第一类鱼抗冻蛋白对冰晶生长界面层结构的影响

根据冰晶在水溶液中生长的基本热力学性质,应用多层界面模型,分别得到了冰晶在纯水及抗冻蛋白溶液中生长界面层的吉布斯自由能.由冰晶生长界面层的吉布斯自由能,分析了冰晶在三种不同第一类鱼抗冻蛋白分子溶液中,热平衡状态下生长界面层的微观平衡结构,发现冰晶在抗冻蛋白溶液中生长与其在纯水中生长相比,界面层结构有明显变化,结合抗冻蛋...     

昆虫抗冻蛋白的研究进展

抗冻蛋白是一类与冰晶有亲合力,能够与冰晶结合并抑制冰晶生长的蛋白或糖蛋白。自20世纪60年代以来,研究人员已经分别从鱼类、昆虫、植物、真菌和细菌中发现多种抗冻蛋白。其中已知鱼类抗冻蛋白有5种,也是研究最详细的。但是,近几年来发现昆虫抗冻蛋白活性普遍比较高,因此受到研究人员重视,研究取得了较快的发展。主要讨论昆虫抗冻蛋白的结构特点、抗冻活性、作用机制和应用,并分析目前的研究现状提出一些待解决的问题,以期望对昆虫抗冻蛋白的研究进行比较系统化的整理。     

抗冻蛋白质——转移冷冻抗性的前景

大量的海洋栖息的动物和陆地的昆虫都能产生大分子的抗冻物质,以有助于它们生存在它们的不被保护的血液和血淋巴的体液的冰点之下的温度环境中。用这些抗冻物质结合和抑制冰晶生长的非浓度相关的方式。这样它们对一旦冰晶形成后的冰的融点就没有多大的影响了,所以研究者比较确切地将这类物质描述为热滞留蛋白质,因此这些蛋白质就成了检测抗冻能力的基础。     

两栖动物耐结冰机制及研究进展

寒带地区的两栖动物在冬眠期间可耐受体内结冰,并通过自身的生理生化机制降低冰晶对细胞的伤害：一方面将冰晶形成控制在细胞外,另一方面控制冰晶的形状和重结晶.其中耐结冰两栖动物体内的抗冻保护剂、冷冻反应基因和冷冻反应蛋白,在结冰期间起着关键的作用.     

植物抗冻基因研究进展

低温是作物生长一大限制因素,许多作物不能在低温下生长或者容易受到冻害,所以通过基因工程的方法,转入抗冻基因,是扩大作物生长区域,稳定作物产量的有效办法。目前通过对植物抗冻基因在抗冻机理、研究技术、应用等方面的研究,已经取得了一定的成果。综述抗冻基因的来源、抗冻机理、研究技术,并做适度的展望。     

差示扫描量热法直接测定抗冻蛋白质溶液的热滞效应

文献上一直用显微镜观察法等测定抗冻蛋白的热滞效应,其冰晶量是靠观察晶核体积估算得得的,人为性很大,用并示扫描量热法直接测定沙冬青抗冻蛋白质溶液的热滞效应,通过熔融焓和冻结焓值准确地测定了冰晶含有量和热滞温度。同文献比较,沙冬青ＡＦＰ具有极高的抗冻活性,而且开创了一个新的有效的测量抗冻蛋白抗冻活性的途径。     

钙与钙调素对柑橘原生质体抗冻性的影响

钙与钙调素对柑橘原生质体低温锻炼过程中抗冻力的获得有影响。加钙螯合剂或钙调素拮抗剂ＴＦＰ,能明显抑制柑橘原生质体抗冻性的表达。钙离子载体Ａ２３１８７可提高未经低温锻炼的原生质体抗冻力,但该作用在钙调素拮抗剂ＴＦＰ参入下则减弱,表明原生质体抗冻力的表达受钙和钙调素的调节。     

南极细菌胞外多糖溶液冻结特性的差示扫描量热研究

采用差示扫描量热法,测定几种南极细菌胞外多糖(简称,EPSs)溶液的结晶、熔融、焓转变以及水合性质等冻结特性,分析了EPSs的浓度和分子量与其抗冻活性的关系.结果表明,在溶液冻结过程中,仅0.25%的Pseudoalteromonas sp.S-15-13 EPSs(分子量,6.2×104Da)可抑制冰核形成,溶液冻结温度较纯水的降低(1.07±0.62)℃;溶液的冻结焓降低说明冰核生长变缓,冰晶形成细小,0.125%的Shewanella sp.5-1-11-4 EPSs(分子量,1.2×103Da)和Moritella sp.2-5-10-1 EPSs(分子量,3.0×103Da)冻结焓分别较纯水的降低17.15%和29.13%,S-15-13 EPSs在0.125%～0.5%的范围内可降低冻结焓,0.125%时冻结焓较纯水的低30%,其不冻水含量为(0.292 ±0.05) g/g.在冰晶熔化过程中,几种EPSs均可降低溶液熔融温度和熔融焓,促进冰晶熔化,使冰晶细小;4.0%的5-1-11-4 EPSs、2-5-10-1 EPSs和0.5% S-15-13 EPSs的熔融温度较纯水的分别降低(2.70±0.15)℃、(2.30±0.39)℃和(4.66±0.42)℃.研究结果阐明EPSs可以通过改变菌体周围水的冻结特性,以抵御冰晶对微生物的损伤,大分子量EPSs对冰晶的抑制作用强于低分子量的.     

抗冻蛋白研究进展(英文)

很多越冬的生物会产生抗冻蛋白,这些抗冻蛋白能够吸附到冰晶的表面改变冰晶形态并抑制冰晶的生长.抗冻蛋白在很多生物体内都被发现,不同的抗冻蛋白结构差异非常大.目前的一些研究揭示了几种抗冻蛋白的结构,并提出了抗冻蛋白与冰晶的结合模型,但是还没有一种机制能解释所有抗冻蛋白的作用机理.抗冻蛋白能被广泛的应用到农业、水产业和低温储藏器官、组织和细胞,利用转基因技术提高植物的抗冻性具有重要应用价值.而抗冻蛋白基因的表达调控则有待进一步阐明.     

抗冻蛋白与植物低温胁迫反应

植物抗冻蛋白是从许多抗冻植物中分离的、参与植物抵御冻害反应的一类新型蛋白.这类抗冻蛋白具有多个亲水性缚冰域,能直接作用于冰晶,阻止冰晶在细胞间隙形成和再结晶.一些植物抗冻蛋白与致病相关蛋白有序列同源性,具有抗冻和抗病双重活性.植物抗冻蛋白的表达和积累,既受控于发育及转录因子调节,又受到低温、短日照、脱水及乙烯等因素的影响.异源超表达抗冻蛋白基因能赋予敏感宿主植物抗冻能力.文中论述了有关植物抗冻蛋白特性和鉴定,抗冻机制和表达调控,以及遗传转化等方面的研究进展.     

甲虫抗冻蛋白热滞活性的二维吸附结合模型

甲虫抗冻蛋白是一种具有规则结构的昆虫抗冻蛋白。在相同浓度条件下,甲虫抗冻蛋白比鱼类抗冻蛋白有更高的热滞活性,目前已成为人们重点研究的一类抗冻蛋白。根据甲虫抗冻蛋白的结构特点及其在冰晶表面的吸附模式,应用二维吸附结合模型计算分析了具有6￣11个β-螺旋(β-helix)结构片段的甲虫抗冻蛋白变体分子,得到了它们的热滞活性随溶液浓度变化的规律,特别是热滞活性与甲虫抗冻蛋白的β-螺旋结构片段数的关系。结果显示,抗冻蛋白在冰晶表面的覆盖度是一个影响其热滞活性的重要因素。     

The importance of dissolved salts to the in vivo efficacy of antifreeze proteins

Antifreeze proteins (AFP) and antifreeze glycoproteins (AFGP) lower the freezing point of marine fish plasma non-colligatively by specifically adsorbing to certain surfaces of ice crystals, modifying their structure and inhibiting further growth. While the freezing point is lowered, the melting point is unaltered and the difference between the two is termed thermal hysteresis (TH). In pure water, the level of TH is directly related to the intrinsic activity of the specific AF(G)P in solution and to their concentration. Results of this study indicate that when AF(G)P are dissolved in salt solutions, such as NaCl, encompassing the range they could encounter in nature, there is a synergistic enhancement of basal TH that is positively related to the salt concentration. This enhancement is likely a result of the hydration shell surrounding the dissolved ions and, as a consequence, reducing freezable water. A secondary reason for the enhancement is that the salt could be influencing the hydration shell surrounding the AF(G)P, increasing their solubility and thus the protein surface area available to adsorb to the ice/water interface. The former hypothesis for the salt enhanced TH has implications for the in vivo function of AF(G)P, particularly at the seawater/external epithelia (gills, skin, stomach) interface. The latter hypothesis is likely only relevant to in vitro situations where freeze dried protein is dissolved in low salt solutions.     

The effect of enhanced alpha-helicity on the activity of a winter flounder antifreeze polypeptide.

The antifreeze polypeptide (AFP) from the winter flounder displays partial alpha-helix formation at lower temperatures. To investigate the relationship between antifreeze activity and alpha-helical structure, we designed and then chemically synthesized an AFP analog with enhanced alpha-helicity, and compared its conformation and antifreeze properties with those of the native AFP. The synthetic analog was more helical than the native AFP; however, the antifreeze activity of both peptides were identical. The antifreeze activity of the peptides displayed a strong pH dependence, which paralleled pH-induced changes in helix content. At pH 8.5, the antifreeze activity of both peptides displayed identical concentration dependences. In addition to antifreeze activity measurements, the effects of the peptides on the rate of ice crystal growth were also measured. While both peptides affected the a- and c-axis growth rates of ice crystals, the highly helical analog was able to exert its effect on ice crystal growth rates at 7-8-fold lower concentrations than the native AFP. These data indicate that there is a direct but complex relationship between alpha-helicity and antifreeze activity.     

Structure-function relationship in a winter flounder antifreeze polypeptide. II. Alteration of the component growth rates of ice by synthetic antifreeze polypeptides

Using synthetic analogs of an alpha-helical winter flounder antifreeze polypeptide (AFP) we investigated some important molecular details of the mechanism of action of this AFP. Of the seven peptides synthesized, all but one were amino-terminal deletions of the native AFP. Three of the seven synthetic analogs possessed the same antifreeze activity as the native polypeptide; the other analogs were devoid of antifreeze activity. The growth rates along the a and c axes of ice in solutions of varying concentrations of the three active AFP analogs were examined. The a axis growth rates of ice were inversely proportional to the concentration of the active peptides. The c-axis growth rates of ice were also dependent on peptide concentration. The active peptides enhanced c-axis growth at lower concentrations, while at higher concentrations they inhibited c axis growth. The ability of the peptides to develop antifreeze activity and to alter the a and c axis growth rates of ice depended on the presence of appropriately positioned amino acid residues with hydrogen bonding side chains. From these observations we propose that at low concentrations the AFP, through dipolar interactions and hydrogen bonding, interact with the prism faces of ice retarding a axis growth. At these concentrations, the electrical field of the AFP helix-dipole, like an externally applied field (Bartlett, J.T., van der Heuval, A.P., and Mason, B.J. (1963) Z. Angew. Math. Phys. 14, 599-610), can enhance ice c axis growth. At higher concentrations, the AFP interact with all ice crystal planes and retard both a and c axis growth.     

抗冻蛋白溶液的热滞理论

鱼抗冻蛋白溶液有热滞效应,这是一种非ｃｏｌｌｉｇａｔｉｖｅ效应．提出冰晶生长的动力学理论,并根据Ｆｌｏｒｙ－Ｈｕｇｇｉｎ晶格模型计算抗冻蛋白溶液的热滞,结果与实验较好地符合。     

The mechanism by which fish antifreeze proteins cause thermal hysteresis

Antifreeze proteins are characterised by their ability to prevent ice from growing upon cooling below the bulk melting point. This displacement of the freezing temperature of ice is limited and at a sufficiently low temperature a rapid ice growth takes place. The separation of the melting and freezing temperature is usually referred to as thermal hysteresis, and the temperature of ice growth is referred to as the hysteresis freezing point. The hysteresis is supposed to be the result of an adsorption of antifreeze proteins to the crystal surface. This causes the ice to grow as convex surface regions between adjacent adsorbed antifreeze proteins, thus lowering the temperature at which the crystal can visibly expand. The model requires that the antifreeze proteins are irreversibly adsorbed onto the ice surface within the hysteresis gap. This presupposition is apparently in conflict with several characteristic features of the phenomenon; the absence of superheating of ice in the presence of antifreeze proteins, the dependence of the hysteresis activity on the concentration of antifreeze proteins and the different capacities of different types of antifreeze proteins to cause thermal hysteresis at equimolar concentrations. In addition, there are structural obstacles that apparently would preclude irreversible adsorption of the antifreeze proteins to the ice surface; the bond strength necessary for irreversible adsorption and the absence of a clearly defined surface to which the antifreeze proteins may adsorb. This article deals with these apparent conflicts between the prevailing theory and the empirical observations. We first review the mechanism of thermal hysteresis with some modifications: we explain the hysteresis as a result of vapour pressure equilibrium between the ice surface and the ambient fluid fraction within the hysteresis gap due to a pressure build-up within the convex growth zones, and the ice growth as the result of an ice surface nucleation event at the hysteresis freezing point. We then go on to summarise the empirical data to show that the dependence of the hysteresis on the concentration of antifreeze proteins arises from an equilibrium exchange of antifreeze proteins between ice and solution at the melting point. This reversible association between antifreeze proteins and the ice is followed by an irreversible adsorption of the antifreeze proteins onto a newly formed crystal plane when the temperature is lowered below the melting point. The formation of the crystal plane is due to a solidification of the interfacial region, and the necessary bond strength is provided by the protein "freezing" to the surface. In essence: the antifreeze proteins are "melted off" the ice at the bulk melting point and "freeze" to the ice as the temperature is reduced to subfreezing temperatures. We explain the different hysteresis activities caused by different types of antifreeze proteins at equimolar concentrations as a consequence of their solubility features during the phase of reversible association between the proteins and the ice, i.e., at the melting point; a low water solubility results in a large fraction of the proteins being associated with the ice at the melting point. This leads to a greater density of irreversibly adsorbed antifreeze proteins at the ice surface when the temperature drops, and thus to a greater hysteresis activity. Reference is also made to observations on insect antifreeze proteins to emphasise the general validity of this approach.     

Cooperative function of ammonium polyacrylate with antifreeze protein type I

Activity of antifreeze proteins (AFPs) and antifreeze glycoproteins (AFGPs) is often determined by thermal hysteresis, which is the difference between the melting temperature and the nonequilibrium freezing temperature of ice in AF(G)P solutions. In this study, we confirmed that thermal hysteresis of AFP type I is significantly enhanced by a cooperative function of ammonium polyacrylate (NH4PA). Thermal hysteresis of mixtures of AFP type I and NH4PA was much larger than the sum of each thermal hysteresis of AFP type I and NH4PA alone. In mixed solutions of AFP type I and NH4PA in the thermal hysteresis region, hexagonal pyramidal-shaped pits densely formed on ice surfaces close to the basal planes. The experimental results suggest that the cooperative function of NH4PA with AFP type I was caused either by the increase in adsorption sites of AFP type I on ice or by the adsorption of AFP type I aggregates on ice.     

The mechanism by which fish antifreeze proteins cause thermal hysteresis

Antifreeze proteins are characterised by their ability to prevent ice from growing upon cooling below the bulk melting point. This displacement of the freezing temperature of ice is limited and at a sufficiently low temperature a rapid ice growth takes place. The separation of the melting and freezing temperature is usually referred to as thermal hysteresis, and the temperature of ice growth is referred to as the hysteresis freezing point. The hysteresis is supposed to be the result of an adsorption of antifreeze proteins to the crystal surface. This causes the ice to grow as convex surface regions between adjacent adsorbed antifreeze proteins, thus lowering the temperature at which the crystal can visibly expand. The model requires that the antifreeze proteins are irreversibly adsorbed onto the ice surface within the hysteresis gap. This presupposition is apparently in conflict with several characteristic features of the phenomenon; the absence of superheating of ice in the presence of antifreeze proteins, the dependence of the hysteresis activity on the concentration of antifreeze proteins and the different capacities of different types of antifreeze proteins to cause thermal hysteresis at equimolar concentrations. In addition, there are structural obstacles that apparently would preclude irreversible adsorption of the antifreeze proteins to the ice surface; the bond strength necessary for irreversible adsorption and the absence of a clearly defined surface to which the antifreeze proteins may adsorb. This article deals with these apparent conflicts between the prevailing theory and the empirical observations. We first review the mechanism of thermal hysteresis with some modifications: we explain the hysteresis as a result of vapour pressure equilibrium between the ice surface and the ambient fluid fraction within the hysteresis gap due to a pressure build-up within the convex growth zones, and the ice growth as the result of an ice surface nucleation event at the hysteresis freezing point. We then go on to summarise the empirical data to show that the dependence of the hysteresis on the concentration of antifreeze proteins arises from an equilibrium exchange of antifreeze proteins between ice and solution at the melting point. This reversible association between antifreeze proteins and the ice is followed by an irreversible adsorption of the antifreeze proteins onto a newly formed crystal plane when the temperature is lowered below the melting point. The formation of the crystal plane is due to a solidification of the interfacial region, and the necessary bond strength is provided by the protein “freezing” to the surface. In essence: the antifreeze proteins are “melted off” the ice at the bulk melting point and “freeze” to the ice as the temperature is reduced to subfreezing temperatures. We explain the different hysteresis activities caused by different types of antifreeze proteins at equimolar concentrations as a consequence of their solubility features during the phase of reversible association between the proteins and the ice, i.e., at the melting point; a low water solubility results in a large fraction of the proteins being associated with the ice at the melting point. This leads to a greater density of irreversibly adsorbed antifreeze proteins at the ice surface when the temperature drops, and thus to a greater hysteresis activity. Reference is also made to observations on insect antifreeze proteins to emphasise the general validity of this approach.