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. 2015 Dec 21;3(2):114-23.
doi: 10.1002/acn3.276. eCollection 2016 Feb.

Pathogenic mechanism of recurrent mutations of SCN8A in epileptic encephalopathy

Affiliations

Pathogenic mechanism of recurrent mutations of SCN8A in epileptic encephalopathy

Jacy L Wagnon et al. Ann Clin Transl Neurol. .

Abstract

Objective: The early infantile epileptic encephalopathy type 13 (EIEE13, OMIM #614558) results from de novo missense mutations of SCN8A encoding the voltage-gated sodium channel Nav1.6. More than 20% of patients have recurrent mutations in residues Arg1617 or Arg1872. Our goal was to determine the functional effects of these mutations on channel properties.

Methods: Clinical exome sequencing was carried out on patients with early-onset seizures, developmental delay, and cognitive impairment. Two mutations identified here, p.Arg1872Leu and p.Arg1872Gln, and two previously identified mutations, p.Arg1872Trp and p.Arg1617Gln, were introduced into Nav1.6 cDNA, and effects on electrophysiological properties were characterized in transfected ND7/23 cells. Interactions with FGF14, G-protein subunit Gβγ, and sodium channel subunit β1 were assessed by coimmunoprecipitation.

Results: We identified two patients with the novel mutation p.Arg1872Leu and one patient with the recurrent mutation p.Arg1872Gln. The three mutations of Arg1872 and the mutation of Arg1617 all impaired the sodium channel transition from open state to inactivated state, resulting in channel hyperactivity. Other observed abnormalities contributing to elevated channel activity were increased persistent current, increased peak current density, hyperpolarizing shift in voltage dependence of activation, and depolarizing shift in steady-state inactivation. Protein interactions were not affected.

Interpretation: Recurrent mutations at Arg1617 and Arg1872 lead to elevated Nav1.6 channel activity by impairing channel inactivation. Channel hyperactivity is the major pathogenic mechanism for gain-of-function mutations of SCN8A. EIEE13 differs mechanistically from Dravet syndrome, which is caused by loss-of-function mutations of SCN1A. This distinction has important consequences for selection of antiepileptic drugs and the development of gene- and mutation-specific treatments.

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Figures

Figure 1
Figure 1
Recurrent mutations of arginine residues 1617 and 1872 in SCN8A. (A) Four‐domain structures of the voltage‐gated sodium channel α subunit. The positions of the recurrently mutated residues Arg1617 (the outermost charged residue in the S4 transmembrane segment of domain IV) and Arg1872 (near the middle of the cytoplasmic C‐terminal domain) are shown. (B) CpG mutation hot spots in the codons for Arg1617 and Arg1872.
Figure 2
Figure 2
Biophysical effects of missense mutations at residue Arg1872 in Nav1.6. (A) Representative traces of families of Na currents from ND7/23 cells transfected with the indicated Nav1.6 cDNAs. (B) Averaged current–voltage (I‐V) relation for cells expressing WT and mutant Nav1.6. Peak currents were normalized to cell capacitance. (C) Average fast time constant obtained from single exponential fits to macroscopic current decays as a function of voltage (mV). (D) Representative traces of normalized currents evoked by a −20 mV stimulus from a holding potential of −120 mV illustrate delays in macroscopic current decay. (E) Representative normalized current traces recorded during a 100‐msec depolarizing pulse from −120 mV to 0 mV illustrating the presence of elevated persistent sodium current for p.Arg1872Leu. (F) Voltage dependence of channel activation. (G) Voltage dependence of steady‐state inactivation. Smooth lines correspond to the least squares fit when average data were fit to a single Boltzmann equation. Data are mean ± SEM. Statistical significance: *P < 0.05. Black, wild type; red, p.Arg1872Leu; orange, p.Arg1872Gln; green, p.Arg1872Trp.
Figure 3
Figure 3
Biophysical effects of the missense mutation p.Arg1617Gln in Nav1.6. (A) Representative traces of families of Na currents from ND7/23 cells transfected with the indicated Nav1.6 cDNA. (B) Averaged current–voltage (I‐V) relation for cells expressing WT and p.Arg1617Gln. Peak currents were normalized to cell capacitance. (C) Average fast time constant obtained from single exponential fits to macroscopic current decays as a function of voltage (mV). (D) Representative traces of normalized currents evoked by a depolarizing step to −20 mV from a holding potential of −120 mV illustrate significant delay in macroscopic current decay in p.Arg1617Gln (blue) compared to WT (black). (E) Representative normalized current traces recorded during a 100‐msec depolarizing pulse from −120 mV to 0 mV illustrating the presence of elevated persistent sodium current. (F) Voltage dependence of channel activation. (G) Voltage dependence of steady‐state inactivation. (H). Representative inactivation traces recorded after a 1‐sec prepulse of −100 mV (larger amplitude) and −45 mV (smaller amplitude). Smooth lines in (F) and (G) correspond to the least squares fit when average data were fit to a single Boltzmann equation. Data are mean ± SEM. Statistical significance: *P < 0.05. Black, wild type; blue, p.Arg1617Gln.

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