| Literature DB >> 35359652 |
Chaseley E Mckenzie1, Chen-Jui Ho2, Ian C Forster1, Ming S Soh1, A Marie Phillips1,3, Ying-Chao Chang4, Ingrid E Scheffer1,5,6, Christopher A Reid1,5, Meng-Han Tsai2,7,8.
Abstract
Variants in HCN1 are associated with a range of epilepsy syndromes including developmental and epileptic encephalopathies. Here we describe a child harboring a novel de novo HCN1 variant, E246A, in a child with epilepsy and mild developmental delay. By parental report, the child had difficulty in discriminating between colors implicating a visual deficit. This interesting observation may relate to the high expression of HCN1 channels in rod and cone photoreceptors where they play an integral role in shaping the light response. Functional analysis of the HCN1 E246A variant revealed a right shift in the voltage dependence of activation and slowing of the rates of activation and deactivation. The changes in the biophysical properties are consistent with a gain-of-function supporting the role of HCN1 E246A in disease causation. This case suggests that visual function, including color discrimination, should be carefully monitored in patients with diseases due to HCN1 pathogenic variants.Entities:
Keywords: HCN1; color vision; developmental and epileptic encephalopathy; epilepsy; missense
Year: 2022 PMID: 35359652 PMCID: PMC8960314 DOI: 10.3389/fneur.2022.834252
Source DB: PubMed Journal: Front Neurol ISSN: 1664-2295 Impact factor: 4.003
Figure 1HCN1 E246A variant causes changes in the biophysical properties consistent with gain of function. (A) Structure of human HCN1 showing location of E246 (shown as spheres). Based on PDB 5u60 for human HCN1 in the depolarized (closed) conformation, rendered using PyMOL (The PyMOL Molecular Graphics System, Version 2.3.4 Schrodinger, LLC.). Upper panel: view from external medium; lower panel: side view. (B) Representative voltage clamp data from oocytes expressing HCN1 wild-type (WT) (left); E246A (middle) and co-expressed WT + E246A (right). Each dataset shows current traces in response to a series of voltage steps (inset) from the holding potential (−30 mV) to test potentials in the range −120 to + 20 mV (activation protocol, see Methods). Gray boxed areas have been enlarged to show tail currents. Note the different scales. Red trace corresponds to voltage step at −120 mV. (C) Box and Whisker plot of maximal steady-state current for HCN1 WT (n = 9); E246A (n = 9),and WT + E246A (n = 9) measured at end of test pulse to −100 mV; ns, not significant. (D) Pooled current-voltage (I–V) data shows a shift in the voltage-dependence of steady state activation for “homozygous” (n = 9 each group) compared to WT (n = 9). (E) Normalized, pooled I-V data reveals the right shift in steady-state activation; each data set was normalized to the steady-state current at −100 mV. The “heterozygous” data lies between the “homozygous” and WT data sets (n = 9 for each data set). (F) Normalized, instantaneous tail currents fit with a single Boltzmann function. Fit values were: V0.5 −71.1 ± 0.4 mV (WT); −60.1 ± 0.4 mV (E246A); −64.1 ± 0.4 mV (WT+E246A) and z: 2.92 ± 0.11 (WT); 3.09 ± 0.12 (E246A); 3.34 ± 0.15 (WT+E246A). (G) Mean activation time constant τ act obtained by fitting the time-dependent component of activating current with a single exponential function (see Methods). (H) Mean deactivation time constant obtained by fitting the time-dependent component of deactivating current with a single exponential function. Data points were joined for visualization. Data are expressed as mean ± s.d; statistical comparisons were made to wild-type using one-way ANOVA with Dunnett's post-hoc test (see Supplementary Tables 1–3 for detailed analyses).