The name is absent



114

Now we discretize the neuron in space, which yields Ns and Nw compartments in
the strong and weak parts, respectively, as well as the transition compartment, for
a total of
N = Ns + Nw + 1 compartments. This implies that the strong and weak
voltage vectors are

vs∈Rjvs, v,λ, ∈ R∕v,".

To construct the coupled “Hines” matrix properly we will need the local indices
of the compartments adjacent to the transition compartment. These local indices are
denoted by
Nw and Np for the adjacent strong and weak compartments, respectively.
Using these local indices, the voltage of the adjacent weak compartment is denoted
by v^w, and the voltage of the adjacent strong compartment is denoted by vfr. The
voltage of the transition compartment is denoted as before as vʃ.

Discretizing (4.19) yields
where
Nx is the compartment length for branch bp- Using the continuity of potential
condition of (4.18) we solve for
vτ:

v^τ — vτ
Nx


vτ~vww'
Nx


vτ = V⅛∙ + ⅛^4
τ 2 s 2 w

Now we are ready to apply the generalized cable equation’s second-derivative oper-
ator. We can use our previously derived results (see Appendix A) for all compartments



More intriguing information

1. Peer Reviewed, Open Access, Free
2. Heavy Hero or Digital Dummy: multimodal player-avatar relations in FINAL FANTASY 7
3. Can we design a market for competitive health insurance? CHERE Discussion Paper No 53
4. Industrial Cores and Peripheries in Brazil
5. Dual Track Reforms: With and Without Losers
6. Target Acquisition in Multiscale Electronic Worlds
7. Life is an Adventure! An agent-based reconciliation of narrative and scientific worldviews
8. Outline of a new approach to the nature of mind
9. Multimedia as a Cognitive Tool
10. New urban settlements in Belarus: some trends and changes