On the involvement of single-bond rotation in the primary photochemistry of photoactive yellow protein

Prior experimental observations, as well as theoretical considerations, have led to the proposal that C₄-C₇ single-bond rotation may play an important role in the primary photochemistry of photoactive yellow protein (PYP). We therefore synthesized an analog of this protein's 4-hydroxy-cinnamic acid chromophore, (5-hydroxy indan-(1E)-ylidene)acetic acid, in which rotation across the C₄-C₇ single bond has been locked with an ethane bridge, and we reconstituted the apo form of the wild-type protein and its R52A derivative with this chromophore analog. In PYP reconstituted with the rotation-locked chromophore, 1), absorption spectra of ground and intermediate states are slightly blue-shifted; 2), the quantum yield of photochemistry is ∼60% reduced; 3), the excited-state dynamics of the chromophore are accelerated; and 4), dynamics of the thermal recovery reaction of the protein are accelerated. A significant finding was that the yield of the transient ground-state intermediate in the early phase of the photocycle was considerably higher in the rotation-locked samples than in the corresponding samples reconstituted with p-coumaric acid. In contrast to theoretical predictions, the initial photocycle dynamics of PYP were observed to be not affected by the charge of the amino acid residue at position 52, which was varied by 1), varying the pH of the sample between 5 and 10; and 2), site-directed mutagenesis to construct R52A. These results imply that C₄-C₇ single-bond rotation in PYP is not an alternative to C₇=C₈ double-bond rotation, in case the nearby positive charge of R52 is absent, but rather facilitates, presumably with a compensatory movement, the physiological Z/E isomerization of the blue-light-absorbing chromophore.     

Salinibacter sensory rhodopsin: sensory rhodopsin I-like protein from a eubacterium

Halobacterium salinarum sensory rhodopsin I (HsSRI), a dual receptor regulating both negative and positive phototaxis in haloarchaea, transmits light signals through changes in protein-protein interactions with its transducer, halobacterial transducer protein I (HtrI). Haloarchaea also have another sensor pigment, sensory rhodopsin II (SRII), which functions as a receptor regulating negative phototaxis. Compared with HsSRI, the signal relay mechanism of SRII is well characterized because SRII from Natronomonus pharaonis (NpSRII) is much more stable than HsSRI and HsSRII, especially in dilute salt solutions and is much more resistant to detergents. Two genes encoding SRI homologs were identified from the genome sequence of the eubacterium Salinibacter ruber. Those sequences are distantly related to HsSRI ( approximately 40% identity) and contain most of the amino acid residues identified as necessary for its function. To determine whether those genes encode functional protein(s), we cloned and expressed them in Escherichia coli. One of them (SrSRI) was expressed well as a recombinant protein having all-trans retinal as a chromophore. UV-Vis, low-temperature UV-Vis, pH-titration, and flash photolysis experiments revealed that the photochemical properties of SrSRI are similar to those of HsSRI. In addition to the expression system, the high stability of SrSRI makes it possible to prepare large amounts of protein and enables studies of mutant proteins that will allow new approaches to investigate the photosignaling process of SRI-HtrI.     

Spectroscopic characterization of the photocycle intermediates of photoactive yellow protein.

The absorption spectra of photocycle intermediates of photoactive yellow protein mutants were compared with those of the corresponding intermediates of wild type to probe which amino acid residues interact with the chromophore in the intermediate states. B and H intermediates were produced by irradiation and trapped at 80 K, and L intermediates at 193 K. The absorption spectra of these intermediates produced from R52Q were identical to those from wild type, whereas those from E46Q and T50V were 7-15 nm red-shifted as those in the dark states. The absorption spectra of M intermediates were measured by flash photolysis at room temperature. Those of Y42F, T50V, and R52Q were identical to that of wild type, whereas that of E46Q was 11 nm red-shifted. Assuming that the intermediates of mutants have a structure comparable to that of wild type, these findings suggest the following: Glu46 interacts with the chromophore throughout the photocycle, interaction between the chromophore and Thr50 as well as Tyr42 is lost upon the formation of M intermediate, and Arg52 never interacts with the chromophore directly. The hydrogen-bonding network around the phenolic oxygen of the chromophore would be thus maintained until L intermediate decays, and the global conformational change would take place by the loss of the hydrogen bond between the chromophore and Tyr42. This model conflicts with some of the results of previous crystallographic studies, suggesting that the reaction mechanism in the crystal may be different from that in solution.     

Light induces destabilization of photoactive yellow protein

To understand the effect of visible light on the stability of photoactive yellow protein (PYP), urea denaturation experiments were performed with PYP in the dark and with PYP(M) under continuous illumination. The urea concentrations at the midpoint of denaturation were 5.26 +/- 0.29 and 3.77 +/- 0.19 M for PYP and PYP(M), respectively, in 100 mM acetate buffer, and 5.26 +/- 0.24 and 4.11 +/- 0.12 M for PYP and PYP(M), respectively, in 100 mM citrate buffer. The free energy change upon denaturation (DeltaG(D)(H2O)), obtained from the denaturation curve, was 11.0 +/- 0.4 and 7.6 +/- 0.2 kcal/mol for PYP and PYP(M), respectively, in acetate buffer, and 11.5 +/- 0.3 and 7.8 +/- 0.1 kcal/mol for PYP and PYP(M), respectively, in citrate buffer. Even though the DeltaG(D)(H2O) value for PYP(M) is almost identical in the two buffer systems, the urea concentration at the midpoint of denaturation is lower in acetate buffer than in citrate buffer. Although their CD spectra indicate that the protein conformations of the denatured states of PYP and PYP(M) are indistinguishable, the configurations of the chromophores in their denatured structures are not necessarily identical. Both denatured states are interconvertible through PYP and PYP(M). Therefore, the free energy difference between PYP and PYP(M) is 3.4-3.7 kcal/mol for the protein moiety, plus the additional contribution from the difference in configuration of the chromophore.     

Mimic of photocycle by a protein folding reaction in photoactive yellow protein

The blue light receptor photoactive yellow protein (PYP) displays rhodopsin-like photochemistry based on the trans to cis photoisomerization of its p-coumaric acid chromophore. Here, we report that protein refolding from the acid-denatured state of PYP mimics the last photocycle transition in PYP. This implies a direct link between transient protein unfolding and photosensory signal transduction. We utilize this link to study general issues in protein folding. Chromophore trans to cis photoisomerization in the acid-denatured state strongly decelerates refolding, and converts the pH dependence of the barrier for refolding from linear to nonlinear. We propose transition state movement to explain this phenomenon. The cis chromophore significantly stabilizes the acid-denatured state, but acidification of PYP results in the accumulation of the acid-denatured state containing a trans chromophore. This provides a clear example of kinetic control in a protein unfolding reaction. These results demonstrate the power of PYP as a light-triggered model system to study protein folding.     

Photoactive yellow protein, bacteriophytochrome, and sensory rhodopsin in purple phototrophic bacteria.

The purple photosynthetic bacteria contain a large variety of sensory and regulatory proteins, and those responding to light are among the most interesting. These currently include bacteriophytochrome (Bph), sensory rhodopsin (SR), and photoactive yellow protein (PYP), which all appear to function as light sensors. We herein interpret new findings within the context of current knowledge. For greater detail, the reader is referred to comprehensive reviews on these topics. Of the three proteins, only PYP has been well-characterized in terms of structure and physical-chemical properties in the purple bacteria, although none have well-defined functions. New findings include a cluster of six genes in the Thermochromatium tepidum genome that encodes presumed sensory rhodopsin and phototaxis proteins. T. tepidum also has a gene for PYP fused to bacteriophytochrome and diguanylate cyclase domains. The genes for PYP and its biosynthetic enzymes are associated with those for gas vesicle formation in Rhodobacter species, suggesting that one function of PYP is to regulate cell buoyancy. The association of bacteriophytochrome genes with those for reaction centers and light-harvesting proteins in Rhodopseudomonas palustris suggests that the photosynthetic antenna as well as the reaction center are regulated by Bphs. Furthermore, Rc. centenum PPR is reversibly photobleached at 702 nm rather than red-shifted as in other phytochromes, suggesting that PPR senses the intensity of white light rather than light quality. PYP from Halorhodospira(aka Ectothiorhodospira)halophila is of special interest because it has become the structural prototype for the PAS domain, a motif that is found throughout the phylogenetic tree and which plays important roles in many signaling pathways. Thus, the structural and photochemical characterization of PYP, utilizing site-directed mutagenesis, provides insights into the mechanism of signal transduction.     

Attempt to simplify the amino-acid sequence of photoactive yellow protein with a set of simple rules

To understand the information encoded in an amino-acid sequence, the authors have attempted to simplify the amino-acid sequence of photoactive yellow protein (PYP) with a set of simple rules. The rules are designed to reduce overlapping structural information. The simplified PYP protein, which was composed of only nine species of amino acids (Ser, Val, Asp, Lys, Phe, Met, Gly, Pro, and Cys), took a completely different structure than the native conformation. Even after the evolutionarily conserved residues were restored in the simplified protein, the PYP variant did not properly fold, indicating that the information encoded in the conserved residues is insufficient for the structure formation. Additional restorations of the substituted hydrophilic or hydrophobic residues did not lead to a variant that formed the native structure. The structural properties of these variants and the wild-type protein in aqueous solution differed. Partial simplification was successfully performed by creating chimeric proteins composed of combinations of wild-type PYP and sPYPIII. The structural characterization of each chimeric protein indicates that the important information on the structure formation is encoded in the beta-scaffold region.     

Properties of a water-soluble, yellow protein isolated from a halophilic phototrophic bacterium that has photochemical activity analogous to sensory rhodopsin

A water-soluble yellow protein, previously discovered in the purple photosynthetic bacterium Ectothiorhodospira halophila, contains a chromophore which has an absorbance maximum at 446 nm. The protein is now shown to be photoactive. A pulse of 445-nm laser light caused the 446-nm peak to be partially bleached and red-shifted in a time less than 1 microsecond. The intermediate thus formed was subsequently further bleached in the dark in a biphasic process occurring in approximately 20 ms. Finally, the absorbance of native protein was restored in a first-order process occurring over several seconds. These kinetic processes are remarkably similar to those of sensory rhodopsin from Halobacterium, and to a lesser extent bacteriorhodopsin and halorhodopsin; although these proteins are membrane-bound, they have absorbance maxima at about 570 nm, and they cycle more rapidly. In attempts to remove the chromophore for identification, it was found that a variety of methods of denaturation of the protein caused transient or permanent conversion to a form which has an absorbance maximum near 340 nm. Thus, by analogy to the rhodopsins, the absorption at 446 nm in the native protein appears to result from a 106-nm red shift of the chromophore induced by the protein. Acid denaturation followed by extraction with organic solvents established that the chromophore could be removed from the protein. It is not identical with all-trans-retinal and remains to be identified, although it could still be a related pigment. The E. halophila yellow protein has a circular dichroism spectrum which indicates little alpha-helical secondary structure (19%).(ABSTRACT TRUNCATED AT 250 WORDS)     

Predicting the signaling state of photoactive yellow protein

As a bacterial blue light sensor the photoactive yellow protein (PYP) undergoes conformational changes upon signal transduction. The absorption of a photon triggers a series of events that are initially localized around the protein chromophore, extends to encompass the whole protein within microseconds, and leads to the formation of the transient pB signaling state. We study the formation of this signaling state pB by molecular simulation and predict its solution structure. Conventional straightforward molecular dynamics is not able to address this formation process due to the long (microsecond) timescales involved, which are (partially) caused by the presence of free energy barriers between the metastable states. To overcome these barriers, we employed the parallel tempering (or replica exchange) method, thus enabling us to predict qualitatively the formation of the PYP signaling state pB. In contrast to the receptor state pG of PYP, the characteristics of this predicted pB structure include a wide open chromophore-binding pocket, with the chromophore and Glu(46) fully solvent-exposed. In addition, loss of alpha-helical structure occurs, caused by the opening motion of the chromophore-binding pocket and the disruptive interaction of the negatively charged Glu(46) with the backbone atoms in the hydrophobic core of the N-terminal cap. Recent NMR experiments agree very well with these predictions.     

Methyl-accepting protein associated with bacterial sensory rhodopsin I.

In vivo radiolabeling of Halobacterium halobium phototaxis mutants and revertants with L-[methyl-3H] methionine implicated seven methyl-accepting protein bands with apparent molecular masses from 65 to 150 kilodaltons (kDa) in adaptation of the organism to chemo and photo stimuli, and one of these (94 kDa) was specifically implicated in phototaxis. The lability of the radiolabeled bands to mild base treatment indicated that the methyl linkages are carboxylmethylesters, as is the case in the eubacterial chemotaxis receptor-transducers. The 94-kDa protein was present in increased amounts in an overproducer of the apoprotein of sensory rhodopsin I, one of two retinal-containing phototaxis receptors in H. halobium. It was absent in a strain that contained sensory rhodopsin II and that lacked sensory rhodopsin I and was also absent in a mutant that lacked both photoreceptors. Based on the role of methyl-accepting proteins in chemotaxis in other bacteria, we suggest that the 94-kDa protein is the signal transducer for sensory rhodopsin I. By [3H]retinal labeling studies, we previously identified a 25-kDa retinal-binding polypeptide that was derived from photochemically reactive sensory rhodopsin I. When H. halobium membranes containing sensory rhodopsin I were treated by a procedure that stably reduced [3H]retinal onto the 25-kDa apoprotein, a 94-kDa protein was also found to be radiolabeled. Protease digestion confirmed that the 94-kDa retinal-labeled protein was the same as the methyl-accepting protein that was suggested above to be the signal transducer for sensory rhodopsin I. Possible models are that the 25- and 94-kDa proteins are tightly interacting components of the photosensory signaling machinery or that both are forms of sensory rhodopsin I.     

Low-temperature Fourier transform infrared spectroscopy of photoactive yellow protein

The photocycle intermediates of photoactive yellow protein (PYP) were characterized by low-temperature Fourier transform infrared spectroscopy. The difference FTIR spectra of PYP(B), PYP(H), PYP(L), and PYP(M) minus PYP were measured under the irradiation condition determined by UV-visible spectroscopy. Although the chromophore bands of PYP(B) were weak, intense sharp bands complementary to the 1163-cm(-1) band of PYP, which show the chromophore is deprotonated, were observed at 1168-1169 cm(-1) for PYP(H) and PYP(L), indicating that the proton at Glu46 is not transferred before formation of PYP(M). Free trans-p-coumaric acid had a 1294-cm(-1) band, which was shifted to 1288 cm(-1) in the cis form. All the difference FTIR spectra obtained had the pair of bands corresponding to them, indicating that all the intermediates have the chromophore in the cis configuration. The characteristic vibrational modes at 1020-960 cm(-1) distinguished the intermediates. Because these modes were shifted by deuterium-labeling at the ethylene bond of the chromophore while labeling at the phenol part had no effect, they were attributed to the ethylene bond region. Hence, structural differences among the intermediates are present in this region. Bands at about 1730 cm(-1), which show that Glu46 is protonated, were observed for all intermediates except for PYP(M). Because the frequency of this mode was constant in PYP(B), PYP(H), and PYP(L), the environment of Glu46 is conserved in these intermediates. The photocycle of PYP would therefore proceed by changing the structure of the twisted ethylene bond of the chromophore.     

Absorption spectra of photoactive yellow protein chromophores in vacuum

The absorption spectra of two photoactive yellow protein model chromophores have been measured in vacuum using an electrostatic ion storage ring. The absorption spectrum of the isolated chromophore is an important reference for deducing the influence of the protein environment on the electronic energy levels of the chromophore and separating the intrinsic properties of the chromophore from properties induced by the protein environment. In vacuum the deprotonated trans-thiophenyl-p-coumarate model chromophore has an absorption maximum at 460 nm, whereas the photoactive yellow protein absorbs maximally at 446 nm. The protein environment thus only slightly blue-shifts the absorption. In contrast, the absorption of the model chromophore in aqueous solution is significantly blue-shifted (lambda(max) = 395 nm). A deprotonated trans-p-coumaric acid has also been studied to elucidate the effect of thioester formation and phenol deprotonation. The sum of these two changes on the chromophore induces a red shift both in vacuum and in aqueous solution.     

Initial events in the photocycle of photoactive yellow protein

The light-induced isomerization of a double bond is the key event that allows the conversion of light energy into a structural change in photoactive proteins for many light-mediated biological processes, such as vision, photosynthesis, photomorphogenesis, and photo movement. Cofactors such as retinals, linear tetrapyrroles, and 4-hydroxy-cinnamic acid have been selected by nature that provide the essential double bond to transduce the light signal into a conformational change and eventually, a physiological response. Here we report the first events after light excitation of the latter chromophore, containing a single ethylene double bond, in a low temperature crystallographic study of the photoactive yellow protein. We measured experimental phases to overcome possible model bias, corrected for minimized radiation damage, and measured absorption spectra of crystals to analyze the photoproducts formed. The data show a mechanism for the light activation of photoactive yellow protein, where the energy to drive the remainder of the conformational changes is stored in a slightly strained but fully cis-chromophore configuration. In addition, our data indicate a role for backbone rearrangements during the very early structural events.     

Incoherent manipulation of the photoactive yellow protein photocycle with dispersed pump-dump-probe spectroscopy

Photoactive yellow protein is the protein responsible for initiating the "blue-light vision" of Halorhodospira halophila. The dynamical processes responsible for triggering the photoactive yellow protein photocycle have been disentangled with the use of a novel application of dispersed ultrafast pump-dump-probe spectroscopy, where the photocycle can be started and interrupted with appropriately tuned and timed laser pulses. This "incoherent" manipulation of the photocycle allows for the detailed spectroscopic investigation of the underlying photocycle dynamics and the construction of a fully self-consistent dynamical model. This model requires three kinetically distinct excited-state intermediates, two (ground-state) photocycle intermediates, I(0) and pR, and a ground-state intermediate through which the protein, after unsuccessful attempts at initiating the photocycle, returns to the equilibrium ground state. Also observed is a previously unknown two-photon ionization channel that generates a radical and an ejected electron into the protein environment. This second excitation pathway evolves simultaneously with the pathway containing the one-photon photocycle intermediates.     

PAS domain receptor photoactive yellow protein is converted to a molten globule state upon activation

Biological signaling generally involves the activation of a receptor protein by an external stimulus followed by protein-protein interactions between the activated receptor and its downstream signal transducer. The current paradigm for the relay of signals along a signal transduction chain is that it occurs by highly specific interactions between fully folded proteins. However, recent results indicate that many regulatory proteins are intrinsically unstructured, providing a serious challenge to this paradigm and to the nature of structure-function relationships in signaling. Here we study the structural changes that occur upon activation of the blue light receptor photoactive yellow protein (PYP). Activation greatly reduces the tertiary structure of PYP but leaves the level secondary structure largely unperturbed. In addition, activated PYP exposes previously buried hydrophobic patches and allows significant solvent penetration into the core of the protein. These traits are the distinguishing hallmarks of molten globule states, which have been intensively studied for their role in protein folding. Our results show that receptor activation by light converts PYP to a molten globule and indicate stimulus-induced unfolding to a partially unstructured molten globule as a novel theme in signaling.     

Light-induced global conformational change of photoactive yellow protein in solution

The light-induced global conformational change of photoactive yellow protein was directly observed by small-angle X-ray scattering (SAXS). The N-terminal 6, 15, or 23 amino acid residues were enzymatically truncated (T6, T15, or T23, respectively), and their near-UV intermediates were accumulated under continuous illumination for SAXS measurements. The Kratky plot demonstrated that illumination induced partial loss of globularity. The change in globularity was marked in T6 but very small in T15 and T23, suggesting that structural change in positions 7-15 mainly reduces the globularity. The radius of gyration (R(g)) estimated by Guinier plot was increased by 1.1 A for T6 and 0.7 A for T15 and T23 upon illumination. As T23 lacks most of the N-terminal loop, structural change in the main part composed of the PAS core, helical connector, and beta-scaffold caused an increase of R(g) by 0.7 A. The structural change of positions 7-15 caused an additional increase by 0.4 A. The decrease of R(g) upon truncation of positions 7-15 for dark state was 0.3 A, while that for the intermediate was 0.7 A, suggesting that this region moves outward on formation of the intermediate. These results indicate that a light-induced structural change of PYP takes place in the main part and N-terminal 15 amino acid residues. The former induces only dimensional increase, but the latter results in additional change in shape.     

Coupling of hydrogen bonding to chromophore conformation and function in photoactive yellow protein

To understand in atomic detail how a chromophore and a protein interact to sense light and send a biological signal, we are characterizing photoactive yellow protein (PYP), a water-soluble, 14 kDa blue-light receptor which undergoes a photocycle upon illumination. The active site residues glutamic acid 46, arginine 52, tyrosine 42, and threonine 50 form a hydrogen bond network with the anionic p-hydroxycinnamoyl cysteine 69 chromophore in the PYP ground state, suggesting an essential role for these residues for the maintenance of the chromophore's negative charge, the photocycle kinetics, the signaling mechanism, and the protein stability. Here, we describe the role of T50 and Y42 by use of site-specific mutants. T50 and Y42 are involved in fine-tuning the chromophore's absorption maximum. The high-resolution X-ray structures show that the hydrogen-bonding interactions between the protein and the chromophore are weakened in the mutants, leading to increased electron density on the chromophore's aromatic ring and consequently to a red shift of its absorption maximum from 446 nm to 457 and 458 nm in the mutants T50V and Y42F, respectively. Both mutants have slightly perturbed photocycle kinetics and, similar to the R52A mutant, are bleached more rapidly and recover more slowly than the wild type. The effect of pH on the kinetics is similar to wild-type PYP, suggesting that T50 and Y42 are not directly involved in any protonation or deprotonation events that control the speed of the light cycle. The unfolding energies, 26.8 and 25.1 kJ/mol for T50V and Y42F, respectively, are decreased when compared to that of the wild type (29.7 kJ/mol). In the mutant Y42F, the reduced protein stability gives rise to a second PYP population with an altered chromophore conformation as shown by UV/visible and FT Raman spectroscopy. The second chromophore conformation gives rise to a shoulder at 391 nm in the UV/visible absorption spectrum and indicates that the hydrogen bond between Y42 and the chromophore is crucial for the stabilization of the native chromophore and protein conformation. The two conformations in the Y42F mutant can be interconverted by chaotropic and kosmotropic agents, respectively, according to the Hofmeister series. The FT Raman spectra and the acid titration curves suggest that the 391 nm form of the chromophore is not fully protonated. The fluorescence quantum yield of the mutant Y42F is 1.8% and is increased by an order of magnitude when compared to the wild type.     

Thermochromatium tepidum photoactive yellow protein/bacteriophytochrome/diguanylate cyclase: characterization of the PYP domain

The purple phototrophic bacterium, Thermochromatium tepidum, contains a gene for a chimeric photoactive yellow protein/bacteriophytochrome/diguanylate cyclase (Ppd). We produced the Tc. tepidum PYP domain (Tt PYP) in Escherichia coli, and found that it has a wavelength maximum at 358 nm due to a Leu46 substitution of the color-tuning Glu46 found in the prototypic Halorhodospira halophila PYP (Hh PYP). However, the 358 nm dark-adapted state is in a pH-dependent equilibrium with a yellow species absorbing at 465 nm (pK(a) = 10.2). Following illumination at 358 nm, photocycle kinetics are characterized at pH 7.0 by a small bleach and red shift to what appears to be a long-lived cis intermediate (comparable to the I(2) intermediate in Hh PYP). The recovery to the dark-adapted state has a lifetime of approximately 4 min, which is approximately 1500 times slower than that for Hh PYP. However, when the Tt PYP is illuminated at pH values above 7.5, the light-induced difference spectrum indicates a pH-dependent equilibrium between the I(2) intermediate and a red-shifted 440 nm intermediate. This equilibrium could be responsible for the sigmoidal pH dependence of the recovery of the dark-adapted state (pK(a) = 8.8). In addition, the light-induced difference spectrum shows that, at pH values above 9.3, there is an apparent bleach near 490 nm superimposed on the 358 and 440 nm changes, which we ascribe to the equilibrium between the protonated and ionized dark-adapted forms. The L46E mutant of Tt PYP has a wavelength maximum at 446 nm, resembling wild-type Hh PYP. The kinetics of recovery of L46E following illumination with white light are slow (lifetime of 15 min at pH 7), but are comparable to those of wild-type Tt PYP. We conclude that Tt PYP is unique among the PYPs studied to date in that it has a photocycle initiated from a dark-adapted state with a protonated chromophore at physiological pH. However, it is kinetically most similar to Rhodocista centenaria PYP (Ppr) despite the very different absorption spectra due to the lack of E46.     

Protein folding thermodynamics applied to the photocycle of the photoactive yellow protein.

Two complementary aspects of the thermodynamics of the photoactive yellow protein (PYP), a new type of photoreceptor that has been isolated from Ectothiorhodospira halophila, have been investigated. First, the thermal denaturation of PYP at pH 3.4 has been examined by global analysis of the temperature-induced changes in the UV-VIS absorbance spectrum of this chromophoric protein. Subsequently, a thermodynamic model for protein (un)folding processes, incorporating heat capacity changes, has been applied to these data. The second aspect of PYP that has been studied is the temperature dependence of its photocycle kinetics, which have been reported to display an unexplained deviation from normal Arrhenius behavior. We have extended these measurements in two solvents with different hydrophobicities and have analyzed the number of rate constants needed to describe these data. Here we show that the resulting temperature dependence of the rate constants can be quantitatively explained by the application of a thermodynamic model which assumes that heat capacity changes are associated with the two transitions in the photocycle of PYP. This result is the first example of an enzyme catalytic cycle being described by a thermodynamic model including heat capacity changes. It is proposed that a strong link exists between the processes occurring during the photocycle of PYP and protein (un)folding processes. This permits a thermodynamic analysis of the light-induced, physiologically relevant, conformational changes occurring in this photoreceptor protein.     

The two photocycles of photoactive yellow protein from Rhodobacter sphaeroides

The absorption spectrum of the photoactive yellow protein from Rhodobacter sphaeroides (R-PYP) shows two maxima, absorbing at 360 nm (R-PYP(360)) and 446 nm (R-PYP(446)), respectively. Both forms are photoactive and part of a temperature- and pH-dependent equilibrium (Haker, A., Hendriks, J., Gensch, T., Hellingwerf, K. J., and Crielaard, W. (2000) FEBS Lett. 486, 52-56). At 20 degrees C, for PYP characteristic, the 446-nm absorbance band displays a photocycle, in which the depletion of the 446-nm ground state absorption occurs in at least three phases, with time constants of <30 ns, 0.5 micros, and 17 micros. Intermediates with both blue- and red-shifted absorption maxima are transiently formed, before a blue-shifted intermediate (pB(360), lambda(max) = 360 nm) is established. The photocycle is completed with a monophasic recovery of the ground state with a time constant of 2.5 ms. At 7 degrees C these photocycle transitions are slowed down 2- to 3-fold. Upon excitation of R-PYP(360) with a UV-flash (330 +/- 50 nm) a species with a difference absorption maximum at approximately 435 nm is observed that returns to R-PYP(360) on a minute time scale. Recovery can be accelerated by a blue light flash (450 nm). R-PYP(360) and R-PYP(446) differ in their overall protein conformation, as well as in the isomerization and protonation state of the chromophore, as determined with the fluorescent polarity probe Nile Red and Fourier Transform Infrared spectroscopy, respectively.