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

机译:初级感觉神经元亚组中超极化激活电流(Ih)的热力学性质

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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°C were fitted with double exponential functions, yielding time constants similar to those of HCN1. The fast activation and deactivation rates showed temperature coefficients (Q 10) of 2.9 and 3.1, respectively, while Q 10 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 ∼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°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 (z g) (3.75 ± 0.32, mean ± SEM, at 25°C) and half-activation potential (V 1/2) (−70.0 ± 1.3 mV at 25°C) did not vary significantly with temperature.
机译:Ih是选择性差的阳离子电流,在超极化时会激活,存在于各种类型的神经元中。我们的目的是对Ih门控动力学进行详细的热力学分析,以评估与其活化和失活相关的推定结构变化。为了选择表现出大Ih的背根神经节神经元,我们应用了Petruska等人的最新签名方法。 (J Neurophysiol 84:2365-2379,2000),并在簇4中找到合适的神经元。在25和33°C下由3,000-ms超极化脉冲引起的电流具有双指数函数,产生的时间常数与HCN1相似。快速活化和失活速率显示的温度系数(Q 10 )分别为2.9和3.1,而绝对电导的Q 10 为1.3。使用Arrhenius-Eyring形式主义,我们为每个速率计算了电压无关的吉布斯自由能和熵壁垒的高度。快速率的自由能垒仅比相应慢速率的自由能垒低约2RT单位(在25°C时激活的31.3 vs. 33.2RT,去激活的24.7 vs. 25.8 RT)。有趣的是,慢速运动的熵壁垒为负:激活分量为-15.2R单位,去激活因子为-11.9R单位,而快速分量分别为4.6和1.3R单位。等效门控电荷(zg )(3.75±0.32,平均值±SEM,在25°C下)和半激活电位(V 1/2 )(-25°C下为-70.0±1.3 mV )随温度变化不大。

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