GTPγs对柴胡皂甙(I)刺激胰腺腺泡酶分泌的影响

为了解柴胡皂甙(I)[SA(I)]刺激大鼠胰腺腺泡酶分泌的信号传导通路,研究了GTPγs对SA(I)剌激通透腺泡细胞酶分泌的影响.用SLO通透细胞的同时,加入GTPγs在15min期间能诱发酶分泌,10'mol·L-1GTPγs有最大促泌效应.GTPγs浓度依赖性的增强SA(I)促酶分泌作用,l0-7 mol·L-1 GTPγs导致10-5mol·L-1 SA(I)刺激酶分泌量增加到1.6倍.用SLO预通透腺泡10min后,加入GTPγs使SA(I)刺激酶分泌的量-效曲线左移,SA(I)的EC50从2 0×10-5mol·L-1减小到1 0×10-5mol·L-1.以上结果提示,SA(I)活化受体偶联的G蛋白包括在其刺激酶分泌的信号传导通路中.     

植物多糖胶流变性质的研究

胡芦巴、皂荚、野皂荚和塔拉多糖胶水溶液随着浓度的增加,溶液表现为假塑性流体．表现粘度随剪切速率增大而减小。通过Cross模型和实验数据计算得到1％多糖胶零剪切速率时表现粘度η0、无穷大剪切速率时表现粘度η∞和弹性松驰时间等重要流变参数。根据Arrhenius方程和实验数据计算得到1％浓度多糖胶的粘度流化能E和常数A,皂荚胶和塔拉胶的粘流活化能大。时间对多糖胶液粘度影响较大,新配制的多糖胶液随着水化时间的延长,胶液表观粘度增大,胶液放置时间超过24h后,表现粘度随时间的延长而降低。pH值、冻融处理和盐离子对多糖胶表现粘度的影响不太大。多糖胶与硼离子形成的冻胶．其粘度因多糖胶品种而异,其中胡芦巴冻胶粘度最高,是野皂荚冻胶粘度的165倍和瓜尔胶冻胶粘度的2．7倍。     

圆叶蒙桑的组织培养与快速繁殖

1植物名称圆叶蒙桑(Morus mongolica var.rotundifolia)。2材料类别茎及茎尖。3培养条件以MS为基本培养基。(1)诱导及增殖培养基:MS+6-BA1mg·L-1(单位下同)+NAA0.1。(2)生根培养基:1/2MS+IBA1。以上培养基中均加入3%的蔗糖和0.8%琼脂,pH5.8。培养温度为(24±2)℃,光照时间12h·d-1,光强40μmol·m-2·s-1左右。4生长与分化情况4.1芽的诱导采集无病虫害、生长健壮的圆叶蒙桑枝条,剪掉叶片后用流水冲洗干净,在超净台上,剪成0.5～1.0cm的茎段和茎尖,放置在75%的酒精中浸泡20s,无菌水冲洗3～4遍,用次氯酸钠灭菌10min,再用无菌水冲洗3～4…     

不同发育阶段尖头斜齿鲨肝油脂酸组成的变化

采用气相色谱仪分析测定了不同发育阶段尖头斜齿鲨肝油的脂肪酸组成与含量。在尖头斜齿鲨肝油总脂肪酸组成中 ,饱和脂肪酸占 15 3%～ 34 6 % ,单不饱和脂肪酸占 13 8%～ 2 5 6 % ,多不饱和脂肪酸 (PUFA)占 38 8%～ 6 8 1%。其中 ,最主要的脂肪酸为 16 :0 ,18:0 ,18:1ω9,2 0 :4ω6和 2 2 :6ω3。尖头斜齿鲨肝油脂肪酸组成与个体的发育状况关系密切。雄性尖头斜齿鲨 ,胚胎阶段肝油的脂肪酸主要由16 :0、 16 :1和 18:1(ω9+ω7)组成 ,2 2 :6ω3的含量很低 (3 8± 1 34 ,n =3) ;雄性幼鱼肝油 2 2 :6ω3的含量较胚胎阶段有了显著的提高 (2 7 1± 2 47,n =3) (P <0 0 5 ) ;性成熟个体肝油 2 2 :6ω3的含量达到最高值 (5 1 0± 7 42 ,n =5 ) ,退化期 2 2 :6ω3的含量明显降低 (34 4± 2 40 ,n =3)。雌性尖头斜齿鲨肝油 2 2 :6ω3的含量随着性腺的发育而逐渐增加 ,妊娠早期达到最高值 (49 7± 4 0 4,n =5 ) ,显著高于未成熟期个体 (2 5 7± 0 6 4,n =3)和卵巢发育期个体 (33 3± 3 46 ,n =4) ,妊娠结束期肝油 2 2 :6ω3的含量显著下降 (2 5 6± 8 0 8,n =3) ,提示 2 2 :6ω3在尖头斜齿鲨胚胎的生长发育中可能起了重要作用。     

黄土高原4种豆科牧草的净光合速率和蒸腾速率日动态及水分利用效率

在晴天条件下 ,研究了 4年生甘肃红豆草 (Onobrychis viciaefolia scop.cv.‘Gansu’)、沙打旺 (Astragalus adsurgens)、东方山羊豆 (Galega orientalis)和多年生香豌豆 (L athyruslatifolius)人工种群花期 (5月 31日 )和再生期 (7月 10日 )的净光合速率、蒸腾速率、气孔导度、水分利用效率以及土壤贮水量和水分利用特征。结果表明 ,自 5月 31日 (花期 )至 7月 10日 (再生期 ) ,4种牧草对土壤水分消耗由大到小依次为 :沙打旺 119.2 mm、多年生香豌豆 91.6 mm、山羊豆 81.9m m和红豆草 73.8m m。红豆草在花期和再生期的净光合速率分别为 12 .4 1和 9.0 6μ mol CO2 / (m2 · s) ,沙打旺为 10 .10和 7.0 1μ m ol CO2 / (m2 · s) ;红豆草在花期和再生期的日均蒸腾速率 8.13和 9.0 5 m m ol H2 O/ (m2· s) ,沙打旺刈割前和刈割后蒸腾速率分别为 7.4 0和 6 .5 4mmol H2 O/ (m2· s) ,属于高光合、高蒸腾型。而山羊豆和多年生香豌豆则属于低蒸腾、低光合类型 ,花期和再生期 ,山羊豆的日均光合速率分别为 4 .74和 4 .88μm ol CO2 / (m2· s) ,多年生香豌豆为 4 .4 1和 4 .6 4 μ mol CO2 / (m2· s) ,相应的蒸腾速率分别达到 3.75和 5 .4 2 m mol H2 O/ (m2 · s) ,4 .74和 4 .34m mol H2 O/ (m2 · s)。     

Willis环状脑动脉瘤的生物数学模型的周期解

本文运用扭转映射的不动点定理,通过Poincare'映射,在(μ/2)+((β~2)/(4a))<1的条件下,证明了Willis环状脑动脉瘤生物数学模型 +μ+αx-βx~2+γx~3=Fcosωt(其中μ,α,β,γ,F,ω都是正常数)至少存在一个(2π)/ω周期解。     

耐高温酵母乙醇间歇发酵动力学研究

该研究采用耐高温型酵母,在不同葡萄糖浓度(5%~30%wt)下进行了乙醇间歇发酵的动力学研究,确定了适合该酵母的最佳底物浓度范围为16%~20%(wt)。同时选取合适的动力学模型,通过实验数据的非线性性拟合,得出了不同底物浓度下对应的动力学参数值,并分析了各动力学参数值随底物浓度增加而变化的趋势。结果显示,该酵母的最大比生长速率μmax随着葡萄糖浓度的增加而有所降低,且呈线性关系:μmax=0.3161-4.1820×104s(100g/L相似文献   

青阳参的组织培养和植株再生

1植物名称青阳参(Cynanchum otophyllumSchneid.),别名青洋参。2材料类别成熟种子。3培养条件(1)芽诱导培养基:MS+6-BA2.0mg·L-1(单位下同)+NAA1.0;(2)芽增殖培养基:MS+6-BA2+NAA0.2;(3)生根培养基:1/4MS。以上培养基中除生根培养基蔗糖含量2%外,其余均为3%。pH5.8,琼脂含量为0.8%。培养温度(25±2)℃,光照12h·d-1,光强为40μmol·m-2·s-1。4生长与分化情况4.1无菌苗的获得将种子用洗衣粉水洗净,流水冲洗30min后,在无菌条件下先用75%酒精浸泡30s,无菌水冲洗3次,再用0.1%升汞水浸泡10min,无菌水冲洗5次,消毒滤纸吸干表面水分,接…     

HPLC法测定麻仁润肠丸大黄素、大黄酚的含量

采用KromacilC18(4 .6mm× 2 5 0mm ,5 μm)色谱柱 ,以甲醇 - 0 .1%磷酸溶液 (85∶15 )为流动相 ,流速为 1mL·min ,柱温为 30℃ ,检测波长为 2 5 4nm ,以外标法测定了麻仁润肠丸中大黄素、大黄酚的含量。大黄素在 8.992× 10 -3 ～ 116 .896× 10 -3 ,大黄酚在 2 1.376× 10 -3 ～ 2 77.85 8× 10 -3 范围内呈线性关系 ,其在制剂中的平均回收率 (n =6 )分别为 10 1.5 6 % (RSD =1.3% )、96 .78% (RSD =1.3% )。     

热水溶胡卢巴胶的流变性研究

主要对胡卢巴胶（热水溶部分）的流变性进行了研究。结果表明：浓度,剪切力,加热时间,pH,冻融等变化与胡卢巴胶的粘度有较大的关系。胡卢巴胶具有较高的粘度,当浓度达到1%时,其粘度为920mpa·s^-1,胡卢巴胶溶液为非牛屯流体;小于1h加热,可使其粘度增高。胡卢巴胶溶液在酸性和酸性溶液中较为稳定。冻融处理可使胡卢巴胶溶液粘度有较大幅度的提高,胡卢巴胶与卡拉胶有一定协效性,但其协效性较低。     

Physicochemical characterization of konjac glucomannan

Four commercial konjac glucomannan (KGM) samples and a glucomannan derived from yeast were characterized by aqueous gel permeation chromatography coupled with multi angle laser light scattering (GPC-MALLS). Disaggregation of aqueous glucomannan solutions through controlled use of a microwave bomb facilitated reproducible molar mass distribution determination alleviating the need for derivatization of the polymer or the use of aggressive solvents. Further characterization was undertaken by use of capillary viscometry and photon correlation spectroscopy (PCS). The weight average molecular masses (M(w)) determined were in the region of 9.0 +/- 1.0 x 10(5) g mol(-1) for KGM samples and 1.3 +/- 0.4 x 10(5) g mol(-1) for the yeast glucomannan. The values determined for KGM in aqueous solution are in agreement with those reported for KGM in aqueous cadoxen. The degradation of samples observed upon autoclaving has been quantified by GPC-MALLS and intrinsic viscosity determination, allowing comparison with reported Mark-Houwink parameters. Shear flow experiments were undertaken for a range of KGM solutions of concentration 0.05 to 2.0% using a combination of controlled stress and controlled strain rheometers. The concentration dependence of the zero shear specific viscosity was determined by analysis of the data using the Ellis model. The dependence of the zero shear specific viscosity on the coil overlap parameter was defined and interpretation discussed in terms of the Martin and Tuinier equations.     

Relationship between the Rheological Properties of Thickener Solutions and Their Velocity through the Pharynx as Measured by the Ultrasonic Pulse Doppler Method

The dependence of the dynamic viscoelastic parameters of carboxymethylcellulose (CMC), xanthan gum, and guar gum solutions on the angular frequency (ω) was compared with that of their viscosity (μ) on the shear rate (γ). In addition, the effect of these rheological properties on the maximum velocity through the pharynx, V _max, as measured by the ultrasonic pulse Doppler method, was investigated. The CMC and guar gum solutions examined were taken as a dilute solution and a true polymer solution, respectively. The xanthan gum solution was taken as a weak gel above 0.5% and a true polymer solution below 0.2%. The maximum velocity, V _max, of the thickener solutions correlated well with μ, the dynamic viscosity η′, and the complex viscosity η^*, especially those measured at γ or ω of 20–30 s^?1 (or rad/s) and above, suggesting that μ, η′, and η^* are suitable indexes for care foods of the liquid type for dysphagic patients.     

Effect of concentration and temperature on the rheological behavior of collagen solution

Dynamic viscoelastic properties of collagen solutions with concentrations of 0.5-1.5% (w/w) were characterized by means of oscillatory rheometry at temperatures ranging from 20 to 32.5 degrees C. All collagen solutions showed a shear-thinning flow behavior. The complex viscosity exhibited an exponential increase and the loss tangent decreased with the increase of collagen concentration (C(COL)) when the C(COL)> or =0.75%. Both storage modulus (G') and loss modulus (G') increased with the increase of frequency and concentration, but decreased with the increase of temperature and behaved without regularity at 32.5 degrees C. The relaxation times decreased with the increase of temperature for 1.0% collagen solution. According to a three-zone model, dynamic modulus of collagen solutions showed terminal-zone and plateau-zone behavior when C(COL) was no more than 1.25% or the stated temperature was no more than 30 degrees C. The concentrated solution (1.5%) behaved being entirely in plateau zone. An application of the time-temperature superposition (TTS) allowed the construction of master curve and an Arrhenius-type TTS principle was used to yield the activation energy of 161.4 kJ mol(-1).     

Physicochemical properties of extrusion-modified konjac glucomannan

Konjac glucomannan was extruded and subsequently ground under four conditions denoted: KGM1 (33% solids, 90 °C), KGM2 (24% solids, 90 °C), KGM3 (24% solids, 90 °C, die restriction), and KGM4 (24% solids, 110 °C). SEM and particle size analysis showed that extruded KGM had slightly larger and rougher particles. The water absorption index was decreased to 47.92-128.80, as compared to 153.64 for the control (KGMC). The crystallinity index increased to 2.97 and 3.42 for KGM3 and KGM4 samples, as compared to 1.72 for the control. Zero-shear viscosity of 0.5% solutions decreased to 0.36-3.01 Pa s. All samples were shear-thinning and data were best fitted by the Cross model. Based on capillary viscometry, molecular weights were decreased to 2.7 × 10⁵-9.9 × 10⁵, as compared to 1.2 × 10⁶ for the control. In most cases, properties were most altered by higher temperature and shear, and to a lesser extent by lower solids in the feed.     

Viscoelastic relaxations in solutions of poly(glutamic acid) and gelatin at ultrasonic frequencies

Complex shear viscosity η* = η′ – iη″ of poly (L -glutarmic acid) solution was measured by the torsional crystal method at 50 kc./sec. as a function of pH. A sharp peak was found at the midpoint of the helix-coil transition region in both η′ and η″. The relaxation time is calculated from η′ and η″ assuming a single relaxation process and the peak value at the midpoint of transition is estimated at 10^?6 sec. Such behavior agrees well with the prediction from the theory of Schwarz. The attenuation of longitudinal sound waves at,3 Me./sec. was measured as a function of pH for solutions of poly(glutamic acid), glutamic acid, and gelatin. A small attenuation peak was observed for the three solutions, the peak height being almost, the same for them. The peak is interpreted in terms of the dissociation reaction of side chains.     

Properties of complexes of galactomannan of Leucaena leucocephala and Al3+, Cu2+ and Pb2+

The use of biopolymers in many industrial processes is on the increase. The different interactions of biopolymers and electrolytes either in aqueous solutions or in solid state provide different physico-chemical properties and a simple correlation cannot be established. In this study, in order to determine the properties of the complexes of galactomannan of Leucaena leucocephala (gal) with the metal ions Al3+ and Pb2+, toxic elements and Cu2+, essential, the logs of the binding constants of the complexes formed in the aqueous solutions were calculated. Their rheological properties, their thermal behavior, the infrared characteristics and shape and form of the films formed by those complexes in solid state were also determined. The aqueous solutions properties have shown a better complexation between gal and Al3+. The species distribution diagrams have shown an existence of complex species going from acidic to basic pH values. Infrared spectra have proved the complexations as well as the viscosity studies. Thermal stabilities in general were smaller in the complexed species than in the native biopolymers and the films obtained from aqueous solutions showed for Cu2+ the most different morphology compared to the biopolymer itself. A use can be suggested of this biopolymer in environmental remediations besides its already established industrial uses.     

The superposition of steady on oscillatory shear and its effect on the viscoelasticity of human blood and a blood-like model fluid

To understand the pulsatility of human blood flow in vivo, it is necessary to separately investigate (1) steady shear and oscillatory flow, and (2) the superposition of steady shear flow on oscillatory flow performed under in vitro conditions. In this study a variable steady shear rate was superimposed in parallel on oscillatory shear at a constant frequency (0.5 Hz) for human blood (45% hematocrit), and an aqueous polyacrylamide polymer solution (AP 30E, concentration 300 ppm). The effect of superposition of the above two shear flows on the viscoelasticity of blood was more pronounced for the elastic (η′') than for the viscous (η′) component of viscoelasticity. With increasing superimposed shear rate, both η′ and η′' decreased, especially at the low shear region. This behavior can be explained by the viscoelastic properties of blood and the phenomena of blood aggregation and disaggregation. Quantitatively, the dependence of the viscous component of complex viscosity on superimposed shear for both blood and polymer solution is described by a modified Carreau equation. The elastic component of complex viscosity decreased exponentially with increasing superimposed shear, and it is described by an exponential model. © 1997 Elsevier Science Ltd     

Studies on the viscosity behavior of alkali halides in aqueous D-xylose solution

The viscosity behavior of ternary systems comprising sodium or potassium halides (concentration range 0.125–3M in aqueous D-xylose solution (0.4M at 25, 30, 35, and 40° has been determined. It is found that Moulik's equation holds for such concentrated solutions beyond the Einstein region. Furthermore, the “effective” rigid molar volume and the apparent B coefficient have been computed from the relative viscosity data by employing the Breslau-Miller treatment. The results are explained in terms of the structure-making or -breaking effects in solution by analyzing the values of the apparent B coefficient obtained for different temperatures.     

The nonequilibrium phase and glass transition behavior of beta-lactoglobulin

Concentrated solutions of bovine beta-lactoglobulin were studied using osmotic stress and rheological techniques. At pH 6.0 and 8.0, the osmotic pressure was largely independent of NaCl concentration and could be described by a hard sphere equation of state. At pH 5.1, close to the isoelectric point, the osmotic pressure was lower at the lower NaCl concentrations (0 mM, 100 mM) and was fitted by an adhesive hard sphere model. Liquid-liquid phase separation was observed at pH 5.1 at ionic strengths of 13 mM and below. Comparison of the liquid-liquid and literature solid-liquid coexistence curves showed these solutions to be supersaturated and the phase separation to be nonequilibrium in nature. In steady shear, the zero shear viscosity of concentrated solutions at pH 5.1 was observed at shear rates above 50 s(-1). With increasing concentration, the solution viscosity showed a progressive increase, a behavior interpreted as the approach to a colloidlike glass transition at approximately 60% w/w. In oscillatory shear experiments, the storage modulus crossed the loss modulus at concentrations of 54% w/w, an indication of the approaching glass transition. Comparison of the viscous behavior with predictions from the Krieger-Dougherty equation indicates the hydrodynamic size of the protein decreases with increasing concentration, resulting in a slower approach to the glass transition than a hard sphere system.     

Generation of small bubbles and small bubble-liquid mass transfer in airlift reactors containing highly viscous liquids

The time-dependent gas hold-up is investigated during the aeration of the Saccharomyces cerevisiae suspension, the aqueous saccharose solutions and the glycerol solutions in the external loop airlift reactor. Due to the time-dependent bubble size distribution the fraction of the small bubble hold-up in the total gas hold-up decreases with an increase of the gas flow rate and with a decrease of the viscosity. The course of the accumulation process of the small bubbles is described by the first-order kinetic equation. The small bubble accumulation rate is investigated in the airlift reactor and the bubble column. It is showed that the small bubbles form and disappear exclusively in the riser of the airlift reactor. It is found that the small bubble-liquid mass transfer coefficient is several times larger than the overall oxygen transfer coefficient.