For the first time, Fourier transform infrared spectroscopy has been applied to cytochrome P-450 to analyze the protein secondary structure. From Fourier self-deconvolution and fitting the infrared spectra in the amide I' region (1600-1700 cm-1), we estimate 44% alpha-helix, 31% beta-sheet, and 18% turns for substrate-free cytochrome P-450cam. In the presence of camphor, 54% alpha-helix and 310-helix, 21% beta-sheet, and 21% turns are obtained which agree with the crystallographic data of 53% alpha-helix, 19% beta-sheet, and 16% turns [Poulos, T. L., Finzel, B. C., & Howard, A. J. (1987) J. Mol. Biol. 195, 687-700]. Cytochrome P-420cam is produced from substrate-free cytochrome P-450cam in two ways(i) by temperature elevation up to 60 degrees C and (ii) by exposure to KSCN up to 1.5 M. The secondary structure composition is determined for each temperature and KSCN concentration and compared with the changes observed in the iron ligand CO stretch vibration bands appearing between 1900 and 2000 cm-1. Thermally induced cytochrome P-420 has an alpha-helix content of 19%, a beta-sheet content of 53%, 14% turns, and 5% antiparallel beta-sheets from intermolecular hydrogen bonds within protein aggregates. The formation of cytochrome P-420 as a function of the KSCN concentration indicates two types of cytochrome P-420. Up to 1 M KSCN, the induced cytochrome P-420 displays only little modification of the secondary structure, whereas at 1.5 M KSCN, larger changes are observed, resulting in 85% cytochrome P-420 without protein precipitation and containing 30% alpha-helix, 48% beta-sheet, and 17% turns. Infrared spectra in the iron ligand CO stretch region show several subconformers for cytochrome P-420. During the cytochrome P-420 formation, the CO stretch modes are shifted to higher frequencies by 3-11 cm-1, with a main feature at about 1964 cm-1, compared to those of substrate-free cytochrome P-450cam-CO.

译文

首次将傅里叶变换红外光谱应用于细胞色素P-450,以分析蛋白质的二级结构。通过傅立叶自反卷积并拟合酰胺I' 区域 (1600-1700厘米-1) 中的红外光谱,我们估计了44% 无底物细胞色素P-450cam的 α-螺旋,31% β-折叠和18% 匝。在樟脑存在的情况下,获得了54% α-螺旋和310-螺旋,21% β-折叠和21% 匝,它们与53% α-螺旋,19% β-折叠和16% 匝的晶体学数据一致 [Poulos,T. L.,Finzel,b.c.,& Howard,A. J. (1987) J. Mol. Biol. 195,687-700]。细胞色素P-420cam以两种方式从无底物的细胞色素P-450cam产生 (i) 通过温度升高高达60 ℃ 和 (ii) 通过暴露于KSCN高达1.5 M。确定每种温度和KSCN浓度的二级结构组成,并将其与在出现1900年和2000厘米-1的铁配体CO拉伸振动带中观察到的变化进行比较。热诱导的细胞色素P-420具有19% 的 α-螺旋含量,53% 的 β-折叠含量,14% 转弯,以及来自蛋白质聚集体内的分子间氢键的5% 反平行 β-折叠。作为KSCN浓度的函数的细胞色素P-420的形成表明两种类型的细胞色素P-420。直到1 M KSCN,诱导的细胞色素P-420仅显示出很少的二级结构修饰,而在1.5 M KSCN处,观察到较大的变化,导致85% 的细胞色素P-420没有蛋白沉淀,并且含有30% 的 α-螺旋,48% 的 β-折叠和17% 转。铁配体CO拉伸区的红外光谱显示了几种用于细胞色素P-420的亚构象体。在细胞色素P-420形成过程中,与无底物细胞色素P-450cam-CO相比,CO拉伸模式向更高频率转移3-11厘米-1,主要特征约为1964厘米-1。

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