“…In order to compute the value of the fluxes J Ca , J NCX , J pCa and J Cab we define their respective current densities I Ca , I NCX , I pCa and I Cab . I NCX and I Cab are functions of the holding potential of voltage-clamp protocol V : with V = 10 mV , for t ∈ (0, 70 ms ], and V = −50 mV , for t ∈ (70 ms , ∞], (see Yao et al [10]) The given current densities I i (µ M/ms ), i = Ca, NCX, pCa, Cab are converted to Ca 2+ influx/efflux J i (µ M/ms ), i = Ca, NCX, pCa, Cab by using an experimentally estimated capacitance to rendered volume ratio, ( C m /V cell = 8.8 pF/pL ) in adult rat ventricular myocytes [10]:
where C m ( pF ) is the cell capacitance, V cell ( pL ) is the cell volume, V mc (µ m 3 ) is the compartment volume of the geometric model used to represent the cell in the numerical experiment, S j (µ m 2 ) is the total surface area where the channel i resides in the geometric model, F is the Faraday’s constant, and β i , i = Ca, NCX, pCa, Cab is a model-dependent scaling parameter for LCCs, NCXs, Ca 2+ pumps and background leak respectively. The values of the scaling parameters are as follows β Ca = 232.3, β NCX = 133.7, β pCa = 390.0, and β Cab = 1345.0.…”