Time-resolved Optical Rotatory Dispersion Research Articles

PH Dependence of the Photoactive Yellow Protein Photocycle Recovery Reaction Reveals a New Late Photocycle Intermediate with a Deprotonated Chromophore

The recovery reaction of the signaling state of photoactive yellow protein includes the following: (i) deprotonation of the p-coumaryl chromophore, (ii) refolding of the protein, and (iii) chromophore re-isomerization from the cis to the trans configuration. Through analysis of the pH dependence of this recovery reaction, we were able to provide proof for the existence of an additional photocycle intermediate. The spectral similarity between this new intermediate and the dark state indicates that the new intermediate has a deprotonated chromophore, which may facilitate chromophore re-isomerization. This spectral similarity also explains why this new intermediate has not been noticed in earlier studies. For our data analysis we introduce a photocycle model that takes into account the effect of the specific light regime selected, a model that was also used for simulations.

Non-Native Heme−Histidine Ligation Promotes Microsecond Time Scale Secondary Structure Formation in Reduced Horse Heart Cytochromec

Previous far-UV time-resolved optical rotatory dispersion (TRORD) studies of the sub-millisecond (burst) phase of secondary structure formation in horse and tuna cytochromes c after photoreduction in denaturant suggested that the non-native His18-Fe-His33 heme ligation dominant in the unfolded horse protein facilitated this fast folding better than did the His18-Fe-His26 coordination dominant in tuna [Chen, E., Goldbeck, R.A., and Kliger, D.S. (2003) J. Phys. Chem. A 107, 8149-8155; Chen, E., Goldbeck, R.A., and Kliger, D.S. (2004) J. Am. Chem. Soc. 126, 11175-11181]. Whether His18-Fe-His33 coordination actually facilitates fast secondary structure formation or just slows folding less than His18-Fe-His26 coordination is probed by examining the double histidine mutant H26QH33N of horse heart cytochrome c. The fast folding phase is absent in H26QH33N, indicating that His18-Fe-His33 misligation does promote fast secondary structure formation, as does His18-Fe-His26 to a lesser extent. His33 may be better able to facilitate folding because it is not as constrained by hydrogen bonding interactions in the denatured state as is His26. A greater flexibility, not only because of weakened or disrupted Van der Waals interactions in the presence of guanidine hydrochloride (GuHCl) but also because of its position relative to His18, may allow His33 to ligate to the heme group more easily than His26. These results are discussed along with the results of far-UV CD and Soret and visible region MCD measurements, which were performed to probe heme ligation in H26QH33N and to understand how GuHCl affects its folding stability and cooperativity.

A LOV Story: The Signaling State of the Phot1 LOV2 Photocycle Involves Chromophore-Triggered Protein Structure Relaxation, As Probed by Far-UV Time-Resolved Optical Rotatory Dispersion Spectroscopy

Light-, oxygen-, or voltage-regulated (LOV1 and LOV2) domains bind flavin mononucleotide (FMN) and activate the phototropism photoreceptors phototropin 1 (phot1) and phototropin 2 (phot2) by using energy from absorbed blue light. Upon absorption of blue light, chromophore and protein conformational changes trigger the kinase domain for subsequent autophosphorylation and presumed downstream signal transduction. To date, the light-induced photocycle of the phot1 LOV2 protein is known to involve formation of a triplet flavin mononucleotide (FMN) chromophore followed by the appearance of a FMN adduct within 4 micros [Swartz, T. E., Corchnoy, S. B., Christie, J. M., Lewis, J. W., Szundi, I., Briggs, W. R., and Bogomolni, R. A. (2001) J. Biol. Chem. 276, 36493-36500] before thermal decay back to the dark state. To probe the mechanism by which the blue light information is relayed from the chromophore to the protein, nanosecond time-resolved optical rotatory dispersion (TRORD) spectroscopy, which is a direct probe of global secondary structure, was used to study the phot1 LOV2 protein in the far-UV region. These TRORD experiments reveal a previously unobserved intermediate species (tau approximately 90 micros) that is characterized by a FMN adduct chromophore and partially unfolded secondary structure (LOV390(S2)). This intermediate appears shortly after the formation of the FMN adduct. For LOV2, formation of a long-lived species that is ready to interact with a receptor domain for downstream signaling is much faster by comparison with formation of a similar species in other light-sensing proteins.

Nanosecond laser temperature-jump optical rotatory dispersion: Application to early events in protein folding/unfolding

Nanosecond time-resolved optical rotatory dispersion (TRORD) techniques are coupled with laser temperature-jump (T-jump) triggering in an instrument that measures ultrafast protein folding-unfolding dynamics with high specificity to secondary structure. Far-ultraviolet (UV) ORD can be measured with this instrument over a wide wavelength range at times as early as 35 ns after a 3 ns laser T-jump pulse. The fundamental of a Nd:YAG laser is passed through a D2-filled Raman shifter to generate a pulse of 1.5μm infrared (IR) light that is efficiently absorbed by water. The resulting T-jump is stable for at least 1 ms before decaying back to the starting temperature with a time constant of ∼30ms. The ability to measure entire TRORD band shapes during this temporal window makes it possible to distinguish between changes in the signal due to a genuine unfolding or refolding process and changes due to artifacts. The technique, applicable to a wide variety of proteins, is demonstrated here in submillisecond unfolding studies of RNAse A and cytochrome c.

The earliest events in protein folding: a structural requirement for ultrafast folding in cytochrome C.

The folding dynamics of reduced cytochrome c (redcyt c) obtained from tuna heart, which contains a tryptophan residue at the site occupied by His33 in horse heart cytochrome c, was studied using nanosecond time-resolved optical rotatory dispersion spectroscopy. As observed previously for horse heart redcyt c, two time regimes were observed for secondary structure formation in tuna redcyt c: a fast (microseconds) and a slow (milliseconds) phase. However, the fast phase of tuna redcyt c folding was much slower and smaller in amplitude than the same phase in horse. The differences in the fast folding phases suggest that for horse heart redcyt c, the conformers that undergo the fastest observed folding have the His18-Fe-His33 heme configuration, which appears to be necessary, but not sufficient, to poise an unfolded chain conformation for fastest folding in redcyt c.

The kinetics of helix unfolding of an azobenzene cross-linked peptide probed by nanosecond time-resolved optical rotatory dispersion.

The unfolding dynamics of a 16 amino acid peptide (Ac-EACAREAAAREAACRQ-NH(2), FK-11-X) was followed using nanosecond time-resolved optical rotatory dispersion (ORD). The peptide was coupled to an azobenzene linker that undergoes subnanosecond photoisomerization and reisomerizes on a time scale of minutes. When the linker is in the trans form, the peptide favors a more helical structure (66% helix/34% disordered) and when in the cis configuration the helical content is reduced. Unfolding of FK-11-X was rapidly triggered by a 7-ns laser pulse at 355 nm, forming cis azobenzene-linked peptides that maintained the secondary structure (helical or disordered) of their trans azobenzene counterparts. The incompatibility of the instantaneous cis photoproduct with helical secondary structure drives the subsequent peptide unfolding to a new conformational equilibrium between cis helix and cis disordered structures. The kinetic results show a approximately 40% decrease in the time-dependent ORD signal at 230 nm that is best fit to a single-exponential decay with a time constant of 55 +/- 6 ns. Folding and unfolding rates for cis FK-11-X are estimated to be approximately 3.0 x 10(6) s(-)(1) (1/330 ns) and approximately 1.5 x 10(7) s(-)(1) (1/66 ns), respectively.

Dynamics of protein and chromophore structural changes in the photocycle of photoactive yellow protein monitored by time-resolved optical rotatory dispersion.

The dynamics of the PYP photocycle have been studied using time-resolved optical rotatory dispersion (TRORD) spectroscopy in the visible and far-UV spectral regions to probe the changes in the chromophore configuration and the protein secondary structure, respectively. The changes in the secondary structure in PYP upon photoisomerization of the chromophore can be described by two exponential lifetimes of 2 +/- 0.8 and 650 +/- 100 ms that correspond to unfolding and refolding processes, respectively. The TRORD experiments that follow the dynamics of the chromophore report three exponential components, with lifetimes of 10 +/- 3 micros, 1.5 +/- 0.5 ms, and 515 +/- 110 ms. A comparison of the kinetic behaviors of the chromophore and protein shows that during the decay of pR(465) an initial relaxation that is localized to the chromophore hydrophobic pocket precedes the formation of the chromophore and protein structures found in pB(355). In contrast, the protein and chromophore processes occur with similar time constants during inactivation of the signaling state.

Nanosecond optical rotatory dispersion spectroscopy: application to photolyzed hemoglobin-CO kinetics

A standard technique for static optical rotatory dispersion (ORD) measurements is adapted to the measurement of ORD changes on a nanosecond (ns) time scale, giving approximately a million-fold improvement in time-resolution over conventional instrumentation. The technique described here is similar in principle to a technique recently developed for ns time-resolved circular dichroism (TRCD) spectroscopy, although the time-resolved optical rotatory dispersion (TRORD) technique requires fewer optical components. As with static ORD, TRORD measurements may be interpreted by empirical comparisons or may be transformed, via the Kramers-Kronig relations, to more easily interpreted TRCD spectra. TRORD can offer experimental advantages over TRCD in studying kinetic processes effecting changes in the chiral structures of biological molecules. In particular, the wider dispersion of ORD bands compared with the corresponding CD bands means that ORD information may often be obtained outside of absorption bands, a signal-to-noise advantage for multichannel measurements. Demonstration of the technique by its application to ns TRORD and the transform-calculated TRCD of carboxy-hemoglobin (Hb-CO) after laser photolysis is presented.