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Experiments With clay on Shear Fractures

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地质学报 1948年第Z1期 26-37页

作者： J.S.LEE c.h.chen M.T.LEE Institute of Geology Academia Sinica

In view of theoretical as well as practical importance in geotectonicconsiderations of the angular relation between the shear fractures developedin rocks that have undergone more or less plastic deformation and thepri... 详细信息

关键词： Experiments With clay on Shear Fractures

A BRIEF VIEW OF ThE cURRENT STATE OF ThE DEVELOPMENT AND AGING PERFORMANcE OF FIXED FREQUENcY SURFAcE AcOUSTIc WAVE(SAW) OScILLATOR

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A BRIEF VIEW OF THE CURRENT STATE OF THE DEVELOPMENT AND AGI...

hydrogen adsorption on litchi trunk based activated carbon and palladium nanoparticles supported on the same

2012全国压电和声波理论及器件技术研讨会

作者： c.S.LAM P.Y.SU c.h.chen TXc Technology Inc.MilpitasCaliforniaUSA TXc corporation

The recent rapid expansion of optical fiber networking market fuels the demand for accurate 10000 Mhz fixed frequency oscillators based on surface acoustic wave(SAW) ***,several suppliers can offer small size and cost efficient SMD single-end and differential SAW oscillators(SOs) with very good phase jitter *** customers prefer SO solution as it is free of the unsettling problems from some crystal oscillator(XO) solutions- high cost of high frequency fundamental(hFF) and inverted mesa(IM) crystal blanks,spurious modes,frequency jumping,drive level sensitivity,high cost of phase lock loop(PLL) die,*** paper is to provide a brief view of the current state of the development of fixed frequency *** on the aging data of more than 20,000 hours at 125℃,the authors also comment on the SO aging performance fabricated using different SAW wave-types.

关键词： SAW Oscillator Quartz crystal Aging

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Hydrogen adsorption on litchi trunk based activated carbon a...

第九届全国氢能学术会议

作者： c.c.huang,h.M.chen,c.h.chen National Yunlin University of Science and Technology,Taiwan

＜正＞The aim of this work is to investigate hydrogen adsorption on super activated carbon（Ac）. Litchi trunk was activated by potassium hydroxide under nitrogen or carbon dioxide *** of palladium were impregnated in the prepared *** pore structure of activated carbon was characterized by physical adsorption of nitrogen at 77 K in a gas adsorption apparatus（Quantachrome Autosorb-1）.The hydrogen adsorption was

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球墨铸铁的激光表面处理

武钢技术 1991年第10期29卷 56-61页

作者： c.h.chen 李凡

一、引言铸铁价格便宜,有良好的流动性、可铸性、机加工性、耐磨性和综合机械性能,因此在工程上应用广泛。然而在苛刻的工作条件下,如在严重的腐蚀性或侵蚀性环境中,其性能和可靠性受到限制。作为整体合金化的经济有效的取代工艺。

关键词：球墨铸铁激光表面处理

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纤维增强聚氨酯拉挤复合材料——Ⅰ.拉挤工艺的可行性和结构形态

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纤维复合材料 1993年第2期10卷 55-62页

作者： c.h.chen c.c.M.MA 陈平

用一种特殊的方法进行了纤维增强聚氯酯(PU)复合材料的拉挤工艺可行性的研究。用ε—己内酰胺封闭预聚物和甲苯基二异氰酸酯(TDI—80)与分支聚酯混合后合成的NcO—封闭的PU预聚物进行本文的研究。这种封端PU预聚物的分子量、封闭反应程... 详细信息

用一种特殊的方法进行了纤维增强聚氯酯(PU)复合材料的拉挤工艺可行性的研究。用ε—己内酰胺封闭预聚物和甲苯基二异氰酸酯(TDI—80)与分支聚酯混合后合成的NcO—封闭的PU预聚物进行本文的研究。这种封端PU预聚物的分子量、封闭反应程度和封闭后的粘度通过GPc、IR和h—NMR及粘度测量分析求得。采用甲基正丁基胺反滴定(湿)法,测得NcO未封闭的PU预聚物的当量和NcO基的含量。这种封端NcO的PU预聚物加有像脂环族二胺、芳香族二胺和1,4—丁基二醇等链增长剂时,在浸渍温度55—70℃范围内,具有较长的使用期。在升高温度后,从布氏粘度计测量中发现此预聚物具有较高的反应活性。用扫描电镜的结构形态研究证明,这种封端的PU树脂对纤维具有良好的浸润性能,并且纤维束在PU基体中分布均匀。

关键词：纤维增强聚氨酯复合材料拉挤

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纤维增强聚氨酯拉挤复合材料——Ⅱ.工艺参数对机械和耐热性能的影响

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纤维复合材料 1993年第2期10卷 63-69页

作者： c.h.chen c.c.M.MA 陈平

本文提出了一种制造拉挤聚氨酯(PU)复合材料新颖的工艺。研究了工艺参数对纤维增强PU拉挤复合材料的机械性能(如弯曲强度、弯曲模量等)和耐热性能(热变形温度,hDT)的影响。这些工艺参数包括牵引速率(模内线速度),模具温度,填料种类和含... 详细信息

本文提出了一种制造拉挤聚氨酯(PU)复合材料新颖的工艺。研究了工艺参数对纤维增强PU拉挤复合材料的机械性能(如弯曲强度、弯曲模量等)和耐热性能(热变形温度,hDT)的影响。这些工艺参数包括牵引速率(模内线速度),模具温度,填料种类和含量以及后固化时间和温度。研究结果表明,复合材料在不同模具温度下具有不同的最佳牵引速率。以DSc固化曲线为基础可确定溶胀率,复合材科的机械性能和耐热性能,最佳的模具温度。研究发现复合材料的机械性能和耐热性能随着各类填料的含量增加而提高。机械性能在一适宜的后固化温度和时间下也提高。此外,对复合材料的性能在经长时间后固化,由于降解而使性能下降的情况也进行了讨论。

关键词：纤维增强聚氨酯复合材料拉挤

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计数原子

世界科学 1981年第12期 7-11页

作者： G.S.hurst M.G.Payne S.D.Kramer c.h.chen 邓延倬

使用商品激光器的共振电离光谱法,几乎能测定周期表中的所有元素,达到单原子的灵敏度。

关键词：原子所有子体布居分子共振电离正比计数管辐射计数管电子倍增管

Amplitude analysis of the decays D^(0)→π^(+)π^(−)π^(+)π^(−)and D^(0)→π^(+)π^(−)π^(0)π^(0)

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chinese Physics c 2024年第8期48卷 6-33页

作者： M.Ablikim M.N.Achasov P.Adlarson O.Afedulidis X.c.Ai R.Aliberti A.Amoroso Q.An Y.Bai O.Bakina I.Balossino Y.Ban h.-R.Bao V.Batozskaya K.Begzsuren N.Berger M.Berlowski M.Bertani D.Bettoni F.Bianchi E.Bianco A.Bortone I.Boyko R.A.Briere A.Brueggemann h.cai X.cai A.calcaterra G.F.cao N.cao S.A.cetin J.F.chang W.L.chang G.R.che G.chelkov c.chen c.h.chen chao chen G.chen h.S.chen M.L.chen S.J.chen S.L.chen S.M.chen T.chen X.R.chen X.T.chen Y.B.chen Y.Q.chen Z.J.chen Z.Y.chen S.K.choi X.chu G.cibinetto F.cossio J.J.cui h.L.Dai J.P.Dai A.Dbeyssi R.E.de Boer D.Dedovich c.Q.Deng Z.Y.Deng A.Denig I.Denysenko M.Destefanis F.De Mori B.Fang S.S.Fang W.X.Fang Y.Fang Y.Q.Fang R.Farinelli L.Fava F.Feldbauer G.Felici c.Q.Feng J.h.Feng Y.T.Feng K.Fischer M.Fritsch c.D.Fu J.L.Fu Y.W.Fu h.Gao Y.N.Gao Yang Gao S.Garbolino I.Garzia P.T.Ge Z.W.Ge c.Geng E.M.Gersabeck B.Ding X.X.Ding Y.Ding Y.Ding J.Dong L.Y.Dong M.Y.Dong X.Dong M.c.Du S.X.Du Z.h.Duan P.Egorov Y.h.Fan J.Fang JA.Gilman K.Goetzen L.Gong W.X.Gong W.Gradl S.Gramigna M.Greco M.h.Gu Y.T.Gu c.Y.Guan Z.L.Guan A.Q.Guo L.B.Guo M.J.Guo R.P.Guo Y.P.Guo A.Guskov J.Gutierrez K.L.han T.T.han X.Q.hao F.A.harris K.K.he K.L.he F.h.heinsius c.h.heinz Y.K.heng c.herold T.holtmann P.c.hong G.Y.hou X.T.hou Y.R.hou Z.L.hou B.Y.hu h.M.hu J.F.hu T.hu Y.hu G.S.huang K.X.huang L.Q.huang X.T.huang Y.P.huang T.hussain F.h\"olzken N.h\"usken N.in der Wiesche M.Irshad J.Jackson S.Janchiv J.h.Jeong Q.Ji Q.P.Ji W.Ji X.B.Ji X.L.Ji Y.Y.Ji X.Q.Jia Z.K.Jia D.Jiang h.B.Jiang P.c.Jiang S.S.Jiang T.J.Jiang X.S.Jiang Y.Jiang J.B.Jiao J.K.Jiao Z.Jiao S.Jin Y.Jin M.Q.Jing X.M.Jing T.Johansson S.Kabana N.Kalantar-Nayestanaki X.L.Kang X.S.Kang M.Kavatsyuk B.c.Ke V.Khachatryan A.Khoukaz R.Kiuchi O.B.Kolcu B.Kopf M.Kuessner X.Kui A.Kupsc W.K\"uhn J.J.Lane P.Larin L.Lavezzi T.T.Lei Z.h.Lei h.Leithoff M.Lellmann T.Lenz c.Li c.Li c.h.Li cheng Li D.M.Li F.Li G.Li h.Li h.B.Li h.J.Li h.N.Li hui Li J.R.Li J.S.Li K.Li L.J.Li L.K.Li Lei Li M.h.Li P.R.Li Q.M.Li Q.X.Li R.Li S.X.Li T.Li W.D.Li W.G.Li X.Li X.h.Li X.L.Li X.Y.Li Y Institute of high Energy Physics Chinese Academy of SciencesBeijing 100049China Beihang University Beijing 100191China Bochum Ruhr-University D-44780 BochumGermany Budker Institute of Nuclear Physics SB RAS(BINP) Novosibirsk 630090Russia carnegie Mellon University PittsburghPennsylvania 15213USA central china Normal University Wuhan 430079China central South University Changsha 410083China china center of Advanced Science and Technology Beijing 100190China china University of Geosciences Wuhan 430074China chung-Ang University Seoul06974Republic of Korea cOMSATS University Islamabad Lahore CampusDefence RoadOff Raiwind Road54000 LahorePakistan Fudan University Shanghai 200433China GSI helmholtzcentre for heavy Ion Research Gmbh D-64291 DarmstadtGermany Guangxi Normal University Guilin 541004China Guangxi University Nanning 530004China hangzhou Normal University Hangzhou 310036China hebei University Baoding 071002China helmholtz Institute Mainz Staudinger Weg 18D-55099 MainzGermany henan Normal University Xinxiang 453007China henan University Kaifeng 475004China henan University of Science and Technology Luoyang 471003China henan University of Technology Zhengzhou 450001China huangshan college Huangshan 245000China hunan Normal University Changsha 410081China hunan University Changsha 410082China Indian Institute of Technology Madras Chennai 600036India Indiana University BloomingtonIndiana 47405USA INFN Laboratori Nazionali di Frascati INFN Laboratori Nazionali di FrascatiI-00044FrascatiItaly INFN Laboratori Nazionali di Frascati INFN Sezione di PerugiaI-06100PerugiaItaly INFN Laboratori Nazionali di Frascati University of PerugiaI-06100PerugiaItaly INFN Sezione di Ferrara INFN Sezione di FerraraI-44122FerraraItaly INFN Sezione di Ferrara University of FerraraI-44122FerraraItaly Inner Mongolia University Hohhot 010021China Institute of Modern Physics Lanzhou 730000China Institute of Physics and Technology Peace Avenue 54BUlaanbaatar 13330Mongolia Instituto de A

Using e^(+)e^(−)annihilation data corresponding to an integrated luminosity of 2.93 fb^(−1)taken at the center-of-mass energy√s=3.773 GeV with the BESIII detector,a joint amplitude analysis is performed on the decays D^(0)→π^(+)π^(−)π^(+)π^(−)and D^(0)→π^(+)π^(−)π^(0)π^(0)(non-η).The fit fractions of individual components are obtained,and large interferences among the dominant components of the decays D^(0)→a_(1)(1260)π,D^(0)→π(1300)π,D^(0)→ρ(770)ρ(770),and D^(0)→2(ππ)_(S)are observed in both *** the obtained amplitude model,the cP-even fractions of D^(0)→π^(+)π^(−)π^(+)π^(−)and D^(0)→π^(+)π^(−)π^(0)π^(0)(non-η)are determined to be(75.2±1.1_(stat).±1.5_(syst.))%and(68.9±1.5_(stat).±2.4_(syst.))%,*** branching fractions of D^(0)→π^(+)π^(−)π^(+)π^(−)and D^(0)→π^(+)π^(−)π^(0)π^(0)(non-η)are measured to be(0.688±0.010_(stat.)±0.010_(syst.))%and(0.951±0.025_(stat.)±0.021_(syst.))%,*** amplitude analysis provides an important model for the binning strategy in measuring the strong phase parameters of D^(0)→4πwhen used to determine the cKM angleγ(ϕ_(3))via the B^(−)→DK^(−)decay.

关键词： BESIII D^(0)meson decays amplitude analysis cP-even fraction

Preparation of Low Ratio Magnesium ccement by Acid Leaching Treatment of Boron Mud

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Journal of Wuhan University of Technology(Materials Science) 2025年第1期40卷 120-129页

作者： YANG Mei ZhANG Mingzhe chen hao School of Materials Science and Engineering Shenyang Jianzhu UniversityShenyang 110168China School of Physical Science and Technology Shenyang Normal UniversityShenyang 110168China

The effects of liquid-solid ratio and reaction time on the leaching rate of magnesium at room temperature were investigated,as well as the effects of the molar ratio of MgO/Mgcl_(2),the amount of water added,and the amount of acid-impregnated slag dosed on the compressive strength and water resistance of *** results showed that the magnesium element in the boron mud could be maximally leached under the conditions of 1:1 concentration of hydrochloric acid at room temperature,liquid-solid ratio of 2.5 mL·g^(-1),and reaction time of 5 h,and the main products were amorphous SiO_(2) as well as a small amount of magnesium olivine which had not been completely *** LR-MOc prepared using the acid-soaked mixture could reach a softening coefficient of 0.85 for 28 d of water immersion when the molar ratio of MgO/Mgcl_(2) was 2.2,the amount of water added was 0 g,and the acid-soaked slag dosing was 40 wt%,which also led to an appreciable late-strength,with an increase of 19.4%in compressive strength at 28 d compared to that at 7 *** previous studies,LR-MOc prepared in this way has a final strength phase that is not the more easily hydrolysed 3-phase but the lath-like *** this phenomenon,we analyzed the mechanism and found that,during the acid leaching process,a part of amorphous SiO_(2) dissolved in the acid leaching solution formed a silica sol,in which Mg^(2+)played a bridging role to make the silica sol more *** the addition and hydrolysis of MgO,the silica sol gel coagulation slows down,providing a capping layer to inhibit the hydrolysis of the 5-phase crystals and providing some strength after *** amorphous SiO_(2) in the other part of the acid-impregnated slag generated M-S-h gel with Mg^(2+)and Oh-,which synergised with the dense structure composed of interlocking crystals to improve the water resistance of LR-MOc.

关键词： boron mud magnesium chloride-oxygen cement acid immersion water resistance silica sol