Department of Physiology and Biophysics, University of California, Irvine, Irvine, California 92697, USA.
J Phys Chem B. 2009 Dec 31;113(52):16643-53. doi: 10.1021/jp907393m.
Time-resolved measurements were performed on wild-type bacteriorhodopsin with an optical multichannel analyzer in the spectral range 350-735 nm, from 100 ns to the photocycle completion, at four temperatures in the 5-30 degrees C range. The intent was to examine the possibility of two K-like bathochromic intermediates and to obtain their spectra and kinetics in the visible. The existence of a second K-like intermediate, termed KL, had been postulated (Shichida et al., Biochim. Biophys. Acta 1983, 723, 240-246) to reconcile inconsistencies in data in the pico- and microsecond time domains. However, introduction of KL led to a controversy, since neither its visible spectrum nor its kinetics could be confirmed. Infrared data (Dioumaev and Braiman, J. Phys. Chem. B 1997, 101, 1655-1662) revealed a state which might have been considered a homologue to KL, but it had a kinetic pattern different from that of the earlier proposed KL. Here, we characterize two distinct K-like intermediates, K(E) ("early") and K(L) ("late"), by their spectra and kinetics in the visible as revealed by global kinetic analysis. The K(E)-to-K(L) transition has a time constant of approximately 250 ns at 20 degrees C, and describes a shift from K(E) with lambda(max) at approximately 600 nm and extinction of approximately 56,000 M(-1) x cm(-1) to K(L) with lambda(max) at approximately 590 nm and extinction of approximately 50,000 M(-1) x cm(-1). The temperature dependence of this transition is characterized by an enthalpy of activation of DeltaH(++) approximately 40 kJ/mol and a positive entropy of activation of DeltaS(++)/R approximately 4. The consequences of multiple K-like states for interpreting the spectral evolution in the early stages of the photocycle are discussed.
对野生型细菌视紫红质进行了时间分辨测量,使用光学多通道分析仪在 350-735nm 的光谱范围内,从 100ns 到光循环完成,在 5-30°C 的四个温度下进行。目的是检查是否存在两个 K 样的远红增色中间态,并获得它们在可见光谱中的光谱和动力学特性。第二个 K 样中间态 KL 的存在(Shichida 等人,生物化学。生物物理学学报 1983, 723, 240-246)是为了解决皮秒和微秒时间域数据中的不一致性。然而,KL 的引入引起了争议,因为既无法证实其可见光谱,也无法证实其动力学特性。红外数据(Dioumaev 和 Braiman,J. Phys. Chem. B 1997, 101, 1655-1662)显示了一个可能被认为与 KL 同源的状态,但它的动力学模式与之前提出的 KL 不同。在这里,我们通过全局动力学分析,用可见光谱和动力学特性来描述两个不同的 K 样中间态 K(E)(“早期”)和 K(L)(“晚期”)。在 20°C 时,K(E)-到-K(L)的转变时间常数约为 250ns,描述了从 K(E)向 K(L)的转变,K(E)的最大吸收波长约为 600nm,消光系数约为 56,000M(-1)xcm(-1),K(L)的最大吸收波长约为 590nm,消光系数约为 50,000M(-1)xcm(-1)。这个转变的温度依赖性的特点是活化焓ΔH(++)约为 40kJ/mol,活化熵ΔS(++)/R 约为正 4。讨论了多个 K 样态对解释光循环早期阶段光谱演化的影响。