Identification of conformational substates involved in nitric oxide binding to ferric and ferrous myoglobin through difference Fourier transform infrared spectroscopy (FTIR)

Hemeproteins play an important role in the signaling processes mediated by nitric oxide (NO), For example, the production of NO by nitric oxide synthase, the activation of guanylate cyclase by binding NO, and the scavenging of NO by hemoglobin, myoglobin, and cytochrome c oxidase all occur through unique mechanisms of interaction between NO and hemeproteins. Unlike carbon monoxide (GO) and oxygen (O-2), which have been studied extensively, the reactions of NO with ferric and ferrous hemeproteins are not as well characterized, In this work, NO binding to myoglobin is studied using cryogenic optical spectroscopy and Fourier transform infrared spectroscopy (FTIR) in order to characterize the ligand-bound and photoproduct states involved in the interaction of NO with the heme iron and the distal pocket of the protein. For ferrous nitrosyl myoglobin (Mb(II)NO), optical spectroscopy is used to show that the ligand-bound state can be converted to >95% stable photoproduct below 10 K. The Soret peak of the photoproduct is red-shifted by 4 nm relative to deoxy-myoglobin (Mb), similar to previous results for carbonmonoxy-(MbCO) and oxy-myoglobin (MbO(2)) (Miller et al., 1996). Mb(II)NO completely rebinds by 35 K, indicating that the rebinding barrier for NO is lower than MbCO, consistent with room temperature picosecond kinetic measurements. For ferric nitrosyl myoglobin (Mb(III)NO), we find that the photoproduct yield at cryogenic temperatures is less than unity and dependent on the distal pocket residue. Native Mb(III)NO has a lower photoproduct yield than the mutant, Mb(III)(H64L)NO, where the distal histidine is replaced by leucine. The rebinding rates for the native and mutant species are similar to each other and to Mb(II)NO. By using FTIR difference spectroscopy (photolyzed/unphotolyzed) of isotopically labeled ferrous nitrosyl myoglobin (Mb(II)NO), the NO stretching frequencies in both the ligand-bound states and photoproduct states are determined. Two ligand-bound conformational states (1607 and 1613 cm(-1)) and two photoproduct conformational states (1852 and 1857 cm(-1)) are observed for Mb(II)NO. This is the first direct observation of photolyzed NO in the distal pocket of myoglobin. The ligand-bound frequencies are consistent with a bent Mb(II)NO moiety, where the unpaired pi*(NO) electron remains localized on NO, causing v(N-O) to be similar to 300 cm(-1) lower than Mb(III)NO. Similar to MbO(2) we suggest that N-epsilon of the distal histidine is protonated, forming a hydrogen bond to the NO Ligand. For native Mb(III)NO, a single ligand-bound conformational state with respect to v(N-O) is observed at 1927 cm(-1). This frequency decreases to 1904 cm(-1) for the mutant, Mb(III)(H64L)NO, contrary to the increase of the carbon monoxide (CO) stretching frequency in the isoelectronic Mb(II)(H64L)CO mutant versus native MbCO, For linear Mb(III)NO, we suggest that backbonding from the unpaired pi*(NO) electron to iron results in an increased positive charge on the NO ligand, Fe(delta-)-NO(delta+). This can be facilitated by tautomerism of the distal histidine, leaving N-epsilon of the imidazole ring unprotonated and able to accept positive charge from the Fe(delta-)-NO(delta+) moiety, resulting in a higher bond order (and a 23 cm(-1) shift to higher frequency) for native Mb(III)NO versus Mb(III)(H64L)NO, where this interaction is absent. These different interactions between the distal histidine and the ferrous versus ferric species illustrate potential ways the protein can stabilize the bound ligand and demonstrate the versatile nature by which NO can bind to hemeproteins.