| Literature DB >> 28330959 |
Johanna Palmio1, Satu Sandell2, Michael G Hanna2, Roope Männikkö2, Sini Penttilä2, Bjarne Udd2.
Abstract
OBJECTIVE: To characterize the clinical phenotype in patients with p.A1156T sodium channel mutation.Entities:
Mesh:
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Year: 2017 PMID: 28330959 PMCID: PMC5395072 DOI: 10.1212/WNL.0000000000003846
Source DB: PubMed Journal: Neurology ISSN: 0028-3878 Impact factor: 9.910
Figure 1Pedigree of the families
*DNA available.
Electrophysiologic findings of patients with p.A1156T
Figure 2Functional characterization of p.A1156T channel
(A) Representative current traces of wild-type and p.A1156T channels in response to test voltages ranging from −60 to 50 mV. Scale bars are 1 millisecond (x-axis) and 20 pA/pF (y-axis). Dashed lines indicate 0 current level. Voltage protocol for voltage steps ranging from −150 to 50 mV is shown in inset. (B) Peak current amplitude in response to test voltages ranging from −150 to 50 mV in 10-mV increments is plotted against the test voltage for wild-type (solid circles) (n = 18) and p.A1156T (open squares) (n = 11) channels. (C) Voltage dependence of activation was estimated by plotting the conductance [peak current/(test voltage − reversal voltage)] against the test voltage for wild-type (solid circles) (V1/2 = −20.3 ± 0.7 mV, n = 18) and p.A1156T (open squares) (V1/2 = −20.4 ± 0.7 mV, n = 11) channels. Individual data were normalized to maximum and minimum amplitude of the Boltzmann fit and averaged. Solid lines represent the fit of the Boltzmann equation to the mean data. (D) Voltage dependence of fast inactivation was estimated by plotting the peak tail current amplitude at −10 mV after 150-millisecond prepulse voltage steps ranging from −150 to 0 mV in 10-mV increments against the prepulse voltage for wild type (solid circles) (V1/2 = −66.2 ± 0.7 mV, n = 18) and p.A1156T (open squares) (V1/2 = −63.5 ± 1.0 mV, n = 11) channels. The voltage protocol is shown on the right. Individual data were normalized to maximum and minimum values of the Boltzmann equation and averaged. Solid lines represent the fit of the Boltzmann equation to the mean data. (E) To estimate the time course of recovery from the inactivation, the current in response to a second voltage pulse to 0 mV (P2) divided by the current in response to the first 10-millisecond pulse to 0 mV (P1) is plotted against the duration of the recovery step at −80 mV between the 2 pulses. Data are shown for wild-type (solid circles) (τ = 6.5 ± 0.4 milliseconds, n = 16) and p.A1156T (open squares) (τ = 3.8 ± 0.3 milliseconds, n = 10) channels. The voltage protocol is shown in the inset. The solid lines represent the fit of exponential function to the mean data. (F) Time course of open-state inactivation was estimated by fitting a double exponential function to the current decay between 90% of peak current amplitude and the current baseline. Time constant (τ) of inactivation at voltages ranging from −20 to 20 mV is shown for wild type (solid circles) (n = 18) and p.A1156T (open squares) (n = 11) channels. Voltage protocol was as in panel (A). Only the time constant of the fast component that carries ≈95% of the amplitude of the inactivating current is shown. (G) Voltage dependence of slow inactivation was studied by plotting the peak tail current amplitude at −10 mV after a 10-second prepulse to voltage steps ranging from −130 to 50 mV in 10-mV increments against the prepulse voltage for wild-type (solid circles) (V1/2 = −51.2 ± 0.9 mV, n = 12) and p.A1156T (open squares) (V1/2 = −58.3 ± 1.0 mV, n = 7) channels. Between the prepulse and the test pulse, the voltage was stepped to −100 mV for 20 milliseconds to allow the channel to recover from fast inactivation. The voltage protocol is shown in the inset. Individual data were normalized by dividing with maximum value of the Boltzmann equation and averaged. Solid lines represent the fit of the Boltzmann equation to the mean data.