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. 2014 Mar 4;289(17):11952–11969. doi: 10.1074/jbc.M114.551473

FIGURE 3.

FIGURE 3.

Differing extracellular turrets in domain II P-loop (exons 12a and 12b) do not alter major features outside of monovalent ion permeability. There were no major differences in most biophysical properties between LCav3-12a and LCav3-12b in 2 mm [Ca2+]ex, including the following: A, current-voltage relationship for activation and steady-state inactivation; B, inactivation kinetics and time to peak (inset); C, current size differences in 2 mm [Ba2+]ex versus [Ca2+]ex, and D, blockade by 300 μm Ni2+. A sample of the blocking effect for nickel for LCav3-12a is shown in the inset of D. A sample of a similar block of nickel for LCav3-12b is shown in Fig. 3, A and B, of Ref. 13. There are measurable differences in faster recovery rate from inactivation (E) and slower deactivation kinetics for LCav3-12a (F). n values are shown in parentheses. The differences in the rate of recovery is observed at the earliest time point, when the time scale range is limited from 0 to 2 s (E, inset). Statistics for Fig. 3 are shown in Table 4.