Department of Physics and Astronomy, Free University, de Boelelaan 1081, 1081 HV, Amsterdam, The Netherlands.
Biophys J. 1991 May;59(5):992-1001. doi: 10.1016/S0006-3495(91)82314-1.
We have used a new and relatively easy approach to study the pigment-organization in chlorosomes from the photosynthetic bacterium Chloroflexus aurantiacus and in B800-850 antenna complexes of the photosynthetic purple bacterium Rhodobacter sphaeroides. These particles were embedded in compressed and uncompressed gels and the polarized fluorescence was determined in a 90 degrees setup. Assuming both a rotational symmetric distribution of the particles in the gel and of the transition dipole moments in the particles, the order parameters <P(2)> and <P(4)>, describing the orientation of the symmetry axis of the particles with respect to the direction of gel expansion can be determined. Moreover, the direction parameters, describing the orientation of the absorption and emission dipole moments with respect to the symmetry axis of the particles can be obtained.The value of <P(2)> is essential for quantitative interpretation of linear dichroism measurements and usually it is estimated from theoretical approaches, which may lead to incorrect results. For the rod-like chlorosomes the value of <P(2)> appears to be the same as predicted by the theoretical approach of Ganago, A. O., M. V. Fok, I. A. Abdourakhmanov, A. A. Solov'ev, and Yu. E. Erokhin (1980. Mol. Biol. [Mosc.]. 14:381-389). The agreement with linear dichroism results, analyzed with this theoretical approach shows that the transition dipole moments are indeed in good approximation distributed in a rotationally symmetric way around the long axis of the chlorosomes. Moreover, it appears those BChl c molecules, which fluoresce, are oriented in the same way with respect to the symmetry axis as the rest of these pigments, with the dipole moments close to parallel to the long axis.The B800-850 complexes appear to orient like discs, whereas the transition dipoles of the BChl a 800- and 850-nm bands are oriented almost perpendicular to the symmetry axis. These findings are in agreement with the minimal model for these complexes proposed by Kramer, H. J. M., R. van Grondelle, C. N. Hunter, W. H. J. Westerhuis, and J. Amesz (1984. Biochim. Biophys. Acta. 156-165).The amount of orientation of the particles appears to vary for different gels and it is lower than predicted by the theory of Ganago et al., showing that application of their approach for these particles leads to incorrect interpretations.The approach that is used in this study allows determination of orientations of those dipole moments, which transfer their excitation energy to the fluorescing species, in contrast to linear dichroism measurements, where the orientations of all absorbing dipole moments are studied. For the polarized fluorescence measurements, the amount of orientation of the particles is determined experimentally, whereas for linear dichroism this amount has to be estimated from theoretical models. The value of <P(2)> that can be determined from the fluorescence measurements can, however, also be used for a quantitative interpretation of the linear dichroism results.
我们使用了一种新的、相对简单的方法来研究来自光合细菌绿屈挠菌的叶绿素体和光合紫色细菌球形红杆菌的 B800-850 天线复合物中的色素组织。这些颗粒被嵌入在压缩和未压缩的凝胶中,并在 90 度设置中确定偏振荧光。假设颗粒在凝胶中的旋转对称分布和颗粒中的跃迁偶极矩的旋转对称分布,那么可以确定描述颗粒对称轴相对于凝胶膨胀方向的取向的有序参数<P(2)>和<P(4)>。此外,可以获得描述吸收和发射偶极矩相对于颗粒对称轴取向的方向参数。<P(2)>的值对于线性二色性测量的定量解释至关重要,通常它是通过可能导致不正确结果的理论方法来估计的。对于棒状叶绿素体,<P(2)>的值似乎与 Ganago 等人的理论方法预测的值相同。A. O., M. V. Fok, I. A. Abdourakhmanov, A. A. Solov'ev, and Yu. E. Erokhin (1980. Mol. Biol. [Mosc.]. 14:381-389)。与用这种理论方法分析的线性二色性结果的一致性表明,跃迁偶极矩确实以旋转对称的方式分布在叶绿素体的长轴周围。此外,似乎那些荧光发射的 BChl c 分子相对于这些色素的其余部分以相同的方式取向,偶极矩接近于平行于长轴。B800-850 复合物似乎呈盘状取向,而 BChl a 800-和 850-nm 带的跃迁偶极矩几乎垂直于对称轴。这些发现与 Kramer 等人提出的这些复合物的最小模型一致。H. J. M., R. van Grondelle, C. N. Hunter, W. H. J. Westerhuis, and J. Amesz (1984. Biochim. Biophys. Acta. 156-165)。不同凝胶中颗粒的取向数量似乎不同,并且低于 Ganago 等人的理论预测,表明应用他们的方法对这些颗粒进行解释会导致不正确的结果。与线性二色性测量不同,该研究中使用的方法可以确定将激发能量传递给荧光物种的那些偶极矩的取向,在线性二色性测量中,研究的是所有吸收偶极矩的取向。对于偏振荧光测量,颗粒的取向数量是通过实验确定的,而对于线性二色性,这个数量必须从理论模型估计。然而,荧光测量可以确定的<P(2)>值也可以用于线性二色性结果的定量解释。