That’s it, dear readers. I can’t thank enough the people who contributed to this project and helped shape T-World into its final form. It was wonderful to work on this with a range of very different people, addressing different aspects of the model development and presentation, from support in formulating details of calcium handling, conceptualizing new components, to demonstrating applicability to interesting and relevant tasks. I’ve been going through memories of different stages of the project, and the project wouldn’t be the same without you all! I am also very grateful to the Wellcome Trust, whose fellowship gave me the freedom to focus properly on the later stages of development and bring the work to completion. At the same time, this project has made me think a bit about how we support the development of substantial computational methodologies. My experience with T-World was ultimately a positive one, but it also highlighted how difficult this kind of work can be to carry ou...
At one point, I noticed how EADs are quite a bit harder to evoke in the Shannon-Bers model than in ToR-ORd. I.e., when I ported key currents (I CaL , I NaL , I Kr , I Ks ) to the newly created model built closer to the Bers/Grandi framework, it would still not generate EADs as readily in the right conditions as models like ToR-ORd. The difference was not huge, but it was noticeable. In a separate investigation, when I was trying to build an understanding of differences in each current in either framework, I noticed how relatively different is the voltage-dependence – near-linear in ToR-ORd, but sublinear in the Shannon model. And there I had a spark of thinking that clarified why the Shannon-like models could be naturally less prone to EAD formation, arising from the sodium-potassium pump differences. Let’s go over this in more detail. Below is shown a comparison of the linear voltage-dependence used in T-World, versus the sublinear voltage-dependence of the sodium-potassium pum...