INa_HH1952v2#
- class brainpy.dyn.INa_HH1952v2(size, keep_size=False, g_max=120.0, phi=1.0, V_sh=-45.0, method='exp_auto', name=None, mode=None)[source]#
The sodium current model described by Hodgkin–Huxley model [1].
The dynamics of this sodium current model is given by:
\[\begin{split}\begin{split} \begin{aligned} I_{\mathrm{Na}} &= g_{\mathrm{max}} m^3 h \\ \frac {dm} {dt} &= \phi (\alpha_m (1-x) - \beta_m) \\ &\alpha_m(V) = \frac {0.1(V-V_{sh}-5)}{1-\exp(\frac{-(V -V_{sh} -5)} {10})} \\ &\beta_m(V) = 4.0 \exp(\frac{-(V -V_{sh}+ 20)} {18}) \\ \frac {dh} {dt} &= \phi (\alpha_h (1-x) - \beta_h) \\ &\alpha_h(V) = 0.07 \exp(\frac{-(V-V_{sh}+20)}{20}) \\ &\beta_h(V) = \frac 1 {1 + \exp(\frac{-(V -V_{sh}-10)} {10})} \\ \end{aligned} \end{split}\end{split}\]where \(V_{sh}\) is the membrane shift (default -45 mV), and \(\phi\) is the temperature-dependent factor (default 1.).
- Parameters:
size (
TypeVar(Shape,int,Tuple[int,...])) – The size of the simulation target.keep_size (
bool) – Keep size or flatten the size?method (
str) – The numerical methodname (
str) – The name of the object.g_max (
Union[int,float,TypeVar(ArrayType,Array,Variable,TrainVar,Array,ndarray),Initializer,Callable]) – The maximal conductance density (\(mS/cm^2\)).E (
float,ArrayType,Callable,Initializer) – The reversal potential (mV).V_sh (
Union[int,float,TypeVar(ArrayType,Array,Variable,TrainVar,Array,ndarray),Initializer,Callable]) – The membrane shift.
References
See also