1. Volume 84, Issue 1, Pages 42-56 (January 2003)
On the Role of Stochastic Channel Behavior in Intracellular Ca2+ Dynamics 
Martin Falcke 
Biophysical Journal 
Volume 84, Issue 1, Pages (January 2003)
DOI: /S (03)
Copyright © 2003 The Biophysical Society Terms and Conditions

2. Figure 1
Lumped states Xjk of a subunit of the IP3 receptor channel. An index is 1 if an ion is bound and 0 if not. The index j stands for the activating Ca2+ site and k for the inhibiting Ca2+ site. The transition rates are given at the edges of the rectangle.
Biophysical Journal  , 42-56DOI: ( /S (03) )
Copyright © 2003 The Biophysical Society Terms and Conditions

3. Figure 2
Concentration of fast buffer with high affinity as solution of the fully coupled Eqs. 8 and 9. Bex=800⁡μM, IP3=0.66⁡μM, Bs=200⁡μM, Bm=0, BEs=200⁡μM, KEs=5⁡μM, BEm=0, Co=72⁡μM, [IP3]=0.24⁡μM,P=800⁡s−1, Pl=0.001⁡s−1, Pp=50⁡μM⁡s−1, d=3.84⁡μm, Rs=84⁡nm. The integration area is 30.72×30.72⁡μm2 and contains 8×8 clusters and a focal site with NF=10 on a 1.6d×1.6d area.
Biophysical Journal  , 42-56DOI: ( /S (03) )
Copyright © 2003 The Biophysical Society Terms and Conditions

4. Figure 3
Global number of open channels No in a simulation solving the fully coupled Eq. 8 and 9 for the concentrations. [IP3] was kept at 0.06μM until t=10⁡s and then set to 0.24μM. Bex=450⁡μM, Bslow=20⁡μM, Bs=200⁡μM, Bm=0, BEs=200⁡μM, KEs=5⁡μM, BEm=0, Co=72⁡μM, Pc=800⁡s−1, Pc=0.001⁡s−1, Pp=50⁡μMs−1, d=3.84⁡μm, Rs=84⁡nm. The integration area is 30.72×30.72⁡μm2 and contains 8×8 clusters.
Biophysical Journal  , 42-56DOI: ( /S (03) )
Copyright © 2003 The Biophysical Society Terms and Conditions

5. Figure 4
Characteristics of single cluster profiles of free Ca2+. (A) Free Ca2+ dependent on the distance from the cluster center for a cluster with 10 open channels. (B) Concentration increase of free Ca2+ relative to the base level cb at a distance of 4.32μm, used in some simulations as cluster spacing d, dependent on the number of open channels in a cluster. (C) Concentration increase of free Ca2+ relative to the base level cb at the center of the cluster. (D) Ratio of the contribution of the open channels Δc=c−cb (cb base level) at r=0 to the contribution at r=d=4.32⁡μm. Circles refer to calculations with Bex=40⁡μM and crosses to Bex=0.
Biophysical Journal  , 42-56DOI: ( /S (03) )
Copyright © 2003 The Biophysical Society Terms and Conditions

6. Figure 5
Array of clusters used in simulations. The area is quadratic with edge length L=120⁡μm. Clusters form a hexagonal grid with distance d. NF additional clusters are scattered randomly around the points (L/4, L/4), (L/4, 3L/4), (3L/4, L/4), (3L/4, 3L/4) within a square with edge length 2.42 d mimicking a focal site; here NF=5.
Biophysical Journal  , 42-56DOI: ( /S (03) )
Copyright © 2003 The Biophysical Society Terms and Conditions

7. Figure 6
Simulations and oscillation characteristics for different IP3 concentrations: (A) I=0.15⁡μM, (B) I=0.18⁡μM, (C) I=0.42⁡μM, (D) Tav and its standard deviation dependent on [IP3].
Biophysical Journal  , 42-56DOI: ( /S (03) )
Copyright © 2003 The Biophysical Society Terms and Conditions

8. Figure 7
The number of open channels (A) and the number of excitable channels (at least three subunits in X00) (B) during repetitive nucleation of waves. (A) is a blow up of panel B in Fig. 10. The transition from X01→X00 was sped up by a factor of 2.5 compared to the standard parameters of Table 1. See Table 1 for parameters except Bex=70⁡μM and NF=10.
Biophysical Journal  , 42-56DOI: ( /S (03) )
Copyright © 2003 The Biophysical Society Terms and Conditions

9. Figure 8
Nucleation of a wave in a regime with long wave periods. (A) shows the number of open channels in the area where the wave nucleates. The nucleation area is bound by a black rectangle in panel (C) frame t=370.9⁡s and comprises several clusters. (B) shows the global number of open channels. (C) shows six snapshots of the simulation area taken at the times indicated. Shown is Ca2+ bound to exogenous buffer. The color scaling is a minimum–maximum scaling with blue indicating minimal values and red maximal ones.
Biophysical Journal  , 42-56DOI: ( /S (03) )
Copyright © 2003 The Biophysical Society Terms and Conditions

10. Figure 9
The number of excitable channels NE (at least three subunits in X00) (A). The number of open channels in an area of the same size like that marked in panel C of Fig. 8 (B). The number of open channels in the same area as in B plus the eight neighboring areas of same size (C). See Table 1 for parameters except Bex=60⁡μM and I=0.18⁡μM, d=5.18⁡μm.
Biophysical Journal  , 42-56DOI: ( /S (03) )
Copyright © 2003 The Biophysical Society Terms and Conditions

11. Figure 10
Repetitive wave nucleation for three concentrations of exogenous buffer: (A) Bex=60⁡μM, (B) Bex=70⁡μM, (C) Bex=75⁡μM. The number of open channels is shown. The average period is in (A) Tav=47.40±10.00⁡s, (B) Tav=64.55±23.45⁡s and in (C) Tav=121.17⁡±⁡57.23⁡s. The transition from X01→X00 was sped up by a factor of 2.5 compared to the standard parameters of Table 1. See Table 1 for further parameters except NF=10.
Biophysical Journal  , 42-56DOI: ( /S (03) )
Copyright © 2003 The Biophysical Society Terms and Conditions

12. Figure 11
Repetitive wave nucleation for different cluster spacing (A) d=1.594⁡μM, I=0.18⁡μM, (B) d=4.800⁡μm, I=0.18⁡μM, (C) d=6.377⁡μm, I=0.21⁡μM. The number of open channels NO is shown. The small peaks in panel (C) are abortive waves. I included an abortive wave into the statistics as a global event, if it traveled across an area larger than 65μm in diameter. That is the size of the area of observation used by Marchant and Parker (2001). (D) shows the period Tav and its standard deviation dependent on the cluster spacing. See Table 1 for further parameters except NF=10, I=0.18⁡μM (circles), NF=5, I=0.195⁡μM (diamonds), and NF=5, I=0.21⁡μM (x).
Biophysical Journal  , 42-56DOI: ( /S (03) )
Copyright © 2003 The Biophysical Society Terms and Conditions

13. Figure 12
Average periods Tav for different numbers of additional clusters in focal sites.
Biophysical Journal  , 42-56DOI: ( /S (03) )
Copyright © 2003 The Biophysical Society Terms and Conditions

14. Figure 13
Simulations using different random realizations of cluster grids with identical average spatial characteristics. (A) Tav=177±135⁡s, (B) Tav=112±24⁡s, (C) Tav=103±29⁡s. See Table 1 for further parameters.
Biophysical Journal  , 42-56DOI: ( /S (03) )
Copyright © 2003 The Biophysical Society Terms and Conditions

15. Figure 14
Simulations using a variety of parameter sets for the local dynamics. Parameters different from those in Table 1 are (top left) Bex=60⁡μM, I=0.18⁡μM, d5=0.83⁡s−1 (increased deactivation), (top right) Tav for different inhibition rate constants a2 (note a2=a4) Bex=60⁡μM, I=0.18⁡μM, (bottom left) Bex=60⁡μM, I=0.42⁡μM, NKmax=13, d=4.6⁡μm, (bottom right) Bex=60⁡μM, I=0.15⁡μM, NF=7.
Biophysical Journal  , 42-56DOI: ( /S (03) )
Copyright © 2003 The Biophysical Society Terms and Conditions

16. Figure 15
Simulations with different NKmax. The single channel radius was chosen proportional to 1/NKmax. (Left) Simulation with NKmax=328; (right) Tav dependent on NKmax⋅Bex=60⁡μM, I=0.15⁡μM. See Table 1 for further parameters.
Biophysical Journal  , 42-56DOI: ( /S (03) )
Copyright © 2003 The Biophysical Society Terms and Conditions

17. Figure 16
Simulations with NKmax=1130, I=0.15⁡μM, and NF=5. The single channel radius was chosen proportional to 1/NKmax as explained in the text. (A) shows the case corresponding to Fig. 6 A (thick line) and with recovery from inhibition sped up by a factor of 2.5 (thin line). (B) shows NO (thick line) and NE (thin line). The simulation is that of panel A (thick line) but perturbed at t=75⁡s. Despite the fact that I increased the number of open channels artificially with the perturbation the consequence is a decrease of NO to almost zero followed by a spike and again stationary behavior.
Biophysical Journal  , 42-56DOI: ( /S (03) )
Copyright © 2003 The Biophysical Society Terms and Conditions

18. Figure 17
Simulations with NKmax=546, I=0.42⁡μM in panel A and NKmax=685, I=0.27⁡μM in panel B, both NF=5. The single channel radius was chosen proportional to 1/NKmax as explained in the text. (A) shows the case corresponding to Fig. 6 C. The system reaches a high activity stationary state for large times.
Biophysical Journal  , 42-56DOI: ( /S (03) )
Copyright © 2003 The Biophysical Society Terms and Conditions

19. Figure 18
Comparison of the experimental data of Fig. 2 in Marchant and Parker (2001) with simulations. Shown is the relative standard deviation of ΔTav/Tav versus Tav.
Biophysical Journal  , 42-56DOI: ( /S (03) )
Copyright © 2003 The Biophysical Society Terms and Conditions

20. Figure 19
Phase space structure which could be imagined as underlying the observed behavior of the stochastic system. Stable stationary point (filled dots); saddle point (shaded dots); outgoing separatrices (thin solid lines) ingoing separatrices (dashed lines); trajectories (thick solid lines) (A) low [IP3], (B) high [IP3].
Biophysical Journal  , 42-56DOI: ( /S (03) )
Copyright © 2003 The Biophysical Society Terms and Conditions