105
must also be adjusted to be with respect to rest, and including the resting ionic term
Φ = (Φ(ws)e).vs(f) - Φ(ws)Ei
(4.11)
achieves this goal.
Also note that the transition compartment is not explicitly represented in (4.9).
Rather, in order to obtain vʃ, equation (4.8) must be used. One implication of this
compartment being left out is that any inputs which would arrive here are ignored.
To remedy this, the present solution is to shift the input into one of the adjacent
compartments.
Defining the matrices
we write the coupled strong-weak “Hines” matrix as
Q Zs 0
Zω Hs
0
(4.12)
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