendix A for details of the simulation procedure.
Figure 3
Figure 3
Probability density corresponding to Model 1. (a) N=1000, average over 300 realizations. (b) N=100, average over 700 realizations. (c) N=50, average over 700 realizations. L=107 mol l−1. See appendix A for details of the simulation procedure.
Figure 4
Figure 4
Simulation results for Model 1 showing (a) Qb(T) and (b) Qx(T) for T=10koff1 as a function of the dimensionless quantity AL, where A is the affinity and L the ligand concentration. Blue lines correspond to N=108 and Θ/N=0.45, red lines to N=1080 and Θ/N=0.045 and black lines to N=10 800 and Θ/N=0.0045. In each case, we have averaged over 100 realizations.
Figure 5
Figure 5
Simulation results for Model 1 showing Qx(T) for T=10koff1 as a function of the dimensionless quantity AL, where A is the affinity and L the ligand concentration. Black lines correspond to N=10 800, red lines to N=1080 and blue lines to N=108. Θ/N=0.45. In each case, we have averaged over 100 realizations.
Figure 6
Figure 6
Simulation results from a single realization corresponding to Model 2. We have taken (a) N=1080, (b) N=540, (c) N=108, (d) N=54. Black lines correspond to x, orange lines to x1, red lines to b, green lines to u and blue lines to y. L=107 mol l−1. See appendix A for details of the simulation procedure.
Figure 7
Figure 7
Probability densities for Model 2 for N=54, 108 and 1080. In all of the different cases, we have averaged over realizations. L=10−7 mol l−1. See appendix A for details of the simulation procedure.
Figure 8
Figure 8
Simulation results for Model 2 showing (a) Qb(T) and (b) Qx(T) for T=10koff1 as a function of the dimensionless quantity AL, where A is the affinity and L the ligand concentration. Black lines correspond to N=10 800 and Θ/N=0.0045, red lines to N=1080 and Θ/N=0.045 and blue lines to N=108 and Θ/N=0.45. In each case, we have averaged over 100 realizations.
Figure 9
Figure 9
Simulation results for Model 2 showing Qx(T) for T=10koff1 as a function of the dimensionless quantity AL, where A is the affinity and L the ligand concentration. These results correspond to varying the threshold value of BCRs engaged in cross-linking necessary for building-up a signal. Black corresponds to N=10 800, red to N=1080 and blue to N=108. Θ/N=0.45. In each case, we have averaged over 100 realizations.
Figure 10
Figure 10
Simulation results from a single realization corresponding to Model 3. We have taken (a) N=1080, (b) N=540, (c) N=108, (d) N=54. Black lines correspond to x, red lines to b, green lines to u, blue lines to y and brown lines to r. L=107 mol l−1. See appendix A for details of the simulation procedure.
Figure 11
Figure 11
Simulation results from a single realization corresponding to Model 3. We have taken N=1080. Panel (a) corresponds to L=1013 mol l−1, panel (b) to L=107 mol l−1 and panel (c) to L=101 mol l−1. Black lines correspond to x, red lines to b, green lines to u, blue lines to y and brown lines to r. L=107 mol l−1. See appendix A for details of the simulation procedure.
Figure 12
Figure 12
Simulation results for Model 1 showing (a) Qb(T) and (b) Qx(T) for T=10koff1 as a function of the dimensionless quantity AL, where A is the affinity and L the ligand concentration. Black lines correspond to N=10 800 and Θ/N=0.0045, red lines to N=1080 and Θ/N=0.045 and blue lines to N=108 and Θ/N=0.45. In each case, we have averaged over 100 realizations.
Figure 13
Figure 13
Simulation results for Model 3 showing Qx(T) for T=10koff1 as a function of the dimensionless quantity AL, where A is the affinity and L the ligand concentration. These results correspond to varying the threshold value of BCRs engaged in cross-linking necessary for building-up a signal. Black corresponds to N=10 800, red to N=1080 and blue to N=108. Θ/N=0.45. In each case, we have averaged over 100 realizations.
Figure 14
Figure 14
Simulation results showing Qx(T) for T=10koff1 as a function of the dimensionless quantity AL, where A is the affinity and L the ligand concentration. These results correspond to varying the threshold value of BCRs engaged in cross-linking necessary for building-up a signal. Blue to Θ/N=0.22 and maroon to Θ/N=0.45 In each case, we have averaged over 100 realizations.
Figure 15
Figure 15
Sensitivity analysis for Ax. Simulation results are shown for Qx(T) the model with trimer formation showing with T=10koff1 as a function of the quantity Ax. Θ/N=0.22 and AL=103 (green line), AL=1 (blackline), AL=104 (blue line) and AL=105 (red line). Circles correspond to results for Model 2 (a), squares to Model 3 (b). We have averaged over 100 realizations.
Figure 16
Figure 16
Flow chart for the ESSA proposed by Gillespie (1977). See text for details.

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