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利用交流阻抗谱实验技术,在0.5~2.0 GPa、573~873 K和10-1~106 Hz条件下,借助YJ-3000t紧装式六面顶高压设备和Solartron-1260阻抗/增益-相位分析仪测定了石英砂岩的电导率。实验结果表明:在测定的频率范围,样品的复阻抗的实部、虚部、模和相角对频率有很强的依赖性。随着温度升高,电导率增大,lgσT与1/T之间符合Arrhenius线性关系。通过拟合计算,获得了表征样品电学性质的指前因子、活化焓、活化能、活化体积等物性参数。杂质离子导电机制对高温高压下石英砂岩的导电行为提供了合理的解释。 相似文献
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《吉林大学学报(地球科学版)》2015,(Z1)
<正>橄榄石是上地幔最重要组成矿物之一,其在高压下电学性质得到了广泛的关注[1-3]。本次工作,在4.0 GPa和573~1373 K条件下,采用多面顶高压设备和Solartron-1260阻抗/增益-相位分析仪,原位测量了沿[100]、[010]和[001]三个不同晶向的含水的San Carlos单晶橄榄石电导率[4]。实验结果表明:(1)在高温高压下原位测量了沿[100]、[010]和[001]三个晶向上含水的橄榄石电导率,发现低温段 相似文献
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高温高压下辉长岩的电导率实验研究 总被引：1，自引：1，他引：1
在 1 .0～2 .0GPa和 3 2 0～ 70 0℃下 ,1 2～ 1 0 5Hz的频率范围内 ,进行了辉长岩的电导率就位测量 ,并用阻抗谱分析了其微观电传导机制。结果表明 ;电导率对测量频率具有依赖性。复阻抗平面上只出现了反映颗粒内部传导机制的阻抗弧 ,在高压下这种机制起主导作用 ,该阻抗弧出现在 1 0 5～n×1 0 2 Hz(n为 1～9的正整数 )的频率范围内。以本实验所获得的电导率结果和前人的工作为依据得出辉长岩不能在中下地壳形成高导层的结论。 相似文献
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在1.0、2 .0GPa和873～12 2 3K的温压条件下,借助于12 6 0阻抗增益相位分析仪测定了叶蜡石的电导率,并用阻抗谱原理分析了其微观导电机制。实验结果表明:样品的电导率对频率具有很强的依赖性;电阻率随着温度的升高而减小,电导率随着温度升高而增大,logσ与1/T之间符合Arrenhius线性关系;叶蜡石在1.0GPa和2 .0GPa的压力下脱水温度分别为10 74K和110 1K。根据本次获得的电导率实验结果并结合前人对滑石族所做的工作,得出了与前人不同的结论:滑石族矿物脱水电导率曲线出现了转折点。 相似文献
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在1．0～4．0GPa和1073～1423K及不同的氧分压条件下，借助YJ-3000t紧装式六面顶高压设备和Sarltron-1260阻抗／增益-相位分析仪，就位测定了斜方辉石的电导率。氧逸度控制由Ni＋NiO、Fe＋Fe3O4、Fe＋FeO和Mo＋MoO2四种固态氧缓冲剂完成的。实验结果表明：①在所选择的频率范围内（10^-1～10^6Hz），复阻抗对频率有很强的依赖性;②随着温度（T）升高，电导率（σ）增大，logσ与1／T之间符合Arrenhius关系； 相似文献
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矿物出溶结构保存有早期母体矿物的物理化学条件信息,对其开展研究不仅有助于了解寄主岩石的来源深度,而且有助于研究减压折返的动力学演化过程.在世界许多高压-超高压带的榴辉岩和石榴辉石岩中,人们普遍发现单斜辉石中有定向排列的针状或棒状SiO2析出物,其矿物相主要为α石英,有时会伴生钙质角闪石等含水矿物.这些定向针状或棒状体通常平行于单斜辉石c[001]轴方向延伸,石英长轴可以为其c[0001]轴或a[1120]轴.电子背散射衍射(EBSD)测试结果表明,多数石英(96%)析出物与寄主单斜辉石具有结晶学取向关系:(1) 50%的石英c轴平行,并且[0001]Qz//[001]Cpx;(2)35%的石英至少有一个a轴平行,并且[1120]Qz//[001]Cpx;(3)11%的石英至少有一个s{1121}面平行,并且(1121)Qz//(100)Cpx.钙质角闪石析出物与寄主单斜辉石也具有密切结晶学取向关系:(100)Amp//(100)Cpx、[010]Amp//[010]Cpx、[001]Amp//[001]Cpx、[100]Amp∧[100]Cpx≈32°.上述定量显微构造证据表明,单斜辉石中定向石英析出物是由出溶作用所形成,并且多数石英出溶体形成于α石英稳定域.已有高温高压实验研究数据表明,单斜辉石中空位的形成和钙埃斯科拉组分(CaEs)的含量均受化学组成、压力、温度等多种因素综合影响:单斜辉石中CaEs含量对化学组成非常敏感,并受到共生矿物体系中自由SiO2相和蓝晶石的共同缓冲;相同化学组成和等压条件下,CaEs含量总体上随温度升高缓慢降低;相同化学组成和等温条件下,CaEs含量在＜6 GPa区间随压力升高而增加,在＞6 GPa区间随压力升高而降低.单斜辉石定向SiO2析出物的形成可能涉及多种因素,高压只是其中必要条件之一.榴辉岩质单斜辉石中“石英±角闪石”析出物很可能形成于开放体系,与熔流体活动密切相关,涉及多阶段物质扩散、晶体成核生长、重结晶、退变质反应等复杂作用过程.单斜辉石中定向SiO2析出物的显微结构特征并非超高压岩石的必要条件,这种特殊显微结构也不能作为证明超高压的充分条件. 相似文献
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河北汉诺坝新生代玄武岩携带的石榴辉石岩为岩浆底侵于上地幔顶部40～45 km形成的堆晶岩,是壳-幔过渡带的典型样品。本文使用Solartron 1260阻抗分析仪,测量1.2 GPa和380～900 ℃下石榴辉石岩WD958的电阻率。样品电导率(σ)与温度的关系遵守Arrhenius方程: σ=σ0exp(-ΔH/kT),其中T是样品的绝对温度,k是Boltzmann常数,指前因子σ0为97.5 S/m,活化焓ΔH为1.27 eV。使用傅立叶红外光谱仪测定样品中单斜辉石的平均含水量为117×10-6 H2O,橄榄石无水,石榴子石的含水量因蚀变无法测定。使用Hashin-Shtrikman平均方法计算样品WD958的电导率,发现样品可看作由含水单斜辉石、无水石榴子石和无水橄榄石组成的高阻集合体,电导率同时受小极化子导电和质子导电的影响。如果原位的石榴辉石岩的矿物含水量保持平衡,其电导率将提高1个数量级,质子导电成为主控导电机制。石榴辉石岩在高温的壳-幔过渡带(～1 000℃)表现为高导层,而在正常地温梯度下,与尖晶石二辉橄榄岩的电导率近似,为高阻层。因此,在岩浆底侵作用下,电性上的壳-幔边界将随着温度和含水量的变化而改变。 相似文献
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玄武岩及其高温高压相—榴辉岩的相组合,经历了长期的地质作用,反映出一定的时空条件。从高温高压实验矿物学,实验岩石学入手,对于以相组合出现的某些化学体系进行平衡条件研究,可揭示此类岩石形成的物理化学环境,并有助于阐明地球内部的物理状态、组成成分以及活动过程。 相似文献
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The enthalpies of solution of a suite of 19 high-structural state synthetic plagioclases were measured in a Pb2B2O5 melt at 970 K. The samples were crystallized from analyzed glasses at 1200°C and 20 kbar pressure in a piston-cylinder apparatus. A number of runs were also made on Amelia albite and Amelia albite synthetically disordered at 1050–1080°C and one bar for one month and at 1200°C and 20 kbar for 10 hr. The component oxides of anorthite, CaO, Al2O3 and SiO2, were remeasured.The ΔH of disorder of albite inferred in the present study from albite crystallized from glass is 3.23 kcal, which agrees with the 3.4 found by Holm and Kleppa (1968). It is not certain whether this value includes the ΔH of a reversible displacive transition to monoclinic symmetry, as suggested by Helgesonet al. (1978) for the Holm-Kleppa results. The enthalpy of solution value for albite accepted for the solid solution series is based on the heat-treated Amelia albite and is 2.86 kcal less than for untreated Amelia albite.The enthalpy of formation from the oxides at 970 K of synthetic anorthite is ?24.06 ± 0.31 kcal, significantly higher than the ?23.16 kcal found by Charluet al. (1978), and in good agreement with the value of ?23.89 ± 0.82 given by Robieet al. (1979), based on acid calorimetry.The excess enthalpy of mixing in high plagioclase can be represented by the expression, valid at 970 K: ΔHex(±0.16 kcal) = 6.7461 XabX2An + 2.0247 XAnX2Ab where XAb and XAn are, respectively, the mole fractions of NaAlSi3O8 and CaAl2Si2O8. This ΔHex, together with the mixing entropy of Kerrick and Darken's (1975) Al-avoidance model, reproduces almost perfectly the free energy of mixing found by Orville (1972) in aqueous cation-exchange experiments at 700°C. It is likely that Al-avoidance is the significant stabilizing factor in the high plagioclase series, at least for XAn≥ 0.3. At high temperatures the plagioclases have nearly the free energies of ideal one-site solid solutions. The Al-avoidance model leads to the following Gibbs energy of mixing for the high plagioclase series: . The entropy and enthalpy of mixing should be very nearly independent of temperature because of the unlikelihood of excess heat capacity in the albite-anorthite join. 相似文献
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A consequence of the biodegradation of petroleum is that lower molecular weight compounds are removed preferentially to higher molecular weight (HMW) compounds greater than triacontane (n-C30). The extent to which the latter compounds are biodegraded has rarely been studied. Reasons for this include the technical difficulties associated with carrying out biodegradability tests with solid, water-insoluble substances and the limits of the analytical techniques, such as gas chromatography (GC).A quantitative high temperature GC (HTGC) method was developed to monitor the biodegradation of the aliphatic fraction of a waxy Indonesian oil by Pseudomonas fluorescens. Recoveries of over 90% were obtained for n-alkanes up to hexacontane (C60) using liquid-liquid continuous extraction. After only 14 days, 80% of the aliphatic hydrocarbons had been degraded. At the end of the 136-day study, 14% of the original fraction remained. This comprised mainly C40+ compounds. No decrease in the concentrations of compounds above C45 was observed. However, the use of a rapid screening biodegradation method provided tentative proof that Pseudomonas fluorescens was capable of utilising n-alkanes up to C60 once the bacteria had acclimated to HMW alkanes. 相似文献
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在俯冲带中,菱镁矿相比于其他碳酸盐矿物会在更高的温度压力环境下稳定存在,常被认为是地球深部碳循环的主要载体,其电学性质的研究对俯冲带及地球深部的电性结构具有重要的意义。本文在YJ-3000t高温高压设备上利用Solartron-1260阻抗/增益-相位分析仪,在1～3 GPa和773～1173 K条件下,对天然菱镁矿的电导率进行了原位测量。实验结果表明,在实验条件下,天然菱镁矿的电导率在10-2～10-7 S/m范围内,菱镁矿的电导率对温度有很强的依赖性,随着温度的升高,电导率增大,电导率与压力的关系呈正相关,随着压力的升高而增强。结合前人的研究成果及样品电导率随温度、压力的效应和活化能,可推断天然菱镁矿导电机制为大极化子导电。 相似文献
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A. Pavese 《Physics and Chemistry of Minerals》1999,26(8):649-657
Numerical simulations, using empirical interatomic potentials within the framework of lattice dynamics and quasi-harmonic
approximation, have been carried out to model the behaviour of the structure and of some thermoelastic properties of pyrope
at high pressure and high temperature conditions (0–50 GPa, 300–1500 K). Comparison with observed data, available as a function
either of P or of T, suggests that the pressure effects are satisfactorily modelled, whilst the effect of T on the simulations is underestimated. The cell edge, bond lengths and polyhedral volumes have been studied as a function
of P along five isotherms, spaced by 300 K steps. These isotherms tend to converge at high pressure, which demonstrates that the
pressure effects become dominant compared to those of thermal origin in affecting the structural properties far from ambient
conditions. The cell parameter, bond distances, and other structural and thermoelastic quantities determined through simulations
have been parametrised as a function of P and T by polynomial expansions. Bulk modulus and thermal expansion have been discussed in the light of the high-temperature-Birch-Murnaghan
and of the Vinet P – V – T equations of state. The predictions of the bulk modulus versus P and T from the present calculations and from the Vinet-EOS agree up to 10 GPa, but they differ at higher pressure.
Received: 23 October, 1998 / Revised, accepted: 23 April, 1999 相似文献
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A. Suzuki E. Ohtani K. Funakoshi H. Terasaki T. Kubo 《Physics and Chemistry of Minerals》2002,29(3):159-165
The viscosity of albite (NaAlSi3O8) melt was measured at high pressure by the in situ falling-sphere method using a high-resolution X-ray CCD camera and a large-volume
multianvil apparatus installed at SPring-8. This system enabled us to conduct in situ viscosity measurements more accurately
than that using the conventional technique at pressures of up to several gigapascals and viscosity in the order of 100 Pa s. The viscosity of albite melt is 5.8 Pa s at 2.6 GPa and 2.2 Pa s at 5.3 GPa and 1973 K. Experiments at 1873 and 1973
K show that the decrease in viscosity continues to 5.3 GPa. The activation energy for viscosity is estimated to be 316(8)
kJ mol−1 at 3.3 GPa. Molecular dynamics simulations suggest that a gradual decrease in viscosity of albite melt at high pressure may
be explained by structural changes such as an increase in the coordination number of aluminum in the melt.
Received: 6 January 2001 / Accepted: 27 August 2001 相似文献
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通过高温高压实验研究了铁橄榄石集合体的流变性.首先,利用高精度的Paterson气体介质变形装置对铁橄榄石集合体Fe2SiO4进行了高温三轴压缩蠕变试验.变形试验条件为:温度1273～1423K,围压300MPa,差应力10～250MPa,应变率10-7～10-4s-1,试件的最大变形量不超过20%.利用三维非线性拟合方法对蠕变试验数据进行分析,得到铁橄榄石集合体的微观变形机制为扩散域和位错域,扩散域的应力指数为1左右.位错蠕变域中,干燥铁橄榄石集合体的应力指数为5.4.活化能为781kJ/mol;含水铁橄榄石集合体的应力指数为3.4,活化能为516kJ/mol.实验结果表明,含水时铁橄榄石的流变强度比干燥时小一个数量级.将实验结果与铁橄榄石单晶的强度进行对比,发现铁橄榄石集合体的流变强度比铁橄榄石单晶的强度高.从而得到了铁橄榄石集合体高温高压流变性(强度)的初步试验结果. 相似文献
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青藏高原北部白榴碧玄岩年代学及地球化学研究 总被引：1，自引：0，他引：1
本文在可可西里北部边缘银顶山地区首次发现含橄榄石的高镁高钾质超基性火山岩。火山岩在阿尼玛卿-昆仑-木孜塔格缝合带南侧呈熔岩残丘形式产出,分布面积约为0.2 km2,其形成时代为上新世(5～4 Ma),是岩浆的快速侵位-喷溢的结果。斑晶主要为橄榄石(10%～12%)+白榴石(21%～27%)+霞石(13%～16%)±透辉石(29%～31%),基质主要为透辉石+云母+Fe-Ti氧化物+玻璃,定名为白榴碧玄岩。对3个样品51个点的橄榄石电子探针数据计算显示,橄榄石牌号为Fo74-87Fa13-26,属贵橄榄石,岩石中的橄榄石均不存在扭折带,表明这些橄榄石很可能是岩浆结晶的产物,而非岩浆捕获体。通过计算,银顶山地区橄榄石的结晶温度大约在1 226 ℃～1 234 ℃左右。白榴碧玄岩的化学组分:SiO2<45%,MgO>10%, Na2O+K2O>8%,Mg#(68.84～70.80),而Cr(149×10-6～156×10-6)和Ni(138×10-6～151×10-6),87Sr/86Sr(约0.708 6)和143Nd/144 Nd(约0.512 4),处于EMII源区范围内。初步认为藏北地区上新世超基性火山岩来自于较深的源区,最有可能是软流圈顶部地幔的局部熔融,并受到俯冲地壳物质的交代。 相似文献