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. 2014 Dec 4;9(12):e114034. doi: 10.1371/journal.pone.0114034

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© 2014 Tong et al

This is an open-access article distributed under the terms of the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original author and source are properly credited.

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A, The same conditions and AP form of the modified USMC model as depicted in Figure 7 wherein _hERG = 0.08 nS pF⁻¹. B-E, the effects of progressively reducing I _hERG conductance. B, _hERG = 0.0464 nS pF⁻¹; C, _hERG = 0.0224 nS pF⁻¹; D, _hERG = 0.0064 nS pF⁻¹; E, _hERG = 0.0008 nS pF⁻¹.

Inline graphic — A, The same conditions and AP form of the modified USMC model as depicted in Figure 7 wherein _hERG = 0.08 nS pF⁻¹. B-E, the effects of progressively reducing I _hERG conductance. B, _hERG = 0.0464 nS pF⁻¹; C, _hERG = 0.0224 nS pF⁻¹; D, _hERG = 0.0064 nS pF⁻¹; E, _hERG = 0.0008 nS pF⁻¹.