微量量热法测定细菌的最佳生长温度

前文＊报导过两个菌种在不同培养基中的临界生长温度．本文在此基础上，对细菌生长过程与温度之间的关系做了进一步探讨，确定了各菌种在相同的培养基中有最适宜的生长温度，对几株杆菌、球菌、弧菌在相同培养基、不同温度下代谢过程的热谱进行了测定，按文献间的方法，求出了它们在不同温度下的生长速率常数，并拟合了k一T非线性方程（有极大值），从该方程出发找出了另一特征温度，即最佳生长温度．1实验部分五．五仪器、苗种与材料本实验采用瑞典Aug司产的新型热导式微量量热计，其结构、原理与操作见前文门．实验所用菌种均由北京药品…     

药物对福氏志贺氏菌代谢抑制的微量热法研究

药物抑制细菌生长的热化学研究是当今热化学法研究的一个活跃领域．在这项研究中，Boling[1]、Nordmark[2]、屈松生[3]等人已做了不少有意义的工作．在前人工作的基础上，我们用热活性检测系统测定了福氏志贺氏菌属中五株细菌在药物抑制下生长的完整的热谱曲线．按指数生长模型计算出细菌代谢抑制下的生长速车常数，并用计算机拟会出生长速率常数与不同浓度药物之间的关系式，进一步得到生长速率常数为零（临界生长参数[4]）时的用药物浓度．此项研究工作的开展对于深入研究药物对细菌的抑制作用，筛选对某细菌抑制的特效药提供了一种新的…     

微量热法测定细菌的最低生长温度

微量热法测定细菌的最低生长温度南照东，刘永军，孙海涛，张洪林（曲阜师范大学化学系曲阜２７３１６５）关键词微量热法，细菌的生长热谱，最低生长温度，生长速率常数我们应用微量热法测定了大肠杆菌（Ｅ．ｃｏｌｉ），白色葡萄球菌（Ｓ．ａｌｂｕｓ），金黄色葡萄球菌...     

微量量热法筛选抑菌特效药的研究

用微量最热计连续测定细菌代谢过程中的热显变化，可获得反映细菌代谢规律的完整的热谱图以按指数生长模型对指数生长期进行处理，可计算出细菌正常代谢的生长速率常数L’．若在培养基中加入合成药物，使细菌在药物抑制作用下生长，也可获得完整的热谱图，从而计算出在药物抑制作用下细菌的生长速率常数．本义对福氏志贺氏Zb菌和金黄色葡萄球莉在四种合成药物抑制作用下的热谱进行了测定，并计算了生长速率常数，找出了细菌生长速率常数与所用药物浓度之间的定量关系，可为筛选抑菌药物和确定用药显提供定量依据’1基本原理设细菌在代谢过…     

Schiff碱药物对产气杆菌代谢抑制的热力学研究

用微量热法测定产气杆菌在不同温度条件下受到Schiff碱药物抑制的热谱曲线, 根据其指数生长期的热谱信息, 确定它在不同温度条件下的生长速率常数和反应活化能, 找出了该细菌的最佳生长温度。同时借用化学反应中的过渡态理论, 得到一系列热力学参数, 对细菌在受到抑制时的生长代谢进行了热力学分析。     

Schiff碱金属配合物在细菌代谢过程中的表征

采用微量热法测定了产气杆菌在四种Schiff碱金属配合物作用下的代谢热谱, 以其对数生长期的生长速率常数k表征了Schiff碱金属配合物对其细菌生长的抑制。不同的配合物其抑制情况不同。Co(II)-NG(NG : D-氨基葡萄糖-β-萘酚醛Schiff碱)对产气杆菌的抑制作用最大, 随着浓度c的增加抑制作用增大, 在350μg.mL^-^1时可完全抑制其生长, 但k-c并不呈线性关系; Fe(II)-NG对产气杆菌的抑制较小, 且在50-300μg.mL^-^1浓度范围内k与浓度无关, 在350μg.mL^-^1时才略表现有一定的抑制作用; Cu(II)-NG和Zn(II)-NG对产气杆菌的抑制作用也较小, 且k随着浓度的变化不规则, 同时发现热谱上最大热输出功率Pmax与生长速率常数存在正比关系, 进而推出在实验条件相同的情况下可用Pmax代替k。     

细胞动力学研究VI. 厌氧菌生长过程热化学特征

用LKB2277生物活性检测系统测定了三种厌氧菌---吉氏类杆菌、艰难梭状芽胞杆菌、黑色消化球菌的生长发热功率曲线。根据广义logistic方程, 建立了细菌生长过程的热动力学方程:ln[P/(Pm-P)^v^+^1]=ln[P0/(Pm-P0)^v^+^1]+k.t。由此热动力学方程, 求得了细菌的生长常数k, 根据Arrhenius公式求得吉氏菌的生长活化能Ea=59.7kj/mol, 应用过渡态理论得到吉氏菌在不同温度下的活化力学参数, 这个热动力学方程描述的是一系列不规则的细菌生长过程发热曲线, 将它与经典的指数模型和logistic模型进行比较, 它具有更广泛的适用性。     

细胞动力学研究VI. 厌氧菌生长过程热化学特征

用LKB2277生物活性检测系统测定了三种厌氧菌---吉氏类杆菌、艰难梭状芽胞杆菌、黑色消化球菌的生长发热功率曲线。根据广义logistic方程, 建立了细菌生长过程的热动力学方程:ln[P/(Pm-P)^v^+^1]=ln[P0/(Pm-P0)^v^+^1]+k.t。由此热动力学方程, 求得了细菌的生长常数k, 根据Arrhenius公式求得吉氏菌的生长活化能Ea=59.7kj/mol, 应用过渡态理论得到吉氏菌在不同温度下的活化力学参数, 这个热动力学方程描述的是一系列不规则的细菌生长过程发热曲线, 将它与经典的指数模型和logistic模型进行比较, 它具有更广泛的适用性。     

环境气氛对微量热安瓿法测定细菌生长速率常数的干扰

采用微量热安瓿法测定细菌生长时,发现细菌的代谢产热曲线在第一指数生长期内出现了停留法没有报导过的显著分阶段现象,且在不同的阶段生长速率常数有很大差异,对药物抗菌性能的评估造成极大干扰.为了寻找此现象的可能原因,以具有代表性的兼性细菌大肠杆菌为例,设计了微量热安瓿法实验,考察了不同环境气氛下大肠杆菌的生长代谢产热;并模拟了停留法条件下细菌的生长环境,通过安瓿法测定了大肠杆菌的生长代谢产热,重新解析了这些条件下细菌的生长速率常数.结果表明环境气氛是造成此现象的主要可能因素,并为在不同环境气氛下采用微量热安瓿法准确评估细菌的生长速率提供了一个可参考的标准.     

生物热动力学研究——大肠杆菌生长速率和激活能

大肠杆菌生长的全热谱已被测定,再进一步根据其指数生长期的热谱信息,确定了它的生长速率和激活能。在指数生长期,细菌数按指数规律增加,可用下式表示:n_t=n_0e~(kt)(1)式中:t为指数生长期开始后的某一时间,n_0,n_t分别为指数生长期开始时和t时的细菌数,k为生长速率常数。因此,同期细菌输出的热功率也是按指数规律同步增长。可表示为:     

微量热法测定细菌的临界生长温度

In this paper, we have determined the multiplication rate constanis (k) of Shigella flexneri and E. coli. at different temperatures and in different culture media by means of a microcalorimeter. From these results a linear equation as k~(1/2)=a+bT can be established for the bacterial growth. The corresponding linear equation for S. flexneri is k~(1/2)=-1.2823+0.0047122 T(r=0.971), so its eritica lgrowth temperature T_0 is equal to 272.1 K. The linear equation for E coli is k~(1/2)=-1.6390+0.005948 T (r=0.994), T_0=275.5 K. The experimental results indicate that the critial growth temperature of E. coli. is nearly a constant (T_0=273.9 K) in different culture media, which is very informative for the study on microorganism growth.     

1,3,3-三硝基氮杂环丁烷的热安全性

借助不同加热速率(β)的非等温DSC曲线离开基线的初始温度(T₀)、onset温度(T_e)和峰顶温度(T_p), Kissinger法和Ozawa法求得的热分解反应的表观活化能(E_k和E_O)和指前因子(A_k), Hu-Zhao-Gao方程ln β_i＝ln[A₀/(b_{e0 or p0}G(α))]＋   b_{e0 or p0}T_{ei or pi}求得的b_{e0 or p0}, Zhao-Hu-Gao方程ln β_i＝ln[A₀/((a_{e0 or p0}＋1)G(α))]＋(a_{e0 or p0}＋1) ln T_{ei or pi}求得的a_{e0 or p0}, 微热量法确定的比热容(C_p), 以及密度(ρ)、热导率(λ)和分解热(Q_d, 取爆热之半)数据, Zhang-Hu-Xie-Li公式、Hu-Yang-Liang-Xie公式、Hu-Zhao-Gao公式、Zhao-Hu-Gao公式、Smith方程、Friedman公式和Bruckman-Guillet公式, 计算了TNAZ在β→0时的T₀, T_e和T_p值(T₀₀, T_eo和T_p0)、热爆炸临界温度(T_be和T_bp)、绝热至爆时间(t_Tlad)、撞击感度50%落高(H₅₀)和热点起爆临界温度(T_cr), 得到了评价TNAZ热安全性的结果: T_SADT＝T_e0＝485.81 K, T_p0＝497.38 K, T_beo＝499.50 K, T_bp0＝513.45 K, t_Tlad＝8.90 s (n＝0), t_Tlad＝8.96 s (n＝1), t_Tlad＝9.01 s (n＝2), H₅₀＝28.88 cm, T_cr＝641.46 K (T_room＝293.15 K), T_cr＝658.89 K (T_room＝300 K), 表明: (1) TNAZ对热是稳定的; (2)撞击感度好于环三亚甲基三硝胺(RDX); (3)热点起爆临界温度高于RDX, 而界于1,3,5-三氨基-2,4,6-三硝基苯(TATB)和六硝基茋(HNS)之间.     

取代羧酸pKa的分子树拓扑研究

基于非氢原子i的酸性点价(δai)建构分子树拓扑指数(mT)及其分支指数(mTC)和叶指数(mTx),并提出表征诱导效应的叶指数(mT′x).通过最佳变量子集算法获得38种羧酸的pKa与0TC、1TC、0T′x的回归方程:pKa=3.0352-1.25700T′x-0.15540TC+0.07811TC,R=0.9766.通过Jackknife法检验,该模型具有总体稳健性.优于文献的七元最佳回归模型(R=0.957),与其分子力学方法(CoMFA)结果(R=0.988)较为接近.结果表明,所建拓扑指数是合理的,具有科学性基础.     

弹性竿模型下超螺旋DNA分子的构象研究

采用弹性竿模型 (Elasticrodmodel) ,用MonteCarlo方法对DNA分子的构象进行研究 .通过计算发现 ,DNA分子的能量是由弯曲势能EB 和扭转势能ET 两部分组成 ,通常EB 比ET 大一至两个数量级 .同时给出了均方回转半径与链长之间的关系为〈R2g〉 =1 1 69 5 -3 5×n +0 0 2 5×n2 ,它体现了DNA分子结构的特点 .验证了公式Lk=Wr+Tw ,得出Lk与Wr比较接近的结论 ,考虑DNA分子的构型 ,意味着DNA分子容易被弯曲而不易被扭转 ,但随着连接系数的增加 ,DNA被扭转的几率也在增加 .这为分析DNA分子的结构特征提供了一种新方法     

从聚合物分子量评价自由基聚合的链终止反应

本文从聚合物的聚合度与反应速度关系论述了自由基聚合过程中链终止方式,并由此估价自由基聚合机理。令各反应物起始浓度比例固定并同步改变,于是各链转移速度与链增长速度之比(R_(tr)/R_p)_i为常,由此得直线方程: 1/_n=R_t/R_p+K 在稳态条件下,链终止方式可从下述各直线方程估价。双基终止 1/_n=k_t/K_p~2·R_p/(c~2(M))+K 单基终止 1/_n=k_(t)/k_p·1/(c(M))+K 初级自由基终止 1/_n=k_(prt)/k_p·c(R·)/c(M)+K 转移终止 1/_n=K 苦双基终止、单基终止和初级自由基终止反应同时并存,则 1/_n=k_t/k_p~2·R_p/(c~2(M))+k_t/k_p·1/(c(M))+fk_d k_(prt)/k_i·k_p·c(I)/(c~2(M))+K 本实验设计和数据处理方法用以研究自由基聚合的链终止过程,与实验结果和动力学推导十分一政。     

Thermodynamic parameters for the binding of inorganic and organic anions by biogenic polyammonium cations

Thermodynamic parameters for the interaction of protonated biogenic polyamines with inorganic or organic polyanions were studied potentiometrically (H(+)-glass electrode) and calorimetrically, at 25 degrees C. No background salt was used in the measurements to avoid interferences, and the formation constants and formation enthalpies were extrapolated to zero ionic strength. Species formed are ALH(r) [L=Cl(-), SO(4)(2-), HPO(4)(2-), P(2)O(7)(4-) and P(3)O(10)(5-); tartrate, malate, citrate, glutamate, 1,2,3-propanetricarboxylate, 1,2,3,4-butanetetracarboxylate], with r=1,2...(n+m-2) and r=1,2...(n+m-1) for inorganic and organic ligands, respectively (n, m=maximum degree of protonation of amine and ligand, respectively). The stability of the various species formed is a function of charges involved in the formation reaction. DeltaH(0) values are generally positive, and therefore these complexes are entropically stabilized. Results are discussed in connection with several previously reported data on similar systems. DeltaG(0) and TDeltaS(0) follow a linear trend as a function of polyammonium cation and inorganic or carboxylic anion charges. DeltaG(0) and TDeltaS(0) charge relationships are reported. In particular, mean values of DeltaG(0) and TDeltaS(0) for single interaction were calculated: DeltaG(0)=7.0 kJ mol(-1) n(-1), TDeltaS(0)=9.1 kJ mol(-1) n(-1) and DeltaG(0)=5.7 kJ mol(-1) n(-1) and TDeltaS(0)=8.7 kJ mol(-1) n(-1), for the species of inorganic and organic polyanions, respectively (n=number of possible salt bridges). A linear relationship was also found for TDeltaS(0) versus DeltaG(0), whose equation is TDeltaS(0)=-7-1.39 DeltaG(0) (with r=0.9409; r, correlation coefficient). The body of correlations found for these thermodynamic parameters shows quite good predictive value.     

Experimental and modeling studies of the pressure and temperature dependences of the kinetics and the OH yields in the acetyl + O2 reaction

The acetyl + O(2) reaction has been studied by observing the time dependence of OH by laser-induced fluorescence (LIF) and by electronic structure/master equation analysis. The experimental OH time profiles were analyzed to obtain the kinetics of the acetyl + O(2) reaction and the relative OH yields over the temperature range of 213-500 K in helium at pressures in the range of 5-600 Torr. More limited measurements were made in N(2) and for CD(3)CO + O(2). The relative OH yields were converted into absolute yields by assuming that the OH yield at zero pressure is unity. Electronic structure calculations of the stationary points of the potential energy surface were used with a master equation analysis to fit the experimental data in He using the high-pressure limiting rate coefficient for the reaction, k(∞)(T), and the energy transfer parameter, (ΔE(d)), as variable parameters. The best-fit parameters obtained are k(∞) = 6.2 × 10(-12) cm(-3) molecule(-1) s(-1), independent of temperature over the experimental range, and (ΔE(d))(He) = 160(T/298?K) cm(-1). The fits in N(2), using the same k(∞)(T), gave (ΔE(d))(N(2)) = 270(T/298?K) cm(-1). The rate coefficients for formation of OH and CH(3)C(O)O(2) are provided in parametrized form, based on modified Troe expressions, from the best-fit master equation calculations, over the pressure and temperature ranges of 1 ≤ p/Torr ≤ 1.5 × 10(5) and 200 ≤ T/K ≤ 1000 for He and N(2) as the bath gas. The minor channels, leading to HO(2) + CH(2)CO and CH(2)C(O)OOH, generally have yields <1% over this range.     

Asymptotic solutions to the Smoluchowski's coagulation equation with singular gamma distributions as initial size spectra

Smoluchowski's coagulation equation is studied for the kernel K(u,v)=E(ualphavbeta+ubetavalpha) with real, non-negative alpha, beta and E, using gamma distributions with a singularity at zero volume as initial size spectra. As the distribution parameter of the gamma distribution, p, approaches its lower limit (p-->0) the distribution becomes approximately pv(p-1) for small v. Asymptotic solutions to the coagulation equation are derived for the two cases p-->0 and v-->0. The constant kernel (alpha=beta=0) is shown to be unique among the studied kernels in the sense that the p-->0 asymptote and the v-->0 asymptote differ.     

海水中二甲基硫亨利常数的测定

 推导了多次相平衡顶空气相色谱法测定海水中二甲基硫 (DMS)亨利常数 (K)的理论关系式 ,根据两次或多次气、液相平衡的关系式 ,只测定DMS在气相中的浓度就可测定亨利常数。实测 2 2℃时DMS在胶州湾海水中的亨利常数是 0 0 89,相对标准偏差为 5 5 0 %。亨利常数的对数与环境水体中NaCl的质量分数 [w(NaCl) ]之间的关系为 :logK =0 0 688·w(NaCl) - 1 3 5 68,相关系数为 0 997。亨利常数的对数与环境水体的绝对温度 (T)的倒数之间的相关方程为 :logK =- 15 4 4 8/T + 4 2 112 ,相关系数为 0 996。     

Ground- and triplet excited-state properties correlation: a computational CASSCF/CASPT2 approach based on the photodissociation of allylsilanes

Excited-state properties, although extremely useful, are hardly accessible. One indirect way would be to derive them from relationships to ground-state properties which are usually more readily available. Herewith, we present quantitative correlations between triplet excited-state (T?) properties (bond dissociation energy, D?(T?), homolytic activation energy, E(a)(T?), and rate constant, k(r)) and the ground-state bond dissociation energy (D?), taking as an example the photodissociation of the C-Si bond of simple substituted allylsilanes CH?=CHC(R1R2)-SiH? (R1 and R2 = H, Me, and Et). By applying the complete-active-space self-consistent field CASSCF(6,6) and CASPT2(6,6) quantum chemical methodologies, we have found that the consecutive introduction of Me/Et groups has little effect on the geometry and energy of the T? state; however, it reduces the magnitudes of D?, D?(T?) and E(a)(T?). Moreover, these energetic parameters have been plotted giving good linear correlations: D?(T?) = α? + β? · D?, E(a)(T?) = α? + β? · D?(T?), and E(a)(T?) = α? + β? · D? (α and β being constants), while k(r) correlates very well to E(a)(T?). The key factor behind these useful correlations is the validity of the Evans-Polanyi-Semenov relation (second equation) and its extended form (third equation) applied for excited systems. Additionally, the unexpectedly high values obtained for E(a)(T?) demonstrate a new application of the principle of nonperfect synchronization (PNS) in excited-state chemistry issues.