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1.
Investigation of the use of a single analytical procedure using the non-suppressed ion chromatographic method with direct spectrophotometric detection capable of determining eight oxoanions simultaneously is presented in this paper. Potassium phosphate was found to be the most suitable eluent for UV absorbance detection at 205 nm. Oxoanions AsO3−3, SeO2−3, AsO3−4, VO3, SeO2−4, WO2−4, MoO2−4 and CrO2−4 were detected at ng ml−1 levels with well separated peaks at retention time < 25 min. The working range is in the range ng ml−1 to 50 μg ml−1. The method is sufficiently sensitive to determine As (V), V(V), Mo(VI) and Cr(VI) anions (and NO3) directly in a river water sample. The accuracy of these results was established by comparison with conventional atomic absorption methods.  相似文献   

2.
Room temperature magnetic circular dichroism spectra have been obtained for MoS2−4, MoO2−4, WS2−4, ReS4, VS3−4, VO3−4 and OsO4 through their first and second charge-transfer bands. These measurements demonstrate that the band at longest wavelength (ν1 band) must be assigned to a t1 → 2e transition for all the compounds investigated.  相似文献   

3.
The crystal and molecular structures of two quarternary salts of 2-oxosparteine (II), the methiodide (IICH+3 • I) and the methperchlorate (IICH+3 • ClO4) have been determined on the basis of X-ray and IR data. The studies were performed by analogy to previously investigated quaternary salts of sparteine (I), the methiodide (ICH+3 • I) and the methperchlorate (ICH+3 • ClO4). As expected, the configurations and conformations of cationic parts within the two pairs of quaternary salts are identical, except for the structure of their A/B fragments, which in ICH+3 cations have the character of tertiary amines, but in IICH+3 that of lactams.

On the basis of accumulated X-ray and IR data the similarities and differences in the modes of interaction of perchlorate and iodide anions with quaternary cations, and especially with their N+---CH3 groups are discussed. In this discussion are also included the methiodide and methperchlorate of -isosparteine: IIICH+3 • X (X = I or ClO4) where N+---CH3 groups are cisoidally oriented to the basic nitrogen atoms. The most interesting observations are as follows: (i) When N+---CH3 groups are easily accessible for direct quasi hydrogen bonding interactions with counter anions and when other positive charged groups, for instance lactam groups, are absent in quaternary cations, perchlorate anions interact more strongly than the iodide anions and in consequence introduce conformational changes into the ring with N+---CH3 group as well as into further rings. (ii) Perchlorate and iodide anions interact with N+---CH3 groups similarly and very weakly if at all, when the N+---CH3 groups are for steric reasons inaccessible to counter anions or when in quaternary cations there are additional groups which attract the counter anions electrostatically. The last mechanism operates in both quaternary salts of 2-oxosparteine and this is the reason why their monocrystals are isosteric and IR spectra almost identical. (iii) The sterically hindered N+---CD3 groups in both IIICD+3 • X salts give rise in their IR spectra to two doubles of sharp, well resolved bands which indicate the presence of two different rotamers stabilized by two modes of weak intramolecular hydrogen bonds with basic N atoms. (iv) In IIICH+3 • X and IIICD+3 • X salts the perchlorate and iodide anions do not interact at all with the rotating and vibrating N+---CH3 (N+---CD3) group but the structures of these salts are not isosteric since the perchlorate anions interact more strongly than iodide anions with the A/B fragment of the IIICH+3 cations. This is visible from the shapes and intensities of the so-called “trans” band in the IR spectra of both salts.  相似文献   


4.
The molecular structures of n-hexane were determined by RHF/4-21G ab initio geometry optimization at 30° grid points in its three-dimensional τ1(C11–C8–C5–C1), τ2(C14–C11–C8–C5), τ3(C17–C14–C11–C8) conformational space. Of the resulting 12×12×12=1728 grid structures, 468 are symmetrically non-equivalent and were optimized constraining the torsions τ1, τ2, and τ3 to the respective grid points, while all other structural parameters were relaxed without any constraints. From the results, complete parameter surfaces were constructed using natural cubic spline functions, which make it possible to calculate parameter gradients, |P|=[(∂P/∂τi)2+(∂P/∂τj)2]1/2, where P is a C–C bond length or C–C–C angle. The parameter gradients provide an effective measure of the torsional sensitivity of the system and indicate that dynamic activities in one part of the molecule can significantly affect the density of states, and thus the contributions to vibrational entropy, in another part. This opens the possibility of dynamic entropic conformational steering in complex molecules; i.e. the generation of free energy contributions from dynamic effects of one part of a molecule on another. When the conformational trends in the calculated C–C bond lengths and C–C–C angles are compared with average parameters taken from some 900 crystallographic structures containing n-hexyl fragments or longer C–C bond sequences, some correlation between calculated and experimental trends in angles is found, in contrast to the bond lengths for which the two sets of data are in complete disagreement. The results confirm experiences often made in crystallography. That is, effects of temperature, crystal structure and packing, and molecular volume effects are manifested more clearly in bond lengths than bond angles which depend mainly on intramolecular properties. Frequency analyses of the τ1, τ2 and τ3 torsional angles in the crystal structures show conformational steering in the sense that, if τ1 is trans peri-planar (170°≤τ1≤180°; −180°≤τ1≤−170°), the values of τ2 and τ3 are clustered closely around the ideal gauche (±60°) and trans (±180°) positions. In contrast, when τ1 is in the region (50°≤τ1≤70°), there is a definite increase in the populations of τ2 and τ3 at −90 and −150°.  相似文献   

5.
Malaiyandi M  Sastri VS 《Talanta》1983,30(12):983-985
Studies on the decomposition rates of the Mn(III) complex of cyclohexanediaminetetra-acetate (DCTA) in light and in darkness have shown that this complex is more stable than the one derived from ethylenediaminetetra-acetate. The optimum pH range for the determination of dissolved oxygen by means of the Mn(III)-DCTA complex is found to be between 3 and 4. The absorbance of this complex is independent of the amount of DCTA used (in the range 0.2–1.0 g) with water samples containing a maximum of 3.2 ppm of dissolved oxygen. Significant interferences are caused by the presence of CO2−3, HCO3, S2O2−3, PO3−4, I, NO2, SO2−3, Ca2+, Fe2+ and Fe3+ at 500 times the oxygen concentration.  相似文献   

6.
The oxygen permeation properties of mixed-conducting ceramics SrFeCo0.5O3−δ (SFCO), Ba0.5Sr0.5Co0.8Fe0.2O3−δ (BSCFO), La0.2Sr0.8Co0.8Fe0.2O3−δ (LSCFO) and Ba0.95Ca0.05Co0.8Fe0.2O3−δ (BCCFO) were studied by thermogravimetric method in the temperature range 600–900 °C. The results show that the oxygen adsorption rate constants ka of all material are larger than oxygen desorption rate constants kd and both ka and kd are not strongly dependent on temperature in the studied temperature range. The oxygen vacancy contents δ(N2) and δ(O2) in nitrogen and oxygen and their difference Δδ = δ(N2) − δ(O2) play an important role in determining the temperature behavior of oxygen permeation flux JO2.  相似文献   

7.
The enthalpy of mixing of three liquid mixtures of NaF and NaMgF3 has been measured by drop calorimetry and was found to be negative. This energy release is attributed to a change in the equilibrium

Mg1/4[MgF2−4]3/4+f å MgF2−4 to the formation of complex MgF2−4-ions. A ΔHM diagram for the system NaF-MgF2 up to 50 mol % MgF2 has been constructed.  相似文献   


8.
Poly(β-phenylpropyl -aspartate), poly(β-phenylbutyl -aspartate), and poly(β-phenylpentyl -aspartate) exhibit a reversible transformation from a right-handed -helix (R) to a left-handed ω-helix (ωL) in the solid state. During this transition, the infrared (IR) dichroism of the side-chain ester group and the birefringence change drastically, showing that the side-chain conformations are different for these two helices. In the present study, for the purpose of elucidating the preferred side-chain conformation in each helix, we performed the computational analyses. The energy contours, the directions of the IR transition moments and the anisotropies in polarizability as functions of the first two dihedral angles of the side chain, χ1 and χ2 were calculated. Then, comparing them with the experimental IR dichroism and birefringence data, we elucidated the specific side-chain conformation preferred for each R or ωL skeleton. The preferred values of (χ1, χ2) were found to be (−75, −60°) for R and (180, 45°) for ωL.  相似文献   

9.
A series of CexPr1−xO2−δ mixed oxides were synthesized by a sol–gel method and characterized by Raman, XRD and TPR techniques. The oxidation activity for CO, CH3OH and CH4 on these mixed oxides was investigated. When the value x was changed from 1.0 to 0.8, only a cubic phase CeO2 was observed. The samples were greatly crystallized in the range of the value x from 0.99 to 0.80, which is due to the formation of solid solutions caused by the complete insertion of Pr into the CeO2 crystal lattices. Raman bands at 465 and 1150 cm−1 in CexPr1−xO2−δ samples are attributed to the Raman active F2g mode of CeO2. The broad band at around 570 cm−1 in the region of 0.3 ≤ x ≤ 0.99 can be linked to oxygen vacancies. The new band at 195 cm−1 may be ascribed to the asymmetric vibration caused by the formation of oxygen vacancies. The TPR profile of Pr6O11 shows two reduction peaks and the reduction process is followed: . The reduction temperature of CexPr1−xO2−δ mixed oxides is lower than those of Pr6O11 or CeO2. TPR results indicate that CexPr1−xO2−δ mixed oxides have higher redox properties because of the formation of CexPr1−xO2−δ solid solutions. The presence of the oxygen vacancies favors CO and CH3OH oxidation, while the activity of CH4 oxidation is mostly related to reduction temperatures and redox properties.  相似文献   

10.
Two carbon-rich starburst gold(I) acetylide complexes [TEE][Au(PCy3)]4 (3, [TEE]H4=tetraethynylethene) and [TEB][Au(PCy3)]3 (6, [TEB]H3=1,3,5-triethynylbenzene) were prepared and their UV–vis absorption, emission and excitation spectra have been recorded. In fluid CH2Cl2 solutions, 3 exhibits prompt 1(ππ*) fluorescence with λ0–0 and λmax at 413 and 428 nm, respectively, while 6 displays 3(ππ*) phosphorescence with λ0–0 and λmax at 446 and 479 nm, respectively. The crystal structure of 3·CH2Cl2 has been determined.  相似文献   

11.
The thermodynamic interactions in aqueous solutions of uncharged polymers were studied. Using a gel-deswelling method, the water activities (chemical potentials) in binary and ternary (two polymers in one solvent) solutions of methylcellulose (MC), polyvinyl alcohol (PVA) and polyvinyl pirrolidone (PVP), respectively were determined at various polymer volume fractions (1.0 × 10−2 < v2 < 1.0 × 10−1). On the theoretical basis of the Flory–Huggins approximations, the relevant solvent–segment (χ12 or χ13) and segment–segment pair interaction parameters (χ23) have been calculated.

The solvent activity curves (ln a1 versus polymer volume fraction) can be well described by a polynomial of third-degree in both the binary and the ternary solutions of the polymers. The solvent–segment interaction parameters exhibit a slight dependence on the polymer concentration. For each binary solution, the χ12v2 function can be fitted by a straight line wich has a small positive slope. In the mixtures of two polymers, the values of the segment–segment (χ23) interaction parameters were close to zero or sligthly negative (χ23 0 ± 0.03), indicating that under the studied conditions, the polymers in the ternary solutions are compatible.  相似文献   


12.
K. Dittrich 《Talanta》1977,24(12):735-739
The atomic-absorption determination of traces of Ga in In, P, As and InAs and of traces of In in Ga, P, As, GaAs and gap is described. The mechanism of the evaporation of the trace element according to the medium used (HCl or HNO3) is discussed. Nitric acid medium is recommended for analytical determinations. The evaporation of the trace elements and matrices was investigated by means of absorbance vs. time curves. It is shown that a thermal fractionation of AsO3−4 and PO3−4 matrices and Ga and In traces is possible in the ashing step. In the case of Ga the thermal fractionation of the matrices (In3+, In3+/AsO3−4) from the trace element is possible in the atomization step. The thermal fractionation of In traces from the matrices (Ga3+, Ga3+/AsO3−4, Ga3+/Po3−4) is impossible. The results and the reasons for the non-specific absorption are discussed. The absolute detection limits are Ga 45 pg, In 35 pg. The relative detection limits are 1 ppm in a 0.1 mg sample.  相似文献   

13.
K. Dittrich 《Talanta》1977,24(12):725-733
The evaporation of the species Ga3+, In3+, PO3−4, AsO3−4, Ga3+/AsO3−4, Ga3+/PO3−4 and In3+/AsO3−4 in HCl and HNO3 medium was investigated by measurement of the non-specific absorption at 250 nm, in a graphite cuvette, with a continuum light source. The maximum of the non-specific absorption is given for the ashing and atomizing phases as a function of the ashing temperatures. Ashing temperatures for analytical determinations can be derived from the results. The mechanisms of evaporation of the substances were investigated by means of extinction-time curves. Absorption spectra of the matrices and of the pure acids used were measured between 190 and 330 nm in the graphite cuvette at different ashing and atomizing temperatures. The InCl- and GaCl-bands of the C-system and new bands of GaO- and InO-molecules were found. The PO-band at 246 nm was detected. The results are discussed and can be applied for thermal fractionation and for background correction by the two-line method in trace analysis by electrothermal AAS.  相似文献   

14.
An analytical flow-injection procedure based on PbSO4 colloidal formation is proposed as a turbidimetric determination of sulphate in natural waters. Ethanol-water was used as a medium in order to improve the sensibility of the method. Both chemical and flow variables as well as interfering species were studied. A detection limit of 0.3 μg SO2−4 ml−1 was found, and the analytical range (according to Beer's law) was 2–20 μg SO2−4 ml−1. The precision was better than 3% R.S.D. and the sample throughput was ca. 35 h−1. The method, when compared with a standard methodology, gave good results when applied to water analysis.  相似文献   

15.
The enthalpies of formation of the complexes between the silver(I) ion and some sulphur-containing aminopyridines of general formula N(CH2)n−1-S-(CH2)m-NH2 where n = 1, and m = 1,2; 1,3; 2,2; 2,3 have been determined by direct calorimetric titration at 25°C in 0.5 M (K)NO3 solution. The corresponding entropy terms, ΔS, have been calculated using the obtained enthalpy values and the previously reported ΔG values.

In acid medium (pH < 3) coordination occurs through the thioether group and the protonated species AgLH3+2 and AgL2H5+4 are enthalpy-stabilized and entropy-destabilized. At higher pH values (pH &>; 3) additional chelation through the pyridine nitrogen is obvious by a marked increase in the enthalpy of formation of the complexes AgL2H4+3, AgL2H3+2 and AgLH2+. The last complex dimerizes into a cyclic dimer Ag2L, H4+2. At still higher pH values (pH &>; 6) the participation of the amino group in the dimeric chelates Ag2L2H3+ and Ag2L2+2 is revealed again by a marked increase in the heat of complexation.  相似文献   


16.
Circular polarization measurements establish a large antisymmetric component of the Raman scattering from the breathing vibration of CuBr2−4 in acetonitrile when excited at 5145 Å in the first Br → Cu charge-transfer (π) absorption band. This is attributable to spin degeneracy and to the 700 cm−1 spin-orbit splitting of the CT excited state.  相似文献   

17.
The gas-phase stabilities of cluster ions SF+m (SF6)n with m = 0−5 were determined by using a high pressure mass spectrometer. The bond energies of SF+m (SF6)1 were found to be less than 10 kcal/mol and to decrease with m = 0 → 5. There appear to be rather large gaps in the bond energies between n = 1 and 2 for the clusters SF+m (SF6)n with m = 0−4. The structures of SF+5, SF+ (SF6)1, SF+3 (SF6)1, and SF+5 (SF6)1 were investigated by ab initio molecular orbital calculations. For SF+5, the D3h geometry is found to be most stable andC4v is a transition state of the Berry pseudorotation. For the ion-molecule complexes, the “on-top hat” models were found to be the most stable structures.  相似文献   

18.
As a part of the European EUROCORE and GRIP (Greenland Ice Core Project) operations aimed at recovering deep ice cores at Summit (Central Greenland), we have for the first time successfully performed ion chromatography measurements in the field and investigated in detail the soluble impurities, including Na+, NH+4, K+, Mg2+, Ca2+, F, CH3COO, CH2 OHCOO, HCOO, CH3SO3, Cl, NO2, SO42− and C2O42−, trapped in ice deposited over some 200 000 years in Greenland.  相似文献   

19.
1H, 13C and 15N NMR spectroscopy has been applied for investigation of amine adducts with rhodium(II) tetraacetate dimer and rhodium(II) tetratrifluoroacetate dimer in CDCl3 solution. Subsequent formation of two adducts, 1:1 and 2:1, was proved by NMR and VIS titration experiments, and by NMR measurements at reduced temperatures, from 233 to 273 K. The adduct formation shift, defined as Δδadductδligand and characterizing complexation reaction, varies from ca. 0 to +1.6 ppm for 1H, from ca. −10 to +6 ppm for 13C and from −4.4 to −39 ppm for 15N NMR. Formation of N–Rh bond slows the inversiof on the nitrogen atom and generates, in the case of N-methyl-(1-phenylethyl)-amine, a nitrogenous chiral center in the molecule. VIS spectra of amine-dirhodium salt mixture contain two bands in the 532–597 nm spectral range, assigned to 1:1- and 2:1-adducts.  相似文献   

20.
To examine the steric effects on the stability of Ln(0) π-arene compounds, molecular mechanics (MMP2) calculations are performed on Gd(η-C6H6)2 and Ln(η-But3C6H3)2 (where Ln is Gd, Yb and Y ). The small potential-well depth ( ≈ 2 kcal mol−1) and the large Gd-C equilibrium distance ( > 3.3 Å) explains the instability of Gd(η-C6H6)2, while the difference in the stability between Gd(η-But3C6H3)2 and Yb(η-But3C6H3)2 can be attributed to the difference in the van der Waalsradii of the two metals and the more contracted 5d orbitals on the Yb atom.  相似文献   

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