Evidence map›Paper›PMID 16676167›Full record

ArticleExperimental brain research2006

Thermodynamic properties of hyperpolarization-activated current (Ih) in a subgroup of primary sensory neurons.

Florentina Pena, Bogdan Amuzescu, Emil Neaga, Maria-Luiza Flonta

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Article in Experimental brain research, 2006. The graph could read no effect estimate from its abstract, so it casts no vote on the map. Cited by 11 papers.

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0cells of the map it votes in
11citing papers in PubMed
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1 · What the graph read from it

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The abstract states no effect estimate the extractor could read, or names no intervention and outcome on the map, so this paper lights no cell and moves no belief. It is still indexed, cited and linked below.

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3 · Its place in the literature

Who cites it

11 citing papers in PubMed.

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  5. Many parameter sets in a multicompartment model oscillator are robust to temperature perturbations.The Journal of neuroscience : the official journal of the Society for Neuroscience · 2014
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4 · The record

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5 · Who and what money

Authors and funding

4 authors.

Florentina PenaDepartment of Animal Physiology and Biophysics, Faculty of Biology, University of Bucharest, Splaiul Independentei 91-95, Bucharest, 76201, Romania.
Bogdan Amuzescu
Emil Neaga
Maria-Luiza Flonta

Funding

No grant is acknowledged in the PubMed record.

6 · The paper itself

Abstract

Ih is a poorly selective cation current that activates upon hyperpolarization, present in various types of neurons. Our aim was to perform a detailed thermodynamic analysis of Ih gating kinetics, in order to assess putative structural changes associated with its activation and deactivation. To select dorsal root ganglia neurons that exhibit large Ih, we applied a current signature method by Petruska et al. (J Neurophysiol 84:2365-2379, 2000) and found appropriate neurons in cluster 4. Currents elicited by 3,000-ms hyperpolarizing pulses at 25 and 33 degrees C were fitted with double exponential functions, yielding time constants similar to those of HCN1. The fast activation and deactivation rates showed temperature coefficients (Q10) of 2.9 and 3.1, respectively, while Q10 of the absolute conductance was 1.3. Using the Arrhenius-Eyring formalism we computed heights of voltage-independent Gibbs free energy and entropy barriers for each rate. The free energy barriers of the fast rates were just approximately 2RT units lower than those of the corresponding slow rates (31.3 vs. 33.2RT for activation, and 24.7 vs. 25.8RT for deactivation, at 25 degrees C). Interestingly, the entropy barriers of the slow rates were negative: -15.2R units for activation and -11.9R units for deactivation, compared to 4.6 and 1.3R units, respectively, for the fast component. The equivalent gating charge (zg) (3.75 +/- 0.32, mean +/- SEM, at 25 degrees C) and half-activation potential (V1/2) (-70.0 +/- 1.3 mV at 25 degrees C) did not vary significantly with temperature.

Indexed as

ThermodynamicsAlgorithmsAnimalsCyclic Nucleotide-Gated Cation ChannelsElectrophysiologyElectroshockGanglia, SpinalHyperpolarization-Activated Cyclic Nucleotide-Gated ChannelsIon Channel GatingIon ChannelsKineticsMaleNeurons, AfferentPatch-Clamp TechniquesPotassium ChannelsRatsCyclic Nucleotide-Gated Cation ChannelsHcn1 protein, ratHyperpolarization-Activated Cyclic Nucleotide-Gated ChannelsIon ChannelsPotassium Channels

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Read under generation 80e0d062 · epoch 390. Bibliography from PubMed, PubMed Central and OpenAlex; grants from NIH RePORTER; trial links from ClinicalTrials.gov; estimates, votes and beliefs from the OpenQuestion graph.