Resonance Raman and EPR investigations of the D251N oxycytochrome P450cam/putidaredoxin complex

We have performed resonance Raman and electron paramagnetic resonance (EPR) studies on the dioxygen bound state of the D251N mutant of cytochrome P450cam (oxy-P450cam) and its complex with reduced putidaredoxin (Pd). The D251N oxy-P450cam/Pd complex has a perturbed proton delivery mechanism and shows a significantly red-shifted UV-visible spectrum as observed in Benson et al. [Benson, D. E., Suslick, K. S., and Sligar, S. G. (1997) Biochemistry 36, 5104-5107]. The red shift has been interpreted to indicate a major perturbation of the electronic structure of the oxy-heme complex. However, we find no evidence that electron transfer has occurred from Pd to the heme active site of D251N oxy-P450cam. This suggests that both electron and proton transfer are perturbed by the D251N mutation and that these processes may be coupled. Three oxygen isotope sensitive Raman features are identified in the Pd complex, and occur at 1137, 536, and 399 cm(-1). These values are not significantly different from those for WT or D251N oxy-P450cam. However, a careful examination of the oxygen stretching feature near 1137 cm(-1) reveals the presence of three peaks at 1131, 1138, and 1146 cm(-1), which we attribute to the presence of conformational substates in oxy-P450cam. A significant change in the conformational substate population is observed for the D251N oxy-P450cam when the Pd complex is formed. We suggest that the conformational population redistribution of oxy-P450cam, along with the red-shifted electronic spectra, reflects a structural equilibrium of the oxy-heme that is perturbed upon Pd binding. We propose that this structural perturbation is connected to the effector function of Pd and may involve changes in the electron donation properties of the thiolate ligand.     

Alteration of conformation and dynamics of bacteriorhodopsin induced by protonation of Asp 85 and deprotonation of Schiff base as studied by 13C NMR

According to previous X-ray diffraction studies, the D85N mutant of bacteriorhodopsin (bR) with unprotonated Schiff base assumes a protein conformation similar to that in the M photointermediate. We recorded (13)C NMR spectra of [3-(13)C]Ala- and [1-(13)C]Val-labeled D85N and D85N/D96N mutants at ambient temperature to examine how conformation and dynamics of the protein backbone are altered when the Schiff base is protonated (at pH 7) and unprotonated (at pH 10). Most notably, we found that the peak intensities of three to four [3-(13)C]Ala-labeled residues from the transmembrane alpha-helices, including Ala 39, 51, and 53 (helix B) and 215 (helix G), were suppressed in D85N and D85N/D96N both from CP-MAS (cross polarization-magic angle spinning) and DD-MAS (dipolar decoupled-magic angle spinning) spectra, irrespective of the pH. This is due to conformational change and subsequent acquisition of intermediate time-range motions, with correlation times in the order of 10(-)(5) or 10(-)(4) s, which interferes with proton decoupling frequency or frequency of magic angle spinning, respectively, essential for an attempted peak-narrowing to achieve high-resolution NMR signals. Greater changes were achieved, however, at pH 10, which indicate large-amplitude motions of transmembrane helices upon deprotonation of Schiff base and the formation of the M-like state in the absence of illumination. The spectra detected more rapid motions in the extracellular and/or cytoplasmic loops, with correlation times increasing from 10(-)(4) to 10(-)(5) s. Conformational changes in the transmembrane helices were located at helices B, G, and D as viewed from the above-mentioned spectral changes, as well as at 1-(13)C-labeled Val 49 (helix B), 69 (B-C loop), and [3-(13)C]Ala-labeled Ala 126 (D-helix) signals, in addition to the cytoplasmic and extracellular loops. Further, we found that in the M-like state the charged state of Asp 96 at the cytoplasmic side substantially modulated the conformation and dynamics of the extracellular region through long-distance interaction.     

pH-induced structural changes in bacteriorhodopsin studied by Fourier transform infrared spectroscopy.

Previous C13-NMR studies showed that two of the four internal aspartic acid residues (Asp-96 and Asp-115) of bacteriorhodopsin (bR) are protonated up to pH = 10, but no accurate pKa of these residues has been determined. In this work, infrared spectroscopy with the attenuated total reflection technique was used to characterize pH-dependent structural changes of ground-state, dark-adapted wild-type bacteriorhodopsin and its mutant (D96N) with aspartic acid-96 replaced by asparagine. Data indicated deprotonation of Asp-96 at high pH (pKa = 11.4 +/- 0.1), but no Asp-115 titration was observed. The analysis of the whole spectral region characteristic to complex conformational changes in the protein showed a more complicated titration with an additional pKa value (pKa1 = 9.3 +/- 0.3 and pKa2 = 11.5 +/- 0.2). Comparison of results obtained for bR and the D96N mutant of bR shows that the pKa approximately 11.5 characterizes not a direct titration of Asp-96 but a protein conformational change that makes Asp-96 accessible to the external medium.     

Time-resolved site-directed spin-labeling studies of bacteriorhodopsin: loop-specific conformational changes in M

A spin-label at site 101 in the C-D loop of bacteriorhodopsin was previously found to detect a conformational change during the M --> N transition [Steinhoff, H. -J., Mollaaghababa, R., Altenbach, C., Hideg, K., Krebs, M. P., Khorana, H. G., and Hubbell, W. L. (1994) Science 266, 105-107]. We have extended these time-resolved electron paramagnetic resonance studies in purple membranes by analyzing conformational changes detected by a spin-label at another site in the C-D loop (103), and at sites in the A-B loop (35), the D-E loop (130), and the E-F loop (160). In addition, we have investigated the motion detected by a spin-label at site 101 in a D96A mutant background that has a prolonged M intermediate. We find that among the examined sites, only spin-labels in the C-D loop detect a significant change in the local environment after the rise of M. Although the D96A mutation dramatically prolongs the lifetime of the M intermediate, it does not perturb either the structure of bacteriorhodopsin or the nature of the light-activated conformational change detected by a spin-label at site 101. In this mutant, a conformational change is detected during the lifetime of M, when no change in the 410 nm absorbance is observed. These results provide direct structural evidence for the heterogeneity of the M population in real time, and demonstrate that the motion detected at site 101 occurs in M, prior to Schiff base reprotonation.     

Expression of Na+,K+-ATPase in Pichia pastoris: analysis of wild type and D369N mutant proteins by Fe2+-catalyzed oxidative cleavage and molecular modeling

Na+,K+-ATPase (pig alpha1,beta1) has been expressed in the methylotrophic yeast Pichia pastoris. A protease-deficient strain was used, recombinant clones were screened for multicopy genomic integrants, and protein expression, and time and temperature of methanol induction were optimized. A 3-liter culture provides 300-500 mg of membrane protein with ouabain binding capacity of 30-50 pmol mg-1. Turnover numbers of recombinant and renal Na+,K+-ATPase are similar, as are specific chymotryptic cleavages. Wild type (WT) and a D369N mutant have been analyzed by Fe2+- and ATP-Fe2+-catalyzed oxidative cleavage, described for renal Na+,K+-ATPase. Cleavage of the D369N mutant provides strong evidence for two Fe2+ sites: site 1 composed of residues in P and A cytoplasmic domains, and site 2 near trans-membrane segments M3/M1. The D369N mutation suppresses cleavages at site 1, which appears to be a normal Mg2+ site in E2 conformations. The results suggest a possible role of the charge of Asp369 on the E1 <--> E2 conformational equilibrium. 5'-Adenylyl-beta,gamma-imidodi-phosphate(AMP-PNP)-Fe2+-catalyzed cleavage of the D369N mutant produces fragments in P (712VNDS) and N (near 440VAGDA) domains, described for WT, but only at high AMP-PNP-Fe2+ concentrations, and a new fragment in the P domain (near 367CSDKTGT) resulting from cleavage. Thus, the mutation distorts the active site. A molecular dynamic simulation of ATP-Mg2+ binding to WT and D351N structures of Ca2+-ATPase (analogous to Asp369 of Na+,K+-ATPase) supplies possible explanations for the new cleavage and for a high ATP affinity, which was observed previously for the mutant. The Asn351 structure with bound ATP-Mg2+ may resemble the transition state of the WT poised for phosphorylation.     

Mutations which decouple the proton pump of the cytochrome c oxidase from Rhodobacter sphaeroides perturb the environment of glutamate 286

Mutants that decouple the proton pump of cytochrome c oxidase from Rhodobacter sphaeroides are postulated to do so by increasing the pK(a) of glutamate 286, which is 20 Angstrom away. The possibility that a conformational change near E286 is induced by the decoupling mutations (N139D and N207D) was investigated by FTIR difference spectroscopy. In both decoupled mutants, the reduced-minus-oxidized FTIR difference spectra show a shift of 2 cm(-1) to lower frequency of the band resulting from the absorbance of E286 in the oxidized enzyme. The decoupling mutants may influence E286 by altering the chain of water molecules which runs from the site of the mutations to E286.     

Protein conformational changes in the bacteriorhodopsin photocycle

We report a comprehensive electron crystallographic analysis of conformational changes in the photocycle of wild-type bacteriorhodopsin and in a variety of mutant proteins with kinetic defects in the photocycle. Specific intermediates that accumulate in the late stages of the photocycle of wild-type bacteriorhodopsin, the single mutants D38R, D96N, D96G, T46V, L93A and F219L, and the triple mutant D96G/F171C/F219L were trapped by freezing two-dimensional crystals in liquid ethane at varying times after illumination with a light flash. Electron diffraction patterns recorded from these crystals were used to construct projection difference Fourier maps at 3.5 A resolution to define light-driven changes in protein conformation.Our experiments demonstrate that in wild-type bacteriorhodopsin, a large protein conformational change occurs within approximately 1 ms after illumination. Analysis of structural changes in wild-type and mutant bacteriorhodopsins under conditions when either the M or the N intermediate is preferentially accumulated reveals that there are only small differences in structure between M and N intermediates trapped in the same protein. However, a considerably larger variation is observed when the same optical intermediate is trapped in different mutants. In some of the mutants, a partial conformational change is present even prior to illumination, with additional changes occurring upon illumination. Selected mutations, such as those in the D96G/F171C/F219L triple mutant, can sufficiently destabilize the wild-type structure to generate almost the full extent of the conformational change in the dark, with minimal additional light-induced changes. We conclude that the differences in structural changes observed in mutants that display long-lived M, N or O intermediates are best described as variations of one fundamental type of conformational change, rather than representing structural changes that are unique to the optical intermediate that is accumulated. Our observations thus support a simplified view of the photocycle of wild-type bacteriorhodopsin in which the structures of the initial state and the early intermediates (K, L and M1) are well approximated by one protein conformation, while the structures of the later intermediates (M2, N and O) are well approximated by the other protein conformation. We propose that in wild-type bacteriorhodopsin and in most mutants, this conformational change between the M1 and M2 states is likely to make an important contribution towards efficiently switching proton accessibility of the Schiff base from the extracellular side to the cytoplasmic side of the membrane.     

Electric field induced conformational changes of bacteriorhodopsin in purple membrane films

Electric field induced conformational changes of bacteriorhodopsin were studied in six types of dried film (randomly and electrically oriented membranes of purple as well as cation-depleted blue bacteriorhodopsin) by measuring the frequency dependence of the optical absorbance change and the dielectric dispersion and absorption. For the purple bacteriorhodopsin the optical absorbance change induced by alternating rectangular electric fields of ±300 kV/cm altered the sign twice in the frequency range from 0.001 Hz to 100 kHz (around 0.03 Hz and 100 kHz), indicating that the electric field induced conformational change in these samples consists of, at least, three steps. Similarly, it was found for the blue bacteriorhodopsin that at least two steps are involved. In accord with optical measurements, the dielectric behaviour due to alternating sinusoidal electric fields of±6kV/cm in the frequency range from 10 Hz to 10 MHz showed two broad dispersion/absorption regions, one below 1 kHz and the other around 10–100 kHz. This suggests that the conformational change of bacteriorhodopsin is also reflected by its dielectrical properties and that it is partially induced at 6 kV/cm. Including previous results obtained by analysis of the action of DC fields on purple membrane films, a model for a field-induced cyclic reaction for purple as well as blue bacteriorhodopsin is proposed. In addition it was found that there are electrical interactions among purple membrane fragments in dried films.     

Hydration dependence of conformational dielectric relaxation of lysozyme

Dielectric response of hen egg white lysozyme is measured in the far infrared (5-65 cm-1, 0.15-1.95 THz, 0.6-8.1 meV) as a function of hydration. The frequency range is associated with collective vibrational modes of protein tertiary structure. The observed frequency dependence of the absorbance is broad and glass-like. For the entire frequency range, there is a slight increase in both the absorbance and index of refraction with increasing hydration for <0.27 h (mass of H2O per unit mass protein). At 0.27 h, the absorbance and index begin to increase more rapidly. This transition corresponds to the point where the first hydration shell is filled. The abrupt increase in dielectric response cannot be fully accounted for by the additional contribution to the dielectric response due to bulk water, suggesting that the protein has not yet achieved its fully hydrated state. The broad, glass-like response suggests that at low hydrations, the low frequency conformational hen egg white lysozyme dynamics can be described by a dielectric relaxation model where the protein relaxes to different local minima in the conformational energy landscape. However, the low frequency complex permittivity does not allow for a pure relaxational mechanism. The data can best be modeled with a single low frequency resonance (nu approximately 120 GHz=4 cm-1) and a single Debye relaxation process (tau approximately .03-.04 ps). Terahertz dielectric response is currently being considered as a possible biosensing technique and the results demonstrate the required hydration control necessary for reliable biosensor applications.     

Photoinduced transformation of 14-F-bacteriorhodopsin gelatin films based on both wild type and D96N mutant

Spectral and kinetic transformations were studied in gelatin films made with 14-F wild type (WT) bacteriorhodopsin (BR) and 14-F D96N mutant BR. Unlike the recent study of water suspensions of the same pigments, where a red shifted species at 660 nm was shown to form under the light in 14-F WT only, there are no drastic differences in photoinduced behavior between gelatin films based on 14-F WT and 14-F D96N. It is not observed any photoinduced formation of red shifted species at 660 nm for both types of films as it is observed for corresponding pigments in water suspension. The observed results are explained in a terms of relationship between the rates of two photoinduced processes that occur in suspensions and films of corresponding pigments. Kinetic characteristics of the photoinduced processes for the films with chemical additives suggest that there are no advantages in using 14-F D96N films when compared to films based on 14-F WT.     

Interrelations of M-intermediates in bacteriorhodopsin photocycle.

The photocycles of the wild-type bacteriorhodopsin and the D96N mutant were investigated by the flash-photolysis technique. The M-intermediate formation (400 nm) and the L-intermediate decay (520 nm) were found to be well described by a sum of two exponents (time constants, tau 1 = 65 and tau 2 = 250 microseconds) for the wild-type bR and three exponents (tau 1 = 55 microseconds, tau 2 = 220 microseconds and tau 3 = 1 ms) for the D96N mutant of bR. A component with tau = 1 ms was found to be present in the photocycle of the wild-type bacteriorhodopsin as a lag-phase in the relaxation of photoresponses at 400 and 520 nm. In the presence of Lu3+ ions or 80% glycerol this component was clearly seen as an additional phase of M-formation. The azide effect on the D96N mutant of bR suggests that the 1-ms component is associated with an irreversible conformational change switching the Schiff base from the outward to the inward proton channel. The maximum of the difference spectrum of the 1-ms component of D96N bR is located at 404 nm as compared to 412 nm for the first two components. We suggest that this effect is a result of the alteration of the inward proton channel due to the Asp96-->Asn substitution. Proton release measured with pyranine in the absence of pH buffers was identical for the wild-type bR and D96N mutant and matched the M-->M' conformational transition. A model for M rise in the bR photocycle is proposed.     

Laser-induced transient grating analysis of dynamics of interaction between sensory rhodopsin II D75N and the HtrII transducer

The interaction between sensory rhodopsin II (SRII) and its transducer HtrII was studied by the time-resolved laser-induced transient grating method using the D75N mutant of SRII, which exhibits minimal visible light absorption changes during its photocycle, but mediates normal phototaxis responses. Flash-induced transient absorption spectra of transducer-free D75N and D75N joined to 120 amino-acid residues of the N-terminal part of the SRII transducer protein HtrII (DeltaHtrII) showed only one spectrally distinct K-like intermediate in their photocycles, but the transient grating method resolved four intermediates (K(1)-K(4)) distinct in their volumes. D75N bound to HtrII exhibited one additional slower kinetic species, which persists after complete recovery of the initial state as assessed by absorption changes in the UV-visible region. The kinetics indicate a conformationally changed form of the transducer portion (designated Tr*), which persists after the photoreceptor returns to the unphotolyzed state. The largest conformational change in the DeltaHtrII portion was found to cause a DeltaHtrII-dependent increase in volume rising in 8 micros in the K(4) state and a drastic decrease in the diffusion coefficient (D) of K(4) relatively to those of the unphotolyzed state and Tr*. The magnitude of the decrease in D indicates a large structural change, presumably in the solvent-exposed HAMP domain of DeltaHtrII, where rearrangement of interacting molecules in the solvent would substantially change friction between the protein and the solvent.     

Drug binding and resistance mechanism of KIT tyrosine kinase revealed by hydrogen/deuterium exchange FTICR mass spectrometry

Mutations of the receptor tyrosine kinase KIT are linked to certain cancers such as gastrointestinal stromal tumors (GISTs). Biophysical, biochemical, and structural studies have provided insight into the molecular basis of resistance to the KIT inhibitors, imatinib and sunitinib. Here, solution‐phase hydrogen/deuterium exchange (HDX) and direct binding mass spectrometry experiments provide a link between static structure models and the dynamic equilibrium of the multiple states of KIT, supporting that sunitinib targets the autoinhibited conformation of WT‐KIT. The D816H mutation shifts the KIT conformational equilibrium toward the activated state. The V560D mutant exhibits two low energy conformations: one is more flexible and resembles the D816H mutant shifted toward the activated conformation, and the other is less flexible and resembles the wild‐type KIT in the autoinhibited conformation. This result correlates with the V560D mutant exhibiting a sensitivity to sunitinib that is less than for WT KIT but greater than for KIT D816H. These findings support the elucidation of the resistance mechanism for the KIT mutants.     

Differential effect of pressure and temperature on the catalytic behaviour of wild-type human butyrylcholinesterase and its D70G mutant.

The combined action of temperature (10-35 degrees C) and pressure (0. 001-2 kbar) on the catalytic activity of wild-type human butyrylcholinesterase (BuChE) and its D70G mutant was investigated at pH 7.0 using butyrylthiocholine as the substrate. The residue D70, located at the mouth of the active site gorge, is an essential component of the peripheral substrate binding site of BuChE. Results showed a break in Arrhenius plots of wild-type BuChE (at Tt approximately 22 degrees C) whatever the pressure (dTt/dP = 1.6 +/- 1.5 degrees C.kbar-1), whereas no break was observed in Arrhenius plots of the D70G mutant. These results suggested a temperature-induced conformational change of the wild-type BuChE which did not occur for the D70G mutant. For the wild-type BuChE, at around a pressure of 1 kbar, an intermediate state, whose affinity for substrate was increased, appeared. This intermediate state was not seen for the mutant enzyme. The wild-type BuChE remained active up to a pressure of 2 kbar whatever the temperature, whereas the D70G mutant was found to be more sensitive to pressure inactivation (at pressures higher than 1.5 kbar the mutant enzyme lost its activity at temperatures lower than 25 degrees C). The results indicate that the residue D70 controls the conformational plasticity of the active site gorge of BuChE, and is involved in regulation of the catalytic activity as a function of temperature.     

The formation of hydrogen bond in the proximal heme pocket of HemAT-Bs upon ligand binding

HemAT-Bs is the heme-based O(2) sensor responsible for aerotaxis control in Bacillus subtilis. In this study, we measured the time-resolved resonance Raman spectra of full-length HemAT-Bs wild-type (WT) and Y133F in the deoxy form and the photoproduct after photolysis of CO-bound form. In WT, the nu(Fe-His) band for the 10 ps photoproduct was observed at higher frequency by about 2 cm(-1) compared with that of the deoxy form. This frequency difference is relaxed in hundreds of picoseconds. This time-dependent frequency shift would reflect the conformational change of the protein matrix. On the other hand, Y133F mutant did not show such a substantial nu(Fe-His) frequency shift after photolysis. Since a hydrogen bond to the proximal His induces an up-shift of the nu(Fe-His) frequency, these results indicate that Tyr133 forms a hydrogen bond to the proximal His residue upon the ligand binding. We discuss a functional role of this hydrogen bond formation for the signal transduction in HemAT-Bs.     

An unexpected role for the active site base in cofactor orientation and flexibility in the copper amine oxidase from Hansenula polymorpha.

The role of the active site aspartate base in the aminotransferase mechanism of the copper amine oxidase from the yeast Hansenula polymorpha has been probed by site-directed mutagenesis. The D319E mutant catalyzes the oxidation of methylamine and phenethylamine, but not that of benzylamine. kcat/Km for methylamine is found to be 80-fold reduced compared to that of the wild type. Viscosogen and substrate and solvent deuteration have no effect on this parameter for D319E, which is suggestive of limitation of kcat/Km by a conformational change. This conformational change is proposed to be the movement of the cofactor into a productive orientation upon the binding of substrate. In the absence of substrate, a flipped cofactor orientation is likely, on the basis of resonance Raman evidence that the C5 carbonyl of the cofactor is less solvent accessible than the C3 hydrogen. kcat for D319E methylamine oxidase is reduced 200-fold compared to that of the wild type and is unaffected by substrate deuteration, but displays a substantial solvent isotope effect. A 428 nm absorbance is evident under conditions of saturating methylamine and oxygen with D319E. The D319N mutant is observed to produce a similar absorbance at 430 nm when treated with ammonia despite the fact that this mutant has no amine oxidase activity. Resonance Raman spectroscopy indicates the formation of a covalent ammonia adduct and identifies it as the deprotonated iminoquinone. In contrast, when the D319E mutant is reacted with ammonia, it gives predominantly a 340-350 nm species. This absorbance is ascribed to a localization of the cofactor oxyanion induced by binding of the cation at the active site and not to covalent adduct formation. Resonance Raman spectroscopic examination of the steady state species of D319E methylamine oxidation, in combination with the kinetic data, indicates that the 428 nm species is the deprotonated iminoquinone produced upon reoxidation of the reduced cofactor. A model is proposed in which a central role of the active site base is to position the free cofactor and several enzyme intermediates for optimal activity.     

Infrared spectroscopic discrimination between the loop and alpha-helices and determination of the loop diffusion kinetics by temperature-jump time-resolved infrared spectroscopy for cytochrome c

The infrared (IR) absorption of the amide I band for the loop structure may overlap with that of the alpha-helices, which can lead to the misassignment of the protein secondary structures. A resolution-enhanced Fourier transform infrared (FTIR) spectroscopic method and temperature-jump (T-jump) time-resolved IR absorbance difference spectra were used to identify one specific loop absorption from the helical IR absorption bands of horse heart cytochrome c in D2O at a pD around 7.0. This small loop consists of residues 70-85 with Met-80 binding to the heme Fe(III). The FTIR spectra in amide I' region indicate that the loop and the helical absorption bands overlap at 1653 cm(-1) at room temperature. Thermal titration of the amide I' intensity at 1653 cm(-1) reveals that a transition in loop structural change occurs at lower temperature (Tm=45 degrees C), well before the global unfolding of the secondary structure (Tm approximately 82 degrees C). This loop structural change is assigned as being triggered by the Met-80 deligation from the heme Fe(III). T-jump time-resolved IR absorbance difference spectra reveal that a T-jump from 25 degrees C to 35 degrees C breaks the Fe-S bond between the Met-80 and the iron reversibly, which leads to a loop (1653 cm(-1), overlap with the helical absorption) to random coil (1645 cm(-1)) transition. The observed unfolding rate constant interpreted as the intrachain diffusion rate for this 16 residue loop was approximately 3.6x10(6) s(-1).     

Beta-amyloid 25 to 35 is intercalated in anionic and zwitterionic lipid membranes to different extents

D96N bacteriorhodopsin has two photointermediates with the deprotonated Schiff base: the M and MN intermediates. We measure the time-resolved x-ray diffraction of the D96N purple membrane after flash photoexcitation (pH 7.0, 25 degrees C). The data clearly show the M-MN transition during the D96N photocycle. Low-resolution projection maps of these states show that the F helix of the MN intermediate shifts from its original position and this shift is much larger than that of the M intermediate. This indicates that the F helix moves in the M-MN transition of the D96N bacteriorhodopsin photocycle. Moreover, the existence of the MN intermediate in the D96N photocycle under neutral pH indicates that the MN intermediate is not peculiar to the alkaline condition. It is notable that the structural transition of M-MN is independent of the protonation state of the Schiff base. Therefore, the F helix movement precedes reprotonation of the Schiff base in the bacteriorhodopsin photocycle. Our previous study showed that the M-MN transition is hydration-dependent and that the MN intermediate is more hydrated than the M intermediate. Considering this together with the present results, we conclude that the movement of the F helix causes hydration of the cytoplasmic side, which promotes the reprotonation of the Schiff base.     

Finding a needle in the haystack: computational modeling of Mg2+ binding in the active site of protein farnesyltransferase

Studies aimed at elucidating the unknown Mg2+ binding site in protein farnesyltransferase (FTase) are reported. FTase catalyzes the transfer of a farnesyl group to a conserved cysteine residue (Cys1p) on a target protein, an important step for proteins in the signal transduction pathways (e.g., Ras). Mg2+ ions accelerate the protein farnesylation reaction by up to 700-fold. The exact function of Mg2+ in catalysis and the structural characteristics of its binding remain unresolved to date. Molecular dynamics (MD) simulations addressing the role of magnesium ions in FTase are presented, and relevant octahedral binding motifs for Mg2+ in wild-type (WT) FTase and the Dβ352A mutant are explored. Our simulations suggest that the addition of Mg2+ ions causes a conformational change to occur in the FTase active site, breaking interactions known to keep FPP in its inactive conformation. Two relevant Mg2+ ion binding motifs were determined in WT FTase. In the first binding motif, WT1, the Mg2+ ion is coordinated to D352β, zinc-bound D297β, two water molecules, and one oxygen atom from the α- and β-phosphates of farnesyl diphosphate (FPP). The second binding motif, WT2, is identical with the exception of the zinc-bound D297β being replaced by a water molecule in the Mg2+ coordination complex. In the Dβ352A mutant Mg2+ binding motif, D297β, three water molecules, and one oxygen atom from the α- and β-phosphates of FPP complete the octahedral coordination sphere of Mg2+. Simulations of WT FTase, in which Mg2+ was replaced by water in the active site, recreated the salt bridges and hydrogen-bonding patterns around FPP, validating these simulations. In all Mg2+ binding motifs, a key hydrogen bond was identified between a magnesium-bound water and Cys1p, bridging the two metallic binding sites and, thereby, reducing the equilibrium distance between the reacting atoms of FPP Cys1p. The free energy profiles calculated for these systems provide a qualitative understanding of experimental results. They demonstrate that the two reactive atoms approach each other more readily in the presence of Mg2+ in WT FTase and mutant. The flexible WT2 model was found to possess the lowest barrier toward the conformational change, suggesting it is the preferred Mg2+ binding motif in WT FTase. In the mutant, the absence of D352β makes the transition toward a conformational change harder. Our calculations find support for the proposal that D352β performs a critical role in Mg2+ binding and Mg2+ plays an important role in the conformational transition step.