Yoshitaka Matsumura

Solvent‐tuning the collapse and helix formation time scales of λ6‐85*

The λ6‐85* pseudo‐wild type of lambda repressor fragment is a fast two‐state folder (kf ≈ 35 μsec−1 at 58°C). Previously, highly stable λ6‐85* mutants with kf > 30 μsec−1 have been engineered to fold nearly or fully downhill. Stabilization of the native state by solvent tuning might also tune λ6‐85* away from two‐state folding. We test this prediction by examining the folding thermodynamics and kinetics of λ6‐85* in a stabilizing solvent, 45% by weight aqueous ethylene glycol at −28°C. Detection of kinetics by circular dichroism at 222 nm (sensitive to helix content) and small angle X‐ray scattering (measuring the radius of gyration) shows that refolding from guanidine hydrochloride denatured conditions exhibits very different time scales for collapse and secondary structure formation: the two processes become decoupled. Collapse remains a low‐barrier activated process, while the fastest of several secondary structure formation time scales approaches the downhill folding limit. Two‐state folding of λ6‐85* is not a robust process.

Slowing Down Downhill Folding: A Three-Probe Study

The mutant Tyr22Trp/Glu33Tyr/Gly46Ala/Gly48Ala of lambda repressor fragment lambda(6-85) was previously assigned as an incipient downhill folder. We slow down its folding in a cryogenic water-ethylene-glycol solvent (-18 to -28 degrees C). The refolding kinetics are probed by small-angle x-ray scattering, circular dichroism, and fluorescence to measure the radius of gyration, the average secondary structure content, and the native packing around the single tryptophan residue. The main resolved kinetic phase of the mutant is probe independent and faster than the main phase observed for the pseudo-wild-type. Excess helical structure formed early on by the mutant may reduce the formation of turns and prevent the formation of compact misfolded states, speeding up the overall folding process. Extrapolation of our main cryogenic folding phase and previous T-jump measurements to 37 degrees C yields nearly the same refolding rate as extrapolated by Oas and co-workers from NMR line-shape data. Taken together, all the data consistently indicate a folding speed limit of approximately 4.5 micros for this fast folder.

Non‐native α‐helix formation is not necessary for folding of lipocalin: Comparison of burst‐phase folding between tear lipocalin and β‐lactoglobulin

Tear lipocalin and β‐lactoglobulin are members of the lipocalin superfamily. They have similar tertiary structures but unusually low overall sequence similarity. Non‐native helical structures are formed during the early stage of β‐lactoglobulin folding. To address whether the non‐native helix formation is found in the folding of other lipocalin superfamily proteins, the folding kinetics of a tear lipocalin variant were investigated by stopped‐flow methods measuring the time‐dependent changes in circular dichroism (CD) spectrum and small‐angle X‐ray scattering (SAXS). CD spectrum showed that extensive secondary structures are not formed during a burst‐phase (within a measurement dead time). The SAXS data showed that the radius of gyration becomes much smaller than in the unfolded state during the burst‐phase, indicating that the molecule is collapsed during an early stage of folding. Therefore, non‐native helix formation is not general for folding of all lipocalin family members. The non‐native helix content in the burst‐phase folding appears to depend on helical propensities of the amino acid sequence. Proteins 2009.

Transient Helical Structure during PI3K and Fyn SH3 Domain Folding

A growing list of proteins, including the β-sheet-rich SH3 domain, is known to transiently populate a compact α-helical intermediate before settling into the native structure. Examples have been discovered in cryogenic solvent as well as by pressure jumps. Earlier studies of λ repressor mutants showed that transient states with excess helix are robust in an all-α protein. Here we extend a previous study of src SH3 domain to two new SH3 sequences, phosphatidylinositol 3-kinase (PI3K) and a Fyn mutant, to see how robust such helix-rich transients are to sequence variations in this β-sheet fold. We quantify helical structure by circular dichroism (CD), protein compactness by small-angle X-ray scattering (SAXS), and transient helical populations by cryo-stopped-flow CD. Our results show that transient compact helix-rich intermediates are easily accessible on the folding landscape of different SH3 domains. In molecular dynamics simulations, force field errors are often blamed for transient non-native structure. We suggest that experimental examples of very fast α-rich transient misfolding could become a more subtle test for further force field improvements than observation of the native state alone.

Relationship between chain collapse and secondary structure formation in a partially folded protein

Chain collapse and secondary structure formation are frequently observed during the early stages of protein folding. Is the chain collapse brought about by interactions between secondary structure units or is it due to polymer behavior in a poor solvent (coil-globule transition)? To answer this question, we measured small-angle X-ray scattering for a series of β-lactoglobulin mutants under conditions in which they assume a partially folded state analogous to the folding intermediates. Mutants that were designed to disrupt the secondary structure units showed the gyration radii similar to that of the wild type protein, indicating that chain collapse is due to coil-globule transitions.

α-Helical burst on the folding pathway of FHA domains from Rad53 and Ki67

We investigated refolding processes of beta-sheeted protein FHA domains (FHA1 domain of Rad53 and Ki67 FHA domain) by cryo-stopped-flow (SF) method combined with far-ultraviolet (far-UV) circular dichroism (CD, the average secondary structure content) and small angle X-ray scattering (SAXS, measuring the radius of gyration). In case of FHA1 domain of Rad53, no detectable time course was observed except the initial burst on its refolding process at 4 degrees C, suggesting that the FHA1 domain of Rad53 was already refolded to its native state within the dead time of the SF apparatus and the rate of the refolding is too fast to be observed at this temperature. In contrast, there was an observable alpha-helical burst at -15 degrees C and -20 degrees C in the presence of 45% ethylene glycol (EGOH) by CD-SF. Besides, the radius of gyration (Rg) of the burst phase intermediate at -20 degrees C shows the intermediate is already compact, and the compaction process was accompanied with the decrease of alpha-helical content at the same temperature. In case of Ki67 FHA domain, ellipticity change at 222 nm was observed on its refolding pathway at -28 degrees C in the presence of 45% EGOH and 2 mM DTT, indicating that Ki67 FHA domain also takes non-native alpha-helix-rich intermediate on its folding pathway. Time-resolved SAXS experiment was done. As the signal/noise ratio is low, we could not observe the time-dependent signal change through the time course. However, the initial Rg value was obtained as 18.2 +/- 0.5 A, which is much smaller than the unfolded Rg value (26.5 +/- 1.2 A), and is slightly larger than the native one (15.9 +/- 1.8 A). These results suggest that Ki67 FHA domain also forms compact non-native alpha-helix-rich intermediate before refolding to its native beta-structure on the refolding pathway. These results are in good agreement with other beta-proteins, such as bovine beta-lactoglobulin (BLG), src SH3 domain proteins. It seems the alpha-helical burst phases appear on the folding pathway of beta-sandwiched proteins.

A Physicochemical and Mutational Analysis of Intersubunit Interactions of Escherichia coli Ferritin A

Ferritin A from Escherichia coli (EcFtnA) is 24-meric protein, which forms spherical cagelike structures called nanocages. The nanocage structure is stabilized by the interface around 4-, 3-, and 2-fold symmetric axes. The subunit structure of EcFtnA comprises a four-helix bundle (helices A-D) and an additional helix E, which forms a 4-fold axis. In this study, we examined the contribution of the interface around three symmetric axes. pH-induced dissociation experiments monitored by analytical ultracentrifugation and small-angle X-ray scattering showed that the dimer related by 2-fold symmetry is the most stable unit. Mutations located near the 3-fold axis revealed that the contribution of each interaction was small. A mutant lacking helix E at the 4-fold axis formed a nanocage, suggesting that helix E is not essential for nanocage formation. Further truncation of the C-terminus of helix D abrogated the formation of the nanocage, suggesting that a few residues located at the C-terminus of helix D are critical for this process. These properties are similar to those known for mammalian ferritins and seem to be common principles for nanocage formation. The difference between EcFtnA and mammalian ferritins was that helix E-truncated EcFtnA maintained an iron-incorporating ability, whereas mammalian mutants lost it.

Helix-rich transient and equilibrium intermediates of equine β-lactoglobulin in alkaline buffer

Acidic buffer conditions are known to stabilize helix-rich states of even those proteins with a predominantly beta-sheet native secondary structure. Here we investigated whether such states also exist under alkaline buffer conditions. The guanidine hydrochloride (GuHCl)-induced unfolding transition and kinetic refolding of equine beta-lactoglobulin (ELG) by GuHCl-jump were investigated at pH 8.7 by far-ultraviolet circular dichroism. We found that an equilibrium intermediate appeared in 45% ethylene glycol (EGOH) buffer with 1.5 M GuHCl. The intermediate is rich in non-native alpha-helix, which is similar to the helix-rich state of ELG at pH 4.0. A kinetic study was done on the folding rate of ELG and compared with bovine beta-lactoglobulin (BLG). Transient intermediates, which were observed as the burst phase of the refolding reaction, were also rich in alpha-helix. The activation enthalpy of ELG was calculated to be c.a. 80 kJ/mol, whereas that of BLG was c.a. 70 kJ/mol in the presence of 45% EGOH. The ellipticities of the transient intermediate of ELG show temperature dependence in the presence of 45% EGOH, whereas that of BLG did not show significant dependence. This study therefore extends the existence of helix-rich equilibrium and transient intermediates of predominantly beta-sheet proteins to alkaline buffer conditions.

Identification of key neoculin residues responsible for the binding and activation of the sweet taste receptor.

Neoculin (NCL) is a heterodimeric protein isolated from the edible fruit of Curculigo latifolia. It exerts a taste-modifying activity by converting sourness to sweetness. We previously demonstrated that NCL changes its action on the human sweet receptor hT1R2-hT1R3 from antagonism to agonism as the pH changes from neutral to acidic values, and that the histidine residues of NCL molecule play critical roles in this pH-dependent functional change. Here, we comprehensively screened key amino acid residues of NCL using nuclear magnetic resonance (NMR) spectroscopy and alanine scanning mutagenesis. We found that the mutations of Arg48, Tyr65, Val72 and Phe94 of NCL basic subunit increased or decreased both the antagonist and agonist activities. The mutations had only a slight effect on the pH-dependent functional change. These residues should determine the affinity of NCL for the receptor regardless of pH. Their locations were separated from the histidine residues responsible for the pH-dependent functional change in the tertiary structure. From these results, we concluded that NCL interacts with hT1R2-hT1R3 through a pH-independent affinity interface including the four residues and a pH-dependent activation interface including the histidine residues. Thus, the receptor activation is induced by local structural changes in the pH-dependent interface.

Crystal structure of a Ca2+-dependent regulator of flagellar motility reveals the open-closed structural transition

Sperm chemotaxis toward a chemoattractant is very important for the success of fertilization. Calaxin, a member of the neuronal calcium sensor protein family, directly acts on outer-arm dynein and regulates specific flagellar movement during sperm chemotaxis of ascidian, Ciona intestinalis. Here, we present the crystal structures of calaxin both in the open and closed states upon Ca2+ and Mg2+ binding. The crystal structures revealed that three of the four EF-hands of a calaxin molecule bound Ca2+ ions and that EF2 and EF3 played a critical role in the conformational transition between the open and closed states. The rotation of α7 and α8 helices induces a significant conformational change of a part of the α10 helix into the loop. The structural differences between the Ca2+- and Mg2+-bound forms indicates that EF3 in the closed state has a lower affinity for Mg2+, suggesting that calaxin tends to adopt the open state in Mg2+-bound form. SAXS data supports that Ca2+-binding causes the structural transition toward the closed state. The changes in the structural transition of the C-terminal domain may be required to bind outer-arm dynein. These results provide a novel mechanism for recognizing a target protein using a calcium sensor protein.