The name is absent



25


ε is small, then the perturbed voltage and gating variables are assumed to be


vb = vb + εvb + C,2)


(2.28)


wbcf = wbcf + εwbcf + O(ε2).


(2.29)


Note here that the rest values vb and wbcf are now spatially-varying. Substituting
(2.28) into (2.17), we construct a linearized model by solving for the perturbation
terms
vb, wbcf of order ε. After substitution we find


Qcf


c=l


∕=ι


I 5b _                       _

- (gbs + εgbs{t)')δ(x - xbs)(yb + εvb - Ebs)


(2.30)


ε¾w6c∕(t) =


wcf,∞(υb + ε⅞) - (wbcf + εwbcf)


τcf (υb + εvb)


(2.31)


The initial conditions are now

vf,(τ,0) = w6c∕(τ,0) = 0

while boundary conditions, because they are already linear, remain the same as in
(2.19), (2.20), (2.24). The soma conditions contain nonlinear terms, but they may be
linearized in the same manner as shown here.



More intriguing information

1. The name is absent
2. DEMAND FOR MEAT AND FISH PRODUCTS IN KOREA
3. Towards a framework for critical citizenship education
4. The name is absent
5. The Challenge of Urban Regeneration in Deprived European Neighbourhoods - a Partnership Approach
6. The Structure Performance Hypothesis and The Efficient Structure Performance Hypothesis-Revisited: The Case of Agribusiness Commodity and Food Products Truck Carriers in the South
7. Towards Learning Affective Body Gesture
8. Innovation in commercialization of pelagic fish: the example of "Srdela Snack" Franchise
9. Regional dynamics in mountain areas and the need for integrated policies
10. Urban Green Space Policies: Performance and Success Conditions in European Cities