Studies of ferroelectric properties of collagen

Dielectric hysteresis loop and differential thermal analysis (DTA) studies of collagen were performed for temperatures ranging from a room temperature to 393 K. The material studied was collagen from Achilles tendon of a bullock, which contained 10% of water. The DTA curve for collagen with 10% of water showed a clear minimum at 353 K. The character of the curve proved that around 353 K an endothermic transformation of collagen took place which could be connected with the transition spiral-ball. A hypothetical dielectric hysteresis loop shows a maximum shift along the direction of the electric field applied in the vicinity of 375 K. Low frequencies of the applied electric field are connected with a great dielectric loss influencing the interpretation of collagen ferroelectricity.     

小麦tae-MIR156前体基因的克隆及其靶基因TaSPL17多态性分析

Squamosa-promoter binding protein (SBP)-box基因是植物特有的一类转录因子, 广泛参与植物生长发育, 其部分成员受miR156调控。文章克隆了小麦(Triticum aestivum) tae-MIR156前体基因, 转录后能够形成茎环结构。小麦10个SBP-box基因中, 仅TaSPL3和TaSPL17在编码区存在tae-miR156识别位点。SPL17在普通小麦的A基因组供体种乌拉尔图小麦(Triticum urartu, AA) UR209和B基因组供体种拟斯卑尔脱山羊草(Aegilops speltoides, BB) Y2001中均为多拷贝(SPL17-A1、SPL17-A2和SPL17-A3; SPL17-B1、SPL17-B2和SPL17-B3), 在D基因组供体种粗山羊草(Aegilops tauschii, DD) Ae38中仅检测到一种序列(SPL17-D); SPL17-A2与SPL17-B2, SPL17-A3与SPL17-B3、SPL17-D两两之间序列的一致性程度均大于99%, 且与普通小麦(中国春、衡观35和双丰收)的TaSPL17序列具有较高的一致性, 提示它们可能来源于共同的祖先基因, 并且在进化过程中高度保守。靶基因TaSPL17中的tae-miR156识别位点非常保守, 在根据单株穗数和基因型多样性挑选的SubP1和SubP2群体中均未检测到tae-miR156识别位点存在变异碱基。     

Role of loop residues and cations on the formation and stability of dimeric DNA G-quadruplexes

Formation of guanine-quadruplexes by four DNA oligonucleotides with common sequence dG4-loop-dG4 has been studied by a combination of NMR and UV spectroscopy. The loops consisted of 1',2'-dideoxyribose, propanediol, hexaethylene glycol, and thymine residues. The comparison of data on modified and parent oligonucleotides gave insight into the role of loop residues on formation and stability of dimeric G-quadruplexes. All modified oligonucleotides fold into dimeric fold-back G-quadruplexes in the presence of sodium ions. Multiple structures form in the presence of potassium and ammonium ions, which is in contrast to the parent oligonucleotide with dT4 loop. 15N-filtered 1H NMR spectra demonstrate that all studied G-quadruplexes exhibit three 15NH4(+) ion binding sites. Topology of intermolecular G-quadruplexes was evaluated by NMR measurements and diffusion experiments. The spherical, prolate-ellipsoid and symmetric cylinder models were used to interpret experimental translational diffusion constants in terms of diameters and lengths of unfolded oligonucleotides and their respective G-quadruplexes. UV melting and annealing curves show that oligonucleotides with non-nucleosidic loop residues fold faster, exhibit no hysteresis, and are less stable than dimeric d(G4T4G4)2 which can be attributed to the absence of H-bonds, stacking between loop residues and the outer G-quartets as well as cation-pi interactions. Oligonucleotide consisting of hexaethylene glycol linkage with only two phosphate groups in the loop exhibits higher melting temperature and more negative deltaH(o) and deltaG(o) values than oligonucleotides with four 1',2'-dideoxyribose or propanediol residues.     

On the existence of a hysteresis loop in open and closed end pores

We have studied the adsorption of argon at 87 K in slit pores of finite length with a smooth graphitic potential, open at both ends or closed at one end. Simulations were carried out using conventional GCMC (grand canonical Monte Carlo) or kMC (kinetic Monte Carlo) in the canonical ensemble with extremely long Markov chain, of at least 2 × 10⁸ configurations; selected simulations with much longer Markov chains do not show any change in the results. When the pore width is in the micropore range (0.65 nm), type I isotherms are obtained for both pore models and for both simulation methods. However, wider pores (1, 2 and 3 nm in width) all exhibit hysteresis loops in the GCMC simulations, while in the canonical ensemble simulations, the isotherms pass through a sigmoid van der Waals type loop in the transition region. This loop locates the true equilibrium transition. For the pores with one closed end, this transition is close to, or coincides with, the adsorption branch of the GCMC hysteresis loop, but for the open-ended pores, it is more closely associated with the desorption branch. In a separate study of adsorption hysteresis in an infinitely long slit pore, using both simulation techniques, the van der Waals loop follows the adsorption branch of the GCMC isotherm to the transition, then reverts to a long vertical section that falls midway between the two hysteresis branches and finally moves to the desorption transition close to the evaporation pressure. An examination of molecular distributions inside the pores reveals two coexisting phases in the canonical simulations, whereas in the grand canonical simulations, the molecules are uniformly distributed along the length of the pores.     

Immunohistochemical analysis of sphingosine phosphate lyase expression during murine development

Sphingosine-1-phosphate lyase (SPL) catalyzes the degradation of sphingosine-1-phosphate (S1P), a bioactive lipid that controls cell proliferation, migration and survival. Mice lacking SPL expression exhibit developmental abnormalities, runting and death during the perinatal period, suggesting that SPL plays a role in mammalian development and adaptation to extrauterine life. We investigated the pattern of SPL expression in the mouse embryo and placenta from day 8 to day 18. Our findings reveal that SPL is expressed in the developing brain and neural tube, Rathke’s pouch, first brachial arch, third brachial arch, optic stalk, midgut loops, and lung buds. Diffuse signal was high at E12, whereas a recognizable adult SPL pattern was evident by E15 and more intensely at E18, with strong expression in skin, nasal epithelium, intestinal epithelium, cartilage, thymus and pituitary gland. These findings suggest SPL may be involved in development of the mammalian central nervous system (CNS), anterior pituitary, trigeminal nerve, palate and facial bones, thymus and other organs. Our findings are consistent with the SPL expression pattern of the adult mouse and with congenital abnormalities observed in SPL mutant mice.     

Spinophilin inhibits the binding of RGS8 to M1-mAChR but enhances the regulatory function of RGS8

We showed previously that RGS8 directly binds to the third intracellular loop (i3L) of the M1 muscarinic acetylcholine receptor using the sequence MPRR at the N-terminus of RGS8 and specifically inhibits signal transduction. Here, we identified spinophilin (SPL) as an RGS8-interacting protein. We found that the SPL-binding site of RGS8 is the MPRR sequence, and the M1 receptor and SPL compete for binding to RGS8. However, we also observed that the expression of SPL significantly enhances the inhibitory function of RGS8, and that SPL can bind to the M1 receptor, demonstrating the indirect binding of RGS8 to the M1 receptor through SPL for an efficient regulatory function.     

Spinophilin/neurabin reciprocally regulate signaling intensity by G protein-coupled receptors

Spinophilin (SPL) and neurabin (NRB) are structurally similar scaffolding proteins with several protein binding modules, including actin and PP1 binding motifs and PDZ and coiled-coil domains. SPL also binds regulators of G protein signaling (RGS) proteins and the third intracellular loop (3iL) of G protein-coupled receptors (GPCRs) to reduce the intensity of Ca(2+) signaling by GPCRs. The role of NRB in Ca(2+) signaling is not known. In the present work, we used biochemical and functional assays in model systems and in SPL(-/-) and NRB(-/-) mice to show that SPL and NRB reciprocally regulate Ca(2+) signaling by GPCRs. Thus, SPL and NRB bind all members of the R4 subfamily of RGS proteins tested (RGS1, RGS2, RGS4, RGS16) and GAIP. By contract, SPL, but not NRB, binds the 3iL of the GPCRs alpha(1B)-adrenergic (alpha(1B)AR), dopamine, CCKA, CCKB and the muscarinic M3 receptors. Coexpression of SPL or NRB with the alpha(1B)AR in Xenopus oocytes revealed that SPL reduces, whereas NRB increases, the intensity of Ca(2+) signaling by alpha(1B)AR. Accordingly, deletion of SPL in mice enhanced binding of RGS2 to NRB and Ca(2+) signaling by alphaAR, whereas deletion of NRB enhanced binding of RGS2 to SPL and reduced Ca(2+) signaling by alphaAR. This was due to reciprocal modulation by SPL and NRB of the potency of RGS2 to inhibit Ca(2+) signaling by alphaAR. These findings suggest a novel mechanism of regulation of GPCR-mediated Ca(2+) signaling in which SPL/NRB forms a functional pair of opposing regulators that modulates Ca(2+) signaling intensity by GPCRs by determining the extent of inhibition by the R4 family of RGS proteins.     

A semi-microscopic Monte Carlo study of permeation energetics in a gramicidin-like channel: the origin of cation selectivity.

The influence of a gramicidin-like channel former on ion free energy barriers is studied using Monte Carlo simulation. The model explicitly describes the ion, the water dipoles, and the peptide carbonyls; the remaining degrees of freedom, bulk electrolyte, non-polar lipid and peptide regions, and electronic (high frequency) permittivity, are treated in continuum terms. Contributions of the channel waters and peptide COs are studied both separately and collectively. We found that if constrained to their original orientations, the COs substantially increase the cationic permeation free energy; with or without water present, CO reorientation is crucial for ion-CO interaction to lower cation free energy barriers; the translocation free energy profiles for potassium-, rubidium-, and cesium-like cations exhibit no broad barriers; the lipid-bound peptide interacts more effectively with anions than cations; anionic translocation free energy profiles exhibit well defined maxima. Using experimental data to estimate transfer free energies of ions and water from bulk electrolyte to a non-polar dielectric (continuum lipid), we found reasonable ion permeation profiles; cations bind and permeate, whereas anions cannot enter the channel. Cation selectivity arises because, for ions of the same size and charge, anions bind hydration water more strongly.     

Hysteresis measurements in intact human tendon

Mechanical hysteresis in tendons has traditionally been quantified from tensile testing of isolated specimens. Limitations associated with tendon displacement measurement and clamping, and uncertainties as to whether in vitro material represents intact tendon function necessitate measuring hysteresis under in vivo conditions. In the present study such measurements were taken in the human tibialis anterior (TA) tendon. Having the foot fixed on a dynamometer footplate, the displacement of the TA tendon during stimulation and relaxation of the TA muscle was recorded by means of ultrasonography in six men. Combining moment data corresponding to 0, 20, 40, 60, 80 and 100% of maximum voltage moment and the respective tendon-displacement data, a hysteresis loop was obtained between the load–displacement curves during contraction and relaxation. Measurement of the hysteresis loop area yielded a value of 19%. This value agrees with results from in vitro tensile tests of low-stress tendons, suitable for tensile force transmission and joint displacement control. In fact, the human TA tendon has such functional characteristics. The methodology presented allows design of longitudinal and cross-sectional experimental protocols, and in vivo assessment of tendon function and propensity to overheat.     

Hydrophobic tendency of polar group hydration as a major force in type I antifreeze protein recognition

The random network model of water quantitatively describes the different hydration heat capacities of polar and apolar solutes in terms of distortions of the water-water hydrogen bonding angle in the first hydration shell (Gallagher and Sharp, JACS 2003;125:9853). The distribution of this angle in pure water is bimodal, with a low-angle population and high-angle population. Polar solutes increase the high-angle population while apolar solutes increase the low-angle population. The ratio of the two populations quantifies the hydrophobicity of the solute and provides a sensitive measure of water structural distortions. This method of analysis is applied to study hydration of type I thermal hysteresis protein (THP) from winter flounder and three quadruple mutants of four threonine residues at positions 2, 13, 24, and 35. Wild-type and two mutants (VVVV and AAAA) have antifreeze (thermal hysteresis) activity, while the other mutant (SSSS) has no activity. The analysis reveals significant differences in the hydration structure of the ice-binding site. For the SSSS mutant, polar groups have a typical polar-like hydration, that is, more high-angle H-bonds than bulk water. For the wild-type and active mutants, polar groups have unusual, very apolar-like hydration, that is, more low-angle H-bonds than bulk water. This pattern of hydration was seen previously in the structurally distinct type III THPs (Yang & Sharp Biophys Chem 2004;109:137), suggesting for the first time a general mechanism for different THP classes. The specific shape, residue size, and clustering of both polar and apoler groups are essential for an active ice binding surface.     

Seasonal hysteresis of net ecosystem exchange in response to temperature change: patterns and causes

Understanding how net ecosystem exchange (NEE) changes with temperature is central to the debate on climate change‐carbon cycle feedbacks, but still remains unclear. Here, we used eddy covariance measurements of NEE from 20 FLUXNET sites (203 site‐years of data) in mid‐ and high‐latitude forests to investigate the temperature response of NEE. Years were divided into two half thermal years (increasing temperature in spring and decreasing temperature in autumn) using the maximum daily mean temperature. We observed a parabolic‐like pattern of NEE in response to temperature change in both the spring and autumn half thermal years. However, at similar temperatures, NEE was considerably depressed during the decreasing temperature season as compared with the increasing temperature season, inducing a counter‐clockwise hysteresis pattern in the NEE–temperature relation at most sites. The magnitude of this hysteresis was attributable mostly (68%) to gross primary production (GPP) differences but little (8%) to ecosystem respiration (ER) differences between the two half thermal years. The main environmental factors contributing to the hysteresis responses of NEE and GPP were daily accumulated radiation. Soil water content (SWC) also contributed to the hysteresis response of GPP but only at some sites. Shorter day length, lower light intensity, lower SWC and reduced photosynthetic capacity may all have contributed to the depressed GPP and net carbon uptake during the decreasing temperature seasons. The resultant hysteresis loop is an important indicator of the existence of limiting factors. As such, the role of radiation, LAI and SWC should be considered when modeling the dynamics of carbon cycling in response to temperature change.     

Hydration structure of antithrombin conformers and water transfer during reactive loop insertion.

The serine protease inhibitor antithrombin undergoes extensive conformational changes during functional interaction with its target proteases. Changes include insertion of the reactive loop region into a beta-sheet structure in the protein core. We explore the possibility that these changes are linked to water transfer. Volumes of water transferred during inhibition of coagulation factor Xa are compared to water-permeable volumes in the x-ray structure of two different antithrombin conformers. In one conformer, the reactive loop is largely exposed to solvent, and in the other, the loop is inserted. Hydration fingerprints of antithrombin (that is, water-permeable pockets) are analyzed to determine their location, volume, and size of access pores, using alpha shape-based methods from computational geometry. Water transfer during reactions is calculated from changes in rate with osmotic pressure. Hydration fingerprints prove markedly different in the two conformers. There is an excess of 61-76 water molecules in loop-exposed as compared to loop-inserted conformers. Quantitatively, rate increases with osmotic pressure are consistent with the transfer of 73 +/- 7 water molecules. This study demonstrates that conformational changes of antithrombin, including loop insertion, are linked to water transfer from antithrombin to bulk solution. It also illustrates the combined use of osmotic stress and analytical geometry as a new and effective tool for structure/function studies.     

Dynamics of viscoelastic spherical membranes—the balloon model of the alveolus

Double-valued pressure-volume relationships in dynamic conditions for spherical membranes, modelling the lung alveoli, were obtained at small deformations. This hysteretic behavior was considered to be produced by at least three independent mechanisms: (1) the lung parenchyma exhibits viscoelastic properties; (2) the lung surface film, independent of the tissue, exhibits viscoelastic properties and (3) the pressure acting on the inner membrane surface depends on the rate of the alveolus volume change, due to the air viscous resistance in the bronchial tree. In each case, the maximum volume change, the hysteresis loop area, the tilt angle of the hysteresis loop and the relaxation time of the system were calculated. The results show pronounced hysteresis at normal breathing due to the air viscous resistance and smaller one due to the tissue and surface viscoelastic properties. In quasistatic conditions the values of the surface viscoelasticity and the tissue viscoelasticity effects are comparable or different, depending on the concrete external conditions. Comparison with the available experimental data is discussed in detail.     

Modeling baroreflex regulation of heart rate during orthostatic stress

During orthostatic stress, arterial and cardiopulmonary baroreflexes play a key role in maintaining arterial pressure by regulating heart rate. This study presents a mathematical model that can predict the dynamics of heart rate regulation in response to postural change from sitting to standing. The model uses blood pressure measured in the finger as an input to model heart rate dynamics in response to changes in baroreceptor nerve firing rate, sympathetic and parasympathetic responses, vestibulo-sympathetic reflex, and concentrations of norepinephrine and acetylcholine. We formulate an inverse least squares problem for parameter estimation and successfully demonstrate that our mathematical model can accurately predict heart rate dynamics observed in data obtained from healthy young, healthy elderly, and hypertensive elderly subjects. One of our key findings indicates that, to successfully validate our model against clinical data, it is necessary to include the vestibulo-sympathetic reflex. Furthermore, our model reveals that the transfer between the nerve firing and blood pressure is nonlinear and follows a hysteresis curve. In healthy young people, the hysteresis loop is wide, whereas, in healthy and hypertensive elderly people, the hysteresis loop shifts to higher blood pressure values, and its area is diminished. Finally, for hypertensive elderly people, the hysteresis loop is generally not closed, indicating that, during postural change from sitting to standing, baroreflex modulation does not return to steady state during the first minute of standing.     

Modeling of Hysteresis in Gene Regulatory Networks

Hysteresis, observed in many gene regulatory networks, has a pivotal impact on biological systems, which enhances the robustness of cell functions. In this paper, a general model is proposed to describe the hysteretic gene regulatory network by combining the hysteresis component and the transient dynamics. The Bouc-Wen hysteresis model is modified to describe the hysteresis component in the mammalian gene regulatory networks. Rigorous mathematical analysis on the dynamical properties of the model is presented to ensure the bounded-input-bounded-output (BIBO) stability and demonstrates that the original Bouc-Wen model can only generate a clockwise hysteresis loop while the modified model can describe both clockwise and counter clockwise hysteresis loops. Simulation studies have shown that the hysteresis loops from our model are consistent with the experimental observations in three mammalian gene regulatory networks and two E.coli gene regulatory networks, which demonstrate the ability and accuracy of the mathematical model to emulate natural gene expression behavior with hysteresis. A comparison study has also been conducted to show that this model fits the experiment data significantly better than previous ones in the literature. The successful modeling of the hysteresis in all the five hysteretic gene regulatory networks suggests that the new model has the potential to be a unified framework for modeling hysteresis in gene regulatory networks and provide better understanding of the general mechanism that drives the hysteretic function.     

The thermodynamics of water-protein interactions

Information about the effects of water on protein structure and function can be obtained from studies on freeze dried protein powders of varying water content. Sorption isotherms of water on proteins can be used to obtain thermodynamic quantities for water-protein interactions. Since such isotherms show hysteresis, there is doubt in regard to their interpretation.General expressions for the thermodynamic quantities of sorption are derived. If isotherms represent data at equilibrium, it is possible to calculate these thermodynamic quantities.There are two types of hysteresis, non-equilibrium hysteresis and equilibrium hysteresis. Absorption and desorption isotherms can show equilibrium hysteresis if different protein conformations, which are only slowly interconvertible, can be present. In this case valid thermodynamic quantities can be obtained. Experimental tests for equilibrium hysteresis are presented. More experiments are needed before definite conclusions can be drawn in regard to isotherms in the literature.If the protein conformation in a protein powder is similar to the protein conformation in aqueous solution, equilibrium data obtained from sorption isotherms can be used to approximate thermodynamic quantities for the interaction of water with proteins in aqueous solution. Examination of what experimental evidence is available indicates that the protein in powders prepared by desorption of water should have a conformation similar to that in solution. Further study of such samples will help to clarify the thermodynamics of water-protein interactions in aqueous solution.     

Influence of soil water stress on evaporation, root absorption, and internal water status of cotton

Diurnal variations in leaf water potential, diffusion resistance, relative water content, stem diameter, leaf temperature, and energy balance components were measured in cotton (Gossypium hirsutum L. var. Lankart 57) during drought stress under field conditions. A plot of leaf water potential against either relative water content or stem diameter during the 24-hour period yielded a closed hysteresis loop. The relation between cell hydration and evaporation is discussed.     

Spinophilin regulates Ca2+ signalling by binding the N-terminal domain of RGS2 and the third intracellular loop of G-protein-coupled receptors

Signalling by G proteins is controlled by the regulator of G-protein signalling (RGS) proteins that accelerate the GTPase activity of Galpha subunits and act in a G-protein-coupled receptor (GPCR)-specific manner. The conserved RGS domain accelerates the G subunit GTPase activity, whereas the variable amino-terminal domain participates in GPCR recognition. How receptor recognition is achieved is not known. Here, we show that the scaffold protein spinophilin (SPL), which binds the third intracellular loop (3iL) of several GPCRs, binds the N-terminal domain of RGS2. SPL also binds RGS1, RGS4, RGS16 and GAIP. When expressed in Xenopus laevis oocytes, SPL markedly increased inhibition of alpha-adrenergic receptor (alphaAR) Ca2+ signalling by RGS2. Notably, the constitutively active mutant alphaAR(A293E) (the mutation being in the 3iL) did not bind SPL and was relatively resistant to inhibition by RGS2. Use of betaAR-alphaAR chimaeras identified the 288REKKAA293 sequence as essential for the binding of SPL and inhibition of Ca2+ signalling by RGS2. Furthermore, alphaAR-evoked Ca2+ signalling is less sensitive to inhibition by SPL in rgs2-/- cells and less sensitive to inhibition by RGS2 in spl-/- cells. These findings provide a general mechanism by which RGS proteins recognize GPCRs to confer signalling specificity.     

Rheological analysis of viscoelastic cell wall changes in maize coleoptiles as affected by auxin and osmotic stress

The effects of auxin and osmotic stress on elongation growth of maize (Zea mays L.) coleoptile segments are accompanied by characteristic changes in the extensibility of the growth-limiting cell walls. At full turgor auxin causes growth by an increase in wall extensibility (wall looseining). Growth can be stopped by an osmotically produced step-down in turgor of 0.45 MPa. Under these conditions auxin causes the accumulation of a potential for future wall extension which is released after restoration of full turgor. Turgor reduction causes a reversible decrease in wall extensibility (wall stiffening) both in the presence and absence of auxin. These changes in vivo are correlated with corresponding changes in the rheological properties of the cell walls in vitro which can be traced back to specific modifications in the shape of the hysteretic stress-strain relationship. The longitudinally load-bearing walls of the coleoptile demonstrate almost perfect viscoelasticity as documented by a nearly closed hysteresis loop. Auxin-mediated wall loosening causes an increase of loop width and thus affects primarily the amount of hysteresis in the isolated wall. In contrast, turgor reduction by osmotic stress reduces loop length and thus affects primarily the amount of viscoelastic wall extensibility. Pretreatment of segments with anoxia and H₂O₂ modify the hysteresis loop in agreement with the conclusion that the wall-stiffening reaction visualized under osmotic stress in vivo is an O₂-dependent process in which O₂ can be substituted by H₂O₂. Cycloheximide specifically inhibits auxin-mediated wall loosening without affecting wall stiffening, and this is mirrored in specific changes of the hysteresis loop. Corroborating a previous in vivo study (Hohl et al. 1995, Physiol. Plant. 94: 491–498) these results show that cell wall stiffening in vivo can also be demonstrated by Theological measurements with the isolated cell wall and that this process can be separated from cell wall loosening by specific changes in the shape of the hysteresis loop.