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The leakage current is modeled with the Kleakparameter.
The capacitive current is modeled in parallel with the charge-transfer process.
Wave-induced nearshore current is modeled using the nonlinear shallow water equations in which wave radiation stresses are provided by wave model for driving current.
Here, unlike some of the previous researches, the load current is modeled as disturbance and also communication time-delay is considered.
As the battery available energy changes with different applied load current profiles, the relationship between the remaining energy loss and the state of charge, the average current as well as the average squared current is modeled.
The LRS current is modeled using a modified form of the current relation of the Chua model [1], given as [118]: i(t)=left{begin{array}{c}Ksqrt{varphi }v(t kern0.75em mathrm{if} varphi <{varphi}_r 0kern4.25em mathrm{if} varphi ={varphi}_rend{array}right.
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Each ion channel current is modelled by the Huxley-Hodgkin formulation which is fitted to experimental data.
The INa L current was modeled using the Hodgkin-Huxley formalism.
Velocity profile and ion current were modeled by numerically solving coupled Poisson Nernst Planck and Navier Stokes equations.
The activation of synaptic currents was modeled by a Poisson process.
The dynamics of the synaptic currents were modeled with a two-state kinetic scheme (Destexhe et al., 1994).
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