Mackin H C, Tsubaki M, Yu N T
Biophys J. 1983 Mar;41(3):349-57. doi: 10.1016/S0006-3495(83)84446-4.
Strong evidence suggests that the stretching vibration of the bound oxygen can be perturbed by an accidentally degenerate porphyrin ring mode, resulting in two split frequencies. In the Co(II)(TpivPP) (pyridine) (18)O(2) complex, we demonstrate that the nu((18)O-(18)O) mode, after being shifted from its nu((16)O-(16)O) value at 1,156 cm(-1), undergoes a resonance interaction with the 1,080 cm(-1) porphyrin mode, giving rise to two lines at 1,067 and 1,089 cm(-1). In the O(2) complex of Co(II) mesoporphyrin IX-substituted sperm whale myoglobin, we observed a dramatic intensity increase at 1,132 cm(-1) upon (16)O(2) --> (18)O(2) substitution, which is due to the reappearance of the 1,132-cm(-1) porphyrin mode after the removal of resonance conditions. A decrease in O(2) binding affinity, caused by the proximal base tension, corresponds to an increase in the Co-O(2) stretching frequency. The nu(Co-O(2)) at 527 cm(-1) for the low affinity Co(II)(TpivPP)(1,2-Me(2)Im) O(2) complex is 11 cm(-1) higher than the 516-cm(-1) value for the high affinity complex (with N-MeIm replacing 1,2-Me(2)Im). However, in the corresponding iron complexes the reverse behavior is observed, i.e., the nu(Fe-O(2)) decreases for the (1,2-Me(2)Im) complex. There is a 24-cm(-1) difference in the Co-O(2) stretching frequencies between Co(II)(TpivPP)(N-MeIm)O(2) (at 516 cm(-1)) and oxy meso CoMb (at 540 cm(-1)), suggesting a protein induced distortion of the Co-O-O linkage. However, the values for nu(Fe-O(2)) are nearly identical between Fe(II)(TpivPP)(N-MeIm)O(2) (at 571 cm(-1)) and oxy Mb (at 573 cm(-1)), indicating that O(2) binds to myoglobin in the same manner as in the sterically unhindered "picket fence" complex. Evidence is presented that suggests the presence of two dioxygen stretching frequencies due to two different conformers in each of the N-MeIm and 1,2-Me(2)Im complex of oxy Co(II)(TpivPP).
有力证据表明,结合氧的伸缩振动会受到卟啉环模式意外简并的干扰,从而产生两个分裂频率。在Co(II)(TpivPP)(吡啶)(18)O(2)配合物中,我们证明,nu((18)O-(18)O)模式在从其1156 cm(-1)的nu((16)O-(16)O)值发生位移后,与1080 cm(-1)的卟啉模式发生共振相互作用,在1067和1089 cm(-1)处产生两条谱线。在Co(II)中卟啉IX取代的抹香鲸肌红蛋白的O(2)配合物中,我们观察到在(16)O(2)→(18)O(2)取代后,1132 cm(-1)处的强度急剧增加,这是由于共振条件消除后1132-cm(-1)的卟啉模式重新出现。由近端碱基张力引起的O(2)结合亲和力降低,对应于Co-O(2)伸缩频率的增加。低亲和力Co(II)(TpivPP)(1,2-Me(2)Im)O(2)配合物在527 cm(-1)处的nu(Co-O(2))比高亲和力配合物(用N-MeIm取代1,2-Me(2)Im)的516-cm(-1)值高11 cm(-1)。然而,在相应的铁配合物中观察到相反的行为,即(1,2-Me(2)Im)配合物的nu(Fe-O(2))降低。Co(II)(TpivPP)(N-MeIm)O(2)(516 cm(-1))和氧合中CoMb(540 cm(-1))之间的Co-O(2)伸缩频率存在24-cm(-1)的差异,表明蛋白质诱导了Co-O-O键的扭曲。然而,Fe(II)(TpivPP)(N-MeIm)O(2)(571 cm(-1))和氧合Mb(573 cm(-1))之间的nu(Fe-O(2))值几乎相同,表明O(2)与肌红蛋白的结合方式与空间位阻较小的“栅栏”配合物相同,并给出证据表明,在氧合Co(II)(TpivPP)的N-MeIm和1,2-Me(2)Im配合物中,由于两种不同的构象体,存在两个双氧伸缩频率。