脲和盐酸胍诱导溶菌酶去折叠的荧光相图法研究

用荧光相图法分别研究了脲和盐酸胍诱导卵清溶菌酶去抓叠的过程。当变性体 系中无还原剂2－巯基乙醇存在、脲浓度从0变化至4.0 mol/L（或盐酸胍浓度从0变 化至3.0 mol/L）时,溶菌酶从天然态转变为部分折叠中间态,当脲浓度从4.0 mol/L变化至8.0 mol/L（或盐酸胍浓度从3.0 mol/L变化至6.0 mol/L）时,溶菌 酶从中间态转变为去折叠态,此时该蛋白的变性过程符合“三态模型”。而当变性 体系中有该还原剂存在时,溶菌酶则由天然态直接转变为去折叠态,此时脲诱导该 蛋白去折叠的过程符合曲型的“二态模型”。实难结果表明荧光相图法可以检测蛋 白南去抓叠的中间态。     

Site-selective probe for investigating the asynchronous unfolding of domains in bovine serum albumin

A convenient method is proposed for precise investigation of the asynchronous structural transition of the domains in bovine serum albumin (BSA) during unfolding process. The method is based on a site-selective probe, alizarin red S (ARS), which has a high affinity to the subdomain IIA of BSA. BSA-ARS complex was formed and gradually unfolded by urea from 0 to 8.0 M. The unfolding occurred in different domains of BSA resulted in distinct alterations of the microenvironment of the bound ARS. The spectral response of BSA-ARS complex, including the color, the UV absorption at 530 and 432 nm, and the intrinsic fluorescence at 342 and 310 nm with the excitation wavelength of 280 nm, showed slight changes in the urea concentration from 0 to 4.5 M, drastic changes from 4.5 to 6.0 M, and almost no changes from 6.0 to 8.0 M. The redox behavior of bound ARS between 0.3 and 0.8 V also showed the same trend. Consequently, a two-step, three-state transition process was monitored by naked eyes, UV-vis spectroscopy and electrochemistry. It is the first report to realize the indicator of the intermediate state during the unfolding process of BSA through convenient methods instead of expensive approaches. The work provides a facile method for the investigation of the unfolding process of multidomain proteins.     

Structural changes of ultrasonicated bovine serum albumin revealed by hydrogen–deuterium exchange and mass spectrometry

The structural changes of bovine serum albumin (BSA) under high-intensity ultrasonication were investigated by fluorescence spectroscopy and mass spectrometry. Evidence for the ultrasonication-induced conformational changes of BSA was provided by the intensity changes and maximum-wavelength shift in fluorescence spectrometry. Matrix-assisted laser desorption–ionization time-of-flight mass spectroscopy (MALDI-TOF MS) revealed the increased intensity of the peak at the charge state +5 and a newly emerged peak at charge state +6, indicating that the protein became unfolded after ultrasonication. Prevalent unfolding of BSA after ultrasonication was revealed by hydrogen–deuterium exchange coupled with mass spectrometry (HDX-MS). Increased intensity and duration of ultrasonication further promoted the unfolding of the protein. The unfolding induced by ultrasonication goes through an intermediate state similar to that induced by a low concentration of denaturant.     

Acetonitrile-induced unfolding of the photosystem II manganese-stabilizing protein studied by electrospray mass spectrometry

In this paper an acetonitrile-induced unfolding of the manganese-stabilizing protein (MSP) of photosystem II was discovered. More distinct unfolding states of MSP were identified than previously by using mainly electrospray ionization mass spectrometry (ESI-MS), together with fluorescence spectra and far-UV circular dichroism (CD) at pH 2.0, 6.2 or 11.6, and with acetonitrile concentrations from 0 to 50%. At pH 6.2 with acetonitrile concentration changing from 0 to 10%, relatively broad charge-state distributions and poor intensity were observed in ESI-MS, indicating the presence of coexisting conformers. It was concluded that the structure of the MSP protein is unlikely to be a tightly folded form. When the concentration of acetonitrile was 20-40%, simulating the state in the biological membrane, changes in the state of unfolding of MSP were observed to a certain extent using ESI-MS, fluorescence and CD spectroscopy. The charge-state distribution in ESI-MS was found to move toward high states (from 13+ to 27+ to 15+ to 31+) with increasing acetonitrile concentration. At pH 2.0, the MSP structure is rearranged into an unfolded state, and at pH 11.6 the MSP structure is induced to assume another unordered state by deprotonation of appropriate residues. An interesting observation was that a second peak envelope emerged with 20-50% acetonitrile in the medium at pH 11.6.     

荧光相图法研究脲诱导牛血清白蛋白的去折叠过程

作为从分子水平上阐明生命奥秘的中心课题之一,蛋白质的折叠问题一直受到生物化学、生物物理学和结构生物学等领域研究工作者的高度关注。在蛋白质的变性过程中,它们往往达不到完全去折叠,而是会形成不同的部分折叠中间态[1-3],这些部分折叠中间态在蛋白质折叠过程中起着重要作     

Temperature dependent equilibrium native to unfolded protein dynamics and properties observed with IR absorption and 2D IR vibrational echo experiments

Dynamic and structural properties of carbonmonoxy (CO)-coordinated cytochrome c(552) from Hydrogenobacter thermophilus (Ht-M61A) at different temperatures under thermal equilibrium conditions were studied with infrared absorption spectroscopy and ultrafast two-dimensional infrared (2D IR) vibrational echo experiments using the heme-bound CO as the vibrational probe. Depending on the temperature, the stretching mode of CO shows two distinct bands corresponding to the native and unfolded proteins. As the temperature is increased from low temperature, a new absorption band for the unfolded protein grows in and the native band decreases in amplitude. Both the temperature-dependent circular dichroism and the IR absorption area ratio R(A)(T), defined as the ratio of the area under the unfolded band to the sum of the areas of the native and unfolded bands, suggest a two-state transition from the native to the unfolded protein. However, it is found that the absorption spectrum of the unfolded protein increases its inhomogeneous line width and the center frequency shifts as the temperature is increased. The changes in line width and center frequency demonstrate that the unfolding does not follow simple two-state behavior. The temperature-dependent 2D IR vibrational echo experiments show that the fast dynamics of the native protein are virtually temperature independent. In contrast, the fast dynamics of the unfolded protein are slower than those of the native protein, and the unfolded protein fast dynamics and at least a portion of the slower dynamics of the unfolded protein change significantly, becoming faster as the temperature is raised. The temperature dependence of the absorption spectrum and the changes in dynamics measured with the 2D IR experiments confirm that the unfolded ensemble of conformers continuously changes its nature as unfolding proceeds, in contrast to the native state, which displays a temperature-independent distribution of structures.     

Fast folding of a four-helical bundle protein

The FK506-FKBP12 binding-domain of the kinase FRAP (FRB) forms a classic up-down four-helical bundle. The folding pathway of this protein has been investigated using a combination of equilibrium and kinetic studies. The native state of the protein is stable with respect to the unfolded state by some 7 kcal mol(-1) at pH 6.0, 10 degrees C. A kinetic analysis of unfolding and refolding rate constants as a function of chemical denaturant concentration suggests that an intermediate state may be populated during folding at low concentrations of denaturant. The presence of this intermediate state is confirmed by refolding experiments performed in the presence of the hydrophobic dye 8-anilinonaphthalene-1 sulfonate (ANS). ANS binds to the partially folded intermediate state populated during the folding of FRB and undergoes a large change in fluorescence that can be detected using stopped-flow techniques. Analysis of the kinetic data suggests that the intermediate state is compact and it may even be a misfolded species that has to partially unfold before it can reach the transition state. Folding and unfolding rate constants in water are approximately 150-200 s(-1) and 0.005-0.06 s(-1), respectively, at neutral pH and 10 degrees C. The folding of FRB is somewhat slower than for other all-helical proteins, probably as a consequence of the formation of a metastable intermediate state. The folding rate constant in the absence of any populated intermediate can be estimated to be 8800 s(-1). Despite the presence of an intermediate state, which effectively slows folding, the protein still folds rapidly with a half-life of 5 ms at 10 degrees C. The dependence of the rate constants on denaturant concentration indicates that the transition state for folding is compact with some 80% of the surface area exposed in the unfolded state buried in the transition state. Data presented for FRB is compared with kinetic data obtained for other all-helical proteins.     

A solution study on the local and global structure changes of cytochrome c: an unfolding process induced by urea

The local and global structural changes of cytochrome c induced by urea in aqueous solution have been studied using X-ray absorption spectroscopy (XAS) and small-angle X-ray scattering (SAXS). According to the XAS result, both the native (folded) protein and the unfolded protein exhibit the same preedge features taken at Fe K-edge, indicating that the Fe(III) in the heme group of the protein maintains a six-coordinated local structure in both the folded and unfolded states. Furthermore, the discernible differences in the X-ray absorption near-edge structure (XANES) of these two states are attributed to a possible spin transition of the Fe(III) from a low-spin state to a high-spin state during the unfolding process. The perseverance of six-coordination and the spin transition of the iron are reconciled by a proposed ligand exchange, with urea and water molecules replacing the methionine-80 and histidine-18 axial ligands, respectively. The SAXS result reveals a significant morphology change of cytochrome c from a globular shape of a radius of gyration R(g) = 12.8 A of the native protein to an elongated ellipsoid shape of R(g) = 29.7 A for the unfolded protein in the presence of concentrated urea. The extended X-ray absorption fine structure (EXAFS) data unveil the coordination geometries of Fe(III) in both the folded and unfolded state of cytochrome c. An initial spin transition of Fe(III) followed by an axial ligand exchange, accompanied by the change in the global envelope, is proposed for what happened in the protein unfolding process of cytochrome c.     

脲和盐酸胍诱导过氧化氢酶去折叠的研究

用荧光相图法分别研究了脲和盐酸胍诱导牛肝过氧化氢酶去折叠的过程。当脲 浓度从0依次增大至0.50,4.5和8.0 mol/L时,过氧化氢酶从天然四聚体依次转变 为蓬松的四聚体、部分折叠的无活性二聚体和去折叠态,而当盐酸胍浓度从0依次 变化至0.65,2.5和6.0 mol/L时,过氧化氢酶则从天然四聚体集资转变为部分折叠 的激活二聚体、部分折叠的单体和去折叠态,这表明无论是用脲还是用盐酸胍作为 变性剂,该蛋白的变性过程都符合“四态模型”,但这两种变性剂诱导该蛋白去折 叠的途径和机制有较大差异。实验结果表明荧光相图法可以检测蛋白质去折叠的中 间态。用等温滴定量去热法研究了盐酸胍诱导过氧化氢酶去折叠过程的热力学, 25.0 ℃时低浓度盐酸胍诱导该蛋白从天然四聚体转变为部分折叠的激活二聚体的 本征摩尔构象变化焓、Gibbs自由能和熵分别为-69.2 kJ·mol~(-1),6.43 kJ· mol~(-1)和-254 J·K~(-1)·mol~(-1),据此推断盐酸胍通过熵效应和静电效应来 稳定和激活该二聚体。     

Evidence for a Molten Globule State in Cicer α-Galactosidase Induced by pH, Temperature, and Guanidine Hydrochloride

Physiologically as well as industrially, α-galactosidases are very important enzymes, but very little is known about the stability and folding aspect of enzyme. In the present study, we have investigated the temperature, pH, and guanidine hydrochloride (GuHCl) induced unfolding of Cicer α-galactosidase using circular dichroism and fluorescence spectroscopy. Strong negative ellipticities at 208, 215, and 222 nm indicate the presence of both α and β structures in Cicer α-galactosidase and showed that its secondary structure belongs to α?+?β class of proteins with 31 % α-helicity. For Cicer α-galactosidase the emission maximum was found to be 345 nm which suggests that tryptophan residues are less exposed to solvent. However, at pH?2.0, protein showed blue-shift. This state of protein lacked activity but it retained significant secondary structure. Enhanced binding of ANS at pH?2.0 indicated significant unfolding and exposure of hydrophobic regions. The unfolded state of Cicer α-galactosidase showed a red-shift of 15 nm with a concomitant decrease in the fluorescence intensity. The enzyme maintained its native structure and full activity up to 40 °C; however, above this temperature, denaturation was observed.     

Native and unfolded cytochrome c--comparison of dynamics using 2D-IR vibrational echo spectroscopy

Unfolded vs native CO-coordinated horse heart cytochrome c (h-cyt c) and a heme axial methionine mutant cyt c552 from Hydrogenobacter thermophilus ( Ht-M61A) are studied by IR absorption spectroscopy and ultrafast 2D-IR vibrational echo spectroscopy of the CO stretching mode. The unfolding is induced by guanidinium hydrochloride (GuHCl). The CO IR absorption spectra for both h-cyt c and Ht-M61A shift to the red as the GuHCl concentration is increased through the concentration region over which unfolding occurs. The spectra for the unfolded state are substantially broader than the spectra for the native proteins. A plot of the CO peak position vs GuHCl concentration produces a sigmoidal curve that overlays the concentration-dependent circular dichroism (CD) data of the CO-coordinated forms of both Ht-M61A and h-cyt c within experimental error. The coincidence of the CO peak shift curve with the CD curves demonstrates that the CO vibrational frequency is sensitive to the structural changes induced by the denaturant. 2D-IR vibrational echo experiments are performed on native Ht-M61A and on the protein in low- and high-concentration GuHCl solutions. The 2D-IR vibrational echo is sensitive to the global protein structural dynamics on time scales from subpicosecond to greater than 100 ps through the change in the shape of the 2D spectrum with time (spectral diffusion). At the high GuHCl concentration (5.1 M), at which Ht-M61A is essentially fully denatured as judged by CD, a very large reduction in dynamics is observed compared to the native protein within the approximately 100 ps time window of the experiment. The results suggest the denatured protein may be in a glassy-like state involving hydrophobic collapse around the heme.     

Direct Observation of the Reversible Two‐State Unfolding and Refolding of an α/β Protein by Single‐Molecule Atomic Force Microscopy

Directly observing protein folding in real time using atomic force microscopy (AFM) is challenging. Here the use of AFM to directly monitor the folding of an α/β protein, NuG2, by using low‐drift AFM cantilevers is demonstrated. At slow pulling speeds (<50 nm s^?1), the refolding of NuG2 can be clearly observed. Lowering the pulling speed reduces the difference between the unfolding and refolding forces, bringing the non‐equilibrium unfolding–refolding reactions towards equilibrium. At very low pulling speeds (ca. 2 nm s^?1), unfolding and refolding were observed to occur in near equilibrium. Based on the Crooks fluctuation theorem, we then measured the equilibrium free energy change between folded and unfolded states of NuG2. The improved long‐term stability of AFM achieved using gold‐free cantilevers allows folding–unfolding reactions of α/β proteins to be directly monitored near equilibrium, opening the avenue towards probing the folding reactions of other mechanically important α/β and all‐β elastomeric proteins.     

Electrostatics of nucleic acid folding under conformational constraint

RNA folding is enabled by interactions between the nucleic acid and its ion atmosphere, the mobile sheath of aqueous ions that surrounds and stabilizes it. Understanding the ion atmosphere requires the interplay of experiment and theory. However, even an apparently simple experiment to probe the ion atmosphere, measuring the dependence of DNA duplex stability upon ion concentration and identity, suffers from substantial complexity, because the unfolded ensemble contains many conformational states that are difficult to treat accurately with theory. To minimize this limitation, we measured the unfolding equilibrium of a DNA hairpin using a single-molecule optical trapping assay, in which the unfolded state is constrained to a limited set of elongated conformations. The unfolding free energy increased linearly with the logarithm of monovalent cation concentration for several cations, such that smaller cations tended to favor the folded state. Mg(2+) stabilized the hairpin much more effectively at low concentrations than did any of the monovalent cations. Poisson-Boltzmann theory captured trends in hairpin stability measured for the monovalent cation titrations with reasonable accuracy, but failed to do so for the Mg(2+) titrations. This finding is consistent with previous work, suggesting that Poisson-Boltzmann and other mean-field theories fail for higher valency cations where ion-ion correlation effects may become significant. The high-resolution data herein, because of the straightforward nature of both the folded and the unfolded states, should serve as benchmarks for the development of more accurate electrostatic theories that will be needed for a more quantitative and predictive understanding of nucleic acid folding.     

小分子热休克蛋白Mj HSP16.5的分级变性

应用荧光光谱、圆二色光谱、体积排阻色谱、激光动态光散射等技术, 研究了来自嗜热古细菌Methanococcus jannaschii (Mj)的小分子热休克蛋白Mj HSP16.5在变性剂作用下的变性过程. 研究表明, 在pH 7时, Mj HSP16.5在8 mol·L-1尿素作用下不会发生变性. 在pH 7条件下, 盐酸胍对Mj HSP16.5的变性表现为一个分级过程,分别在2.0、3.0和6.0 mol·L-1盐酸胍浓度附近,出现明显的结构变化; 到7.0 mol·L-1盐酸胍时, Mj HSP16.5才完全变性. 降低溶液pH值将使Mj HSP16.5的变性变得更为容易.     

荧光素在明胶片中的光吸收及稳定性

由于对非线性光学材料的需求,近年来已有很多工作对荧光素的光学及光化学性质进行研究,研究对象既有溶液也有聚合物薄膜。本工作使用明胶片研究荧光素在明胶片中的光吸收、荧光及光稳定性。     

光谱法研究尿素对水溶液中血红蛋白构象的影响

应用荧光猝灭法和动态光散射法测定尿素-水混合溶剂中血红蛋白(Hb)与联苯胺的结合距离和Hb的流体动力学半径. 结合Hb的荧光光谱和吸收光谱, 探讨尿素与蛋白质分子在水溶液中相互作用的机理及其对蛋白质构象的影响. 结果显示, 尿素分子取代水分子在蛋白质周围形成溶剂化层, 并与骨架肽链和亲水侧链形成氢键, 从而积聚在蛋白质分子表面. 尿素分子与蛋白质分子之间的直接相互作用对蛋白质的构象具有复杂的影响, 高浓度的尿素-水混合溶剂破坏蛋白质的构象, 而低浓度的混合溶剂则有利于蛋白质形成更紧密的构象. 在高浓度的尿素-水混合溶剂中, Hb血红素疏水空穴失去原有的三级结构后形成一个与熔球态相类似的结构.     

Photophysical properties of ricin

The molar absorption coefficient of ricin in phosphate-buffered saline (PBS) at 279 nm was measured as (93,900+/-3300) L mol(-1) cm(-1). The concentration of ricin was determined using amino acid analysis. The absorption spectrum of ricin was interpreted in terms of 69% contribution from absorption by tryptophan residues and 31% contribution from absorption by tyrosine residues. The total dipole strength of the ricin band at 280 nm was determined to be (147+/-8) D2 and was consistent with the combined dipole strengths of 10 tryptophan ([11.7+/-1.0] D2) and 23 tyrosine ([1.4+/-0.2] D2) residues. The structure of ricin was used to determine the coupling of the tryptophan residues in ricin. The maximum interaction energy was found to be 424 cm(-1)/epsilon while the average interaction between any two pairs of tryptophan residues was approximately 18 cm(-1)/epsilon. In this study, epsilon is the dielectric constant inside the protein. The fluorescence from ricin, excited at 280 nm, was dominated by fluorescence from tryptophan residues suggesting the presence of energy transfer from tyrosine to tryptophan residues. The absorbance and fluorescence of ricin increased slightly when ricin was denatured in a high concentration of guanidine. Irreversible thermal unfolding of ricin occurred between 65 degrees C and 70 degrees C. (D=3.3364*10(-30) Cm, not SI unit, convenient unit for the magnitude of the electric dipole moment of molecules.).     

Probing the transition state ensemble of a protein folding reaction by pressure-dependent NMR relaxation dispersion

The F61A/A90G mutant of a redesigned form of apocytochrome b562 folds by an apparent two-state mechanism. We have used the pressure dependence of 15N NMR relaxation dispersion rate profiles to study the changes in volumetric parameters that accompany the folding reaction of this protein at 45 degrees C. The experiments were performed under conditions where the folding/unfolding equilibrium could be studied at each pressure without addition of denaturants. The exquisite sensitivity of the methodology to small changes in folding/unfolding rates facilitated the use of relatively low-pressure values (between 1 and 270 bar) so that pressure-induced changes to the unfolded state ensemble could be minimized. A volume change for unfolding of -81 mL/mol is measured (at 1 bar), a factor of 1.4 larger (in absolute value) than the volume difference between the transition state ensemble (TSE) and the unfolded state. Notably, the changes in the free energy difference between folded and unfolded states and in the activation free energy for folding were not linear with pressure. Thus, the difference in the isothermal compressibility upon unfolding (-0.11 mL mol(-1) bar(-1)) and, for the first time, the compressibility of the TSE relative to the unfolded state (0.15 mL mol(-1) bar(-1)) could be calculated. The results argue for a TSE that is collapsed but loosely packed relative to the folded state and significantly hydrated, suggesting that the release of water occurs after the rate-limiting step in protein folding. The notion of a collapsed and hydrated TSE is consistent with expectations based on earlier temperature-dependent folding studies, showing that the barrier to folding at 45 degrees C is entropic (Choy, W. Y.; Zhou, Z.; Bai, Y.; Kay, L. E. J. Am. Chem. Soc. 2005, 127, 5066-5072).     

Effect of Molecular Crowding on the Temperature–Pressure Stability Diagram of Ribonuclease A

FT‐IR spectroscopic and thermodynamic measurements were designed to explore the effect of a macromolecular crowder, dextran, on the temperature and pressure‐dependent phase diagram of the protein Ribonuclease A (RNase A), and we compare the experimental data with approximate theoretical predictions based on configuration entropy. Exploring the crowding effect on the pressure‐induced unfolding of proteins provides insight in protein stability and folding under cell‐like dense conditions, since pressure is a fundamental thermodynamic variable linked to molecular volume. Moreover, these studies are of relevance for understanding protein stability in deep‐sea organisms, which have to cope with pressures in the kbar range. We found that not only temperature‐induced equilibrium unfolding of RNase A, but also unfolding induced by pressure is markedly prohibited in the crowded dextran solutions, suggesting that crowded environments such as those found intracellularly, will also oppress high‐pressure protein unfolding. The FT‐IR spectroscopic measurements revealed a marked increase in unfolding pressure of 2 kbar in the presence of 30 wt % dextran. Whereas the structural changes upon thermal unfolding of the protein are not significantly influenced in the presence of the crowding agent, through stabilization by dextran the pressure‐unfolded state of the protein retains more ordered secondary structure elements, which seems to be a manifestation of the entropic destabilization of the unfolded state by crowding.