Mechanism of the CO-sensing heme protein CooA: new insights from the truncated heme domain and UVRR spectroscopy

The bacterial CO-sensing heme protein CooA activates expression of genes whose products perform CO-metabolism by binding its target DNA in response to CO binding. The required conformational change has been proposed to result from CO-induced displacement of the heme and of the adjacent C-helix, which connects the sensory and DNA-binding domains. Support for this proposal comes from UV Resonance Raman (UVRR) spectroscopy, which reveals a more hydrophobic environment for the C-helix residue Trp110 when CO binds. In addition, we find a tyrosine UVRR response, which is attributable to weakening of a Tyr55-Glu83 H-bond that anchors the proximal side of the heme. Both Trp and Tyr responses are augmented in the heme domain when the DNA-binding domain has been removed, apparently reflecting loss of the inter-domain restraint. This augmentation is abolished by a Glu83Gln substitution, which weakens the anchoring H-bond. The CO recombination rate following photolysis of the CO adduct is similar for truncated and full-length protein, though truncation does increase the rate of CO association in the absence of photolysis; together these data indicate that truncation causes a faster dissociation of the endogenous Pro2 ligand. These findings are discussed in the light of structural evidence that the N-terminal tail, once released from the heme, selects the proper orientation of the DNA-binding domain, via docking interactions.     

Heme displacement mechanism of CooA activation: mutational and Raman spectroscopic evidence

The heme-containing protein CooA of Rhodospirillum rubrum regulates the expression of genes involved in CO oxidation. CooA binds its target DNA sequence in response to CO binding to its heme. Activity measurements and resonance Raman (RR) spectra are reported for CooA variants that bind DNA even in the absence of CO, those in which the wild-type residues at the 121-126 positions, TSCMRT, are replaced by the residues AYLLRL or RYLLRL, and also for variants that bind DNA poorly in the presence of CO, such as L120S and L120F. The Fe-C and C-O stretching resonance Raman (RR) frequencies of all CooAs examined deviate from the expected back-bonding correlation in a manner indicating weakening of the Fe-His-77 proximal ligand bond, and the extent of weakening correlates positively with DNA binding activity. The (A/R) YLLRL variants have detectable populations of a 5-coordinate heme resulting from partial dissociation of the endogenous distal ligand, Pro-2. Selective excitation of this population reveals downshifted Fe-His-77-stretching RR bands, confirming the proximal bond weakening. These results support our previous hypothesis that the conformational change required for DNA binding is initiated by displacement of the heme into an adjacent hydrophobic cavity once CO displaces the Pro-2 ligand. Examination of the crystal structure reveals a physical basis for these results, and a mechanism is proposed to link heme displacement to conformational change.     

Site-specific protein dynamics in communication pathway from sensor to signaling domain of oxygen sensor protein, HemAT-Bs: Time-resolved Ultraviolet Resonance Raman Study

HemAT-Bs is a heme-based signal transducer protein responsible for aerotaxis. Time-resolved ultraviolet resonance Raman (UVRR) studies of wild-type and Y70F mutant of the full-length HemAT-Bs and the truncated sensor domain were performed to determine the site-specific protein dynamics following carbon monoxide (CO) photodissociation. The UVRR spectra indicated two phases of intensity changes for Trp, Tyr, and Phe bands of both full-length and sensor domain proteins. The W16 and W3 Raman bands of Trp, the F8a band of Phe, and the Y8a band of Tyr increased in intensity at hundreds of nanoseconds after CO photodissociation, and this was followed by recovery in ～50 μs. These changes were assigned to Trp-132 (G-helix), Tyr-70 (B-helix), and Phe-69 (B-helix) and/or Phe-137 (G-helix), suggesting that the change in the heme structure drives the displacement of B- and G-helices. The UVRR difference spectra of the sensor domain displayed a positive peak for amide I in hundreds of nanoseconds after photolysis, which was followed by recovery in ～50 μs. This difference band was absent in the spectra of the full-length protein, suggesting that the isolated sensor domain undergoes conformational changes of the protein backbone upon CO photolysis and that the changes are restrained by the signaling domain. The time-resolved difference spectrum at 200 μs exhibited a pattern similar to that of the static (reduced - CO) difference spectrum, although the peak intensities were much weaker. Thus, the rearrangements of the protein moiety toward the equilibrium ligand-free structure occur in a time range of hundreds of microseconds.