富含Na~ 、Ca~(2 )、Al~(3 )、Cr~(3 )蒙脱石对垃圾渗滤液中有机物的吸附

由于层间含有高价态金属阳离子的蒙脱石对特定有机物的吸附能力可大大增强 ,故分别用层间含有Na 、Ca2 、Al3 和Cr3 的蒙脱石对垃圾渗滤液中的有机物进行吸附实验 ,研究它们吸附苯酚、二甲苯和COD的能力及离子形态对吸附效果的影响。结果表明 ,含高价金属阳离子的蒙脱石对苯酚和COD的吸附能力较高 ,吸附能力由小到大的顺序为 :Na 相似文献   

Thermodynamics of multicomponent pyroxenes: III. Calibration of Fe2+(Mg)-1, TiAl2(MgSi2)-1, TiFe 2 3+ (MgSi2)-1, AlFe3+(MgSi)-1, NaAl(CaMg)-1, Al2(MgSi)-1 and Ca(Mg)-1 exchange reactions between pyroxenes and silicate melts

A thermodynamic model for the Gibbs free energy of igneous pyroxenes with the general formula [Na, Ca, Fe²⁺, Mg]^M2[Fe²⁺, Mg, Ti, Al, Fe³⁺]^M1[Al, Fe³⁺, Si]^TetSiO₆ is calibrated from experimentally determined compositions of coexisting pyroxene and silicate melt. The model is based upon the general formulation, and relies upon the calibration of the “quadrilateral” subsystem, previously published by the present authors. The calibration database of pyroxene-liquid equilibria spans a broad spectrum of temperature, pressure and oxygen fugacity conditions, ranging from 1000°–1600°C, 0.001–30 kbar and iron-wüstite to air. Chemical potentials of endmember pyroxene components as well as exchange potentials between pyroxenes and coexisting liquids are defined utilizing the present authors' thermodynamic melt model. Model parameters are extracted from these relations by regression analysis. The resulting model and derivative endmember properties are internally consistent with an existing standard state thermodynamic database. The success of the model and its applicability to igneous petrogenesis are demonstrated by comparing calculated and experimentally determined liquidus compositions, temperatures and symmetry states for pyroxenes crystallizing from a variety of silicate melts, ranging in composition from tholeiites and angrites through rhyolites to potash ankaratrites.     

1-（4-硝基苯基）-3-（3，5-二溴吡啶）三氮烯的合成及其与镍的显色反应

合成了1-(4-硝基苯基)-3-(3,5-二溴吡啶)三氮烯(NPDBPDT),并研究了NPD-BPDT与镍的显色反应。在pH 10.0的Na2B4O7-NaOH缓冲溶液介质中,表面活性剂Triton X-100存在下,镍与试剂生成摩尔比为1∶4的络合物在470 nm处有最大正吸收峰,表观摩尔吸光系数为1.02×105L.mol-1.cm-1;在540 nm处有最大负吸收峰,表观摩尔吸光系数为1.15×105L.mol-1.cm-1;以540 nm为参比波长、470 nm为测量波长进行双波长测定,表观摩尔吸光系数为2.17×105L.mol-1.cm-1。镍含量在0~480μg/L内符合比尔定律。方法用于合金样品中镍的测定,结果与原子吸收法相符,加标回收率为98.0%~102.0%;精密度小于5%(RSD,n=6)。     

离子色谱法同时测定地质样品中氟氯磷硫

本文研究了离子色谱同时测定地质样品中F~-、Cl~-、PO_4~(3-)、SO_4~(2-)的前处理过程,选择了色谱测定最佳条件。在Na_2CO_3全熔的样品溶液中,加入(NH_4)_2CO_3使Si、Al随大多数金属离子同时沉淀;再用预处理柱除去熔剂引入的大量Na~+及CO_3~(2-)消除其干扰;并在流出液中补加相应试剂与淋洗液相匹配,实现了多种地质样品中F~-、Cl~-、PO_4~(3-)和SO_4~(2-)的测定。方法检出限(3s,μg/ml)分别为F~-0.05、Cl~-0.1、PO_4~(3-)0.3、SO_4~(2-)0.5。测定范围为F~-0.05—3μg/ml,Cl~-0.1—6μg/ml,PO_4~(3-)0.3 —30μg/ml,SO_4~(2-)0.5—30μg/ml。     

2-（2′-苯并噻唑偶氮）-7-（4-甲氧基偶氮）-1,8-二羟基萘-3,6-二磺酸的合成及与铝的显色反应

合成一种新的显色剂2-(2′-苯并噻唑偶氮)-7-(4-甲氧基偶氮)-1,8-二羟基萘-3,6-二磺酸(BTAMoPACA)。研究了试剂的结构和与A l(Ⅲ)的显色反应,结果表明:在pH为5.6~6.0的邻苯二甲酸氢钾-氢氧化钠缓冲介质中,A l(Ⅲ)与BTAMoPACA及溴化十六烷基三甲铵(CTMAB)形成1∶3∶1的三元络合物,其最大吸收波长为674 nm,表观摩尔吸光系数ε=3.04×105L.mol-1.cm-1。络合反应在20 m in后趋向稳定,A l(Ⅲ)浓度在0~0.20mg/L符合比尔定律。拟定方法应用于实际样品中A l(Ⅲ)的测定,获得较满意的结果。     

1-（4-硝基苯基）-3-（3-硝基-5-氯吡啶）三氮烯的合成及其与锌的显色反应

报道了1-(4-硝基苯基)-3-(3-硝基-5-氯吡啶)三氮烯(NPNCPDT)的合成及其与锌的显色反应研究。在Triton X-100存在下,pH 10.5的Na2B4O7-NaOH缓冲溶液中,该试剂能与锌发生显色反应,锌与NPNCPDT形成摩尔比为1∶2的黄色配合物,在450 nm处有一最大正吸收,540 nm处有一最大负吸收。以450 nm为参比波长、540 nm为测量波长进行双波长测定,表观摩尔吸光系数为2.50×105L.mol-1.cm-1。锌量在0~480μg/L符合比尔定律。用拟定方法测定人发中的微量锌,方法精密度小于2.5%(RSD,n=6)。     

青藏高原科学讨论会在北京举行

由中国科学院发起组织的青藏高原科学讨论会于1980年5月25日至31日在北京举行。出席会议的我国科学工作者有180多位,澳大利亚、巴基斯坦、孟加拉、加拿大、法国、德意志联邦共和国、荷兰、印度、意大利、日本、尼泊尔、新西兰、瑞士、土耳其、英国、美国、南斯拉夫等17个国家近80位学者也应邀参加了讨论会,其中地学界代表42人。     

北京怀柔HR_（88－1）钻孔剖面磁性地层学研究

在系统古地磁样品采集、处理和测量的基础上，运用磁性地层学的研究方法，对北京怀柔地区ＨＲ（８８－１）钻孔剖面进行了详细地层划分，分别确定了该区上新统、下更新统、中更新统和上更新统的分布深度及地质年代。     

北京怀柔HR_（88－1）钻孔剖面磁性地层学研究

在系统古地磁样品采集、处理和测量的基础上，运用磁性地层学的研究方法，对北京怀柔地区ＨＲ（８８－１）钻孔剖面进行了详细地层划分，分别确定了该区上新统、下更新统、中更新统和上更新统的分布深度及地质年代。     

Geochemistry of Late Cretaceous (60-67 Ma) igneous activities in the Hebrides Terrace seamount (guyot) area, Scotland

1Introduction Seamountsarethewell knownfeaturesinthe world’soceans,beingmostcommoninthePacific (Smith,1988;Pringleetal.,1991;Hasse,1991). Recentvolcanicactivityoccursinthezonesondi vergentorconvergentplatemarginsorintheintraplate regimes.Seamountsexisteitherasisolatedvolcanic edifices(Gardneretal.,1984;MertzandRenne, 1995)or,sometimes,formlinearchainstogetherwith oceanislands.Anumberofgeochronologicalinvestiga tionsonoceanislands(DuncanandMcDougall,1974; Dymond,1975;McDougall,1979…     

Enthalpies in (Na,Ca)- and (K,Ca)-feldspar binaries: a high-temperature solution calorimetric study

A series of high structural state plagioclases (Ab-An) was crystallized from glasses. By exchanging Na for K in KCl melts, metastable K-plagioclases (Or-An) were prepared which possess the same structural state as the starting plagioclases. Both series were investigated at 980 K by lead borate solution calorimetry. Continuing the ideas of Carpenter and McConnell (1984) and Carpenter (1992a), the results can be interpreted as follows. In the high plagioclase series, the enthalpies of solution, jH_sol, reflect the schemes of Al,Si ordering: (1) analbite-like (C2/m) ordering in the An-poor region 0hX_AnА.2, (2) high albite-like (C1¥) ordering in intermediate plagioclases, and (3) anorthite-like (I1¥) ordering in the An-rich region 0.7AnБ. In regions 1 and 2, jH_sol decreases as a function of X_An, but increases in region 3 as a consequence of the C1¥MI1¥ ordering reaction. Therefore, it is not a mixing effect but a compositionally restricted ordering effect which causes the excess enthalpies, jH^ex, to be positive in the plagioclase binary as a whole. Neglecting the existence of phase transitions at X_An=0.2 and X_An=0.7, jH^ex can be approximated by a two-parameter Margules model yielding W^H_AnAb=14Dž kJ/mol and W^H_AbAn=40Dž kJ/mol. jH_sol values of I1¥ plagioclases (X_An>0.7) can be "corrected" for the C1¥MI1¥ ordering effect (Carpenter 1992a). When combining the corrected values with the jH_sol data which were actually measured on the C1¥ plagioclases (X_An<0.7), negative excess enthalpies are generated in the plagioclase binary. This may be expected when C1¥ ordering occurs relative to topochemically monoclinic reference states of analbite and hypothetical anorthite devoid of I1¥ order. The solution experiments on the K-plagioclases resulted in similar characteristics as those found for the plagioclases. However, in addition to the ordering effects observed in the plagioclase binary, volume mismatch effects contribute to jH^ex in the K-plagioclase series. jH^ex can be represented by a Margules model with W^H_AnOr=60ᆞ kJ/mol and W^H_OrAn=91ᆢ kJ/mol when the phase transitions at X_An=0.2 and X_An=0.7 are again neglected. The contribution of the volume mismatch effect to jH^ex is considerable, as appears from the large difference between the K-plagioclase and the plagioclase Margules parameters. Their difference corresponds to a practically symmetrical dependence of jH^ex_volmism on composition, with W^H_volmism=48ᆡ kJ/mol.