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Kinetics of Evaporation of Manganese, Copper and Sulfur from Iron Alloys in Vacuum Induction Melting(Metallurgy) 铁合金中锰、铜和硫在真空感应熔炼中的蒸发动力学(冶金)
R. Ohno
Synopsis The eva/)oration-rate COllstallt K i (kg . m2 .r l ).for each o.f mallgalleJe, cupper alld sulfur in the vacuum induction melting qf iroll alloys has beell rletermilled . The rale cOllslnll1 Kv or K~ (kg . m2 . r ' ).!or the va/Jori :;:alion o.f these elements al the vacuum-melt interface is calculaled. I II each Q( the FeCMn, FcCCu and FcCSiS vstems, the value Q( K i at a lower stirring rale is about one half o.f Ihat at a higher stirring rate; hence mass trans.fer in the melt must be involved in the rate-determining ste/).fol' their evaporation at the lower slirring rale. In the FeCu and FeMn syslems, the value of Kcu at J 973 K is obviously g realer thall that at J 873 K , but those of KM n at bolh lemperatures nre close to each olher. The rales o.f evaporation o.f manganese must be determined prer/ominanliv by Ihe rale qf ils trallsf er in Ihe meLl in view of the vaLues o.f pK ", at both temperatures, which were calcul(lted on Ihe basis q( the equatioll K i = p K",Kvl (.oK", + Kv ), where p (kg .mO) is the densi!)' o.f the meLt and K ,n (m . sI ) is Ihe mass-tranrfer co~fficien t in the melt. i n the Fe-M n, Fe-Cu and FeS n sy slems at J 873 K , most o( the reported experimental values o.f K,II n' Kcu and KSn agree well with their respective values ca!CIl/ated from Ihe equatioll b_v laking .oK", = 6.8 x 101 (kg . m2. s' ), but the present experimenlal values Qf Kcu are smaller than the calculaled value. The plols o.f Ksl.fs vs . as; in Ihe FeSisystem are Linear at two different stirring rates. The rate (onstanls k, and k2 given by this linear relation at a lower stirring rale are smaller than those al a higher slirring role, respectively, and must involve K'lL' III the desulfuri;;ation (I.f FeS, F CS, Fe-Si -5 and FeCSiS alloys at temperatures in the range 1 688J 873 K , the relatioll between K s and K: is rep resented by a curve calculated .from the equation by taking Kv= O.24 K : and p K,n =2. 5 regardless o.f the lemperatures and the alloy systems. This value o.f .oK", is much greater than the value o.f .oK", f or FeMn , F e-C u and FeSn systems. Oxy gCll and sulfur hardly affect Ihe rate of evaporation o.f copper .from molten iroll at J 873 K .
eva/)的运行速率为(kg)。M2 .r (l)。真空感应熔炼的铜和硫在真空感应熔炼的铜合金中被很好地精炼。数值为1kv或K~ (kg)。平方米。R ') !或这些元素的va/Jori:; alion所有的真空熔体界面计算。每一个Q(FeCMn、FcCCu和fccsi)在较低搅拌速率下的Q(ki)值约为较高搅拌速率下的一半;于是就有了大规模运输。熔体中的铁必须参与速率决定阶段。在较低的旋转速率下观察它们的蒸发。在FeCu和FeMn体系中,j973 K时的Kcu值明显大于j873 K时的Kcu值,但两个温度下的kkn值相差不大。根据两种温度下的pK”值,锰的蒸发速率必须优先/主要由溶液中钾的蒸发速率来确定,这两个温度下的pK”值是根据q(等于K i = pK”,Kvl())计算的。oK”,+ Kv),其中p (kg . mo)是熔体的密度,K,n (m。sI)为熔体中的传质系数。在J 873 K的Fe-M - n、Fe-Cu和FeS - n体系中,大多数(报告的)K、II、Kcu和KSn的实验值与它们各自的值吻合得很好。根据当量b_v (k), = 6.8 x 101 (kg)。平方米。s’),但目前的实验值Qf Kcu小于计算值。Ksl的plols。f vs。作为;在两种不同的搅拌速率下,festo系统中的液体呈线性。率(onstanls k, k2,这种线性关系较低搅拌罗音是小于al更高slirring角色,分别和必须包括k会“三世desulfuri;;信息(I.f菲斯,F CS, Fe-Si 5和FeCSiS合金在温度范围688 j 873 k, k和k之间的relatioll:由一条曲线代表憎恨从今以后方程计算通过Kv = O.24 k: p和k, n = 2。不管温度和合金体系如何。对于FeMn, f - c - u和FeSn系统,这个值“。ok”要比“。ok”大得多。在j873 K下,氧和硫对铜的蒸发速率几乎没有影响。
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引用次数: 5
Random Walks on Three-Dimensional Lattices : A Matrix Method for Calculating the Probability of Eventual Return(Physics) 三维格子上的随机行走:计算最终返回概率的矩阵方法(物理)
M. Koiwa
Abstract A matrix method for calculating the number of visits to the origin in random-walks on periodic lattices is developed. The method is applied to three-dimensional lattices: the f.c.c., b.c.c. and the diamond lattices. For the f.c.c. and the b.c.c. lattices the results are in good agreement with those obtained by Montroll. The probability of eventual return in the diamond lattice is evaluated for the first time: it is about 0·442. A new concept, the effective coordination number, is defined on the basis of a calculation of random walks on an imaginary lattice.
摘要提出了一种计算周期格随机行走中到达原点次数的矩阵方法。将该方法应用于三维晶格:f.c.c、b.c.c和菱形晶格。对于f.c.c和b.c.c晶格,所得结果与Montroll的结果一致。在菱形晶格中最终返回的概率第一次被评估:它大约是0·442。在虚格上随机游走计算的基础上,定义了有效配位数这一新概念。
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引用次数: 16
The Fermi Surfaces of Cu-Pd Alloys Studied by Positron Annihilation(Physics) 用正电子湮没研究Cu-Pd合金的费米表面(物理学)
M. Hasegawa, Toshiharu Suzuki, M. Hirabayashi
The Fermi surfaces of Cu–Pd alloys below 63% Pd are studied by means of the angular correlation of positron annihilation with crossed- and long-slit geometries. The - and -radii decrease with increasing palladium content up to 30% in agreement with a calculation based on the rigid band model. The neck radius also decreases with increasing composition, and it is suggested that the Fermi surface detaches from the hexagonal face of the Brillouin zone around 20% Pd, but remains to bulge in this direction at higher compositions. No detectable change is found in the correlation curves of the ordered and disordered states at 15 and 19% Pd. The origin of stabilization of the long period ordered structure near Cu 3 Pd is discussed in the light of the present results.
利用正电子湮灭与交叉和长狭缝几何的角相关性,研究了63% Pd以下Cu-Pd合金的费米表面。随着钯含量的增加,-半径和-半径减小了30%,这与基于刚性带模型的计算结果一致。颈部半径也随着成分的增加而减小,表明费米表面在20% Pd左右脱离布里渊带的六边形面,但在较高的成分下仍向该方向凸起。在15和19% Pd下,有序态和无序态的相关曲线没有明显变化。在此基础上,讨论了Cu - 3pd附近长周期有序结构稳定化的原因。
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引用次数: 8
Phase-Transition Pressures of Fe_3O_4 and GaAs Determined from Shock-Compression Experiments(Physics) 冲击压缩实验测定Fe_3O_4和GaAs的相变压力(物理)
Y. Syono, T. Goto, Y. Nakagawa
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引用次数: 29
High Magnetic Permeability Amorphous Alloys of the Fe-Ni-Si-B System(Metallurgy) Fe-Ni-Si-B系高磁导率非晶合金(冶金)
T. Masumoto, K. Watanabe, M. Mitera, S. Ohnuma
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引用次数: 6
Diffusion of Hydrogen at High Temperatures in the Group V Transition Metals and Alloying Effect on the Diffusion(Metallurgy) 氢在V族过渡金属中的高温扩散及其合金化效应(冶金学)
M. Tokiwai, S. Morozumi
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引用次数: 24
Recovery of Lattice Defects in Cementite in Cold-Rolled Carbon Steels(Metallurgy) 冷轧碳钢渗碳体晶格缺陷的修复(冶金)
A. Inoue, T. Ogura, T. Masumoto
Transmission electron microscopic observations were made on the recovery process of lattice defects in cementite in high carbon steels annealed after 92%cold rolling. Thermomagnetic and X-ray analyses were also performed as additional examinations. No observable change in the defect structure of cementite occurs at temperatures below about 400°C.Annealing at higher temperatures results in the disappearance of the moirc pattern, a considerable decrease of dislocation density and the formation of well-developed subboundaries. Above about 600°C, these defects disappear gradually with the progress of spheroidization. These results suggest that the recovery of lattice defects in cementite is caused by polygonization accompanied by climbing or cross slipping of dislocations.
对高碳钢经92%冷轧后退火后渗碳体中晶格缺陷的恢复过程进行了透射电镜观察。热磁和x射线分析也作为附加检查。当温度低于400℃时,渗碳体的缺陷结构没有明显变化。高温退火导致莫尔纹图案消失,位错密度显著降低,形成发育良好的亚边界。在600℃以上,随着球化的进行,这些缺陷逐渐消失。这些结果表明,渗碳体中晶格缺陷的恢复是由多角化引起的,同时伴有位错的爬升或交叉滑移。
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引用次数: 4
High Corrosion Resistance of Chromium-Bearing Amorphous Iron Alloys in Neutral and Acidic Solutions Containing Chloride 含铬非晶铁合金在含氯化物的中性和酸性溶液中的高耐蚀性
M. Naka, K. Hashimoto, T. Masumoto
Abstract The corrosion resistance of amorphous iron alloys, whose practical application is expected because of their outstanding mechanical properties, has been studied by total immersion tests and...
非晶铁合金具有优异的力学性能,有望在实际应用中得到广泛应用。
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引用次数: 129
High Permeability Properties of Amorphous Co-Fe Base Alloys 非晶态Co-Fe基合金的高导磁性能
H. Fujimori, K. Arai, Hisanori Shirae, H. Saito, T. Masumoto, N. Tsuya
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引用次数: 4
Amorphous Phase in Yttrium-Cobalt-Boron System 钇-钴-硼体系中的非晶相
S. Yajima, K. Okamura, T. Shishido
By rapid quenching of the melt, an amorphous phase of yttrium-cobalt-boron system was obtained. The phase is stable at room temperature, and its crystallization takes place in the vicinity of 700°C on heating at 10°C/min. Electrical resistivity of the amorphous phase is constant at about 10−3Ωcm in the temperature range below 660°C; the variation in the resistivity with the transition from the amorphous to the equilibrium state was measured.
通过快速淬火,得到了钇-钴-硼体系的非晶相。该相在室温下是稳定的,在10℃/min加热时,其结晶发生在700℃附近。在660℃以下的温度范围内,非晶相的电阻率恒定在10−3Ωcm左右;测量了电阻率随非晶态向平衡态转变的变化。
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引用次数: 3
期刊
Science reports of the Research Institutes, Tohoku University. Ser. A, Physics, chemistry and metallurgy
全部 Acc. Chem. Res. ACS Applied Bio Materials ACS Appl. Electron. Mater. ACS Appl. Energy Mater. ACS Appl. Mater. Interfaces ACS Appl. Nano Mater. ACS Appl. Polym. Mater. ACS BIOMATER-SCI ENG ACS Catal. ACS Cent. Sci. ACS Chem. Biol. ACS Chemical Health & Safety ACS Chem. Neurosci. ACS Comb. Sci. ACS Earth Space Chem. ACS Energy Lett. ACS Infect. Dis. ACS Macro Lett. ACS Mater. Lett. ACS Med. Chem. Lett. ACS Nano ACS Omega ACS Photonics ACS Sens. ACS Sustainable Chem. Eng. ACS Synth. Biol. Anal. Chem. BIOCHEMISTRY-US Bioconjugate Chem. BIOMACROMOLECULES Chem. Res. Toxicol. Chem. Rev. Chem. Mater. CRYST GROWTH DES ENERG FUEL Environ. Sci. Technol. Environ. Sci. Technol. Lett. Eur. J. Inorg. Chem. IND ENG CHEM RES Inorg. Chem. J. Agric. Food. Chem. J. Chem. Eng. Data J. Chem. Educ. J. Chem. Inf. Model. J. Chem. Theory Comput. J. Med. Chem. J. Nat. Prod. J PROTEOME RES J. Am. Chem. Soc. LANGMUIR MACROMOLECULES Mol. Pharmaceutics Nano Lett. Org. Lett. ORG PROCESS RES DEV ORGANOMETALLICS J. Org. Chem. J. Phys. Chem. J. Phys. Chem. A J. Phys. Chem. B J. Phys. Chem. C J. Phys. Chem. Lett. Analyst Anal. Methods Biomater. Sci. Catal. Sci. Technol. Chem. Commun. Chem. Soc. Rev. CHEM EDUC RES PRACT CRYSTENGCOMM Dalton Trans. Energy Environ. Sci. ENVIRON SCI-NANO ENVIRON SCI-PROC IMP ENVIRON SCI-WAT RES Faraday Discuss. Food Funct. Green Chem. Inorg. Chem. Front. Integr. Biol. J. Anal. At. Spectrom. J. Mater. Chem. A J. Mater. Chem. B J. Mater. Chem. C Lab Chip Mater. Chem. Front. Mater. Horiz. MEDCHEMCOMM Metallomics Mol. Biosyst. Mol. Syst. Des. Eng. Nanoscale Nanoscale Horiz. Nat. Prod. Rep. New J. Chem. Org. Biomol. Chem. Org. Chem. Front. PHOTOCH PHOTOBIO SCI PCCP Polym. Chem.
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