Eckert R, Sibaoka T
J Gen Physiol. 1968 Aug;52(2):258-82. doi: 10.1085/jgp.52.2.258.
The action potential which elicits luminescence in Noctiluca is recorded from the flotation vacuole as a transient all-or-none hyperpolarization in response to either local or general application of inward (bath to vacuole) current. Experiments were performed to determine whether the unorthodox polarities of both the stimulus current and the potential response resulted from uncommon bioelectric mechanisms or from special morphological features of this species. The findings all indicate that the action potential belongs to the familiar class of responses which have their origin in voltage- and time-dependent selective increases in membrane permeability, and that morphological factors account for the observed deviations from normal behavior. Both the stimulus and the response have orthodox polarities provided the vacuole is designated as an "external" extracytoplasmic compartment. Differential recording between vacuole and cytoplasm showed that the action potential occurs across the vacuolar membrane, with the cytoplasmic potential, which at rest is negative with respect to the vacuole, overshooting zero and reversing sign to become transiently electropositive. The rising phase of the action potential therefore depends on active current flow through the vacuolar membrane from the vacuole into the cytoplasm. Propagation of the action potential over the subspherical cell from the locus of stimulation is thought to depend largely on the core conductor properties of the thin perivacuolar shell of cytoplasm which is bounded on its inner surface by the excitable membrane and on its outer surface by inexcitable membranes.
在夜光虫中引发发光的动作电位是从漂浮液泡记录到的,它是对局部或全身性内向(从外部溶液到液泡)电流施加的一种瞬时全或无超极化。进行了实验以确定刺激电流和电位响应的非正统极性是源于不常见的生物电机制还是该物种的特殊形态特征。所有研究结果均表明,动作电位属于常见的响应类型,其起源于膜通透性在电压和时间依赖性上的选择性增加,并且形态学因素解释了观察到的与正常行为的偏差。如果将液泡指定为“外部”胞外区室,那么刺激和响应都具有正统极性。液泡和细胞质之间的差分记录表明,动作电位发生在液泡膜上,静止时相对于液泡呈负性的细胞质电位超过零并反转符号,暂时变为电正性。因此,动作电位的上升阶段取决于从液泡到细胞质的主动电流通过液泡膜的流动。动作电位从刺激部位在近球形细胞上的传播被认为很大程度上取决于细胞质薄的液泡周围壳层的核心导体特性,该壳层的内表面由可兴奋膜界定,外表面由不可兴奋膜界定。