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Image Search Results
Journal: PLoS ONE
Article Title: Energy-Optimal Electrical-Stimulation Pulses Shaped by the Least-Action Principle
doi: 10.1371/journal.pone.0090480
Figure Lengend Snippet: As with the IM, bvp4c was used to numerically solve the BVP of eqn. (34). The figure follows a quite similar format to Fig. 5. can also be assumed higher or lower. All the maximal ionic conductances in the HHM (see also ) are temperature-dependent and are linearly proportional to the coefficient . The 3 solutions shown correspond to the ionic current at (cyan trace), twice higher (thin red dash-dot), or twice lower (thick dashed black) respectively. From eqn. (42) we can see that = 1.6047 (half the nominal) at , and = 6.4188 (twice the nominal) for at . Box: Resting-state and asymptotic-state ionic currents for the 0D HHM; Markers are inserted at the resting and threshold membrane-voltage points, respectively = −77 , = −64.55 and = −52.35 .
Article Snippet: Hence, we used the
Techniques: Membrane