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偶极装置反映激电异常的能力 总被引：1，自引：0，他引：1
“偶极－偶极装置”简称“偶极装置”,具有装置轻便、工作灵活、电磁耦合效应小等优点。偶极装置反映异常的能力如何?通过我队近几年来在变频法普查中的部分成果来谈一谈这个问题。为便于说明,我们与激电法常用的中间梯度装置进行了对比。 相似文献
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磁源瞬变电磁法常用于金属矿的勘探工作中,为了加大勘探深度和提高工作效率,常采用大定源回线装置进行测量。本文给出了一个在深部找矿工作中大定源回线装置磁源瞬变电磁法应用实例,通过Occam一维反演工作,提出和探讨了一些实际应用问题。 相似文献
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介绍一种自行设计和加工的直接雾化石墨炉进样装置的结构、工作原理和操作方法。该装置由微机控制与石墨炉加热程序同步工作,可以实现自动控制和自动测量。对雾化进样石墨炉分析的仪器参数和实验条件进行了研究和选择。结果表明,该装置与石墨炉结合具有自动化程度高、重现性好、样品利用率高和分析速度快等特点。 相似文献
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本文阐述ΠC-64型计数装置的简单改装方法。经过改装,可以提高仪器的分辨时间和工作的可靠性。在实验室中广泛采用的ΠC-64型计数装置所具有的分辨时间为50微秒,它的计数率可达到6400脈冲/秒。为了提高上述参数和仪器工作的可靠性,可以把计数装置加以改装。这种改装很容易,其实质是改变触发器[注二]和输入部分的线路。 相似文献
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通过在已知在已揭露的地下人防巷道上方高密度电阻率法中温纳装置、三极装置的试验以及异常特征分析,说明利用地下介质的电阻率差异,采用高密度电阻率法探测地下人防巷道工作时,应选择好装置类型,且要正确地识别其异常标志。 相似文献
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论述了在植被发育和地形恶劣的李子地区利用双频激电轴向偶极装置快速寻找金矿的应用成果,总结了岩矿石电性参数特征和工作方案及工作装置。认为双频激电法仪及其工作时使用的轴向偶极装置在北秦岭金银多金属成矿带天水段高山林区寻找金属硫化物金矿床具有轻便、快速、成本低、效率高、效果好的优点。结合扫面异常规模,多极距剖面测量数据的有限元最优化法幅频率数字反演,可有效的获得激电异常的半定量解释。异常查证结果表明,激电异常体与金矿体之间有很好的对应关系,文中轻便激电的工作方案在地面工作条件困难的地区值得推广。 相似文献
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在钻探施工过程中,由于工程要求,必须对钻孔做孔口压水试验,根据钻孔吸水量、压力数据,检验钻孔的漏失及其他情况。传统孔口压水试验使用的孔口装置,必须把孔内钻具提出孔外,严重地影响工程施工进度。分体式不提钻钻孔压水试验孔口装置的研发,可在不提钻的情况下完成孔口压水试验作业,大幅度缩短施工工期,减轻工人的劳动强度,减少安全事故的发生,对钻探工程施工具有一定的经济价值和现实意义。本文详细介绍了研制的分体式不提钻钻孔压水试验孔口装置的结构、工作原理及使用方法,并与传统孔口压水装置进行了试验对比,验证了分体式不提钻孔口压水试验孔口装置工作的可靠性及优势。 相似文献
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M. Zhang G. J. Redhammer E. K. H. Salje M. Mookherjee 《Physics and Chemistry of Minerals》2002,29(9):609-616
Synthetic aegirine LiFeSi2O6 and NaFeSi2O6 were characterized using infrared spectroscopy in the frequency range 50–2000 cm−1, and at temperatures between 20 and 300 K. For the C2/c phase of LiFeSi2O6, 25 of the 27 predicted infrared bands and 26 of 30 predicted Raman bands are recorded at room temperature. NaFeSi2O6 (with symmetry C2/c) shows 25 infrared and 26 Raman bands. On cooling, the C2/c–P21/c structural phase transition of LiFeSi2O6 is characterized by the appearance of 13 additional recorded peaks. This observation indicates the enlargement of the unit
cell at the transition point. The appearance of an extra band near 688 cm−1 in the monoclinic P21/c phase, which is due to the Si–O–Si vibration in the Si2O6 chains, indicates that there are two non-equivalent Si sites with different Si–O bond lengths. Most significant spectral
changes appear in the far-infrared region, where Li–O and Fe–O vibrations are mainly located. Infrared bands between 300 and
330 cm−1 show unusually dramatic changes at temperatures far below the transition. Compared with the infrared data of NaFeSi2O6 measured at low temperatures, the change in LiFeSi2O6 is interpreted as the consequence of mode crossing in the frequency region. A generalized Landau theory was used to analyze
the order parameter of the C2/c–P21/c phase transition, and the results suggest that the transition is close to tricritical.
Received: 21 January 2002 / Accepted: 22 July 2002 相似文献
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L. A. Olsen K. Friese E. Makovicky T. Balić-Žunić W. Morgenroth A. Grzechnik 《Physics and Chemistry of Minerals》2011,38(1):1-10
The crystal structure of Pb6Bi2S9 is investigated at pressures between 0 and 5.6 GPa with X-ray diffraction on single-crystals. The pressure is applied using diamond anvil cells. Heyrovskyite (Bbmm, a = 13.719(4) Å, b = 31.393(9) Å, c = 4.1319(10) Å, Z = 4) is the stable phase of Pb6Bi2S9 at ambient conditions and is built from distorted moduli of PbS-archetype structure with a low stereochemical activity of the Pb2+ and Bi3+ lone electron pairs. Heyrovskyite is stable until at least 3.9 GPa and a first-order phase transition occurs between 3.9 and 4.8 GPa. A single-crystal is retained after the reversible phase transition despite an anisotropic contraction of the unit cell and a volume decrease of 4.2%. The crystal structure of the high pressure phase, β-Pb6Bi2S9, is solved in Pna2 1 (a = 25.302(7) Å, b = 30.819(9) Å, c = 4.0640(13) Å, Z = 8) from synchrotron data at 5.06 GPa. This structure consists of two types of moduli with SnS/TlI-archetype structure in which the Pb and Bi lone pairs are strongly expressed. The mechanism of the phase transition is described in detail and the results are compared to the closely related phase transition in Pb3Bi2S6 (lillianite). 相似文献
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We present results from low-temperature heat capacity measurements of spinels along the solid solution between MgAl2O4 and MgCr2O4. The data also include new low-temperature heat capacity measurements for MgAl2O4 spinel. Heat capacities were measured between 1.5 and 300 K, and thermochemical functions were derived from the results.
No heat capacity anomaly was observed for MgAl2O4 spinel; however, we observe a low-temperature heat capacity anomaly for Cr-bearing spinels at temperatures below 15 K. From
our data we calculate standard entropies (298.15 K) for Mg(Cr,Al)2O4 spinels. We suggest a standard entropy for MgAl2O4 of 80.9 ± 0.6 J mol−1 K−1. For the solid solution between MgAl2O4 and MgCr2O4, we observe a linear increase of the standard entropies from 80.9 J mol−1 K−1 for MgAl2O4 to 118.3 J mol−1 K−1 for MgCr2O4. 相似文献
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Durgesh C Rai 《Journal of Earth System Science》2003,112(3):421-429
The current designs of supporting structures of elevated water tanks are extremely vulnerable under lateral forces due to
an earthquake and the Bhuj earthquake provided another illustration when a great many water tank stagings suffered damage
and a few collapsed. The more popular shaft type stagings suffer from poor ductility of thin shell sections besides low redundancy
and toughness whereas framed stagings consist of weak members and poor brace-column joints. A strength analysis of a few damaged
shaft type stagings clearly shows that all of them either met or exceeded the strength requirements of IS:1893-1984, however,
they were all found deficient when compared with requirements of the International Building Code. IS:1893-1984 is unjustifiably
low for these systems which do not have the advantage of ductility and redundancy and are currently being underestimated at
least by a factor of 3 and need an upward revision of forces immediately. 相似文献
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Shigeto Hirai Yohei Kojima Hiroaki Ohfuji Norimasa Nishiyama Tetsuo Irifune Stephan Klemme Geoffrey Bromiley J. Paul Attfield 《Physics and Chemistry of Minerals》2011,38(8):631-637
Raman spectroscopy and heat capacity measurements have been used to study the post-perovskite phase of CaIr0.5Pt0.5O3, recovered from synthesis at a pressure of 15 GPa. Laser heating CaIr0.5Pt0.5O3 to 1,900 K at 60 GPa produces a new perovskite phase which is not recoverable and reverts to the post-perovskite polymorph
between 20 and 9 GPa on decompression. This implies that Pt-rich CaIr1−xPtxO3 perovskites including the end member CaPtO3 cannot easily be recovered to ambient pressure from high P–T synthesis. We estimate an increase in the thermodynamic Grüneisen
parameter across the post-perovskite to perovskite transition of 34%, of similar magnitude to those for (Mg,Fe)SiO3 and MgGeO3, suggesting that CaIr0.5Pt0.5O3 is a promising analogue for experimental studies of the competition in energetics between perovskite and post-perovskite
phases of magnesium silicates in Earth’s lowermost mantle. Low-temperature heat capacity measurements show that CaIrO3 has a significant Sommerfeld coefficient of 11.7 mJ/mol K2 and an entropy change of only 1.1% of Rln2 at the 108 K Curie transition, consistent with the near-itinerant electron magnetism. Heat capacity results for post-perovskite
CaIr0.5Rh0.5O3 are also reported. 相似文献
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Correction to: A Deep-Learning-Based Geological Parameterization for History Matching Complex Models
Mathematical Geosciences - In the original paper, the units noted on the x-axes in Fig. 17a and b are incorrect. 相似文献
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The temperature (T) evolution of the barium carbonate (BaCO3) structure was studied using Rietveld structure refinements based on synchrotron X-ray diffraction and a powdered synthetic
sample. BaCO3 transforms from an orthorhombic, Pmcn, α phase to a trigonal, R3m, β phase at 811°C. The orthorhombic BaCO3 structure is isotypic with aragonite, CaCO3. In trigonal R3m BaCO3, the CO3 group occupies one orientation and shows no rotational disorder. The average <Ba–O> distances increase while the <C–O> distances
decrease linearly with T in the orthorhombic phase. After the 811°C phase transition, the <Ba–O> distances increase while C–O distances decrease.
There is also a significant volume change of 2.8% at the phase transition. 相似文献
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V. L. Vinograd O. G. Safonov D. J. Wilson L. L. Perchuk L. Bindi J. D. Gale B. Winkler 《Petrology》2010,18(4):447-459
Atomistic model was proposed to describe the thermodynamics of mixing in the diopside-K-jadeite solid solution (CaMgSi2O6-KAlSi2O6). The simulations were based on minimization of the lattice energies of 800 structures within a 2 × 2 × 4 supercell of C2/c diopside with the compositions between CaMgSi2O6 and KAlSi2O6 and with variable degrees of order/disorder in the arrangement of Ca/K cations in M2 site and Mg/Al in Ml site. The energy
minimization was performed with the help of a force-field model. The results of the calculations were used to define a generalized
Ising model, which included 37 pair interaction parameters. Isotherms of the enthalpy of mixing within the range of 273–2023
K were calculated with a Monte Carlo algorithm, while the Gibbs free energies of mixing were obtained by thermodynamic integration
of the enthalpies of mixing. The calculated T-X diagram for the system CaMgSi2O6-KAlSi2O6 at temperatures below 1000 K shows several miscibility gaps, which are separated by intervals of stability of intermediate
ordered compounds. At temperatures above 1000 K a homogeneous solid solution is formed. The standard thermodynamic properties
of K-jadeite (KAlSi2O6) evaluated from quantum mechanical calculations were used to determine location of several mineral reactions with the participation
of the diopside-K-jadeite solid solution. The results of the simulations suggest that the low content of KalSi2O6 in natural clinopyroxenes is not related to crystal chemical factors preventing isomorphism, but is determined by relatively
high standard enthalpy of this end member. 相似文献
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Cation tracer diffusion coefficients, DMe *, for Me=Fe, Mn, Co and Ti, were measured using radioactive isotopes in the spinel solid solution (Ti x Fe 1−x )3−δO4 as a function of the oxygen activity. Experiments were performed at different cationic compositions (x=0, 0.1, 0.2 and 0.3) at 1100, 1200, 1300 and 1400 °C. The oxygen activity dependence of all data for DMe * at constant temperature and cationic composition can be described by equations of the type DMe *=D∘ Me[V]. CV·a O2 2/3+DMe[I] ∘·a O2 −2/3·DMe[V] ∘ and DMe[I] ∘ are constants and CV is a factor of the order of unity which decreases with increasing δ. All log DMe * vs. loga O2 curves obtained for different values of x and for different temperatures go through a minimum due to a change in the type of point defects dominating the cation diffusion with oxygen activity. Cation vacancies prevail for the cation diffusion at high oxygen activities while cation interstitials become dominant at low oxygen activities. At constant values of x, DMe[V] ∘ decreases with increasing temperature while DMe[I] ∘ increases. 相似文献