The name is absent



143

Table B.l: Uniform channel model and kinetics, which corresponds to the Hodgkin-Huxley
squid giant axon parameters at 6.3oC (Hodgkin and Huxley, 1952).

Ionic Current Gating Variables G(x) (mS∕cm2) E (mV)

Leak                                   0.3

INa                m3, h             120

Iκ                  ni               36

-54.3

56
-77

Gating Var.

a

_______β_______

T

Woo

0.1(v+40)

4exp(- + 65)/18)

1

a

772

1—exp(-0.1(v÷40))

a+β

a+β

h

0.07exp(- ÷ 65)/20)

____________ι____________

1

a

l+exp(0.1(~ 35—υ))

a+β

a+β

0.01(τι+55)

∣exp(-(u + 65)/80)

1

a

TL

1—exp(-0.1(-υ+55))

α+∕3

a+β

Table B.2: Non-uniform channel model and kinetics, Lv ɑ. and ⅛ use Hodgkin-Huxley
type kinetics, while
Ia uses Connor-Stevens type kinetics and a spatial distribution of
conductance based on Hoffman’s work. For G(rr),
x is measured in pm from the soma.
Note that the
Ia channel kinetics do not have a and β functions explicitly defined (Connor
and Stevens, 1971) (Hoffman et al., 1997).

Ionic Current

Gating Variables

G{x) (mS∕cm2)

E (mV)

Leak

0.3

-47

Ino.

m3, h

60

55

Ik

ni

20

-72

Ia____________

α3, b

yy(0.2 + 0.002τ)

-75

Gating Var.

a                       β              τ woo

m
h

10r⅛299Λbiω     15.2exp(-0.0556(v + 54.7)) ɪ ɪ

1—exp(-(t∕÷29.7)/10)                               ∖ 1       √/ α+p α+∕3

0.266exp(-0.05(v + 48))      ⅛¾4⅛7i°>      ⅛ ⅛

n

!-.,“pÎXS/.o)     0.25exp(-0.0125(v + 55.7)) ⅛ ⅛

Gating Var.

W00

∩ 3632 __1158_______

U.OOO^ 1- 1+exp(0.0497(t)+55.96))

1 24 3__2678_______

1.^⅛-Γ ι+p(0.0624(v+50))

0.0761exp(0.0314(t>+94.22)) λ ^3
l+exp(0.0346(v+1.17)) )
/                         ∖ 4

/ 1 ʌ

l+exp(0.0688(v+53.3))



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