IntroductionThe isolated papillary muscle is a standard preparation for investigation of drug induced effects on the ventricular AP. To facilitate model based analysis of mechanisms underlying drug effects in this preparation, we adapted the rabbit ventricular AP model published by Shannon et al.[1] to reproduce parameters of our baseline transmembrane AP recordings. The adapted model will be applied in future investigation of drug effects.
Methods and materialsData collection was previously described in detail [2]. APs were recorded in right ventricular papillary muscles isolated from 21 female New Zealand white rabbits. For all rabbits, APs were recorded at baseline without any drugs at pacing rates of 0.5 and 2.0 Hz. Sequences of baseline recordings were obtained from approximately eight different cells from each rabbit, and a median AP was calculated for each cell. We used a current MatLab implementation of the Shannon rabbit ventricular AP model published online. Adaptation of the model was done by changes in the maximal current conductance of membrane currents. The major transmembrane currents investigated were: the fast inward sodium current (INa), the rapid and slow components of the delayed rectifier potassium current (I Kr , I Ks ), the fast and slow components of the transient outward potassium current (I tof , I tos ), the inward rectifier potassium current (I K1 ), the L-type calcium current (I CaL ), the sodium-potassium pump (I NaK ), and the sodium-calcium exchanger (I NaCa ).
Baseline adaptationThe default model AP displayed longer APD 90 and greater amplitude compared to experiment. The mean and 95 % confidence interval of measured AP amplitude (defined as the maximal value of the upstroke) was 21.4 ± 2.5 mV and 23.8 ± 2.4 mV at 2.0 and 0.5 Hz pacing respectively. The default model AP amplitude was 42.7 mV and 43.7 mV. Before adaptation to APD, the model AP amplitude was reduced by reduction in INa current conductance determined by minimization of the error between model and measured AP amplitude.The mean and 95 % confidence interval of measured APD 90 was 113.9 ± 11.2 ms and 150.2 ± 13.1 ms at 2.0 and 0.5 Hz pacing respectively. The model APD 90 was 190 ms and 221.5 ms and was adapted to experiment by reduction of the I CaL , I NaK , and I NaCa currents by multiplication of the current conductances with an identical factor to minimize the error between model and measured APD 90 across both frequencies. This approach was based in part on the results of the sensitivity analysis as described in the discussion.
ISSN 2325-8861Computing in Cardiology 2015; 42:429-432.