From: Changes in the criticality of Hopf bifurcations due to certain model reduction techniques in systems with multiple timescales
Ä’ N a =0.5
Ä’ K =-0.77
Ä’ L =-0.544
ḡ k =0.3
ḡ l =0.0025
k v = 100 mV
ε = 0.0083
Ï„ m = 1
Ï„ n = 1
Ï„ h = 1
a n ( v ) = 0 . 01 ( k v v + 55 ) 1 - e x p - k v v + 55 10
a m ( v ) = 0 . 1 ( k v v + 40 ) 1 - e x p - k v v + 40 10
a h ( v ) =0.07exp ( - k v v - 65 20 )
b n ( v ) =0.125 exp ( - k v v - 65 80 )
b m ( v ) =4 exp ( - k v v - 65 18 )
b h ( v ) = 1 e x p - k v v - 35 10 + 1
n ∞ ( v ) = a n ( v ) a n ( v ) + b n ( v )
m ∞ ( v ) = a m ( v ) a m ( v ) + b m ( v )
h ∞ ( v ) = a h ( v ) a h ( v ) + b h ( v )
t n ( v ) = 1 a n ( v ) + b n ( v )
t m ( v ) = 1 a m ( v ) + b m ( v )
t h ( v ) = 1 a h ( v ) + b h ( v )