2011
DOI: 10.1002/cnm.1453
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A localized meshless approach for modeling spatial–temporal calcium dynamics in ventricular myocytes

Abstract: SUMMARY Spatial-temporal calcium dynamics due to calcium release, buffering and re-uptaking plays a central role in studying excitation-contraction (E-C) coupling in both normal and diseased cardiac myocytes. In this paper, we employ a meshless method, namely, the local radial basis function collocation method (LRBFCM) to model such calcium behaviors by solving a nonlinear system of reaction-diffusion partial differential equations. In particular, a simplified structural unit containing a single transverse-tub… Show more

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Cited by 14 publications
(11 citation statements)
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“…The kinetics satisfies the equilibrium condition R B m = R B s = 0 and gives the following initial conditions, [ CaB 1 ] = 11.917µ M , [ CaB 2 ] = 0.968µ M , [ CaB 3 ] = 0.130µ M , [ CaB s ] = 6.364µ M . Following [10], we define the J Ca flux through the cell surface and T-tubule as: J Ca flux = J Ca + J NCX − J pCa + J Cab , where J Ca denotes the total Ca 2+ influx via the L-type Ca 2+ channels (LCCs), J NCX the total Ca 2+ influx (or efflux) via the Na + - Ca 2+ exchangers (NCXs), J pCa the total Ca 2+ pumps efflux and J Cab the total background Ca 2+ leak influx. 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 .…”
Section: Methodsmentioning
confidence: 99%
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“…The kinetics satisfies the equilibrium condition R B m = R B s = 0 and gives the following initial conditions, [ CaB 1 ] = 11.917µ M , [ CaB 2 ] = 0.968µ M , [ CaB 3 ] = 0.130µ M , [ CaB s ] = 6.364µ M . Following [10], we define the J Ca flux through the cell surface and T-tubule as: J Ca flux = J Ca + J NCX − J pCa + J Cab , where J Ca denotes the total Ca 2+ influx via the L-type Ca 2+ channels (LCCs), J NCX the total Ca 2+ influx (or efflux) via the Na + - Ca 2+ exchangers (NCXs), J pCa the total Ca 2+ pumps efflux and J Cab the total background Ca 2+ leak influx. 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 .…”
Section: Methodsmentioning
confidence: 99%
“…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]: Ji=βiVmcSjtrue(12FCmVitaliccelltrue)Ii, 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.…”
Section: Methodsmentioning
confidence: 99%
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“…At these scales, deterministic methods utilizing partial differential equations (PDEs) are more appropriate than stochastic methods [4,5]. The local radial basis function collocation method (LRBFCM) developed by S̃arler and Vertnik [6] has been applied to solving the PDEs in our earlier work [7]. This meshless method eliminates the generation of meshes, as commonly required in finite element methods.…”
Section: Introductionmentioning
confidence: 99%