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猫γ运动神经元的电紧张结构

Electrotonic architecture of cat gamma motoneurons.

作者信息

Burke R E, Fyffe R E, Moschovakis A K

机构信息

Laboratory of Neural Control, National Institute of Neurological Disorders and Stroke, National Institute of Health, Bethesda, Maryland 20892.

出版信息

J Neurophysiol. 1994 Nov;72(5):2302-16. doi: 10.1152/jn.1994.72.5.2302.

Abstract
  1. Experimental measures of input resistance, RN, and responses to brief hyperpolarizing current pulses were obtained in identified gamma-motoneurons in pentobarbital-anesthetized cats using conventional sharp micropipettes. The same cells were subsequently injected with horseradish peroxidase and completely reconstructed. In two cells, the electrophysiological and morphological data were of sufficient quality to permit estimation of specific membrane resistance, Rm, using biologically plausible ranges of specific cytoplasmic resistance, Ri, and membrane capacitance, Cm. 2. A combination of steady-state and dynamic computer models were employed to reconcile cell morphology with RN and the trajectories of the voltage decay following brief current pulses delivered to the soma. Simulated transient responses matched the tails of the observed transient when generated with the same current injections used experimentally. With Cm < or = 1.0 microF cm-2, the most satisfactory fits were obtained when the values of Rm assigned to the soma, Rms, were much smaller than the spatially uniform value assigned to the dendrites, Rmd and Ri = 60-70 omega cm. With Cm = 1.0 microF cm-2, Rms ranged from 260 to 427 omega cm2, whereas Rmd was approximately 33 K omega cm2. With Cm = 0.8 microF cm-2, Rms ranged from 235 to 357 omega cm2 and Rmd was between 62 and 68 K omega cm2. When Rm was constrained to be spatially uniform (i.e., Rm = Rms), implausibly high values of Cm (2.5-5.0 microF cm-2; Ri = 70 omega cm) were required to match the observed tail time constant, tau o,peel, but the simulated transients did not otherwise match those obtained experimentally. 3. With best fit values of Rms and Rmd, both gamma-motoneurons were electronically relatively compact (80% of total membrane area within 0.85 length constants from the soma). However, the calculated average steady-state inward attenuation factor (AFin) for voltages generated at any point within the dendrites increased rapidly with distance from the soma, reaching levels of < or = 90 and < or = 45 for the proximal 80% of membrane area for the respective motoneurons in the presence of a somatic shunt (Rms << Rmd). If we assume that the somatic shunt is an artifact of sharp micropipette penetration (i.e., that Rms = Rmd for uninjured cells), then AFin decreased to < or = 20 and < or = 15, respectively, for the proximal 80% of cell membrane.(ABSTRACT TRUNCATED AT 400 WORDS)
摘要
  1. 使用传统的尖锐微电极,在戊巴比妥麻醉的猫的已识别γ运动神经元中,获得了输入电阻RN以及对短暂超极化电流脉冲的反应的实验测量值。随后,向相同的细胞中注射辣根过氧化物酶并进行完全重建。在两个细胞中,电生理和形态学数据质量足够高,能够利用特定细胞质电阻Ri和膜电容Cm的生物学合理范围来估计比膜电阻Rm。2. 采用稳态和动态计算机模型相结合的方法,将细胞形态与RN以及向胞体施加短暂电流脉冲后电压衰减的轨迹进行协调。当使用与实验相同的电流注入进行模拟时,模拟的瞬态反应与观察到的瞬态反应的尾部相匹配。当Cm≤1.0 μF/cm²时,当赋予胞体的Rm值Rms远小于赋予树突的空间均匀值Rmd且Ri = 60 - 70 Ω·cm时,能获得最满意的拟合。当Cm = 1.0 μF/cm²时,Rms范围为260至427 Ω·cm²,而Rmd约为33 KΩ·cm²。当Cm = 0.8 μF/cm²时,Rms范围为235至357 Ω·cm²,Rmd在62至68 KΩ·cm²之间。当Rm被限制为空间均匀时(即Rm = Rms),需要不合理的高Cm值(2.5 - 5.0 μF/cm²;Ri = 70 Ω·cm)才能匹配观察到的尾部时间常数τo,peel,但模拟的瞬态反应在其他方面与实验获得的不匹配。3. 采用Rms和Rmd的最佳拟合值时,两个γ运动神经元在电学上相对紧凑(80%的总膜面积在距胞体0.85个长度常数范围内)。然而,对于在树突内任何点产生的电压,计算出的平均稳态内向衰减因子(AFin)随着距胞体距离的增加而迅速增加,在存在胞体分流(Rms << Rmd)的情况下,对于各自运动神经元近端80%的膜面积,达到≤90和≤45的水平。如果我们假设胞体分流是尖锐微电极穿透的伪像(即未受损细胞的Rms = Rmd),那么对于近端80%的细胞膜,AFin分别降至≤20和≤15。(摘要截断于400字)

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