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. 2022 Nov 17;23(22):14215. doi: 10.3390/ijms232214215

Figure 4.

Figure 4

R930H does not alter activation and inactivation parameters of Cav1.3S and Cav1.3L. (a) Voltage-dependence of activation of the wild-type and mutant Cav1.3S and (b) Cav1.3L variants. (c) Voltage-dependence of inactivation of wild-type Cav1.3S versus R930HS and (d) wild-type Cav1.3L versus R930HL. (e) Recovery from inactivation of wild-type Cav1.3S versus R930HS (τ Cav1.3S: 270.1 ± 14.4 ms, n = 10; τ R930HS: 261.9 ± 18.2 ms, n = 12; not significant, unpaired Student’s t-test) and (f) wild-type Cav1.3L versus R930HL (τ Cav1.3L: 166.1 ± 20.56 ms, n = 5; τ R930HL: 180.6 ± 36.4 ms, n = 5; not significant, unpaired Student’s t-test. Consistent with the literature, recovery from inactivation was faster in the Cav1.3L variant (τ Cav1.3L vs. τ Cav1.3S p = 0.0011, unpaired Student’s t-test) [20]. However, this parameter was not affected by the R930H variant. Recovery from inactivation was determined by 10 ms test pulses to Vmax at different time points after a 5-s conditioning pulse to the potential of the peak currents followed by a test pulse, as described in the Materials and Methods section. Data were fitted using a mono-exponential function. Data in (ad) are shown as mean ± S.E.M. For parameters and statistics see Table 2.