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菠菜叶绿体光合机构中的能量转移与激发能分布

Energy transfer and the distribution of excitation energy in the photosynthetic apparatus of spinach chloroplasts.

作者信息

Strasser R J, Butler W L

出版信息

Biochim Biophys Acta. 1977 May 11;460(2):230-8. doi: 10.1016/0005-2728(77)90209-2.

Abstract

Equations are derived from our model of the photochemical apparatus of photosynthesis to show that the yield of energy transfer from Photosystem II to Photosystem I, phi T(II leads to I), can be obtained from measurements on an individual sample of chloroplasts frozen to -196 degrees C by comparing the sum of two specifically defined fluorescence excitation spectra with the absorption spectrum of the sample. Then, given that value of phiT(II leads to I), the fraction of the quanta absorbed by the photochemical apparatus which is distributed initially to Photosystem I, alpha, can be determined as a function of the wavelength of excitation from the same fluorescence excitation spectra. The results obtained in this study of individual samples of chloroplasts frozen to -196 degrees C in the absence of divalent cations, namely, that phi T(II leads to I)varies from a minimum value of 0.10 when the Photosystem II reaction centers are all open to a maximum value of 0.25 when the centers are all closed and that alpha has a value of about 0.30 which is almost independent of wavelength for wavelength shorter than 675 nm (alpha increases rapidly toward unity at wavelength longer than 675 nm), agrees quite well with results obtained previously from comparative measurements of chloroplasts frozen to -196 degrees C in the presence and absence of divalent cations.

摘要

从我们的光合作用光化学装置模型推导出的方程式表明,通过比较两个特定定义的荧光激发光谱之和与样品的吸收光谱,可以从冷冻至-196℃的单个叶绿体样品的测量中获得从光系统II到光系统I的能量转移产率,即φT(II→I)。然后,给定φT(II→I)的值,可以根据相同荧光激发光谱中激发波长的函数来确定光化学装置吸收的量子中最初分配给光系统I的部分α。在不存在二价阳离子的情况下,对冷冻至-196℃的单个叶绿体样品进行这项研究得到的结果,即当光系统II反应中心全部开放时,φT(II→I)从最小值0.10变化到当中心全部关闭时的最大值0.25,并且对于波长小于675nm,α的值约为0.30,几乎与波长无关(在波长大于675nm时,α迅速趋近于1),这与先前在存在和不存在二价阳离子的情况下对冷冻至-196℃的叶绿体进行比较测量所得到的结果相当吻合。

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