Post-assembly α-helix to β-sheet structural transformation within SAF-p1/p2a peptide nanofibers

Soft Matter ◽  
2018 ◽  
Vol 14 (44) ◽  
pp. 8986-8996 ◽  
Author(s):  
Evan K. Roberts ◽  
Kong M. Wong ◽  
Elizabeth J. Lee ◽  
Melina M. Le ◽  
Dipam M. Patel ◽  
...  

The SAF-p1/p2a binary peptide system co-assembles in water into α-helical coiled coils, but can convert post-assembly into a β-sheet structure.

2014 ◽  
Vol 941-944 ◽  
pp. 989-993
Author(s):  
Yuan Zhou

This paper was concerned with the effects of ultrasonication on the gelation behavior of silk fibroins (SF), and a comparison of Domestic and Wild silkworms was studied. The results show that: with the increase of ultrasonic power, the gelation time of domestic (Bombyx Mori) SF solution decreased sharply. But wild silkworms (Antheraea yamamai and Antheraea pernyi) SF were different, When the power of utrasonication was lower than 400-500 W, the velocity of gelation were accelerated, and when the ultrasonic power was higher than 400-500W, the gelation time were delayed. Whatever domestic or wild silkworms, the mechanism of the effects of ultrasonication on the gelation behavior was that the ultrasonication promoted the structural transformation of SF molecules from random coil or α-helix to β-sheet.


1981 ◽  
Vol 59 (7) ◽  
pp. 519-523 ◽  
Author(s):  
Janice B. Y. Richman ◽  
Jacob A. Verpoorte

The α2-macroglobulin (α2-M) was purified from the plasma of normal individuals and from that of cystic fibrosis patients. The proteins exhibited identical optical properties. Both proteins have an absorbance coefficient of A = 1060 g∙cm−2 at 280 nm. The circular dichroism spectra are identical and indicate about 45% β-sheet structure and almost no α-helix. The spectra of solutions at pH 8.0 do not change when trypsin is added.The fluorescence spectra of the α2-M measured at pH 8.0 have contributions by tyrosine and tryptophan residues. The fluorescence intensities are identical and are enhanced about 30% when trypsin is added in 2:1 molar ratios.


Blood ◽  
2012 ◽  
Vol 120 (21) ◽  
pp. 2217-2217
Author(s):  
Rustem I. Litvinov ◽  
Dzhigangir A. Faizullin ◽  
Yuriy F. Zuev ◽  
Artyom Zhmurov ◽  
Olga Kononova ◽  
...  

Abstract Abstract 2217 A new field of biomedical research, biomechanics of hemostasis and thrombosis, has been quickly developing over the past few years. The mechanical properties of fibrin are essential in vivo for the ability of clots to stop bleeding in flowing blood but also determine the likelihood of obstructive thrombi that cause heart attack and stroke. Despite such critical importance, the structural basis of clot mechanics is not well understood. The structural changes underlying deformation of fibrin polymer occur at different spatial scales from macroscopic to submolecular, including molecular unfolding, about which relatively little is known. In this work, fibrin mechanics was studied with respect to molecular structural changes during fibrin deformation. The results of atomic force microscopy-induced unfolding of fibrinogen monomers and oligomers were correlated with force-extension curves obtained using Molecular Dynamics simulations. The mechanical unraveling of fibrin(ogen) was shown to be determined by molecular transitions that couple reversible extension-contraction of the α-helical coiled-coil regions with unfolding of the terminal γ-nodules. The coiled-coils act as molecular springs to buffer external mechanical perturbations, transmitting and distributing force as the γ-nodules unfold. Unfolding of the γ-nodules, stabilized by strong inter-domain interactions with the neighboring β-nodules, was characterized by an average force of ∼90 pN and peak-to-peak distance of ∼25 nm. All-atom Molecular Dynamics simulations further showed a transition from α-helix to β-sheet at higher extensions. To reveal the force-induced α-helix to β-sheet transition in fibrin experimentally, we used Fourier Transform infrared spectroscopy of hydrated fibrin clots made from human blood plasma. When extended or compressed, fibrin showed a shift of absorbance intensity mainly in the amide I band but also in the amide II and III bands, demonstrating an increase of the β-sheets and a corresponding reduction of the α-helices. These structural conversions correlated directly with the strain or pressure and were partially reversible at the conditions applied. The spectra characteristic of the nascent inter-chain β-sheets were consistent with protein aggregation and fiber bundling during clot deformation observed using scanning electron microscopy. Additional information on the mechanically induced α-helix to β-sheet transition in fibrin was obtained from computational studies of the forced elongation of the entire fibrin molecule and its α-helical coiled-coil portions. We found that upon force application, the coiled-coils undergo ∼5–50 nm extension and 360-degree unwinding. The force-extension curves for the coiled-coils showed three distinct regimes: the linear elastic regime, the constant-force plastic regime, and the non-linear regime. In the linear regime, the coiled-coils unwind but not unfold. In the plastic regime, the triple α-helical segments rewind and re-unwind while undergoing a non-cooperative phase transition to form parallel β-sheets. We conclude that under extension and/or compression an α-helix to β-sheet conversion of the coiled-coils occurs in the fibrin clot as a part of forced protein unfolding. These regimes of forced elongation of fibrin provide important qualitative and quantitative characteristics of the molecular mechanisms underlying fibrin mechanical properties at the microscopic and macroscopic scales. Furthermore, these structural characteristics of the dynamic mechanical behavior of fibrin at the nanometer scale determine whether or not clots have the strength to stanch bleeding and if thrombi become obstructive or embolize. Finally, this knowledge of the functional significance of different domains of fibrin(ogen) suggests new approaches for modulation of these properties as potential therapeutic interventions. Disclosures: No relevant conflicts of interest to declare.


ACS Omega ◽  
2019 ◽  
Vol 4 (8) ◽  
pp. 13086-13099 ◽  
Author(s):  
Katarzyna Kopeć ◽  
Marta Pędziwiatr ◽  
Dominik Gront ◽  
Olga Sztatelman ◽  
Jakub Sławski ◽  
...  

2011 ◽  
Vol 175-176 ◽  
pp. 328-332 ◽  
Author(s):  
Wei Zhang ◽  
Jian Xin He ◽  
Yan Wang

Differences in secondary structure among Bombyx mori (B. mori) silk and two wild silks of Antheraea yamamai (A. yamamai) and Antheraea pernyi (A. pernyi) were investigated by CP/MAS 13C NMR Spectroscopy. The β-sheet structure was primary in three silk, and B. mori silk had the highest β-sheet structure. Although amino acid compositions are very similar for two wild silk, their secondary structures had significant difference. A. yamamai silk contained more α-helix structure, whereas more β-turn and random coil structures formed in A. pernyi silk. B. mori silk was mainly composed of anti-parallel β-sheet structure, however, the parallel β-sheet structure was advantage in the two wild silks, and A. yamamai silk contained more anti-parallel β-sheet conformation than A. pernyi silk.


2018 ◽  
Vol 232 (7-8) ◽  
pp. 1111-1125 ◽  
Author(s):  
Jim-Marcel Knop ◽  
Roland Winter

Abstract FTIR spectroscopy has been used to reveal the effects of different types of cosolvents (TMAO, urea) as well as macromolecular crowding (using the crowding agent Ficoll) on the temperature and pressure dependent structure of poly-L-lysine, poly-D-lysine and their racemic mixture. Compared to the effects of cosolvents on the unfolding transition of proteins, their effects on the α-helix to aggregated β-sheet transition of polylysine are quite small. High hydrostatic pressure has been found to favor the α-helical state over the aggregated β-sheet structure which is reflected in a volume decrease of ΔV=−32 mL mol−1, indicating that the packing mode is more efficient in the α-helical structure. Both, addition of urea and TMAO lead to a decrease in pressure stability of the aggregated β-sheet structure, which is accompanied by a three-fold decrease in ΔV, whereas the macromolecular crowder has little effect on the β-to-α transition. The more than 3 kbar higher β-to-α transition pressure of the racemic mixture compared with PLL confirms the drastic stabilization of β-sheet aggregates if the stereoisomers PLL and PDL are combined. Changes in hydration and packing of the polypeptide occurs upon interaction and fine packing of the polypeptide’s chains of opposed chirality, which are slightly modulated by the properties of cosolute and crowding, only. The underlying solvational and packing mechanisms observed here may be decisive factors responsible for the spontaneous protein aggregation in general and, as such, may shed additional light on the molecular basis of amyloid-associated diseases.


2020 ◽  
Vol 01 ◽  
Author(s):  
Zheng Zuo ◽  
Zongyun Chen ◽  
Zhijian Cao ◽  
Wenxin Li ◽  
Yingliang Wu

: The scorpion toxins are the largest potassium channel-blocking peptide family. The understanding of toxin binding interfaces is usually restricted by two classical binding interfaces: one is the toxin α-helix motif, the other is the antiparallel β-sheet motif. In this review, such traditional knowledge was updated by another two different binding interfaces: one is BmKTX toxin using the turn motif between the α-helix and antiparallel β-sheet domains as the binding interface, the other is Ts toxin using turn motif between the β-sheet in the N-terminal and α-helix domains as the binding interface. Their interaction analysis indicated that the scarce negatively charged residues in the scorpion toxins played a critical role in orientating the toxin binding interface. In view of the toxin negatively charged amino acids as “binding interface regulator”, the law of scorpion toxin-potassium channel interaction was proposed, that is, the polymorphism of negatively charged residue distribution determines the diversity of toxin binding interfaces. Such law was used to develop scorpion toxin-potassium channel recognition control technique. According to this technique, three Kv1.3 channel-targeted peptides, using BmKTX as the template, were designed with the distinct binding interfaces from that of BmKTX through modulating the distribution of toxin negatively charged residues. In view of the potassium channel as the common targets of different animal toxins, the proposed law was also shown to helpfully orientate the binding interfaces of other animal toxins. Clearly, the toxin-potassium channel interaction law would strongly accelerate the research and development of different potassium channelblocking animal toxins in the future.


2021 ◽  
Vol 11 (1) ◽  
Author(s):  
Ukrit Thamma ◽  
Tia J. Kowal ◽  
Matthias M. Falk ◽  
Himanshu Jain

AbstractThe nanostructure of engineered bioscaffolds has a profound impact on cell response, yet its understanding remains incomplete as cells interact with a highly complex interfacial layer rather than the material itself. For bioactive glass scaffolds, this layer comprises of silica gel, hydroxyapatite (HA)/carbonated hydroxyapatite (CHA), and absorbed proteins—all in varying micro/nano structure, composition, and concentration. Here, we examined the response of MC3T3-E1 pre-osteoblast cells to 30 mol% CaO–70 mol% SiO2 porous bioactive glass monoliths that differed only in nanopore size (6–44 nm) yet resulted in the formation of HA/CHA layers with significantly different microstructures. We report that cell response, as quantified by cell attachment and morphology, does not correlate with nanopore size, nor HA/CHO layer micro/nano morphology, or absorbed protein amount (bovine serum albumin, BSA), but with BSA’s secondary conformation as indicated by its β-sheet/α-helix ratio. Our results suggest that the β-sheet structure in BSA interacts electrostatically with the HA/CHA interfacial layer and activates the RGD sequence of absorbed adhesion proteins, such as fibronectin and vitronectin, thus significantly enhancing the attachment of cells. These findings provide new insight into the interaction of cells with the scaffolds’ interfacial layer, which is vital for the continued development of engineered tissue scaffolds.


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