Mid- to low-frequency Fourier transform infrared spectra of S-state cycle for photosynthetic water oxidation in Synechocystis sp. PCC 6803

Flash-induced Fourier transform infrared (FTIR) difference spectra for the four-step S-state cycle and the effects of global (15)N- and (13)C-isotope labeling on the difference spectra were examined for the first time in the mid- to low-frequency (1200-800 cm(-1)) as well as the mid-frequency (1700-1200 cm(-1)) regions using photosystem (PS) II core particles from cyanobacterium Synechocystis sp. PCC 6803. The difference spectra clearly exhibited the characteristic vibrational features for each transition during the S-state cycling. It is likely that the bands that change their sign and intensity with the S-state advances reflect the changes of the amino acid residues and protein matrices that have functional and/or structural roles within the oxygen-evolving complex (OEC). Except for some minor differences, the trends of S-state dependence in the 1700-1200 cm(-1) frequency spectra of the PS II cores from Synechocystis were comparable to that of spinach, indicating that the structural changes of the polypeptide backbones and amino acid side chains that occur during the oxygen evolution are inherently identical between cyanobacteria and higher plants. Upon (13)C-labeling, most of the bands, including amide I and II modes and carboxylate stretching modes, showed downward shifts; in contrast, (15)N-labeling induced isotopic shifts that were predominantly observed in the amide II region. In the mid- to low-frequency region, several bands in the 1200-1140 cm(-1) region were attributable to the nitrogen- and/or carbon-containing group(s) that are closely related to the oxygen evolution process. Specifically, the putative histidine ligand exhibited a band at 1113 cm(-1) which was affected by both (15)N- and (13)C-labeling and showed distinct S-state dependency. The light-induced bands in the 900-800 cm(-1) region were downshifted only by (13)C-labeling, whereas the bands in the 1000-900 cm(-1) region were affected by both (15)N- and (13)C-labeling. Several modes in the mid- to low-frequency spectra were induced by the change in protonation state of the buffer molecules accompanied by S-state transitions. Our studies on the light-induced spectrum showed that contributions from the redox changes of Q(A) and the non-heme iron at the acceptor side and Y(D) were minimal. It was, therefore, suggested that the observed bands in the 1000-800 cm(-1) region include the modes of the amino acid side chains that are coupled to the oxidation of the Mn cluster. S-state-dependent changes were observed in some of the bands.     

Vibration spectroscopy reveals light-induced chromophore and protein structural changes in the LOV2 domain of the plant blue-light receptor phototropin 1

Phototropins (phot1 and phot2), the plant blue-light receptors for phototropism, chloroplast movement, and stomatal opening, are flavoproteins that contain two approximately 12 kDa FMN-binding domains, LOV1 and LOV2, at their N-terminus, and a serine/threonine protein kinase domain at their C-terminus. The light-activated LOV2 domain forms a metastable intermediate which has been shown to be a protein-chromophore cysteinyl adduct (Cys39) at C(4a) of FMN. This species thermally relaxes back to the ground state in the dark. We measured the light-minus-dark FTIR difference spectra for the LOV2 domain of oat phot1. These spectra show the disappearance of bands at 1580, 1550, and 1350 cm(-1) that originate from, or are strongly coupled to, the N5=C(4a) stretching vibrations, consistent with the perturbations expected upon C(4a) adduct formation. Assignment of these negative difference FTIR bands to native chromophore vibrations is based on the alignment with resonance Raman bands of FMN. Prominent positive bands include a doublet at 1516 and 1536 cm(-1) and one at 1375 and 1298 cm(-1). Normal-mode vibrational-frequency calculations for both lumiflavin and lumiflavin with a sulfur attached at the C(4a) position agree with many of the positive and negative bands observed in the difference spectra. Both calculated and experimental difference FTIR spectra for deuterium isotope substitutions at exchangeable positions in the flavin chromophore are consistent with the assignment of the above positive bands to vibrational modes involving both the newly formed tetrahedral geometry of C(4a) and the N5-H bond in the long-lived LOV2(S)(390) cysteinyl species.     

Vibrational modes of ubiquinone in cytochrome bo(3) from Escherichia coli identified by Fourier transform infrared difference spectroscopy and specific (13)C labeling.

In this study we present the infrared spectroscopic characterization of the bound ubiquinone in cytochrome bo(3) from Escherichia coli. Electrochemically induced Fourier transform infrared (FTIR) difference spectra of DeltaUbiA (an oxidase devoid of bound ubiquinone) and DeltaUbiA reconstituted with ubiquinone 2 and with isotopically labeled ubiquinone 2, where (13)C was introduced either at the 1- or at the 4-position of the ring (C=O groups), have been obtained. The vibrational modes of the quinone bound to the discussed high-affinity binding site (Q(H)) are compared to those from the synthetic quinones in solution, leading to the assignment of the C=O modes to a split signal at 1658/1668 cm(-)(1), with both carbonyls similarly contributing. The FTIR spectra of DeltaUbiA reconstituted with the labeled quinones indicate an essentially symmetrical and weak hydrogen bonding of the two C=O groups from the neutral quinone with the protein and distinct conformations of the 2- and 3-methoxy groups. Perturbations of the vibrational modes of the 5-methyl side groups are discussed for a signal at 1452 cm(-)(1). Only negligible shifts of the aromatic ring modes can be reported for the reduced and the protonated form of the quinone. Alterations of the protein upon quinone binding are reflected in the electrochemically induced FTIR difference spectra. In particular, difference signals at 1640-1633 cm(-)(1) and 1700-1670 cm(-)(1) indicate variations of beta-sheet secondary structure elements and loops, bands at 1706 and 1678 cm(-)(1) are tentatively attributed to individual amino acids, and a difference signal a 1540 cm(-)(1) is discussed to reflect an influence on C=C modes of the porphyrin ring or on deprotonated propionate groups of the hemes. Further tentative assignments are presented and discussed. The (13)C labeling experiments allow the assignment of the vibrational modes of a bound ubiquinone 8 in the electrochemically induced FTIR difference spectra of wild-type bo(3).     

Redox-induced conformational changes in plastocyanin: an infrared study.

The conformational changes associated with the redox transition of plastocyanin (PC) were investigated by absorption and reaction-induced infrared spectroscopy. In addition to spectral features readily ascribed to beta and turn protein secondary structures, the amide I band shows a major component band at 1647 cm(-1) in both redox states of the protein. The sensitivity of this component to deuteration and increasing temperature suggests that PC adopts an unusual secondary structure in solution, which differs from those described for other type I copper proteins, such as azurin and halocyanin. The conformations of oxidized and reduced PC are different, as evidenced (1) by analysis of their amide I band contour and the electrochemically induced oxidized-minus-reduced difference spectrum and (2) by their different thermal stability. The redox-induced difference spectrum exhibits a number of difference bands within the conformationally sensitive amide I band that could be assigned to peptide C=O modes, in light of their small shift upon deuteration, and to signals attributable to side chain vibrational modes of Tyr residues. Lowering the pH to 4.8 induces destabilization of both redox states of the protein, more pronounced for reduced PC, without significantly affecting their secondary structure. Besides the conformational differences obtained at neutral pH, the oxidized-minus-reduced difference spectrum shows two broad and strong negative bands at 1405 and 1571 cm(-1), assigned to COO(-) vibrations, and a broad positive band at 1710 cm(-1), attributed to the C=O vibration of a COOH group(s). These bands are indicative of a protonation of (an) Asp or Glu side chain(s) upon plastocyanin oxidation at acidic pH.     

A1 reduction in intact cyanobacterial photosystem I particles studied by time-resolved step-scan Fourier transform infrared difference spectroscopy and isotope labeling

Time-resolved step-scan Fourier transform infrared (FTIR) difference spectroscopy, with 5 mus time resolution, has been used to produce P700(+)A(1)(-)/P700A(1) FTIR difference spectra in intact photosystem I particles from Synechococcus sp. 7002 and Synechocystis sp. 6803 at 77 K. Corresponding spectra were also obtained for fully deuterated photosystem I particles from Synechococcus sp. 7002 as well as fully (15)N- and (13)C-labeled photosystem I particles from Synechocystis sp. 6803. Static P700(+)/P700 FTIR difference spectra at 77 K were also obtained for all of the unlabeled and labeled photosystem I particles. From the time-resolved and static FTIR difference spectra, A(1)(-)/A(1) FTIR difference spectra were constructed. The A(1)(-)/A(1) FTIR difference spectra obtained for unlabeled trimeric photosystem I particles from both cyanobacterial strains are very similar. There are some mode frequency differences in spectra obtained for monomeric and trimeric PS I particles. However, the spectra can be interpreted in an identical manner, with the proposed band assignments being compatible with all of the data obtained for labeled and unlabeled photosystem I particles. In A(1)(-)/A(1) FTIR difference spectra obtained for unlabeled photosystem I particles, negative bands are observed at 1559 and 1549-1546 cm(-)(1). These bands are assigned to amide II protein vibrations, as they downshift approximately 86 cm(-)(1) upon deuteration and approximately 13 cm(-)(1) upon (15)N labeling. Difference band features at 1674-1677(+) and 1666(-) cm(-)(1) display isotope-induced shifts that are consistent with these bands being due to amide I protein vibrations. The observed amide modes suggest alteration of the protein backbone (possibly in the vicinity of A(1)) upon A(1) reduction. A difference band at 1754(+)/1748(-) cm(-)(1) is observed in unlabeled spectra from both strains. The frequency of this difference band, as well as the observed isotope-induced shifts, indicate that this difference band is due to a 13(3) ester carbonyl group of chlorophyll a species, most likely the A(0) chlorophyll a molecule that is in close proximity to A(1). Thus A(1) reduction perturbs A(0), probably via a long-range electrostatic interaction. A negative band is observed at 1693 cm(-)(1). The isotope shifts associated with this band are consistent with this band being due to the 13(1) keto carbonyl group of chlorophyll a, again, most likely the 13(1) keto carbonyl group of the A(0) chlorophyll a that is close to A(1). Semiquinone anion bands are resolved at approximately 1495(+) and approximately 1414(+) cm(-)(1) in the A(1)(-)/A(1) FTIR difference spectra for photosystem I particles from both cyanobacterial strains. The isotope-induced shifts of these bands could suggest that the 1495(+) and 1414(+) cm(-)(1) bands are due to C-O and C-C modes of A(1)(-), respectively.     

FTIR spectroscopic evidence for the involvement of an acidic residue in quinone binding in cytochrome bd from Escherichia coli

In this work, FTIR difference spectroscopy is used to search for possible binding partners and protonable groups involved in the binding of the quinol to cytochrome bd from Escherichia coli. In addition, the electrochemically induced FTIR difference spectra are compared for preparations of the enzyme isolated from cells grown at different oxygen levels in which the quinone content of the membrane is altered. On this basis, difference signals can be tentatively attributed to the vibrational modes of the different quinones types that are associated with the enzyme depending on growth conditions. Furthermore, vibrational modes due to the redox-dependent reorganization of the protein vary depending on the quinone associated with the isolated enzyme. Of particular interest are the observations that a mode at 1738 cm(-1) is decreased and a mode at 1595 cm(-1) is increased as observed in direct comparison to the data obtained from samples grown anaerobically. These signals indicate a change in the protonation state of an aspartic or glutamic acid. Since these changes are observed when the ubiquinone ratio in the preparation increases, the data provide evidence for the modulation of the binding site by the interacting quinone and the involvement of an acidic group in the binding site. The tentative assignments of the vibrational modes are supported by electrochemically induced FTIR difference spectra of cytochrome bd in the presence of the specific quinone binding site inhibitors heptylhydroxyquinoline-N-oxide (HQNO) or 2-methyl-3-undecylquinolone-4. Whereas HQNO leads to strong shifts in the FTIR redox difference spectrum, 2-methyl-3-undecylquinolone-4 induces a specific shift of a mode at 1635 cm(-1), which likely originates from the displacement of the C=O group of the bound quinone.     

Structural changes of the sarcoplasmic reticulum Ca(2+)-ATPase upon nucleotide binding studied by fourier transform infrared spectroscopy

Changes in the vibrational spectrum of the sarcoplasmic reticulum Ca(2+)-ATPase upon nucleotide binding were recorded in H(2)O and (2)H(2)O at -7 degrees C and pH 7.0. The reaction cycle was triggered by the photochemical release of nucleotides (ATP, ADP, and AMP-PNP) from a biologically inactive precursor (caged ATP, P(3)-1-(2-nitrophenyl) adenosine 5'-triphosphate, and related caged compounds). Infrared absorbance changes due to ATP release and two steps of the Ca(2+)-ATPase reaction cycle, ATP binding and phosphorylation, were followed in real time. Under the conditions used in our experiments, the rate of ATP binding was limited by the rate of ATP release (k(app) congruent with 3 s(-1) in H(2)O and k(app) congruent with 7 s(-1) in (2)H(2)O). Bands in the amide I and II regions of the infrared spectrum show that the conformation of the Ca(2+)-ATPase changes upon nucleotide binding. The observation of bands in the amide I region can be assigned to perturbations of alpha-helical and beta-sheet structures. According to similar band profiles in the nucleotide binding spectra, ATP, AMP-PNP, and ADP induce similar conformational changes. However, subtle differences between ATP and AMP-PNP are observed; these are most likely due to the protonation state of the gamma-phosphate group. Differences between the ATP and ADP binding spectra indicate the significance of the gamma-phosphate group in the interactions between the Ca(2+)-ATPase and the nucleotide. Nucleotide binding affects Asp or Glu residues, and bands characteristic of their protonated side chains are observed at 1716 cm(-1) (H(2)O) and 1706 cm(-1) ((2)H(2)O) and seem to depend on the charge of the phosphate groups. Bands at 1516 cm(-1) (H(2)O) and 1514 cm(-1) ((2)H(2)O) are tentatively assigned to a protonated Tyr residue affected by nucleotide binding. Possible changes in Arg, Trp, and Lys absorption and in the nucleoside are discussed. The spectra are compared with those of nucleotide binding to arginine kinase, creatine kinase, and H-ras P21.     

Redox-triggered FTIR difference spectra of FAD in aqueous solution and bound to flavoproteins

Flavin adenine dinucleotide (FAD) and three different flavoproteins in aqueous solution were subjected to redox-triggered Fourier transform infrared difference spectroscopy. The acquired vibrational spectra show a great number of positive and negative peaks, pertaining to the oxidized and reduced state of the molecule, respectively. Density functional theory calculations on the B3LYP/6-31G(d) level were employed to assign several of the observed bands to vibrational modes of the isoalloxazine moiety of the flavin cofactor in both its oxidized and, for the first time, its reduced state. Prominent modes measured for oxidized FAD include nu(C(4)=O) and nu(C(2)=O) at 1716 and 1674 cm(-1), respectively, nu(C(4a)=N(5)) at 1580 cm(-1), and nu(C(10a)=N(1)) at 1548 cm(-1). Measured modes of the reduced form of FAD include nu(C(2)=O) at 1692 cm(-1), nu(C(4)=O) at 1634 cm(-1), and nu(C(4a)=C(10a)) at 1600 cm(-1). While the overall shape of the enzyme spectra is similar to the shape of the spectrum of free FAD, there are numerous differences in detail. In particular, the nu(C=N) modes of the flavin exhibit frequency shifts in the protein-bound form, most prominently for pyruvate oxidase where nu(C(10a)=N(1)) downshifts by 14 cm(-1) to 1534 cm(-1). The significance of this shift and a possible explanation in connection with the bent conformation of the flavin cofactor in this enzyme are discussed.     

Changes of low-frequency vibrational modes induced by universal 15N- and 13C-isotope labeling in S2/S1 FTIR difference spectrum of oxygen-evolving complex

The effects of universal (15)N- and (13)C-isotope labeling on the low- (650-350 cm(-1)) and mid-frequency (1800-1200 cm(-1)) S(2)/S(1) Fourier transform infrared (FTIR) difference spectrum of the photosynthetic oxygen-evolving complex (OEC) were investigated in histidine-tagged photosystem (PS) II core particles from Synechocystis sp. PCC 6803. In the mid-frequency region, the amide II modes were predominantly affected by (15)N-labeling, whereas, in addition to the amide II, the amide I and carboxylate modes were markedly affected by (13)C-labeling. In the low-frequency region, by comparing a light-induced spectrum in the presence of ferricyanide as the electron acceptor, with the double difference S(2)/S(1) spectrum obtained by subtracting the Q(A)(-)/Q(A) from the S(2)Q(A)(-)/S(1)Q(A) spectrum, considerable numbers of bands found in the light-induced spectrum were assigned to the S(2)/S(1) vibrational modes in the unlabeled PS II core particles. Upon (13)C-labeling, changes were observed for most of the prominent bands in the S(2)/S(1) spectrum. Although (15)N-labeling also induced changes similar to those by (13)C-labeling, the bands at 616(-), 605(+), 561(+), 555(-), and 544(-) cm(-1) were scarcely affected by (15)N-labeling. These results indicated that most of the vibrational modes found in the low-frequency spectrum are derived from the coupling between the Mn-cluster and groups containing nitrogen and/or carbon atom(s) in a direct manner and/or through hydrogen bonding. Interestingly, an intensive band at 577(-) cm(-1) was not affected by (15)N- and (13)C-isotope labeling, indicating that this band arises from the mode that does not include either nitrogen or carbon atoms, such as the skeletal vibration of the Mn-cluster or stretching vibrational modes of the Mn-ligand.     

Observation of terahertz vibrations in Pyrococcus furiosus rubredoxin via impulsive coherent vibrational spectroscopy and nuclear resonance vibrational spectroscopy--interpretation by molecular mechanics

We have used impulsive coherent vibrational spectroscopy (ICVS) to study the Fe(S-Cys)(4) site in oxidized rubredoxin (Rd) from Pyrococcus furiosus (Pf). In this experiment, a 15 fs visible laser pulse is used to coherently pump the sample to an excited electronic state, and a second <10 fs pulse is used to probe the change in transmission as a function of the time delay. PfRd was observed to relax to the ground state by a single exponential decay with time constants of approximately 255-275 fs. Superimposed on this relaxation are oscillations caused by coherent excitation of vibrational modes in both excited and ground electronic states. Fourier transformation reveals the frequencies of these modes. The strongest ICV mode with 570 nm excitation is the symmetric Fe-S stretching mode near 310 cm(-1), compared to 313 cm(-1) in the low temperature resonance Raman. If the rubredoxin is pumped at 520 nm, a set of strong bands occurs between 20 and 110 cm(-1). Finally, there is a mode at approximately 500 cm(-1) which is similar to features near 508 cm(-1) in blue Cu proteins that have been attributed to excited state vibrations. Normal mode analysis using 488 protein atoms and 558 waters gave calculated spectra that are in good agreement with previous nuclear resonance vibrational spectra (NRVS) results. The lowest frequency normal modes are identified as collective motions of the entire protein or large segments of polypeptide. Motion in these modes may affect the polar environment of the redox site and thus tune the electron transfer functions in rubredoxins.     

Ab initio vibrational calculations on ara-T molecule: application to analysis of IR and Raman spectra

The FTIR and FT-Raman spectra are reported for the arabinonucleoside ara-T (1-beta-D-arabinofuranosylthymine), which shows antiviral activity. The accurate knowledge of the vibrational modes is a prerequisite for the elucidation of drug-nucleotide and drug-enzyme interactions. The FTIR and FT-Raman spectra of ara-T were recorded from 4000 to 30 cm(-1). A tetradeuterated derivative (deuteration at N3, and hydroxyl groups O'2, O'3, and O'5) was synthesized and the observed isotopic shifts in its spectra were used for the vibrational analysis of ara-T. The theoretical frequencies and the potential energy distribution (PED) of the vibrational modes of ara-T were calculated using the ab initio Hartree-Fock/3-21G method. An assignment of the vibrational spectra of ara-T is proposed considering the scaled PED and the observed band shifts under deuteration. The scaled ab initio frequencies were in reasonable agreement with the experimental data.     

A conformational intermediate between the resting and desensitized states of the nicotinic acetylcholine receptor

The structural changes induced in the nicotinic acetylcholine receptor by two noncompetitive channel blockers, proadifen and phencyclidine, have been studied by infrared difference spectroscopy and using the conformationally sensitive photoreactive noncompetitive antagonist 3-(trifluoromethyl)-3-m-([(125)I]iodophenyl)diazirine. Simultaneous binding of proadifen to both the ion channel pore and neurotransmitter sites leads to the loss of positive markers near 1663, 1655, 1547, 1430, and 1059 cm(-)(1) in carbamylcholine difference spectra, suggesting the stabilization of a desensitized conformation. In contrast, only the positive markers near 1663 and 1059 cm(-)(1) are maximally affected by the binding of either blocker to the ion channel pore suggesting that the conformationally sensitive residues vibrating at these two frequencies are stabilized in a desensitized-like conformation, whereas those vibrating near 1655 and 1430 cm(-)(1) remain in a resting-like state. The vibrations at 1547 cm(-)(1) are coupled to those at both 1663 and 1655 cm(-)(1) and thus exhibit an intermediate pattern of band intensity change. The formation of a structural intermediate between the resting and desensitized states in the presence of phencyclidine is further supported by the pattern of 3-(trifluoromethyl)-3-m-([(125)I]iodophenyl)diazirine photoincorporation. In the presence of phencyclidine, the subunit labeling pattern is distinct from that observed in either the resting or desensitized conformations; specifically, there is a concentration-dependent increase in the extent of photoincorporation into the delta-subunit. Our data show that domains of the nicotinic acetylcholine receptor interconvert between the resting and desensitized states independently of each other and suggest a revised model of channel blocker action that involves both low and high affinity agonist binding conformational intermediates.     

Simultaneous resonance Raman detection of the heme a3-Fe-CO and CuB-CO species in CO-bound ba3-cytochrome c oxidase from Thermus thermophilus. Evidence for a charge transfer CuB-CO transition

Understanding of the chemical nature of the dioxygen and nitric oxide moiety of ba3-cytochrome c oxidase from Thermus thermophilus is crucial for elucidation of its physiological function. In the present work, direct resonance Raman (RR) observation of the Fe-C-O stretching and bending modes and the C-O stretching mode of the CuB-CO complex unambiguously establishes the vibrational characteristics of the heme-copper moiety in ba3-oxidase. We assigned the bands at 507 and 568 cm(-1) to the Fe-CO stretching and Fe-C-O bending modes, respectively. The frequencies of these modes in conjunction with the C-O mode at 1973 cm(-1) showed, despite the extreme values of the Fe-CO and C-O stretching vibrations, the presence of the alpha-conformation in the catalytic center of the enzyme. These data, distinctly different from those observed for the caa3-oxidase, are discussed in terms of the proposed coupling of the alpha-and beta-conformations that occur in the binuclear center of heme-copper oxidases with enzymatic activity. The CuB-CO complex was identified by its nu(CO) at 2053 cm(-1) and was strongly enhanced with 413.1 nm excitation indicating the presence of a metal-to-ligand charge transfer transition state near 410 nm. These findings provide, for the first time, RR vibrational information on the EPR silent CuB(I) that is located at the O2 delivery channel and has been proposed to play a crucial role in both the catalytic and proton pumping mechanisms of heme-copper oxidases.     

Correlation between acetylcholine receptor function and structural properties of membranes

Protein-lipid interactions were studied by using Torpedo californica acetylcholine receptor (AChR) as a model system by reconstituting purified AChR into membranes containing various synthetic lipids and native lipids. AChR function was determined by measuring two activities at 4 degrees C: (1) low to high agonist affinity-state transition of AChR in the presence of an agonist (carbamylcholine) in either membrane fragments or sealed vesicles and (2) ion-gating activity of AChR-containing vesicles in response to carbamylcholine. Sixteen samples were examined, each containing different lipid compositions including phosphatidylcholine, cholesterol, phosphatidic acid, phosphatidylethanolamine, asolectin, neutral lipid depleted asolectin, native lipids, and cholesterol-depleted native lipids. Phosphatidylcholines with different configurations of fatty acyl chains were used. The dynamic structures of these membranes were probed by incorporating spin-labeled fatty acid into AChR-containing vesicles and measuring the order parameters. It was found that both aspects of AChR function were highly dependent on the lipid environment even though carbamylcholine binding itself was not affected. An appropriate membrane fluidity was necessarily required to allow the interconversion between the low and high affinity states of AChR. An optimal fluidity hypothesis is proposed to account for the conformational transition properties of membrane proteins. In addition, the conformational change was only a necessary, but not sufficient, condition for the AChR-mediated ion flux activity. Among membranes in which AChR manifested the affinity-state transition, only those containing both cholesterol and negatively charged phospholipids (such as phosphatidic acid) retained the ion-gating activity.     

On the binding determinants of the glutamate agonist with the glutamate receptor ligand binding domain

Ionotropic glutamate receptors (GluRs) are ligand-gated membrane channel proteins found in the central neural system that mediate a fast excitatory response of neurons. In this paper, we report theoretical analysis of the ligand-protein interactions in the binding pocket of the S1S2 (ligand binding) domain of the GluR2 receptor in the closed conformation. By utilizing several theoretical methods ranging from continuum electrostatics to all-atom molecular dynamics simulations and quantum chemical calculations, we were able to characterize in detail glutamate agonist binding to the wild-type and E705D mutant proteins. A theoretical model of the protein-ligand interactions is validated via direct comparison of theoretical and Fourier transform infrared spectroscopy (FTIR) measured frequency shifts of the ligand's carboxylate group vibrations [Jayaraman et al. (2000) Biochemistry 39, 8693-8697; Cheng et al. (2002) Biochemistry 41, 1602-1608]. A detailed picture of the interactions in the binding site is inferred by analyzing contributions to vibrational frequencies produced by protein residues forming the ligand-binding pocket. The role of mobility and hydrogen-bonding network of water in the ligand-binding pocket and the contribution of protein residues exposed in the binding pocket to the binding and selectivity of the ligand are discussed. It is demonstrated that the molecular surface of the protein in the ligand-free state has mainly positive electrostatic potential attractive to the negatively charged ligand, and the potential produced by the protein in the ligand-binding pocket in the closed state is complementary to the distribution of the electrostatic potential produced by the ligand itself. Such charge complementarity ensures specificity to the unique charge distribution of the ligand.     

Thermal difference circular dichroism of Pf1 filamentous virus and effects of mercury(II), silver(I), and copper(II)

The circular dichroism (CD) of Pfl filamentous virus has been examined over the temperature range 0-40 degrees C, in the absence and presence of Hg(II), Ag(I), and Cu(II). Thermal difference CD spectra were obtained by subtraction of spectra recorded above and below a thermally induced structure transition near 12 degrees C. The thermal difference spectra look like they arise from shifts in two exciton bands, one centered at 230 nm and the other at 290 nm. The amplitudes on either side of a crossover at 230 nm are 10 times those of a crossover at 290 nm. It is proposed that the difference spectra result from thermally induced shifts in coupled oscillator interactions between Tyr40 residues of the coat protein and the guanine and cytosine bases of the DNA. Metal ions can reduce or block these shifts. The changes in ellipticities at 220, 237, and 270 nm induced by changing the temperature have inflections near 12 degrees C. Ag(I) and Hg(II), which are known to bind to the DNA bases in Pfl, reduce or eliminate the inflections in the thermal profiles, depending on the metal ion type and concentration. Cu(II) ions do not affect the profiles. The spectral changes and the effects of the metal ions indicate intimate contact between the DNA bases and the protein subunits in the virion.     

Hydrogen bond interactions of G proteins with the guanine ring moiety of guanine nucleotides.

We have utilized Raman difference spectroscopy to investigate hydrogen bonding interactions of the guanine moiety in guanine nucleotides with the binding site of two G proteins, EF-Tu (elongation factor Tu from Escherichia coli) and the c-Harvey ras protein, p21 (the gene product of the human c-H-ras proto-oncogene). Raman spectra of proteins complexed with GDP (guanosine 5' diphosphate), IDP (inosine 5' diphosphate), 6-thio-GDP, and 6-18O-GDP were measured, and the various difference spectra were determined. These were compared to the difference spectra obtained in solution, revealing vibrational features of the nucleotide that are altered upon binding. Specifically, we observed significant frequency shifts in the vibrational modes associated with the 6-keto and 2-amino positions of the guanine group of GDP and IDP that result from hydrogen bonding interactions between these groups and the two proteins. These shifts are interpreted as being proportional to the local energy of interaction (delta H) between the two groups and protein residues at the nucleotide binding site. Consistent with the tight binding between the nucleotides and the two proteins, the shifts indicate that the enthalpic interactions are stronger between these two polar groups and protein than with water. In general, the spectral shifts provide a rationale for the stronger binding of GDP and IDP with p21 compared to EF-Tu. Despite the structural similarity of the binding sites of EF-Tu and p21, the strengths of the observed hydrogen bonds at the 6-keto and 2-amino positions vary substantially, by up to a factor of 2.(ABSTRACT TRUNCATED AT 250 WORDS)     

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.     

Agonist-induced changes in the structure of the acetylcholine receptor M2 regions revealed by photoincorporation of an uncharged nicotinic noncompetitive antagonist.

To characterize structural changes induced in the nicotinic acetylcholine receptor (AChR) by agonists, we have mapped the sites of photoincorporation of the cholinergic noncompetitive antagonist 3-(trifluoromethyl)-3-(m-[125I]iodophenyl)diazirine (]125I]TID) in the presence and absence of 50 microM carbamylcholine. [125I]TID binds to the AChR with similar affinity under both these conditions, but agonist inhibits photoincorporation into all subunits by greater than 75% (White, B. H., Howard, S., Cohen, S. G., and Cohen, J. B. (1991) J. Biol. Chem. 266, 21595-21607). [125I]TID-labeled sites on the beta- and delta-subunits were identified by amino-terminal sequencing of both cyanogen bromide (CNBr) and tryptic fragments purified by Tricine sodium dodecyl sulfate-polyacrylamide gel electrophoresis followed by reversed-phase high-performance liquid chromatography. In the absence of agonist, [125I]TID specifically labels homologous aliphatic residues (beta L-257, delta L-265, beta V-261, and delta V-269) in the M2 region of both subunits. In the presence of agonist, labeling of these residues is reduced approximately 90%, and the distribution of labeled residues is broadened to include a homologous set of serine residues at the amino terminus of M2. In the beta-subunit residues beta S-250, beta S-254, beta L-257, and beta V-261 are all labeled in the presence of carbamylcholine. This pattern of labeling supports an alpha-helical model for M2 with the labeled face forming the ion channel lumen. The observed redistribution of label in the resting and desensitized states provides the first direct evidence for an agonist-dependent rearrangement of the M2 helices. The efficient labeling of the resting state channel in a region capable of structural change also suggests a plausible model for AChR gating in which the aliphatic residues labeled by [125I]TID form a permeability barrier to the passage of ions. We also report increased labeling of the M1 region of the delta-subunit in the presence of agonist.     

Allosteric interactions between muscarinic agonist binding sites and effector sites demonstrated by the use of bisquaternary pyridinium oximes

Agonist binding to muscarinic receptors from rat brain stem and cerebral cortex was studied using bisquaternary pyridinium oximes for detecting possible interactions between agonist binding sites and sites of the effector guanosine 5' (beta, gamma-imino) triphosphate (Gpp(NH)p) and Co2+. Pretreatment of either brain stem or cortical homogenates with 200 microM 1-(2-hydroxyiminoethylpyridinium) 1-(3-phenylcarboxypyridinium) dimethylether (HGG-12) reduced the affinity of muscarinic agonists. No change was observed in the relative proportions of high (RH) and low (RL) affinity agonist binding sites. However, the oxime affected the processes of interconversion between these sites. Thus, unlike in control membranes, HGG-12 treated brain stem membranes, Gpp(NH)p could not induce conversion of RH to RL, and in cortical membranes Co2+ could not induce conversion of RL to RH. These results suggest that HGG-12 inactivates a component which is involved in both processes of induced-interconversion. Induced-interconversion between RH and RL was not affected in membranes treated with HGG-12 in the presence of carbamylcholine in concentrations at which mainly RH is occupied by the agonist. The occupation of RH by carbamylcholine protected both RH and RL from the effects of the oxime. The possible role of the molecular events involved is discussed.