Institut für Chemie, Biophysikalische Chemie, Kernforschungsanlage Jülich GmbH, Postfach 1913, D-5170, Jülich.
Planta. 1980 Feb;147(5):396-404. doi: 10.1007/BF00380179.
Etioplasts, etiochloroplasts, and chloroplasts of Avena sativa L. purified on a Percoll gradient were subjected to increasing electric field strengths in the orifice of a hydrodynamically focussing Coulter Counter. The change in resistance of the orifice when an organelle is present correlates well with the size of the plastid for field strengths up to about 3.5 kV cm(-1). Beyond this field strength, depending on the size of the organelle, the size is underestimated. The underestimation of the size is caused by the dielectric breakdown of the envelope membranes once a critical membrane potential has been exceeded. Beyond breakdown the signal of the particle is predominately determined both by the internal conductivity and the increased membrane conductivity. Measurements of the breakdown voltage of different developmental stages of the plastids reveal that the breakdown voltage decreases from 1.2 V in etioplasts to about 0.9 V in chloroplasts after 48 h illumination. The decrease in breakdown voltage can be explained in terms of increasing incorporation of proteins into the inner envelope membrane during development.This view is consistent with conclusions drawn by other authors from transport and biochemical studies. The underestimation of the size beyond breakdown is about 20% and increases to a constant value of about 40% during the first 3 h of illumination. The underestimation decreases again to about 10% when the chloroplast stage is reached. This result is consistent with the current view of chloroplast development. Mobilisation of glucans, the transformation of the prolamellar body of etioplasts into thylacoid membranes as well as an intensive synthesis of pigments and enhanced rates of ions transport in the first hour of illumination gives rise to an increased pool of ionic compounds within the plastid stroma.It should be noted that purification of the plastids on Percoll gradient leads to size distributions which are almost normally distributed over the whole field range, suggesting that the preparations are also electrically homogeneous (U. Zimmermann, F. Riemann and G. Pilwat: Biochim. Biophys. Acta 436, 460-474 (1976)). In contrast with results of Lürssen, K., Z. Naturforsch. 25b, 1113-1119 (1970) only a slight increase of the modal volume from the etioplast stage to the chloroplast stage is observed.
在聚蔗糖梯度上纯化的燕麦质体、黄化质体和叶绿体,在水力聚焦库尔特计数器的孔中受到逐渐增强的电场强度的作用。当细胞器存在时,孔的电阻变化与质体的大小密切相关,在大约 3.5 kV/cm 的场强下。超过这个场强,根据细胞器的大小,大小会被低估。一旦超过临界膜电位,包膜膜的介电击穿会导致大小的低估。在击穿之后,颗粒的信号主要由内部电导率和增加的膜电导率决定。对不同发育阶段质体的击穿电压的测量表明,从黄化质体的 1.2 V 到光照 48 小时后的叶绿体的约 0.9 V,击穿电压降低。在发育过程中,内包膜中蛋白质的不断掺入可以解释击穿电压的降低。这一观点与其他作者从运输和生化研究中得出的结论是一致的。击穿后大小的低估约为 20%,在光照的前 3 小时内增加到一个恒定值约 40%。当达到叶绿体阶段时,低估再次减小到约 10%。这一结果与叶绿体发育的当前观点是一致的。在光照的第一个小时内,糖的动员、黄化质体的前板层体向类囊体膜的转化以及色素的大量合成和离子运输速率的提高,导致质体基质内离子化合物的增加。应该注意的是,在聚蔗糖梯度上对质体的纯化导致在整个场范围内几乎呈正态分布的大小分布,这表明制剂也是电均匀的(U. 齐默尔曼、F. 里曼和 G. 皮拉特:生物化学。生物物理学学报 436, 460-474 (1976))。与 Lürssen, K. 的结果相反,仅观察到从黄化质体阶段到叶绿体阶段的模态体积略有增加。