共查询到20条相似文献,搜索用时 78 毫秒
1.
铅—试铁灵络合物吸附波及溴化十六烷基三甲基铵增敏效应的研究 总被引:1,自引:0,他引:1
在030mol/LHAc介质中,Pb(Ⅱ)与7_碘_8_羟基喹啉_5_磺酸(试铁灵,Feron)的络合物于-054V(vs.SCE)产生一尖锐的极谱波,加入溴化十六烷基三甲基铵(CTMAB)显著增敏,可使极谱波增高约4倍。峰电流与Pb(Ⅱ)浓度在96×10-9~48×10-6mol/L呈良好的线性关系,检出限为48×10-9mol/L。用多种电化学方法研究了该极谱波的性质及电极反应机理表明,络合物组成比为nPb(Ⅱ)∶nFeron=1∶1,极谱波为吸附波,峰电流由中心离子Pb(Ⅱ)还原产生,电子转移数为2。试验了多种离子对峰电流的影响,拟定的方法用于矿样分析,结果与原结果相符。 相似文献
2.
单扫描示波极谱法测定痕量钒 总被引:3,自引:0,他引:3
提出单扫描示波极谱测定痕量V的极谱催化波体系,选定4.8×10 ̄-6mol/L PAR-0.048%H_2O_2-0.025mol/LNaBrO_3-0.003mol/LH_2SO_4的底液条件,测定V的线性范围为0.04~12ng/ml,检出限0.02ng/ml。将该体系应用于水样、人发及矿样中痕量V的测定,结果满意。 相似文献
3.
4.
镍与邻羧基苯基重氮氨基偶氮苯的显色反应及其应用 总被引:6,自引:0,他引:6
在乳化剂OP存在下,于pH9.7~10.0的Na_2B_4O_7-NaOH缓冲介质中,Ni ̄(2+)与邻羧基苯基重氮氨基偶氮苯(CDAA)形成组成比为1:2的稳定的红色配合物,其吸收峰波长在540nm,对比度△λ=126nm,表观摩尔吸光系数为1.99×10 ̄5L·mol ̄(-1)·cm ̄(-1),室温下20min内显色反应完全,有色配合物至少稳定12h。方法线性范围是0~0.20μg/mlNi,检测限为0.0004μg/ml。在掩蔽剂存在下,方法用于矿样和低合金钢的分析,结果与标准值相符,其RSD(n=6)分别为1.8%和3.1%,标准加入回收率为95.0%~101.2%。 相似文献
5.
钛—邻氯苯基荧光酮—Trutib X—100显色反应的研究及微量钛的测定 总被引:2,自引:0,他引:2
本文研究了在非离子表面活性剂Tritonx-100存在的情况下,邻氯苯基荧光酮(O-Cl-PF)与钛的显色反应。试验表明,在0.10~0.14mol·L ̄(-1)H_2SO_4介质中,O-Cl-PF与钛形成灵敏度极高的红紫色配合物,其最大吸收峰位于540nm处,表现摩尔吸光系数为1.8×10 ̄5L·mol ̄(-1)·cm ̄(-1),钛含量在0~3μg/25ml范围内服从比尔定律。该方法用样少,操作简便,灵敏度高,选择性好,适于测定地质样品中的微量钛。 相似文献
6.
甲基异丁基甲酮萃取-石墨炉平台原子吸收法测定地质样品中痕量硒和碲 总被引:1,自引:1,他引:1
样品经HNO_3-HF-HClO_4分解,在5.4mol/L的HCl介质中,以抗坏血酸为还原剂用甲基异丁基甲酮同时萃取样品中的Se、Te。以Pd和Ni作混合基体改进剂,使用自制的涂锆石墨平台直接测定有机相中的Se、Te。方法的检出限分别为0.21×10 ̄(-9)gSe,0.13×10 ̄(-9)gTe;测定0.06gSe、0.03gTe的RSD(n=11)分别为7.0%和8.9%。 相似文献
7.
8.
研究结果表明,在混合表面活性剂CTMAB-吐温-60存在下的pH5.7~6.5的缓冲介质中,Sc(Ⅲ)与4,5-二溴苯基荧光酮(DBPF)形成高灵敏的多元配合物,其ε_(590)=2.26×10 ̄5L·mol ̄(-1)·cm ̄(-1),组成比为:Sc:DBPF:CTMAB=1:2:4。采用混合表面活性剂使增溶增敏作用更为显著,并加速了显色反应,增强了配合物的稳定性。而Na_2SO_4的加入能显著地提高体系的灵敏度。Sc量在0~0.36ug/ml范围内遵守比尔定律。方法可直接测定合成混合稀土中的Sc,回收率在98%~105%;结合沉淀分离和PMBP萃取分离,实现了地质试样中痕量Sc的测定。 相似文献
9.
在pH4.0的HAc-NaAc介质中,Pb(Ⅱ)与1-苯基-3-基-4-苯甲酰基-吡啉酮-5(PMBN)生成络合物,于一0.56V(vs.SCE)处出现一尖锐、灵敏的极谱峰。Pb浓度在4.83×l0 ̄-9~1.69×10 ̄-6mol/L与峰高呈线性关系。用多种电化学方法研究了极谱波的性质及反应机理,证明-0.56V处的极谱波为络合物吸附波,峰电流由中心离子Pb(Ⅲ)还原产生。用直线法测得络合物组成比为l:l。试验了30多种离子对峰电流的影响。方法已用于矿石中痕量pb的测定。 相似文献
10.
常温下在pH4的HAc-NaAc缓冲体系中,Ga与1,5-二(2-羟基-5-磺基苯基)-3-氰基甲 (DSPCF)形成稳定的蓝色配合物。该配合物在波长630nm处有最大吸收,其表观摩尔吸光系数为3.8×10 ̄4L·mol ̄-1·cm ̄-1,配合比为n(Ga):n(DSPCF)=1:2,显色反应在20min内完成,稳定时间至少24h,Ga量在0~1.8mg/L时遵守比尔定律。采用TBP萃淋树脂分离干扰元素后可实现煤矸石中Ga的测定。 相似文献
11.
12.
考虑核电厂地基-基础的动力相互作用,应用显式动力有限差分法分析了地震作用下极软岩、较软岩、坚硬岩上核电厂建筑结构基础的地震响应特征,比较了岩石坚硬程度对基础加速度反应谱的影响。研究表明:随着岩石坚硬程度的提高,核电厂建筑物结构基础的地震响应有增加的趋势;在周期轴上,基础处的加速度反应谱曲线会随着岩石坚硬程度的提高逐渐向短周期(高频段)方向移动。在高频段,建造于较坚硬岩石上基础结构的加速度反应谱值偏大;在中等频段,建造于较软岩石上基础结构的加速度反应谱值偏大;在低频段,岩石坚硬程度对加速度反应谱的影响不显著。 相似文献
13.
M. D. Sharma 《Journal of Earth System Science》2004,113(2):247-257
Three dimensional scattering of near-field is studied for dilatation and rotation in the time domain. The perturbation method
is applied to solve the equation of motion for the first order scattering from a weak inhomogeneity in an otherwise homogeneous
medium. The inhomogeneity is assumed close enough to the point source so that the near-field intermediate wave is dominating
over the far-field sphericalP andS pulses. The integral expressions are derived to relate dilatation and rotation of scattering to the radial fluctuations of
velocities and density in the inhomogeneity. These integrals are solved to calculate the strains of scattering from (a part
of) an inhomogeneous spherical shell of arbitrary curvature. Variable curvature may allow the shape of inhomogeneity volume
element to change uniformly from spherical to rectangular. Rotation of scattering from a spherical shell is independent ofP wave velocity inhomogeneity. Dilatation of scattering does not involveS wave velocity inhomogeneity but its gradient. The back scattering results are obtained as a special case. Strains are computed
numerically, for hypothetical models to study the effects of various parameters viz., velocity inhomogeneity, distance of
source from inhomogeneity and from receiver, and thickness of inhomogeneity. The curvature of the spherical shell is varied
to study the effects of the shape of inhomogeneous volume element on scattering. 相似文献
14.
15.
16.
地震次生地质灾害风险评估集对态势分析 总被引:2,自引:0,他引:2
5.12四川汶川8级强震引发了大量次生地质灾害,加剧了灾情并严重影响抗震救灾。地震次生地质灾害受多重因素制约,其孕育与致灾过程具有不确定性。利用集对分析原理与方法,对地震次生地质灾害进行同异反态势分析,拟定了风险评估的集对分析同一度、差异度、对立度等指标体系的构建原则与赋值标准,对承灾体系统的不确定性及其作用作了刻画与分析,建立了不同风险分区代表性的集对分析联系度表达式,为地震灾害研究提供了可资借鉴的新思路和技术方法。 相似文献
17.
Ivan V. BRAGIN Georgy A. CHELNOKOV Oleg V. CHUDAEV Natalia A. KHARITONOVA Sergey V. VYSOTSKIY 《《地质学报》英文版》2016,90(1):276-284
Studied waters belong to warm(T=30-50℃),alkaline(pH=8.9-9.3),low mineralized(TDS235 mg/1)Na-HCO_3 or Na-SO_4-HCO_3 thermal waters with high content of SiO_2(up to 81 mg/l)and F(up to 3.9 mg/1),occur on modern volcano-tectonic rejuvenated areas of Eastern Sikhote-Alin orogenic belt.Low~3He concentration as well as N_2/O_2 and N_2/Ar ratios exclude influence of deep mantle fluid.New rare earth element data constrain our understandmg of water-rock interaction occurring in the water source region.Meteoric origin of waters is proved by stable isotope values varying from-71‰to-136.1‰and from-10.8‰to-18.8‰forδ~2U andδ~(18)O respectively.REE patterns reflect high pH,resultfing from water-rock interaction and oxidative conditions.Calculations of deep aquifer temperature using Na-K and quartz geothermometers show 116.8-131.1°C and 82.2-125.8℃respectively.Presence of deep faults both with abnormal thermal gradient(~45-50 K/km)define unique geochemical shape of thermal waters of Sikhote-Alin,area,where no present volcanic activity is registered. 相似文献
18.
下扬子区三叠纪古地理演化 总被引:2,自引:2,他引:0
下扬子区在三叠纪期间接受了早-中三叠世海相碳酸盐沉积、中-晚三叠世海陆交互相和陆相湖沼沉积.沉积相带的空间分布和古地理格局的变迁明显地受到区域构造的控制.区内盆地发育与演化是在华南板块与扬子板块、扬子板块与华北板块相互作用的背景下进行的.早-中三叠世末期的印支运动是下扬子区构造-古地理格局改变的决定性因素,使下扬子海盆闭合,沉积类型由海相沉积变为陆相沉积.下扬子区三叠纪古地理的演化特征也为板块碰撞提供了沉积证据. 相似文献
19.
20.
Isothermal thermogravimetric experiments have been carried out to determine the reaction kinetics of the dehydration processes
in fuller's earth, a natural Ca-montmorillonite. Dehydration in swelling clays is a complex reaction, and analysis of the
thermogravimetric data using empirical rate equations and time-transformation analysis reveals that the nature of the rate
controlling mechanism is dependent upon both the temperature regime of the sample as well as the extent of reaction. For fuller's
earth, we find that the dehydration kinetics are dominated by a nucleation and growth mechanism at low temperatures and fractions
transformed (stage I), but above 90 °C the last stages of the reaction are diffusion controlled (stage II). The activation
energy for dehydration during stage I is around 35 kJ · mol−1, whereas the removal of water during stage II requires an activation energy of around 50 kJ · mol−1. These two stages of dehydration are associated with primary collapse of the interlayer (stage I) and movement of water that
is hydrated to cations within the interlayer (stage II).
Received: 28 August 1998 / Revised, accepted: 27 January 1999 相似文献