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Thermo-mechanical and Thermophysical Properties of Ferro-siliceous Sacrificial Concrete on Exposure to Elevated Temperatures 硅铁人造混凝土在高温下的热机械性能和热物理性能
IF 2.5 4区 工程技术 Q3 CHEMISTRY, PHYSICAL Pub Date : 2024-06-20 DOI: 10.1007/s10765-024-03391-7
P. V. P. Moorthi, Anuj Kumar, Shyamprasad Karagadde, P. K. Baburajan, Anuj Kumar Deo, Arunkumar Sridharan, Prakash Nanthagopalan, S. V. Prabhu

Heavy density concrete made of hematite-based aggregates commonly known as ferro-siliceous sacrificial concrete (FSSC) can be used effectively against radiation shielding in case of nuclear melt down. However, performance assessment of such concretes on exposure to elevated temperatures are not available widely. In the present study, thermo-mechanical and thermophysical properties of hematite-based FSSC concrete are evaluated on exposure to elevated temperatures. The porosity and water absorption capacity of FSSC are investigated on its exposure to higher temperatures ranging from 30 °C to 1000 °C. Similarly, various thermo-mechanical [compression, split tension, modulus of elasticity (MOE)] and thermophysical (specific heat, thermal conductivity, thermal diffusivity, and thermal effusivity) properties are evaluated on exposure to elevated temperatures. The mechanical properties of the concrete such as compression, split tension, MOE decrease monotonically with increase in the exposed temperature. Porosity and water absorption of the concrete increases with the increase in temperature. Relationship between damage and the exposed temperature can be described by Weibull model. Thermophysical property such as specific heat of the concrete increases, while thermal conductivity, thermal diffusivity and effusivity decrease with the increase in temperature. Correlations for the variation in thermal conductivity, specific heat and thermal diffusivity are proposed. The variations in the mechanical and thermophysical properties are explained through the porosity variations and correlation coefficient between porosity and various mechanical and thermophysical properties.

由赤铁矿骨料制成的高密度混凝土通常被称为铁硅质牺牲混凝土(FSSC),可在核熔化情况下有效屏蔽辐射。然而,对这类混凝土暴露于高温下的性能评估并不多见。本研究评估了赤铁矿基 FSSC 混凝土在暴露于高温时的热机械性能和热物理性能。研究了 FSSC 在 30 °C 至 1000 °C 高温下的孔隙率和吸水能力。同样,还评估了暴露在高温下的各种热机械性能(压缩、劈裂拉伸、弹性模量 (MOE))和热物理性能(比热、热导率、热扩散率和热辐射率)。随着暴露温度的升高,混凝土的压缩、劈裂拉伸和 MOE 等力学性能单调下降。混凝土的孔隙率和吸水率随温度升高而增加。损坏与暴露温度之间的关系可以用 Weibull 模型来描述。混凝土的热物理性质(如比热)随温度升高而增加,而热导率、热扩散率和膨胀率则随温度升高而降低。提出了导热系数、比热和热扩散率变化的相关性。通过孔隙率的变化以及孔隙率与各种力学和热物理性能之间的相关系数,解释了力学和热物理性能的变化。
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引用次数: 0
Exploring Density, Viscosity, and Friction Theory in the Interaction of Linalool (3,7-Dimethylocta-1,6-dien-3-ol) with 2-Alkanol 探索芳樟醇(3,7-二甲基辛-1,6-二烯-3-醇)与 2-烷醇相互作用的密度、粘度和摩擦理论
IF 2.5 4区 工程技术 Q3 CHEMISTRY, PHYSICAL Pub Date : 2024-06-17 DOI: 10.1007/s10765-024-03392-6
Zeinab Rafiee, Mohammad Almasi

This investigation undertakes a thorough examination of the thermophysical properties of linalool (C10H18O) blended with a series of 2-alkanols (ranging from 2-propanol to 2-hexanol) across a temperature spectrum of 293.15 K to 323.15 K. The primary objective of this study is to elucidate the density and viscosity behavior of these binary systems. The experimental results reveal negative deviations from ideality in excess molar volume for linalool with 2-propanol up to 2-pentanol, and positive values for linalool with 2-hexanol, accompanied by negative viscosity deviations across all examined mixtures. The observed negative excess volume suggests the presence of strong intermolecular interactions between linalool and the 2-alkanols, which is indicative of the formation of hydrogen bonds in the mixtures. The positive values of excess molar volumes in linalool and 2-hexanol are indicative of the governing of steric hindrance effects on attractive intermolecular forces. Moreover, the Friction theory (f-theory) was utilized to model the viscosity of the binary mixtures, yielding an excellent concordance with the experimental data, with a maximum discrepancy of merely 2.25 % observed in the linalool + 2-pentanol system. This negligible deviation underscores the efficacy of the f-theory in accurately capturing the viscosity measurements, thereby validating its applicability in predicting the rheological behavior of such binary systems.

本研究对芳樟醇(C10H18O)与一系列 2-烷醇(从 2-丙醇到 2-己醇)混合后在 293.15 K 到 323.15 K 的温度范围内的热物理性质进行了深入研究。实验结果表明,芳樟醇与 2-丙醇直至 2-戊醇的过量摩尔体积与理想状态存在负偏差,芳樟醇与 2-己醇的过量摩尔体积与理想状态存在正偏差,同时所有研究混合物的粘度偏差均为负值。观察到的负过量体积表明芳樟醇和 2-烷醇之间存在强烈的分子间相互作用,这表明混合物中形成了氢键。芳樟醇和 2-己醇的过量摩尔体积为正值,表明立体阻碍效应对分子间吸引力的影响。此外,摩擦理论(f 理论)被用来模拟二元混合物的粘度,结果与实验数据非常吻合,在芳樟醇 + 2-戊醇体系中观察到的最大偏差仅为 2.25%。这一可忽略不计的偏差强调了 f 理论在准确捕捉粘度测量值方面的功效,从而验证了其在预测此类二元体系流变行为方面的适用性。
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引用次数: 0
Bubble Point Measurements of cis-1,1,1,4,4,4-Hexafluorobutene [R-1336mzz(Z)] + trans-1,2-Dichloroethene [R-1130(E)] mixtures 顺式-1,1,1,4,4,4-六氟丁烯 [R-1336mzz(Z)] + 反式-1,2-二氯乙烯 [R-1130(E)] 混合物的气泡点测量值
IF 2.5 4区 工程技术 Q3 CHEMISTRY, PHYSICAL Pub Date : 2024-06-12 DOI: 10.1007/s10765-024-03388-2
Aaron J. Rowane, Stephanie L. Outcalt

Saturation pressures of pure R-1336mzz(Z) and R-1130(E) and bubble point pressures of three R-1336mzz(Z)/1130(E) blends were measured from 265 K to 360 K. For each pure refrigerant or refrigerant blend, a total of twenty unique saturation pressures or bubble points were measured. In total 100 unique state points were obtained. Presently, no Helmholtz-energy-explicit type equation of state (EoS) is available for R-1130(E). While an extended corresponding states EoS for R-1130(E) is available to estimate the properties of the R-1336mzz(Z)/1130(E) blend, this model does not resolve the azeotropic behavior of the mixture. Therefore, the perturbed-chain statistical-associating fluid theory (PC-SAFT) EoS is used to model the vapor–liquid equilibria of the R-1336mzz(Z)/1130(E) blend. PC-SAFT model parameters are reported, and the overall performance of the model is characterized by deviations from the experimental data.

在 265 K 至 360 K 的温度范围内测量了纯 R-1336mzz(Z) 和 R-1130(E)的饱和压力以及三种 R-1336mzz(Z)/1130(E) 混合物的气泡点压力。总共获得了 100 个独特的状态点。目前,还没有针对 R-1130(E)的亥姆霍兹能量显式状态方程 (EoS)。虽然 R-1130(E)的扩展相应状态 EoS 可用于估算 R-1336mzz(Z)/1130(E) 混合物的特性,但该模型无法解决混合物的共沸行为。因此,我们使用扰动链统计关联流体理论 (PC-SAFT) EoS 来模拟 R-1336mzz(Z)/1130(E) 混合物的汽液平衡。报告了 PC-SAFT 模型参数,并通过与实验数据的偏差对模型的整体性能进行了描述。
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引用次数: 0
Densities and Molar Volumes for Binary Solutions of Tri-iso-Amyl Phosphate and n-Dodecane in the Temperature Range of 283.15–363.15 K 磷酸三异戊酯和正十二烷的二元溶液在 283.15-363.15 K 温度范围内的密度和摩尔体积
IF 2.5 4区 工程技术 Q3 CHEMISTRY, PHYSICAL Pub Date : 2024-06-12 DOI: 10.1007/s10765-024-03384-6
Shekhar Kumar

Tri-n-butyl phosphate (TBP) has remained workhorse of PUREX based nuclear recycle operations since 1956. However due to its associated disadvantages like third phase formation and tendency to react violently with nitric acid at elevated temperatures generated requirement of an alternate extractant for PUREX process. Tri-iso-amyl phosphate (TiAP) has better attributes than TBP on both the counts. Density of solutions is an important process parameter for design of equipment, process operations and control and safety analysis. In this work, experimental data on the density of binary solution of tri-iso amyl phosphate and n-dodecane are reported for several temperature levels. The related volumetric parameters were also estimated from experimental data as well as Kirkwood–Buff integrals. Derivative parameters like linear coefficients of preferential solvation (delta_{ij(i ne j)}^{o}) and local mole fractions (x_{ij(i ne j)}) at 298.15 K were also estimated and reported.

Graphical Abstract

自 1956 年以来,磷酸三丁酯(TBP)一直是基于 PUREX 的核循环操作的主力。然而,由于其相关的缺点,如第三相的形成以及在高温下与硝酸发生剧烈反应的倾向,PUREX 工艺需要一种替代萃取剂。磷酸三异戊酯(TiAP)在这两方面都比 TBP 具有更好的特性。溶液密度是设备设计、工艺操作、控制和安全分析的重要工艺参数。本研究报告了磷酸三异戊酯和正十二烷二元溶液在不同温度下的密度实验数据。还根据实验数据和 Kirkwood-Buff 积分估算了相关的体积参数。还估算并报告了 298.15 K 时的线性优先溶解系数(delta_{ij(ine j)}^{o})和局部摩尔分数((x_{ij(ine j)})等衍生参数。
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引用次数: 0
Rayleigh–Benard Convection of Carbopol Yield Stress Fe3O4 Nanofluids Under Magnetic Field: An Experimental Investigation and ANN Modelling 磁场下卡波聚屈服应力 Fe3O4 纳米流体的瑞利-贝纳尔对流:实验研究与 ANN 建模
IF 2.5 4区 工程技术 Q3 CHEMISTRY, PHYSICAL Pub Date : 2024-06-12 DOI: 10.1007/s10765-024-03390-8
M. A. Hassan, Rishikesh Kumar, N. H. Khan

This study presents a comprehensive experimental investigation aimed at elucidating the influence of magnetic fields, nanoparticle concentration, and the presence of polymer on Rayleigh–Benard convection in yield stress nanofluids. The test fluid comprises Ultrez 30 polymeric powder and Iron oxide nanoparticles. Herschel–Bulkley's model is applied to capture the rheological behaviour. The concentration of both Ultrez 30 polymeric gel and Iron oxide nanoparticles varies from 0.05 % to 0.10 %. The in-house developed experimental set-up is exposed to the magnetic field in the 0 mT to 100 mT range. Without a magnetic field, heat transfer increases with the elevation of nanoparticle fraction in the fluid. However, in the presence of a magnetic field, the convection effect weakens as the nanoparticle concentration rises. Furthermore, an optimised artificial neural network (ANN) model featuring a single hidden layer with nine hidden neurons is presented to predict the Nusselt number.

本研究介绍了一项全面的实验研究,旨在阐明磁场、纳米粒子浓度和聚合物的存在对屈服应力纳米流体中瑞利-贝纳德对流的影响。测试流体由 Ultrez 30 聚合物粉末和氧化铁纳米颗粒组成。Herschel-Bulkley 模型用于捕捉流变行为。Ultrez 30 聚合凝胶和氧化铁纳米颗粒的浓度从 0.05 % 到 0.10 % 不等。内部开发的实验装置暴露在 0 mT 至 100 mT 范围内的磁场中。在没有磁场的情况下,传热会随着流体中纳米粒子比例的增加而增加。然而,在有磁场的情况下,对流效应会随着纳米粒子浓度的增加而减弱。此外,还提出了一个优化的人工神经网络(ANN)模型,该模型具有一个单隐层和九个隐神经元,用于预测努塞尔特数。
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引用次数: 0
Two-Phase Isochoric Heat Capacity, Phase Transition, and Theoretically Important Physical Parameters of Methyl Dodecanoate 十二酸甲酯的两相等热容、相变和重要理论物理参数
IF 2.5 4区 工程技术 Q3 CHEMISTRY, PHYSICAL Pub Date : 2024-06-10 DOI: 10.1007/s10765-024-03386-4
R. G. Batyrova, N. V. Ibavov, S. M. Rasulov, I. M. Abdulagatov
<div><p>The two-phase isochoric heat capacity (<span>(C_{{text{V2}}})</span> <i>VT</i>), liquid–gas phase transition (<span>(T_{text{S}})</span>,<span>(rho_{{text{s}}}^{prime })</span>), vapor-pressure (<span>(P_{{text{S}}})</span>,<span>(T_{text{S}})</span>), and thermal -pressure coefficient <span>(left( {dP_{text{S}} /dT} right))</span> of methyl dodecanoate, a key biofuels component, have been measured along nine liquid isochores between (180.90 and 845.31) kg·m<sup>−3</sup> and three near-critical liquid and vapor (180.90, 234.52, and 374.11) kg·m<sup>−3</sup> isochores. The temperature range covers the liquid–vapor phase transition temperature <span>(T_{text{S}} left( rho right))</span> for each measured isochore to near the thermal decomposition temperature, 450 K. The measurements were performed using a high-temperature and high-pressure, nearly constant-volume adiabatic calorimeter previously used for the measurements of the <span>(C_{text{V}})</span> <i>VT</i> relationship of biofuel components in the two- and single-phase region. The combined expanded uncertainty of the density (<i>ρ</i>), temperature (<i>T</i>), and isochoric heat capacity (<span>(C_{{text{V2}}})</span>) measurements at the 95% confidence level with a coverage factor of <i>k</i> = 2 is estimated to be 0.15%, 15 mK, and 2%, respectively. The isochoric heat capacity discontinuity point was used as the criteria of the liquid–gas phase transition temperature, <span>(T_{{text{S}}})</span>. For each experimental liquid isochore, most measurements were concentrated in the immediate vicinity of the liquid–gas phase transition temperature (<span>(T_{{text{S}}})</span>) to precisely determine the phase boundary properties (<span>(rho_{{text{S}}})</span>, <span>(T_{{text{S}}})</span>, <span>(C_{text{V1}})</span>, and <span>(C_{text{V2}})</span>) using an isochoric heat -capacity abrupt-behavior technique. For nine liquid isochores between (745.16 and 845.31) kg·m<sup>−3</sup> the phase transition temperatures (<span>(T_{{text{S}}})</span>) were experimentally determined. For two vapor (180.90 and 234.52) kg·m<sup>−3</sup> and liquid near-critical (374.11) kg·m<sup>−3</sup> isochores, for which the transition temperatures are very high (above the thermal decomposition temperature, 473 K), we failed to reach the phase-transition temperatures, <span>(T_{{text{S}}})</span>, because for these isochores the thermal decomposition of methyl dodecanoate occurs before reaching the phase transition temperature (above 673 K). The measured two-phase (<span>(C_{text{V2}})</span>) isochoric heat capacities as a function of specific volume (<i>V</i>) along the various isotherms (below 473 K) were used to accurately estimate the values of the second temperature derivatives of chemical potential, <span>(frac{{{text{d}}^{{2}} mu }}{{{text{d}}T^{2} }})</span>, and vapour-pressure,<span>(frac{{{text{d}}^{2} P_{{text{S}}} }}{{{text{d}}T^{2} }})</span>, based on the Yang–Yang theoretical relation. The
两相等时热容(C_{text{V2}}} VT)、液-气相变(T_{text{S}})、蒸汽压(P_{text{S}}})和热-压系数(left( {dP_{text{S}} /dT} right))、和热压系数 (left( {dP_{text{S}} /dT} right))。90 和 845.31)kg-m-3 之间的九个液态等距线以及三个近临界液态和汽态(180.90、234.52 和 374.11)kg-m-3 等距线进行了测量。温度范围涵盖了液-气相转变温度 (T_{text{S}}测量使用的是一个高温高压、近乎恒容的绝热量热仪,以前曾用于测量生物燃料成分在两相和单相区域中的(C_{text{V}}) VT 关系。密度 (ρ)、温度 (T) 和等时热容 ((C_{text{V2}})) 测量值在 95% 置信度下的综合扩展不确定性(覆盖因子为 k = 2)估计分别为 0.15%、15 mK 和 2%。等时热容不连续点被用作液气相变温度的标准,即 (T_{{/text{S}}})。对于每种实验液体等时,大多数测量都集中在液气相变温度((T_{{text{S}}})附近,以精确确定相界特性((rrh_{text{S}}})、(T_{{text{S}}})、(C_{text{V1}})和(C_{text{V2}}))。实验测定了介于(745.16 和 845.31)kg-m-3 之间的九种液体等时相变温度((T_{{text{S}}))。对于两个汽态(180.90 和 234.52)kg-m-3 和液态近临界(374.11)kg-m-3 等位体,其转变温度非常高(高于热分解温度 473 K),我们未能达到相变温度,(T_{{text{S}}) ,因为对于这些等位体,十二酸甲酯在达到相变温度(高于 673 K)之前就发生了热分解。)沿着各种等温线(低于 473 K)测得的两相((C_{text{V2}}))等时热容是比容(V)的函数,用于精确估计化学势的第二温度导数值、(frac{{text{d}}^{2}}mu }}{{text{d}}T^{2}}}),以及蒸气压,(frac{{text{d}}^{2}P_{text{S}}}}{{text{d}}T^{2}}})。蒸汽压力的贡献(C_{{text{VP}}}} = VTfrac{{{text{d}}^{2}P_{{text{S}}}}}{{{text{d}}T^{2}),以及化学势,C_{{text{V}}mu }} = - Tfrac{{{text{d}}^{{text{2}}}}{{{text{d}}T^{2}}})的热容量与温度的函数关系进行了估算。此外,测量到的(C_{text{V2}})和相界((rrh_{text{S}}),(T_{text{S}}),(P_{text{S}}))属性数据被用来计算关键的热力学属性数据(C_{text{P}})、(C_{text{sat}}),(K_{text{TS}}),(W_{text{S}}),(Delta H_{{text{V}}}),(left( {frac{partial P}{{partial T}}} right)_{{text{V}}}^{{{text{sat}}{.),(left( {frac{partial V}}{{partial T}}} right)_{{text{P}}}^{{{text{sat}}.}}) 沿着饱和曲线。测得的蒸汽压力((P_{text{S}}}) - (T_{text{S}}}))和饱和液体密度((rho_{text{S}}}) - (T_{text{S}}))被用来建立扩展的基于理论的缩放相关性,并估算临界特性数据((T_{text{C}}})、(P_{{text{C}}})和 (rrh_{{text{C}}}))、渐近临界振幅和非对称参数。
{"title":"Two-Phase Isochoric Heat Capacity, Phase Transition, and Theoretically Important Physical Parameters of Methyl Dodecanoate","authors":"R. G. Batyrova,&nbsp;N. V. Ibavov,&nbsp;S. M. Rasulov,&nbsp;I. M. Abdulagatov","doi":"10.1007/s10765-024-03386-4","DOIUrl":"10.1007/s10765-024-03386-4","url":null,"abstract":"&lt;div&gt;&lt;p&gt;The two-phase isochoric heat capacity (&lt;span&gt;(C_{{text{V2}}})&lt;/span&gt; &lt;i&gt;VT&lt;/i&gt;), liquid–gas phase transition (&lt;span&gt;(T_{text{S}})&lt;/span&gt;,&lt;span&gt;(rho_{{text{s}}}^{prime })&lt;/span&gt;), vapor-pressure (&lt;span&gt;(P_{{text{S}}})&lt;/span&gt;,&lt;span&gt;(T_{text{S}})&lt;/span&gt;), and thermal -pressure coefficient &lt;span&gt;(left( {dP_{text{S}} /dT} right))&lt;/span&gt; of methyl dodecanoate, a key biofuels component, have been measured along nine liquid isochores between (180.90 and 845.31) kg·m&lt;sup&gt;−3&lt;/sup&gt; and three near-critical liquid and vapor (180.90, 234.52, and 374.11) kg·m&lt;sup&gt;−3&lt;/sup&gt; isochores. The temperature range covers the liquid–vapor phase transition temperature &lt;span&gt;(T_{text{S}} left( rho right))&lt;/span&gt; for each measured isochore to near the thermal decomposition temperature, 450 K. The measurements were performed using a high-temperature and high-pressure, nearly constant-volume adiabatic calorimeter previously used for the measurements of the &lt;span&gt;(C_{text{V}})&lt;/span&gt; &lt;i&gt;VT&lt;/i&gt; relationship of biofuel components in the two- and single-phase region. The combined expanded uncertainty of the density (&lt;i&gt;ρ&lt;/i&gt;), temperature (&lt;i&gt;T&lt;/i&gt;), and isochoric heat capacity (&lt;span&gt;(C_{{text{V2}}})&lt;/span&gt;) measurements at the 95% confidence level with a coverage factor of &lt;i&gt;k&lt;/i&gt; = 2 is estimated to be 0.15%, 15 mK, and 2%, respectively. The isochoric heat capacity discontinuity point was used as the criteria of the liquid–gas phase transition temperature, &lt;span&gt;(T_{{text{S}}})&lt;/span&gt;. For each experimental liquid isochore, most measurements were concentrated in the immediate vicinity of the liquid–gas phase transition temperature (&lt;span&gt;(T_{{text{S}}})&lt;/span&gt;) to precisely determine the phase boundary properties (&lt;span&gt;(rho_{{text{S}}})&lt;/span&gt;, &lt;span&gt;(T_{{text{S}}})&lt;/span&gt;, &lt;span&gt;(C_{text{V1}})&lt;/span&gt;, and &lt;span&gt;(C_{text{V2}})&lt;/span&gt;) using an isochoric heat -capacity abrupt-behavior technique. For nine liquid isochores between (745.16 and 845.31) kg·m&lt;sup&gt;−3&lt;/sup&gt; the phase transition temperatures (&lt;span&gt;(T_{{text{S}}})&lt;/span&gt;) were experimentally determined. For two vapor (180.90 and 234.52) kg·m&lt;sup&gt;−3&lt;/sup&gt; and liquid near-critical (374.11) kg·m&lt;sup&gt;−3&lt;/sup&gt; isochores, for which the transition temperatures are very high (above the thermal decomposition temperature, 473 K), we failed to reach the phase-transition temperatures, &lt;span&gt;(T_{{text{S}}})&lt;/span&gt;, because for these isochores the thermal decomposition of methyl dodecanoate occurs before reaching the phase transition temperature (above 673 K). The measured two-phase (&lt;span&gt;(C_{text{V2}})&lt;/span&gt;) isochoric heat capacities as a function of specific volume (&lt;i&gt;V&lt;/i&gt;) along the various isotherms (below 473 K) were used to accurately estimate the values of the second temperature derivatives of chemical potential, &lt;span&gt;(frac{{{text{d}}^{{2}} mu }}{{{text{d}}T^{2} }})&lt;/span&gt;, and vapour-pressure,&lt;span&gt;(frac{{{text{d}}^{2} P_{{text{S}}} }}{{{text{d}}T^{2} }})&lt;/span&gt;, based on the Yang–Yang theoretical relation. The","PeriodicalId":598,"journal":{"name":"International Journal of Thermophysics","volume":"45 7","pages":""},"PeriodicalIF":2.5,"publicationDate":"2024-06-10","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"141361649","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
引用次数: 0
Thermal Conductivity of Liquid Cyclohexane, n-Decane, n-Hexadecane, and Squalane at Atmospheric Pressure up to 353 K Determined with a Steady-State Parallel-Plate Instrument 用一台稳态平行板仪器测定液态环己烷、正癸烷、正十六烷和角鲨烷在大气压力下至 353 K 的导热率
IF 2.5 4区 工程技术 Q3 CHEMISTRY, PHYSICAL Pub Date : 2024-06-05 DOI: 10.1007/s10765-024-03383-7
Francisco E. Berger Bioucas, Michael H. Rausch, Thomas M. Koller, Andreas P. Fröba

The present work reports experimental data on the thermal conductivity of the four hydrocarbons cyclohexane, n-decane, n-hexadecane, and squalane in the liquid state at ambient pressure up to temperatures of 353.15 K. Absolute measurements were performed with a steady-state guarded parallel-plate instrument (GPPI) with an average expanded (coverage factor k = 2) measurement uncertainty of 2 %. For the linear alkanes n-decane and n-hexadecane as well as the cyclic compound cyclohexane, the measured thermal conductivities agree with reference correlations in the literature, indicating the reliability of the technique used for the study of fluids with relatively low thermal conductivities and weak absorption of radiation. For the first time, experimental data are determined for the long-branched alkane squalane between (278 and 353) K, which cannot be accurately represented with estimation methods commonly used in the literature. In summary, the present measurement results confirm the existing database for representative linear and cyclic hydrocarbons and provide first experimental thermal conductivities for squalane.

本研究报告了四种碳氢化合物环己烷、正癸烷、正十六烷和角鲨烷在环境压力下至 353.15 K 温度的液态热导率的实验数据。绝对测量采用稳态保护平行板仪器 (GPPI),平均扩展(覆盖因子 k = 2)测量不确定性为 2%。对于线性烷烃正癸烷和正十六烷以及环状化合物环己烷,测得的热导率与文献中的参考相关性一致,这表明该技术在研究热导率相对较低且对辐射的吸收较弱的流体时非常可靠。首次测定了长支链烷烃角鲨烷在 (278 和 353) K 之间的实验数据,而文献中常用的估算方法无法准确表示这种烷烃。总之,本测量结果证实了现有的代表性线性和环状碳氢化合物数据库,并首次提供了角鲨烷的实验热导率。
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引用次数: 0
Ethylcyclohexane + 2-Alkanol Mixtures: Thermodynamic Properties and Viscosity Modeling Using Friction Theory 乙基环己烷 + 2-烷醇混合物:热力学性质和利用摩擦理论建立粘度模型
IF 2.5 4区 工程技术 Q3 CHEMISTRY, PHYSICAL Pub Date : 2024-05-29 DOI: 10.1007/s10765-024-03379-3
Mohammad Almasi

A thorough evaluation of the thermophysical properties of ethylcyclohexane (ECH) mixed with 2-alkanols (2-propanol to 2-hexanol) is presented across the temperature range of 293.15 to 323.15 K. The focus of this study is on the density and viscosity behavior of these systems. The experimental results demonstrate positive deviations from ideality in excess molar volume, while viscosity deviations are negative for all examined mixtures. This observation suggests the presence of weak intermolecular interactions between ECH and the 2-alkanol. These findings are consistent with the self-association behavior of 2-alkanol and the nonpolar nature of ECH, which disrupts the associated structures of the alcohols. Furthermore, the Friction theory (f-theory) was employed to model the viscosity of the binary mixtures. The f-theory exhibits excellent agreement with the experimental data, with a maximum deviation of only 2.24% observed in the ECH + 2-butanol system. This minimal discrepancy underscores the f-theory's efficacy in accurately correlating the viscosity measurements.

本研究对乙基环己烷(ECH)与 2-烷醇(从 2-丙醇到 2-己醇)混合后在 293.15 至 323.15 K 温度范围内的热物理性质进行了全面评估。实验结果表明,过量摩尔体积与理想状态存在正偏差,而所有研究混合物的粘度偏差均为负值。这一观察结果表明,ECH 和 2-烷醇之间存在微弱的分子间相互作用。这些发现与 2-烷醇的自结合行为和 ECH 的非极性一致,后者会破坏醇的相关结构。此外,摩擦理论(f 理论)被用来模拟二元混合物的粘度。f 理论与实验数据非常吻合,在 ECH + 2-丁醇体系中观察到的最大偏差仅为 2.24%。这种极小的偏差凸显了 f 理论在准确关联粘度测量值方面的功效。
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引用次数: 0
Optical (n(p, T_{90})) Measurement Suite 2: H(_2)O and D(_2)O 光学 $$n(p, T_{90})$$ 测量套件 2:H $$_2$$ O 和 D $$_2$$ O
IF 2.5 4区 工程技术 Q3 CHEMISTRY, PHYSICAL Pub Date : 2024-05-28 DOI: 10.1007/s10765-024-03380-w
Patrick F. Egan, Yuanchao Yang

A suite of measurements of refractive index (n(p, T_{90})) is reported for gas phase ordinary water H(_2)O and heavy water D(_2)O. The methodology is optical refractive index gas metrology, operating at laser wavelength (633 text {nm}) and covering the range ((293< T_{90} < 433) text {K}) and (p < 2 text {kPa}). A key output of the work is the determination of molar polarizabilities (A_{text {R}} = 3.7466(18) cdot [1 + 1.5(6) times 10^{-6} (T/text {K} - 303) ] text{cm}^3 cdot text{mol}^{-1}) for ordinary water, and (A_{text {R}} = 3.7135(18) cdot [1 + 4.4(10) times 10^{-6} (T/text {K} - 303) ] text{cm}^3 cdot text{mol}^{-1}) for heavy water, with the numbers in parentheses expressing standard uncertainty. For heavy water, this work appears to be only the second gas phase measurement to date. For both ordinary and heavy water, this work agrees within (0.15 %) with recent ab initio theoretical results for (A_{text {R}}), but the comparison is affected by imperfect knowledge of dispersion. For ordinary water, the close agreement between the present work and theory suggests problems at the (2 %) level in the low density limit of the reference formulation for refractivity.

报告了气相普通水 H(_2)O 和重水 D(_2)O 折射率 (n(p, T_{90})) 的一套测量方法。该方法是光学折射率气体计量学,在激光波长(633)和覆盖范围((293< T_{90} < 433)和(p < 2)上运行。这项工作的一个重要成果是确定了普通水的摩尔极化率(A_{text {R}} = 3.7466(18) cdot [1 + 1.5(6) times 10^{-6} (T/text {K} - 303) ] text{cm}^3 cdot text{mol}^{-1} ),以及(A_{text {R}} = 3.7466(18) cdot [1 + 1.5(6) times 10^{-6} (T/text {K} - 303) ]text{cm}^3 cdot text{mol}^{-1} )。7135(18) cdot [1 + 4.4(10) times 10^{-6} (T/text {K} - 303) ] text{cm}^3 cdot text{mol}^{-1}}),括号中的数字表示标准不确定性。对于重水,这项工作似乎只是迄今为止的第二次气相测量。对于普通水和重水,这项工作与最近关于 (A_{text {R}}) 的ab initio 理论结果的吻合度都在 (0.15%) 以内,但由于对弥散的认识不完善,比较结果受到了影响。对于普通水来说,目前的工作与理论之间的密切一致表明,在折射率参考公式的低密度极限水平上存在问题。
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引用次数: 0
Liquid Density Measurement in High-Pressure Region Using Quartz Crystal Resonators 利用石英晶体谐振器测量高压区的液体密度
IF 2.5 4区 工程技术 Q3 CHEMISTRY, PHYSICAL Pub Date : 2024-05-28 DOI: 10.1007/s10765-024-03387-3
Hiroshi Yamawaki

Numerous attempts have been made to measure the viscosity of liquids under high pressure by analyzing the response of a quartz crystal resonator. However, because the response of the resonator yields the product of density and viscosity, separating each value is necessary. A procedure was devised to measure the density changes of a liquid under high pressure by considering the fact that the response of a TiO2-coated quartz crystal resonator is correlated with density. The resonance frequency shift of the TiO2-coated quartz crystal resonator is the sum of terms that depend on (rho ) and (sqrt{eta rho }). Each effect can be separated using plane equation fitting. By applying ethyl laurate, densities up to 300 MPa were obtained at 313 K and 333 K. These values agreed with previously reported values within ± 1 %, thereby demonstrating the effectiveness of this method. Since the pressure dependence of (sqrt{eta rho }) is also obtained in the process of obtaining density data, the pressure dependence of the viscosity (eta ) can be estimated. The viscosities of ethyl laurate at 313 K and 333 K were calculated. Although the viscosity values differed significantly from the reported values and the measurements are still inaccurate, the possibility of using this method as a density measurement method under high pressure was demonstrated. Therefore, this study introduces a method with the potential to conveniently measure high-pressure physical properties.

人们曾多次尝试通过分析石英晶体谐振器的响应来测量高压下液体的粘度。然而,由于谐振器的响应会产生密度和粘度的乘积,因此必须将两个值分开。考虑到涂有二氧化钛的石英晶体谐振器的响应与密度相关这一事实,我们设计了一种程序来测量高压下液体的密度变化。TiO2 涂层石英晶体谐振器的共振频率偏移是取决于 (rho ) 和 (sqrt{eta rho }) 的项的总和。每种效应都可以通过平面方程拟合来分离。通过应用月桂酸乙酯,在 313 K 和 333 K 时获得了高达 300 MPa 的密度。这些值与之前报道的值一致,在 ± 1 % 的范围内,从而证明了这种方法的有效性。由于在获得密度数据的过程中也获得了 (sqrteta rho }) 的压力依赖性,因此可以估算出粘度 (eta ) 的压力依赖性。计算了月桂酸乙酯在 313 K 和 333 K 时的粘度。虽然粘度值与报告值相差很大,测量结果也不准确,但证明了在高压下使用这种方法作为密度测定方法的可能性。因此,本研究介绍了一种有可能方便测量高压物理性质的方法。
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International Journal of Thermophysics
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