The name is absent

129

h-current kinetics

n_h = 1 - ((1 - m_hy + 4m_h(l - m⅛)³)
m_h = a_h(l - m_h) - β_hm_h

ан - 18/(1 + exp((v + 88)/12))

βh = 18/(1 + exp(-(v + 18)/19))

Probability of ≥ 2 of 4 particles being open

Probability of one particle being open

kx-current kinetics

∏^kx ~ ɑfeæ(l ^ʃɪfeʃ) βkx^kx
a_kx = 0.66exp ((υ + 50)/(2 ■ 5.7))
∕3_fcτ = 0.66 exp (-(υ + 50)/(2 ■ 5.7))

Two-state noninactivating kinetics

kv-current kinetics

τ⅛_υ = r∏l,_υhk_v Gating with 3 activation and 1 inactivation particles

τri_kυ = a_mkv ( 1 - m_mkυ ) - β_mkυm_mkυ Activation particle

a_mkv = 5(100 - 77)∕exp((lOO - t>)∕42) - 1)

βmkυ = 9exp(-(z? - 20)/40)

hkυ ~ ɑftfet)(l h_kυ) βhkvh_kv

Inactivation particle

a_hkv = 0.15exp(-w∕22)

β_hkυ = 0.4125/exp(-(t> - 10)/7 + 1)