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Solubility and metastable zone width measurement of 3,4-bis (3-nitrofurazan-4-yl) furoxan (DNTF) in ethanol + water 被引量:9
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作者 Lizhen Chen Liang Song +1 位作者 Guanchao Lan Jianlong Wang 《Chinese Journal of Chemical Engineering》 SCIE EI CAS CSCD 2017年第5期646-651,共6页
The solubility and supersolubility of 3,4-bis(3-nitrofurazan-4-yl)furoxan(DNTF) in ethanol + water at different operation were determined by laser monitoring system under atmospheric pressure to study the metastable z... The solubility and supersolubility of 3,4-bis(3-nitrofurazan-4-yl)furoxan(DNTF) in ethanol + water at different operation were determined by laser monitoring system under atmospheric pressure to study the metastable zone width(MSZW). The modified Apelblat equation was adopted to correlate the experimental solubility data, and the correlation result showed perfect consistent with the experimental data. The standard dissolution enthalpy, standard dissolution entropy and Gibbs energy were calculated according to the experimental solubility data. The effect of the cooling rate, stirring rate, temperature and the concentration of ethanol + water on the MSZW was studied. It was found that the MSZW of DNTF increased with the increasing cooling rate, decreasing temperature, decreasing stirring rate and decreasing ratio of water. And the apparent nucleation order of DNTF in ethanol + water was calculated by the relationship between the cooling rate and the MSZW. 展开更多
关键词 3 4-Bis(3-nitrofurazan-4-yl)furoxan SOLUBILITY Metastable zone width Apparent nucleation order
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Solubility and metastable zone width measurement of 2,4-diaminobenzenesulfonic acid in(H_(2)SO_(4)+H_(2)O)system
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作者 Fanfan Shen Lizhen Chen +2 位作者 Pengbao Lian Jianlong Wang Duanlin Cao 《Chinese Journal of Chemical Engineering》 SCIE EI CAS CSCD 2022年第4期384-391,共8页
The equilibrium solubility of 2,4-diaminobenzenesulfonic acid and super solubility as well as metastable zone width were measured in(H_(2)SO_(4)+H_(2)O) system by the laser dynamic method at elevate temperature range ... The equilibrium solubility of 2,4-diaminobenzenesulfonic acid and super solubility as well as metastable zone width were measured in(H_(2)SO_(4)+H_(2)O) system by the laser dynamic method at elevate temperature range from 298.15 K to 338.15 K.2,4-Diaminobenzenesulfonic acid solubility dependence on the temperature and solvent composition were correlated by the modified Apelblat equation,(CNIBS)/Redlich-Kister model and Jouyban-Acree model.The correlated results by three correlation models were in good accord with the experimental values according to relative average deviations(RD),root-mean-square deviations(RMSD),and correlation coefficients(R^(2)).The metastable zone width increased with temperature and sulfuric acid content.The dissolution enthalpy,dissolution entropy and the Gibbs energy were calculated from the experimental values,which indicated that dissolution process of the 2,4-diaminobenzenesulfonic acid was endothermic.The solubility and calculation models of 2,4-diaminobenzenesulfonic acid in(sulfuric acid+water)system could provide the basic data to the crystallization and purifying of the 2,4-diaminobenzenesulfonic acid. 展开更多
关键词 2 4-Diaminobenzenesulfonic acid SOLUBILITY CORRELATION Metastable zone width
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Determination of the Metastable Zone Width, Nucleation Kinetics, Structural and Optical Properties of KCl Doped KAP Crystal
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作者 M. A. Rahman M. M. Rahman 《Journal of Crystallization Process and Technology》 2015年第2期31-42,共12页
Slow evaporation method was used to grow pure and KCl (10 mol%) doped KAP single crystal. The solubility and metastable zone width of aqueous solutions of pure and KCl (10 mol%) doped KAP crystal were evaluated to ana... Slow evaporation method was used to grow pure and KCl (10 mol%) doped KAP single crystal. The solubility and metastable zone width of aqueous solutions of pure and KCl (10 mol%) doped KAP crystal were evaluated to analyze the crystallization process. Measuring the induction period τ, the critical nucleation parameters like interfacial energy (σ), energy of formation of the critical nucleus (&#916G*) were determined using the classical theory of nucleation. The structural properties and optical constants of the grown crystals have been put to test and observed that the addition of KCl results in an enhancement of properties of the crystal. Grown crystals were characterized by powder X-ray diffraction. FTIR spectra confirmed the presence of KCl in pure KAP crystal. UV- Visible spectroscopic studies revealed that addition of KCl in pure KAP crystal increased transparency from 75% to 80%. The analysis of the optical absorption data revealed the presence of both indirect and direct transitions and both of these band gaps increased with the addition of KCl. The transmittance data was analyzed to calculate the refractive index, oscillator energy, dispersion energy, electric susceptibility, zero-frequency dielectric constant and both the real and imaginary parts of the dielectric permittivity as a function of photon energy. The moments of ε(E) were also determined. The dispersion i.e. spectral dependence of the refractive index was discussed according to the single-effective oscillator model proposed by Wemple and DiDomenico. 展开更多
关键词 Single CRYSTAL Growth from Solution METASTABLE zone width FTIR UV-VISIBLE Spectroscopy Optical CONSTANTS
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Residual Stresses and Micro-Hardness Testing in Evaluating the Heat Affected Zone’s Width of Ferritic Ductile Iron Arc Welds 被引量:1
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作者 Georgios K. Triantafyllidis Dimitrios I. Zagliveris +5 位作者 Dionysios L. Kolioulis Christos S. Tsiompanis Titos N. Pasparakis Athanasios P. Gredis Melina L. Sfantou Ioannis E. Giouvanakis 《Materials Sciences and Applications》 2016年第1期73-82,共10页
Shielded Metal Arc Welding (SMAW) in Ductile Irons (DI) is often required by foundries for practical manufacturing reasons. The mechanical properties of the welded structures are strongly dependent on their HAZ’s wid... Shielded Metal Arc Welding (SMAW) in Ductile Irons (DI) is often required by foundries for practical manufacturing reasons. The mechanical properties of the welded structures are strongly dependent on their HAZ’s width. A model based on the behaviour of the ferritic matrix of high-Si DIs in order to make an approach in measuring their HAZ’s width is developed in this study. A series of thermal treatments on 3.35 and 3.75 wt% Si as-cast DIs and spot SMAWs is applied on these materials. The applied SMAWs are done on non-preheated and preheated samples (150℃ - 300℃). For welding we modify the amperage (100 - 140A). The micro-hardness Vickers changes in the ferrite of the as-cast samples and inside the HAZ of the welded ones can be attributed to the existence of residual stresses (RS) in the ferritic matrix and assist in estimating the HAZ’s width. 展开更多
关键词 WELDS Heat Affected zone Residual Stresses Micro-Hardness Vickers Heat Affected zone’s width
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Numerical Simulation of the Relationship between the Width of Destressed Zone and Blasthole Depth 被引量:1
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作者 Jiansheng Tian Qingru Wu Zhijun Liu 《Engineering(科研)》 2020年第4期269-279,共11页
Overstress in the surrounding rock of the roadway is a key reason that causes failures of deep roadways. Destressing blasting is one of the promising techniques that could improve the supporting quality. If the depth ... Overstress in the surrounding rock of the roadway is a key reason that causes failures of deep roadways. Destressing blasting is one of the promising techniques that could improve the supporting quality. If the depth of the pressure relief blast hole is too shallow, the surrounding rock of the roadway will be broken or even collapsed. If the pressure relief blast hole is too deep, the pressure relief area will be located in the deep part of the surrounding rock of the roadway, which cannot achieve the purpose of releasing the stress in the shallow part of the surrounding rock and cause waste of the blast hole. The width or range of the pressure relief area should just fall in the high stress area of the surrounding rock of the roadway, so the pressure relief blast hole should have a reasonable depth. In order to quantitatively describe the relationship between borehole depth and the width of the stress relief zone, numerical simulations were carried out in ANSYS according to different borehole depths. The results show that the optimal destressing effect is achieved when borehole depth is 4 m. Peak stress of and is significantly reduced by 30.51% and 49.07% after blasting. Meanwhile, the high-stress area shifts about 4.8 m from the roadside to the depth of surrounding rock, thus a 3.8 m wide stress relief zone is formed around the roadside, thus, the aim of quantizing the effects of destress blasting is achieved. 展开更多
关键词 Rock BURST Deep ROADWAY Supporting width of Stress RELIEF zone Destress BLASTING Numerical Simulation
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Spatial-temporal characterization of the San Andreas Fault by fault-zone trapped waves at seismic experiment site,Parkfield,California 被引量:2
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作者 Yong-Gang Li 《Earthquake Science》 2021年第3期261-285,共25页
In this article,we review our previous research for spatial and temporal characterizations of the San Andreas Fault(SAF)at Parkfield,using the fault-zone trapped wave(FZTW)since the middle 1980s.Parkfield,California h... In this article,we review our previous research for spatial and temporal characterizations of the San Andreas Fault(SAF)at Parkfield,using the fault-zone trapped wave(FZTW)since the middle 1980s.Parkfield,California has been taken as a scientific seismic experimental site in the USA since the 1970s,and the SAF is the target fault to investigate earthquake physics and forecasting.More than ten types of field experiments(including seismic,geophysical,geochemical,geodetic and so on)have been carried out at this experimental site since then.In the fall of 2003,a pair of scientific wells were drilled at the San Andreas Fault Observatory at Depth(SAFOD)site;the main-hole(MH)passed a~200-m-wide low-velocity zone(LVZ)with highly fractured rocks of the SAF at a depth of~3.2 km below the wellhead on the ground level(Hickman et al.,2005;Zoback,2007;Lockner et al.,2011).Borehole seismographs were installed in the SAFOD MH in 2004,which were located within the LVZ of the fault at~3-km depth to probe the internal structure and physical properties of the SAF.On September 282004,a M6 earthquake occurred~15 km southeast of the town of Parkfield.The data recorded in the field experiments before and after the 2004 M6 earthquake provided a unique opportunity to monitor the co-mainshock damage and post-seismic heal of the SAF associated with this strong earthquake.This retrospective review of the results from a sequence of our previous experiments at the Parkfield SAF,California,will be valuable for other researchers who are carrying out seismic experiments at the active faults to develop the community seismic wave velocity models,the fault models and the earthquake forecasting models in global seismogenic regions. 展开更多
关键词 San Andreas fault fault-zone trapped wave low-velocity zonewave guide effect dispersion strong ground motion earthquake hazard propagator matrix finite-difference simulation dynamic rupture fault zone width and depth co-mainshock damage post-seismic healing seismic experimental site SAFOD
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Semi-analytical solution for mechanical analysis of tunnels crossing strike-slip fault zone considering nonuniform fault displacement and uncertain fault plane position
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作者 YANG Heng-hong WANG Ming-nian +1 位作者 YU Li ZHANG Xiao 《Journal of Central South University》 SCIE EI CAS CSCD 2024年第6期2116-2136,共21页
The tunnel subjected to strike-slip fault dislocation exhibits severe and catastrophic damage.The existing analysis models frequently assume uniform fault displacement and fixed fault plane position.In contrast,post-e... The tunnel subjected to strike-slip fault dislocation exhibits severe and catastrophic damage.The existing analysis models frequently assume uniform fault displacement and fixed fault plane position.In contrast,post-earthquake observations indicate that the displacement near the fault zone is typically nonuniform,and the fault plane position is uncertain.In this study,we first established a series of improved governing equations to analyze the mechanical response of tunnels under strike-slip fault dislocation.The proposed methodology incorporated key factors such as nonuniform fault displacement and uncertain fault plane position into the governing equations,thereby significantly enhancing the applicability range and accuracy of the model.In contrast to previous analytical models,the maximum computational error has decreased from 57.1%to 1.1%.Subsequently,we conducted a rigorous validation of the proposed methodology by undertaking a comparative analysis with a 3D finite element numerical model,and the results from both approaches exhibited a high degree of qualitative and quantitative agreement with a maximum error of 9.9%.Finally,the proposed methodology was utilized to perform a parametric analysis to explore the effects of various parameters,such as fault displacement,fault zone width,fault zone strength,the ratio of maximum fault displacement of the hanging wall to the footwall,and fault plane position,on the response of tunnels subjected to strike-slip fault dislocation.The findings indicate a progressive increase in the peak internal forces of the tunnel with the rise in fault displacement and fault zone strength.Conversely,an augmentation in fault zone width is found to contribute to a decrease in the peak internal forces.For example,for a fault zone width of 10 m,the peak values of bending moment,shear force,and axial force are approximately 46.9%,102.4%,and 28.7% higher,respectively,compared to those observed for a fault zone width of 50 m.Furthermore,the position of the peak internal forces is influenced by variations in the ratio of maximum fault displacement of the hanging wall to footwall and the fault plane location,while the peak values of shear force and axial force always align with the fault plane.The maximum peak internal forces are observed when the footwall exclusively bears the entirety of the fault displacement,corresponding to a ratio of 0:1.The peak values of bending moment,shear force,and axial force for the ratio of 0:1 amount to approximately 123.8%,148.6%,and 111.1% of those for the ratio of 0.5:0.5,respectively. 展开更多
关键词 strike-slip fault tunnel engineering semi-analytical solution fault zone width nonuniform fault displacement uncertain fault plane position
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fmax and fault zone property of Lushan earthquake of 20 April 2013,Sichuan,China
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作者 Jian Wen Xiaofei Chen 《Earthquake Science》 2013年第3期179-183,共5页
In this study, we determined fnax from near- field accelerograms of the Lushan earthquake of April 20, 2013 through spectra analysis. The result shows that the values of fmax derived from five different seismography s... In this study, we determined fnax from near- field accelerograms of the Lushan earthquake of April 20, 2013 through spectra analysis. The result shows that the values of fmax derived from five different seismography stations are very close though these stations roughly span about 100 km along the strike. This implies that the cause offmax is mainly the seismic source process rather than the site effect. Moreover, according to the source-cause model of Papageorgiou and Aki (Bull Seism Soc Am 73:693-722, 1983), we infer that the cohesive zone width of the rupture of the Lushan earthquake is about 204 with an uncertainty of 13 m. We also find that there is a significant bulge between 30 and 45 Hz in the amplitude spectra of accel- erograms of stations 51YAL and 51QLY, and we confirm that it is due to seismic waves' reverberation of the sedi- mentary soil layer beneath these stations. 展开更多
关键词 Lushan earthquake fmax Strongground motion Fault-zone width Cohesive zone
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井下作业面U型及L型高效通风技术的应用
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作者 张晓威 《煤矿现代化》 2026年第1期59-63,共5页
为了解决煤矿井下采用“U+L”型综合通风系统依靠经验设计缺乏合理性,通风效率和经济性较低的不足。在建立井下通风系统综合评价指标的基础上,利用三维建模软件建立了“U+L”型综合通风系统,通过理论分析和数值模拟分析的方法,从井下瓦... 为了解决煤矿井下采用“U+L”型综合通风系统依靠经验设计缺乏合理性,通风效率和经济性较低的不足。在建立井下通风系统综合评价指标的基础上,利用三维建模软件建立了“U+L”型综合通风系统,通过理论分析和数值模拟分析的方法,从井下瓦斯浓度控制、采空区煤炭防自燃、通风经济性和管理便捷性等角度出发对联络巷在不同区域情况下井下风量分布和氧化带分布情况进行了分析。分析发现,当把井下上隅角处瓦斯浓度极限值为1%、采空区内氧化带最大宽度为45 m作为控制标准的情况下,若作业面的风量需求不超过1 000 m^(3)/min,则联络巷的分布距离不能超过12 m;若作业面的风量需求不超过2 000 m^(3)/min,则联络巷的分布距离不能超过36 m,为优化井下通风系统结构,提高通风安全性奠定了基础。 展开更多
关键词 综合通风 数值模拟 瓦斯浓度 氧化带宽度
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基于变区间宽度广义预测控制的供热机组灵活协调控制策略
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作者 王玮 谢欣言 +2 位作者 蔚伟 胡勇 曾德良 《中国电机工程学报》 北大核心 2025年第13期5173-5184,I0020,共13页
充分利用热网蓄热实施供热抽汽调节是提升供热机组(cogeneration,combined heat and power,CHP)自动发电控制(automatic generation control,AGC)调节性能的有效方案,为克服供热抽汽调节对机组热负荷的影响,提出一种基于变区间广义预测... 充分利用热网蓄热实施供热抽汽调节是提升供热机组(cogeneration,combined heat and power,CHP)自动发电控制(automatic generation control,AGC)调节性能的有效方案,为克服供热抽汽调节对机组热负荷的影响,提出一种基于变区间广义预测控制的供热机组灵活协调控制策略,该策略通过引入热负荷柔性区间控制,实现了基于电负荷快速响应和热负荷自适应恢复的电热协同优化。首先,通过模型仿真数据建立了直流炉供热机组的受控自回归积分滑动平均(controlled auto-regressive integrated moving average,CARIMA)模型;进一步,引入了双曲正切函数,设计了基于机组电热负荷的动态区间优化函数,并采用粒子群算法寻优确定被控量权重系数,构建了基于热负荷柔性区间控制的滚动优化目标;采用带遗忘因子的递推最小二乘法算法进行预测模型在线辨识实现反馈校正,与所设计的滚动优化目标,协调配合求取最优控制律。仿真结果表明,所提出的控制策略在保障热负荷供应的同时,使机组AGC综合指标提升了62%,满足电网的调峰需求。 展开更多
关键词 供热机组(CHP) 广义预测控制 变区间宽度 灵活性
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钢-UHPC组合梁负弯矩区抗裂性能试验研究 被引量:2
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作者 李立峰 彭浩 +2 位作者 邹德强 黄心仪 李凌霄 《建筑科学与工程学报》 北大核心 2025年第3期15-25,共11页
为解决钢-混凝土组合连续梁负弯矩区桥面板的开裂问题,提出了采用超高性能混凝土(UHPC)代替负弯矩区桥面板的部分普通混凝土(NC),利用UHPC超高的力学性能解决负弯矩区桥面板的开裂问题,对其抗裂性能进行研究;设计并完成了3片钢-UHPC组... 为解决钢-混凝土组合连续梁负弯矩区桥面板的开裂问题,提出了采用超高性能混凝土(UHPC)代替负弯矩区桥面板的部分普通混凝土(NC),利用UHPC超高的力学性能解决负弯矩区桥面板的开裂问题,对其抗裂性能进行研究;设计并完成了3片钢-UHPC组合梁负弯矩区抗裂试验,获得开裂荷载、跨中位移、裂缝宽度和应变等试验数据。结合国内外裂缝宽度计算公式,提出了简易的适用于钢-UHPC组合梁的桥面板裂缝宽度计算公式,并根据已有钢-UHPC组合梁文献的裂缝宽度试验数据,验证了提出的桥面板裂缝宽度计算公式的可靠性和适用性。结果表明:UHPC能提高组合梁负弯矩区的开裂荷载,具有抑制桥面板裂缝发展的能力,能明显提高桥面板负弯矩区的抗裂性能,有效解决负弯矩区桥面板的开裂问题;根据试验结果计算的名义应力均大于工程实际设计值,负弯矩区采用UHPC代替NC的结构具有优异的抗裂性能;建议组合梁负弯矩区UHPC纵向铺设长度宜为0.2L~0.25L(L为计算跨径),铺设厚度宜为60~70 mm。 展开更多
关键词 钢-UHPC组合梁 负弯矩区 抗裂性能 裂缝宽度
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汶水河流域滨水缓冲带安全宽度规划研究
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作者 秦志强 邹晔 +3 位作者 郭人泰 郭刘鹏 王超 薛良方 《环境污染与防治》 北大核心 2025年第4期35-41,47,I0002,I0003,共10页
基于SWAT模型建立了汶水河流域非点源污染模型,估算了流域内污染物负荷,利用经验公式预测了径流通过滨水缓冲带边界时的污染物浓度,通过相关性分析识别了决定该河段滨水缓冲带最小安全宽度的关键变量。结果表明:1)SWAT模型适合进行径流... 基于SWAT模型建立了汶水河流域非点源污染模型,估算了流域内污染物负荷,利用经验公式预测了径流通过滨水缓冲带边界时的污染物浓度,通过相关性分析识别了决定该河段滨水缓冲带最小安全宽度的关键变量。结果表明:1)SWAT模型适合进行径流、总氮(TN)和总磷(TP)模拟。2)地表径流中TN和TP负荷由上游至下游呈增加趋势。3)滨水缓冲带安全宽度受到连接度、坡度、耕地面积和人口密度的影响。上、中、下游滨水缓冲带应各自维持77.90、33.37、60.65 m的安全宽度。 展开更多
关键词 非点源污染 SWAT模型 滨水缓冲带 安全宽度 径流
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基于轧制力判定的薄带材极限可轧厚度理论研究
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作者 李伟 李松松 于辉 《工程力学》 北大核心 2025年第11期251-259,共9页
极限可轧厚度是薄带材轧制过程中判断轧件是否可以继续减薄的重要理论判据,然而现有的理论公式很少考虑轧件可轧性的工艺相关性,该文通过有限元手段研究了薄带轧制变形区特征随轧制工艺的变化规律,并基于赫兹弹性理论和一点弹塑性应力... 极限可轧厚度是薄带材轧制过程中判断轧件是否可以继续减薄的重要理论判据,然而现有的理论公式很少考虑轧件可轧性的工艺相关性,该文通过有限元手段研究了薄带轧制变形区特征随轧制工艺的变化规律,并基于赫兹弹性理论和一点弹塑性应力状态开展了以轧制力作为判别依据的极限可轧厚度理论研究。结果表明:轧件可轧性与轧制工艺密切相关,临近极限可轧厚度时变形区内以弹性变形为主,所对应的接触压力分布符合赫兹弹性理论。通过比较极值点的等效应力与轧件屈服强度的大小关系可以准确判断轧件的弹塑性状态,而采用极限单位宽度轧制力可较好地预测给定工艺下轧件的可轧性,并反推给定轧制力下的极限可轧厚度。 展开更多
关键词 薄带材轧制 单位宽度轧制力 变形区理论 极限可轧厚度 赫兹接触
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穿越软弱破碎带隧道稳定性分析
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作者 包龙生 王选晗 +2 位作者 刘衎 刘博 赵国庆 《沈阳建筑大学学报(自然科学版)》 北大核心 2025年第4期523-532,共10页
研究不同产状因素软弱破碎带下隧道施工时围岩的变形规律、受力情况及稳定性,为该类隧道工程提供数据支撑和参考。利用Midas GTS NX有限元软件,根据不同的软弱破碎带产状因素(倾向、走向、宽度)建立多种数值模型,研究不同产状软弱破碎... 研究不同产状因素软弱破碎带下隧道施工时围岩的变形规律、受力情况及稳定性,为该类隧道工程提供数据支撑和参考。利用Midas GTS NX有限元软件,根据不同的软弱破碎带产状因素(倾向、走向、宽度)建立多种数值模型,研究不同产状软弱破碎带作用下施工时隧道结构的变形规律。不同产状因素的软弱破碎带作用下,围岩竖向、水平位移均呈现出先增大后减小的趋势,位移在破碎带中心达到最大值,并逐渐向两侧减小,整体呈“正态分布”,位移突变量基本是破碎带宽度的2~3倍。保持隧道行进方向与软弱破碎带正交,可有效提升隧道结构稳定性,同一监测断面的各个测点接触压力由大至小依次为拱脚、边墙、拱肩、拱顶、仰拱,可见拱脚至边墙区域为支护结构的薄弱部位。 展开更多
关键词 软弱破碎带 隧道稳定性 数值模拟 倾向 走向 宽度
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CL-20/MTNP共晶在乙醇中的介稳特性和成核行为 被引量:1
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作者 秦康怡 段勇威 +2 位作者 曹云杉 范雯婧 段晓惠 《火炸药学报》 北大核心 2025年第1期22-32,I0004,共12页
为探究六硝基六氮杂异伍兹烷(CL-20)/1-甲基-3,4,5-三硝基吡唑(MTNP)共晶的成核过程,对比研究了CL-20/MTNP共晶与两种单体在乙醇中的溶解度和介稳区宽度(MSZW),并采用修正的Sangwal模型进一步分析其成核行为。结果表明,CL-20/MTNP共晶... 为探究六硝基六氮杂异伍兹烷(CL-20)/1-甲基-3,4,5-三硝基吡唑(MTNP)共晶的成核过程,对比研究了CL-20/MTNP共晶与两种单体在乙醇中的溶解度和介稳区宽度(MSZW),并采用修正的Sangwal模型进一步分析其成核行为。结果表明,CL-20/MTNP共晶及其单体的介稳区宽度均随饱和温度(T_(s))升高和冷却速率(q)降低而减小,且当q较大时,q对介稳区宽度的影响更显著;3种物质的界面能(γ)和成核动力学因子(A)随T_(s)升高而减小,说明T_(s)的增加有利于成核;CL-20/MTNP拥有最大的γ、临界核尺寸(r_(crit))和吉布斯自由能(ΔG crit)以及最小的A,其介稳区宽度最宽,成核最困难;MTNP拥有最小的γ、r_(crit)和ΔG crit以及最大的A,其介稳区宽度最窄,成核最容易,CL-20则介于两者之间。 展开更多
关键词 物理化学 CL-20 MTNP 共晶 介稳区宽度 界面能 成核动力学
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基于单电流传感器的永磁同步电机混合脉宽调制技术 被引量:1
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作者 田里思 宗耐龙 +2 位作者 刘立伟 张珈铭 胡东方 《电工技术学报》 北大核心 2025年第8期2451-2463,共13页
针对采用单电流传感器的永磁同步电机在低调制区与扇区边界区的重构死区问题,该文提出一种将改进的正三角形脉宽调制法与测量相位后移调制法结合的混合脉宽调制策略,在有效实现死区内电流重构的同时,突破传统正三角形脉宽调制无法单独... 针对采用单电流传感器的永磁同步电机在低调制区与扇区边界区的重构死区问题,该文提出一种将改进的正三角形脉宽调制法与测量相位后移调制法结合的混合脉宽调制策略,在有效实现死区内电流重构的同时,突破传统正三角形脉宽调制无法单独实现电机中高转速运行的局限性。同时针对单电流传感器分时采样所导致的重构误差问题以及补偿过程过于复杂的问题,提出一种新的特殊点电流采样策略,通过固定电流传感器两次采样时刻与采样间隔,使传统的两步电流补偿简化为一步电流补偿,在提高电流重构准确性的同时简化了控制算法,显著提升了电机的控制性能。 展开更多
关键词 永磁同步电机 单电流传感器 重构死区 混合脉宽调制 电流补偿
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丁二酸的溶解度与介稳区测定及关联
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作者 朱化雷 吕清林 +3 位作者 包洪洲 韩冰 房畅 李澜鹏 《石油化工》 北大核心 2025年第9期1272-1277,共6页
建立了基于原位反应的衰减全反射傅里叶变换红外光谱法的丁二酸(SA)水溶液含量的在线分析方法,选定1178 cm^(-1)处特征吸收峰与SA含量进行关联,相关系数(R2)为0.9999,可满足分析要求。通过该分析方法测定了SA在纯水中的溶解度,实验值与... 建立了基于原位反应的衰减全反射傅里叶变换红外光谱法的丁二酸(SA)水溶液含量的在线分析方法,选定1178 cm^(-1)处特征吸收峰与SA含量进行关联,相关系数(R2)为0.9999,可满足分析要求。通过该分析方法测定了SA在纯水中的溶解度,实验值与文献值吻合良好。并采用van’tHoff,Apelblat,λh方程对溶解度实验数据进行关联,三者拟合R2分别为0.9990,0.9999,0.9980,相对平均偏差分别为1.616%,1.613%,2.292%,三者中Apelblat方程具有更高的拟合度。以溶解度数据为基础,采用聚焦光束反射测量法根据实验测定的介稳区宽度(ΔT_(max)),考察了降温速率(r)与搅拌转速(n)对ΔTmax的影响,SA的ΔT_(max)与饱和温度和n负相关,与r正相关,并采用自洽Nývlt型方程结合实验数据计算得到成核动力学参数m在3.1~5.3之间。 展开更多
关键词 丁二酸 溶解度 介稳区宽度 成核动力学
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Fe和Ni共掺杂ZnO复合光催化剂的制备及其光催化活性研究
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作者 王远港 杨蕊萌 +1 位作者 王有杰 赵显一 《化工新型材料》 北大核心 2025年第6期202-208,共7页
纳米ZnO因来源广、廉价和无毒性等优点得到广泛的研究,但其可见光响应范围窄、较宽的禁带宽度和光生电子-空穴复合较快等问题已成为纳米ZnO实际应用的瓶颈。采用水热合成法制备了铁和镍共掺杂ZnO复合光催化剂Fe_(0.02)/Ni_(x)-ZnO,通过... 纳米ZnO因来源广、廉价和无毒性等优点得到广泛的研究,但其可见光响应范围窄、较宽的禁带宽度和光生电子-空穴复合较快等问题已成为纳米ZnO实际应用的瓶颈。采用水热合成法制备了铁和镍共掺杂ZnO复合光催化剂Fe_(0.02)/Ni_(x)-ZnO,通过X射线衍射仪、扫描电子显微镜、透射电子显微镜、X射线光电子能谱仪、紫外-可见漫反射光谱仪、光致发光光谱仪、电化学交流阻抗测试等对复合光催化剂的相结构、微观形貌、元素价态、光学性质和电化学性质进行表征,考察了复合光催化剂对罗丹明B的光催化活性。结果表明:当Fe^(3+)掺杂量为2%、Ni^(2+)掺杂量为10%(均为质量分数)时,Fe_(0.02)/Ni_(0.1)-ZnO复合光催化剂的禁带宽度明显减小,对罗丹明B的降解率最高。自由基捕获和电子自旋共振波谱分析证实,空穴是光降解罗丹明B的主要活性物种。 展开更多
关键词 ZNO 光响应范围 共掺杂 禁带宽度
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基于CFD模拟的缓倾斜煤层下行通风模式下采空区自燃风险研究
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作者 杨扬 《陕西煤炭》 2025年第11期40-45,共6页
为剖析缓倾斜煤层工作面在采用下行通风方式时,其采空区内自燃风险区域的分布规律,构建了倾斜采空区的流体渗流数学模型,运用计算流体动力学(CFD)模拟了采空区内遗煤不同自燃条件下,下行通风采空区内氧气浓度与温度场的空间分布特性,并... 为剖析缓倾斜煤层工作面在采用下行通风方式时,其采空区内自燃风险区域的分布规律,构建了倾斜采空区的流体渗流数学模型,运用计算流体动力学(CFD)模拟了采空区内遗煤不同自燃条件下,下行通风采空区内氧气浓度与温度场的空间分布特性,并在山西温家庄煤矿81煤层回采工作面进行工程验证。研究结果表明,随着采空区内遗煤自燃倾向性的增强,采空区内的火风压效应显著加剧,在采用下行通风方式时,采空区进风侧与回风侧之间的氧化带宽度差异逐渐缩减。根据研究区工程概况确定了进、回风侧以及工作面中部对应的采空区内窒息带起始位置,分别距离工作面约200 m、290 m和175 m。实测数据与模拟火源功率为65 W/m^(2)时的计算结果一致,证明了该模型在探究倾斜易自燃煤层工作面自燃分布特征方面具备有效性。 展开更多
关键词 缓倾斜煤层 数值模拟 遗煤自然 氧化带宽度
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倾斜煤层采空区上煤体卸压防突宽度研究
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作者 许小波 范尚崇 +3 位作者 覃佐亚 熊学仁 曹远林 刘荣涛 《煤》 2025年第6期18-22,共5页
针对水井头煤矿沿空掘巷位置选择不清,缺少理论及材料支撑的问题,对当前采空区侧煤体卸压防突宽度的4个观点进行评价分析,确定了卸压防突宽度的合理考察范围,并利用理论计算和数值模拟确定了该考察范围,最终在考察范围内对残余瓦斯含量... 针对水井头煤矿沿空掘巷位置选择不清,缺少理论及材料支撑的问题,对当前采空区侧煤体卸压防突宽度的4个观点进行评价分析,确定了卸压防突宽度的合理考察范围,并利用理论计算和数值模拟确定了该考察范围,最终在考察范围内对残余瓦斯含量防突指标进行现场测定,确定了倾斜煤层采空区上煤体卸压防突宽度。结果表明:塑性区范围可作为卸压防突宽度的考察范围,并且塑性区范围应为卸压防突宽度的上限;理论计算和数值模拟结果显示,倾斜煤层塑性区宽度为9.03~9.98 m,并将考察范围确定为12 m;根据残余瓦斯含量现场实测结果,在距采空区9.3 m位置处残余瓦斯含量为5.36 m^(3)/t,处于防突标准以下,在距采空区11.8 m位置处残余瓦斯含量最大为6.79 m^(3)/t.最终将3624工作面上部采空区卸压防突范围确定为沿煤层层面9.03 m. 展开更多
关键词 沿空掘巷 卸压防突宽度 残余瓦斯含量 倾斜煤层 塑性区宽度
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