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1.
Mixed rare earth hydrogen selenite crystals, neodymium praseodymium hydrogen selenite (NdxPr1−x(HSeO3)(SeO3)⋅2H2O), Neodymium samarium hydrogen selenite (NdxSm1−x(HSeO3)(SeO3)⋅2H2O) and praseodymium samarium hydrogen selenite (PrxSm1−x(HSeO3)(SeO3)⋅2H2O) were prepared by gel diffusion technique. Simultaneous thermogravimetric and differential thermal analysis were carried out on the grown crystals. Decomposition is observed to occurs in six steps, which gives the evidence of successive losses of H2O and SeO2. The final product due to decomposition is a mixed rare earth oxides. FT-IR spectrum of the crystal samples heated at different temperatures complemented to the TG-DTA results. This revised version was published online in July 2006 with corrections to the Cover Date.  相似文献   

2.
The present work describes the crystal structure, thermal behavior, and infrared absorption spectrum of cesium hydrogen selenite-selenious acid (12), CsHSeO3 · 2H2SeO3. This compound crystallizes in the monoclinic crystal system withP21c-C52b (Z = 4) as the space group. The unit cell dimensions are as follows:a = 8.9897(20), b = 8.5078(21), c = 12.6476(31)A˚, and β = 95.141(19)°. The crystal structure consists of discrete H2SeO3 molecules which are weakly hydrogen bonded to form layers which are further connected by (HSeO3) ions with much stronger hydrogen bonds. The hydrogen atoms show no disorder within the hydrogen bonds. The Cs+ ions are coordinated to oxygens from both selenious acid molecules and hydrogen selenite ions. The thermal decomposition of CsHSeO3 · 2H2SeO3 in air starts with incongruent melting due to rupture of hydrogen bonds at 310 K and is followed later by the formation of cesium diselenite phase. At higher temperatures (700 K) this compound decomposes with oxidation of selenium to yield cesium selenate. Both deformation and stretching vibrations of SeOH groups from both (HSeO3) ions and H2SeO3 molecules can be found in the IR absorption spectrum of CsHSeO3 · 2H2SeO3. This confirms the ordered position of hydrogen atoms in hydrogen bonds. The OH vibrations corresponding to hydrogen bonded species can be found also.  相似文献   

3.
The kinetics of the reaction between the two-electron reduced form of cobalamin (super-reduced cobalamin, cob(I)alamin, or Cbl(I)) and sodium selenite in an alkaline medium is studied spectrophotometrically. It is shown that the selenite rapidly oxidizes Cbl(I) to cob(II)alamin (Cbl(II)). It is established that the active form of the oxidant is the protonated selenite anion (HSeO3-), which receives six electrons during the reaction and transforms into HSe. The reactions of cob(I)alamin oxidation by selenite and sulfite are compared.  相似文献   

4.
The new hybrid material tetrapropylammonium hydrogen selenate bis (selenic acid), N(C3H7)4[HSeO4][H2SeO4]2 (hereafter abbreviated TPSe) has been synthesized by slow evaporation technique at room temperature. Crystal structure, DTA-TGA measurements, Raman, Infrared spectroscopy, nuclear magnetic resonance (NMR) electrical properties, and optical properties were provided to characterize the TPSe. This crystal structure contains one organic cation [N(C3H7)4]+, one [HSeO4] tetrahedra, and two neutral selenic acids H2SeO4. The inorganic [HSeO4] and H2SeO4 species consist of infinite two-dimensional inter-linkers via strong hydrogen bonds (O-H⋯O), giving birth to trimmers [(H2SeO4)2 HSeO4]nn−. The IR and Raman spectra of the compound recorded at room temperature were studied in regard to the literature data, and on the basis of theoretical group analysis. The theoretical calculations using the density functional theory DFT at the B3LYP/6-31G(d) level, are made to study the optimized molecular structure, the vibrational spectra, and the optical properties of TPSe compound. Good agreements were found between the theoretical results and the experimental Raman, IR spectra and the molecular structure. The polarizability α, the hyperpolarizability β, and the electric dipole μ calculated using DFT/B3LYP-31G(d) exhibit the non-zero hyperpolarizability β of the TPSe, indicating that this material could be used in certain NLO applications. The thermal DTA-TGA analyses did not show any phase transition in the 333–500 K temperature domain. The complex impedance spectroscopy is measured and discussed in the temperature (290–363 K) and frequency (1 kHz−13 MHz) domains to study the electrical propreties of the compound.  相似文献   

5.
A selenous acid (H2SeO3) precursor was intercalated as biselenite (HSeO3) ions into the interlayer gallery of carbonated magnesium aluminum layered double hydroxide (MgAl-LDH) in aqueous solution. Reduction reaction of selenous ions by aqueous hydrazine solution produced polyselenide intercalated LDHs which were consecutively exchanged with iodide through redox reaction under iodine vapor. The polyselenide containing LDHs adsorbed iodine vapor spontaneously and triiodide was incorporated in the interlayer space followed by formation of selenium polycrystalline phase. Two dimensional framework of MgAl-LDH is strong enough to resist against the reducing power of hydrazine as well as oxidation condition of iodine. The SEM data demonstrated that the shapes of LDH polycrystalline have little changed after the above redox reactions. The polyselenide and iodide LDH products were analyzed by XRD, Infrared and Raman spectra which strongly suggested the horizontal arrangement of polyselenide and triiodide in gallery space of LDHs.  相似文献   

6.
The selenite/hydroselenite compounds Ce(SeO3)(HSeO3), Tb(SeO3)(HSeO3)·2H2O, and Cs[U(SeO3)(HSeO3)]·3H2O were synthesized by hydrothermal means at 453 K from the reaction of CeO2 or Tb4O7 or UO2 with SeO2 and CsCl (as a mineralizer). Ce(SeO3)(HSeO3) crystallizes in the non-centrosymmetric orthorhombic space group Pca21. The structure comprises a two-dimensional network of interconnected CeO10 bicapped distorted square antiprisms and SeO3 trigonal pyramids. Tb(SeO3)(HSeO3)·2H2O crystallizes in the non-centrosymmetric orthorhombic space group P212121. The structure features a two-dimensional layer of interconnected TbO8 distorted square antiprisms and SeO3 trigonal pyramids. Cs[U(SeO3)(HSeO3)]·3H2O crystallizes in the centrosymmetric monoclinic space group P21/n. The structure consists of two-dimensional layers of interconnected UO7 pentagonal bipyramids and SeO3 trigonal pyramids. The layers in all three structures are held together by hydrogen-bonding networks.  相似文献   

7.
The first selenite chloride hydrates, Co(HSeO3)Cl · 3 H2O and Cu(HSeO3)Cl · 2 H2O, have been prepared from solution and characterised by single‐crystal X‐ray diffraction. The cobalt phase adopts an unusual “one‐dimensional” structure built up from vertex‐sharing pyramidal [HSeO3]2–, and octahedral [CoO2(H2O)4]2– and [CoO2(H2O)2Cl2]4– units. Inter‐chain bonding is by way of hydrogen bonds or van der Waals' interactions. The atomic arrangement of the copper phase involves [HSeO3]2– pyramids and Jahn‐Teller distorted [CuCl2(H2O)4] and [CuO4Cl2]8– octahedra, sharing vertices by way of Cu–O–Se and Cu–Cl–Cu bonds. Crystal data: Co(HSeO3)Cl · 3 H2O, Mr = 276.40, triclinic, space group P 1 (No. 2), a = 7.1657(5) Å, b = 7.3714(5) Å, c = 7.7064(5) Å, α = 64.934(1)°, β = 68.894(1)°, γ = 71.795(1)°, V = 337.78(7) Å3, Z = 2, R(F) = 0.036, wR(F) = 0.049. Cu(HSeO3)Cl · 2 H2O, Mr = 263.00, orthorhombic, space group Pnma (No. 62), a = 9.1488(3) Å, b = 17.8351(7) Å, c = 7.2293(3) Å, V = 1179.6(2) Å3, Z = 8, R(F) = 0.021, wR(F) = 0.024.  相似文献   

8.
The chemical composition and peculiarities of the structure of a salt that precipitates from aqueous solution of NH4HSeO3 at the 25 °C was studied by NMR and Raman spectroscopy methods using the single crystal samples with different heavy water contents. It was proved that this salt is actually monohydrate of hydrogen selenite, NH4HSeO3H2O but not trihydrate of pyroselenite, (NH4)2Se2O53H2O as was assumed previously based on the data cited in the literature.  相似文献   

9.
Preparation, Crystal Structure and IR Spectra of BeSeO3 · H2O – Hydrogen Bonds and Correlation of IR and Structure Data in the Monohydrates MSeO3 · H2O (M = Be, Ca, Mn, Co, Ni, Zn, Cd) BeSeO3 · H2O (oP32) has been obtained by treating amorphous BeSeO3 · 4 H2O precipitated from Be(HSeO3)2 solutions hydrothermally at 150 °C. The crystal structure (P212121, a = 560.59(4), b = 755.25(5), c = 781.14(5) pm, Z = 4, DX = 3.092 gcm–3, R = 0.018 for the 2034 reflections with I > 2σI of the enantiomer investigated) contains BeO3(H2O) tetrahedra built up from three selenite and one water oxygen atoms. The BeO3(H2O) tetrahedra are 3 D‐connected via Se atoms of trigonal pyramidal SeO32– ions. The Be–O distances are 161.8 to 164.4 pm. The Se–O bond lenghts (169.2–170.3 pm) and the O–Se–O bond angles (98.1–101.4°) are normal. The water molecules of crystallization form together with the SeO32– ions screw‐like hydrogen bond systems along [100]. Despite the strong synergetic effect of the Be2+ ions, the hydrogen bonds (d(OH…O) = 267.4 and 276.4 pm, respectively; νOD of matrix isolated HDO molecules: 2244 and 2405 cm–1, respectively) are normal compared to other neutral selenite hydrates. Together with the hitherto known monohydrates MIISeO3 · H2O and other beryllium salt hydrates, the hydrogen bonds of BeSeO3 · H2O are discussed with regard to their geometry and IR spectroscopy.  相似文献   

10.
The vibrational spectra (IR and Raman) of CH2ClPO3H2 and of its anions in solutions of H2O and D2O are reported. The IR spectra of the solid dibasic sodium and potassium salts, the solid normal and O-deuterated monobasic sodium and potassium salts and of the solid normal and O-deuterated acid are discussed. Symmetry and internal stretching force constants, stretch-stretch interactions and potential energy distributions are obtained from normal coordinate analysis of CH2C1PO3H2, CH2ClPO3H? and CH2C1PO32?, and the calculated and observed frequencies for O-deuterated acid and monobasic anion are compared.  相似文献   

11.
The organically‐templated uranyl selenite, (H2en)[(UO2)(SeO3)(HSeO3)](NO3) · 0.5H2O ( 1 ) (en = 1,2‐ethylenediamine) was synthesized and characterized by elemental analyses, IR spectroscopy, TG, and single‐crystal X‐ray diffraction. Compound 1 crystallizes in the orthorhombic system, space group Pbca, with a = 13.170(3) Å, b = 11.055(2) Å, c = 18.009(4) Å, V = 2621.8(9) Å3, M = 1316.19, Z = 4, Dcal = 3.334 g · cm–3, μ(Mo‐Kα) = 17.998 mm–1, GOF = 1.059, R1 = 0.0263, wR2 = 0.0532 [I>2σ(I)]. The X‐ray diffraction analysis reveals that compound 1 has a three‐dimensional (3D) supramolecular structure. It contains negatively charged [UO2(HSeO3)(SeO3)] inorganic anion layers and is balanced by [H2en]2+ cations and NO3 anions located in the interlayers. Furthermore, the photoluminescence properties of 1 were investigated.  相似文献   

12.
Compound Na[UO2(SeO3)(HSeO3)] · 4H2O (I) has been synthesized and studied by single-crystal X-ray diffraction. The crystals of I are monoclinic with the unit cell parameters a = 8.8032(5) Å, b = 10.4610(7) Å, c = 13.1312(7) Å, β = 105.054(2)°, space group P21/n, Z = 4, V = 1167.76(12) Å3, R = 0.0394. The main structural units of crystals I are the [UO2(SeO3)(HSeO3)]? layers belonging to the AT3B2 crystal-chemical group (A = UO 2 2+ , T3 = SeO 3 2? , B2 =HSeO 3 ? ) of the uranyl complexes. The sodium ions are linked with oxygen atoms of two uranyl ions of the same layer and with four water molecules. Electroneutral packets that formed are linked into a three-dimensional framework through a system of hydrogen bonds.  相似文献   

13.
The electrochemical Peltier effect was studied at a gold electrode in solutions containing some Fe(II)/Fe(III) redox couples by measuring the local temperature change in the electrode/solution interphase under controlled-potential and controlled-current polarization. Relative values of the electrochemical Peltier coefficient for the cathodic process at equilibrium potential, which is denoted by (Πc)I=0, were determined by analyzing the observed temperature change as a function of current. The values of (Πc)I=0 were found to be positive for the Fe(H2O)62+/Fe(H2O)63+ systems in HClO4 (1 M), HNO3 (1 M), H2SO4 (0.5 M), and HCl (1 M), their magnitudes being very similar in the first three acid solutions, but smaller in the HCl solution. On the other hand, a negative value of (Πc)I=0 was obtained in the case of a Fe(CN)64?/Fe(CN)63? couple in a H2SO4 (0.5 M) solution. Such a difference in the Peltier coefficient is considered to be due to the difference in the ionic species of iron involved in the electrode reaction.  相似文献   

14.
Synthesis and Crystal Structure of Hydrogen Selenates of Divalent Metals – M(HSeO4)2 (M = Mg, Mn, Zn) and M(HSeO4)2 · H2O (M = Mn, Cd) New hydrogen selenates M(HSeO4)2 (M = Mg, Mn, Zn) and M(HSeO4)2 · H2O (M = Mn, Cd) have been synthesized using MSeO4 (M = Mg, Mn, Zn, Cd) and 90% selenic acid as starting materials. The crystal structures have been determined by X-ray single crystal crystallography. The compounds M(HSeO4)2 (M = Mg, Zn) belong to the structure type of Mg(HSO4)2, whereas Mn(HSeO4)2 forms a new structure type. Both hydrogen selenate monohydrates are isotypic to Mg(HSO4)2 · H2O. In all compounds the metal atoms are octahedrally coordinated by oxygen atoms of different HSeO4-tetrahedra. In the HSeO4-tetrahedra the Se–OH-distances (mean value 1.70 Å) are about 0.1 Å longer than Se–O-distances (mean value 1.62 Å). In the structure of M(HSeO4)2 (M = Mg, Zn) there are zigzag chains of hydrogen bonded HSeO4-tetrahedra. The structure of Mn(HSeO4)2 is characterized by chains of HSeO4-tetrahedra in form of screws. Hydrogen bonds from and to water molecules connect double layers of MO6-octahedra and HSeO4-tetrahedra in the structures of M(HSeO4)2 · H2O.  相似文献   

15.
On the Hydrates M(HSeO3)2 · 4H2O (M = Mg, Co, Ni, Zn) – Crystal Structures, IR, Raman, and Thermoanalytical Investigations From aqueous solutions of M(HSeO3)2 single crystals of Mg(HSeO3)2 · 4H2O and of the hitherto unknown compounds Co(HSeO3)2 · 4H2O, Ni(HSeO3)2 · 4H2O and Zn(HSeO3)2 · 4H2O could be obtained. The crystal structures, X-ray powder, IR, Raman and thermoanalytical (DTA, TG, Raman heating) data are presented and discussed. The crystal data of the isotypic compounds are: monoclinic, space group C2/c, Z = 4, Mg: a = 1 464.6(2), b = 755.3(1), c = 1 099.9(1) pm, β = 126.59(1)°, V = 0.9769(1) nm3, Co: a = 1 462.5(2), b = 756.5(2), c = 1 102.2(2) pm, β = 126.53(1)°, V = 0.9798(2) nm3, Ni: a = 1 452.2(2), b = 751.0(1), c = 1 091.5(1) pm, β = 126.28(1)°, V = 0.9595(1) nm3, Zn: a = 1 468.3(2), b = 755.8(1), c = 1 103.1(1) pm, β = 126.79(1)°, V = 0.9804(2) nm3. The crystal structures consist of hexagonal packed [M(HSeO3)2 · 2H2O]n chains of [MO4(H2O)2] octahedra linked by Se atoms. They contain trigonal pyramidal SeO2OH?ions with “free” hydroxyl groups and also “free” molecules of water of crystallization. The hydroxyl groups build strong H-bonds (O? H …? O distances: 265–268 pm). The IR spectra show AB doublett bands in the OH stretching mode region of the hydroxyl groups. The water molecules of crystallization are linked to planar (H2O)4 tetramers by H-bonds with unusually short O? H …? O bond distances of 271–273 pm. DTA and TG measurements indicate that thermal decomposition results in the direct formation of the respective diselenite MSe2O5. Raman heating measurements show under quasi static conditions the intermediate formation of the anhydrous hydrogen selenites.  相似文献   

16.
Tetra­ammonium cadmium di­hydrogenselenite(IV) diselen­ate(VI), (NH4)4Cd(HSeIVO3)2(SeVIO4)2, is the third example of a compound containing both hydrogen selenite and selenate anions, and has a new structure type. It contains kröhnkite‐like heteropolyhedral chains in which CdO6 octahedra are linked via bridging HSeO3 groups, having their remaining two trans apices decorated by SeO4 groups. The charge‐balancing NH4 groups are involved in weak hydrogen bonding, whereas the H atom of the HSeO3 group provides a strong hydrogen bond [O⋯O = 2.614 (5) Å]. The average Cd—O bond length is 2.298 Å. All atoms are on general positions except Cd (on ). Relations to the kröhnkite‐type compounds Na2Mg(SO3)·2H2O, Ba2CoCl2(SeO3)2 and Ba2Ca(HPO4)2(H2PO4)2, and to the mineral curetonite are dis­cussed. Unit‐cell data are given for an isotypic MnII analogue.  相似文献   

17.
A new compound, Rb4Be(SeO4)2(HSeO4)2·4H2O, crystallizes in a comparatively wide concentration range from mixed beryllium rubidium selenate solutions (from solutions containing 29.06 mass% beryllium selenate and 25.75 mass% rubidium selenate up to solutions containing 12.53 mass% beryllium selenate and 55.32 mass% rubidium selenate).Rb4Be(SeO4)2(HSeO4)2·4H2O crystallizes in the acentric orthorhombic space group Pmn21 (a = 32.607(4), b = 10.676(2), c = 6.069(1) Å, V = 2112.8 Å3, Z = 4, R1 = 0.047 for 4059 Fo > 4σ(Fo) and 311 variables). The crystal structure is composed of Be(H2O)4 tetrahedra arranged in layers at x = 0 and x = ½, alternating with broad layers built up from SeO4 and HSeO4 selenate tetrahedra and Rb cations. The beryllium–water layers are linked to the rest of the structure via hydrogen bonds only. The H2O molecules as well as the OH molecules of the acid HSeO4 groups form strong to very strong hydrogen bonds with donor–acceptor distances between 2.58 and 2.74 Å.Vibrational spectra (infrared and Raman) of Rb4Be(SeO4)2(HSeO4)2·4H2O are presented and discussed in the region of the fundamentals of both the selenate and the beryllium tetrahedra (skeleton motions) as well as in the region of the OH vibrations at ambient and liquid nitrogen temperature (LNT). The appearance of four Raman bands corresponding to ν1 of the selenate ions reflects the existence of four crystallographically different selenate tetrahedra in the structure. The spectroscopic experiments reveal that the ν1 modes of the selenate ions appear at higher frequencies than some components of ν3. Bands of an AB doublet structure (2950, 2390 cm?1) arising from the OH stretching modes of the HSeO4- ions are recognized in the infrared spectra. The appearance of two infrared bands (1308, 1250 cm?1) corresponding to δ(OH) (in-plane bending modes of the OH groups) confirms the structural data regarding the existence of two crystallographically different OH groups. The water librations are also briefly commented. The appearance of a band at a comparatively large wavenumber (1013 cm?1) corresponding to rocking librations of the water molecules indicate that strong hydrogen bonds are formed in the title compound.  相似文献   

18.
Four new substituted amino acid ligands, N-(3-hydroxybenzyl)-glycine acid (HL1), N-(3-hydroxybenzyl)-alanine acid (HL2), N-(3-hydroxybenzyl)-phenylalanine acid (HL3), and N-(3-hydroxybenzyl)-leucine acid (HL4), were synthesized and characterized on the basis of 1H NMR, IR, ESI-MS, and elemental analyses. The crystal structures of their copper(II) complexes [Cu(L1)2]·2H2O (1), [Cu(L2)2(H2O)] (2), [Cu(L3)2(CH3OH)] (3), and [Cu(L4)2(H2O)]·H2O (4) were determined by X-ray diffraction analysis. The ligands coordinate with copper(II) through secondary amine and carboxylate in all complexes. In 2, 3, and 4, additional water or methanol coordinates, completing a distorted tetragonal pyramidal coordination geometry around copper. Fluorescence titration spectra, electronic absorption titration spectra, and EB displacement indicate that all the complexes bind to CT-DNA. Intrinsic binding constants of the copper(II) complexes with CT-DNA are 1.32?×?106?M?1, 4.32?×?105?M?1, 5.00?×?105?M?1, and 5.70?×?104?M?1 for 1, 2, 3, and 4, respectively. Antioxidant activities of the compounds have been investigated by spectrophotometric measurements. The results show that the Cu(II) complexes have similar superoxide dismutase activity to that of native Cu, Zn-SOD.  相似文献   

19.
An experimental and computational study on the conformational preference of 1,n′-disubstituted ferrocenoyl amino acids and dipeptides is presented. Only l-amino acids were used for the synthesis of Fe[C5H4-CO-Met-Met-OMe]2 (4), but according to the X-ray structure a 4:1 mixture of l,d,M,d,l and l,d,M,l,l isomers is obtained (l describes amino acid chirality and M the helical chirality of the ferrocene core). This result is in agreement with IR and CD solution phase data and can be explained with a racemization by 1 M NaOH during the synthesis. In order to determine the relative stabilities of the different conformations, DFT calculations on model compounds Fe[C5H4-CO-Gly-NH2]2 (5) and Fe[C5H4-CO-Ala-OMe]2 (6) were performed using the B3LYP/LanL2DZ method with ECPs on the heavy atoms. Conformers 5A-5C with different hydrogen bond patterns have significantly different stabilities with a stabilization by about 30 kJ mol−1 per hydrogen bond. The “Herrick conformation” 5A with two hydrogen bonds is the most stable in the gas phase, in accordance with the solution and solid phase data. In contrast, only small energetic differences (less than 10 kJ mol−1) were calculated for conformers l,P,l-6A, l,P,d-6A and d,P,d-6A, which differ only in amino acid chirality.  相似文献   

20.
The crystal structure of RbH3(SeO3)2 has been determined from three-dimensional single crystal X-ray diffractometer data obtained at room temperature. Four formula units crystallize in an orthorhombic unit cell of dimensions: a = 5.9192(2), b = 17.9506(5), and c = 6.2519(3) Å. The space group is P212121. The structure consists of two types of chains at a right angle. One chain is built up of H2SeO3 molecules linked by 2.594(8)-Å hydrogen bonds and the other of HSeO3? ions linked by 2.571(12)-Å hydrogen bonds. These two types of chains are cross-linked by a third hydrogen bond of length 2.521(7) Å. The rubidium ion is surrounded by eight oxygen atoms forming a distorted cube. The Rb+O distances are in the range 2.94–3.19 Å.  相似文献   

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