| Simulator: opencor 2021-10-05 | |
| CPU cores: 1 | |
| RAM: 8 GB | |
| Max time: 20 m |
| Submitted: 2022-04-21 03:30:07 PM | |
| Updated: 2022-04-21 03:30:34 PM | |
Status: Succeeded |
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12.01 KB
14.59 KB
20.20 KB
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| Simulator: opencor 2021-10-05 | |
| CPU cores: 1 | |
| RAM: 8 GB | |
| Max time: 20 m |
| Submitted: 2022-04-21 03:30:07 PM | |
| Updated: 2022-04-21 03:30:34 PM | |
Status: Succeeded |
This is the original unchecked version of the model imported from the previous CellML model repository, 24-Jan-2006.
Often it is not necessary to model the ionic currents of a cell with the accuracy and complexity inherent in the biophysically based models. With a view to investigating phenomena on a larger spatial and temporal scale, several ionic current models have been developed that do not seek to model subcellular processes but only to provide an action potential at a minimal computational cost.
The model created by van Capelle and Durrer (1980) follows the same general form as the FitzHugh-Nagumo model (see The FitzHugh-Nagumo Model, 1961), with a single activation variable and a single recovery variable. It also includes the ability to add more complex parameter representations.
The complete original paper reference is cited below:
Computer simulation of arrhythmias in a network of coupled excitable elements, van Capelle, F.J.L., Durrer, D., 1980, Circ. Res., 47, 454-466. PubMed ID: 7408126
The raw CellML description of the simplified cardiac myocyte models can be downloaded in various formats as described in . For an example of a more complete documentation for an electrophysiological model, see The Hodgkin-Huxley Squid Axon Model, 1952.
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