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本文运用FLUENT软件,通过大量的计算机模拟,研究了真空高压气淬炉中淬火气体压力、进口速度、气体类型对工件冷却性能的影响.通过对比氮气在0.45 MPa、0.6 MPa、1.0 MPa和1.5 MPa淬火压力下工件的冷却速度,量化了淬火压力对工件冷却速度的影响程度.氮气在0.6 MPa下,将气体速度由40 m/s增至60m/s,工件冷却速度提高27%,但风机功率增加3.4倍.由于气体体积流量一定的情况下,淬火气体比热和密度的协同影响了换热系数的大小,通过计算机模拟了四种淬火气体氢气、氦气、氮气和氩气对工件冷却速度的影响,得出在相同气体压力和流量下,四种气体的冷却能力是:氮气>氢气>氦气>氩气;在消耗相同的风机功率下,密度小比热大的气体冷却能力高,四种气体的冷却能力依次是氢气>氦气>氮气>氩气. 相似文献
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(上接2006年第6期第63页)热态真空度又称工作真空度,是指从开始加热到充气冷却这段时间的炉内真空度,这是由于加热时,零件、夹具要析出气体;使用膏状钎料时粘结剂要挥发。这些因素都会不同程度地引起冷态真空度的降低。但是在钎焊温度下,要求炉内真空度基本恢复到冷态真空度,通常是采用适当延长稳定时间的方法来实现的。如果钎料中含有蒸气压较高的合金元素,为了防止合金元素大量挥发而污染炉膛,这时热态真空度与冷态真空度相差较大。例如用铜基钎料时,因为铜在940℃时的蒸气压为1Pa, 相似文献
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通过在H363炉中测试冷却过程曲线,研究气体在真空炉内热变换规律,并比较不同压力及空冷,油冷冷却速度,掌握了H3636炉冷却能力与压力的关系,对今后生产,研究起到指导作用。 相似文献
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采用直接模拟蒙特卡罗方法对过渡流态下盘型分子泵的抽气特性进行了模拟研究,并讨论了盘型分子泵通道几何参数对流动特性的影响.指出了通过改变泵的尺寸参数提高抽气系数的途径.最后,进行了实验研究和模拟研究结果的对比,证明模拟计算结果在允许的误差范围内. 相似文献
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目的针对集装箱供需矛盾的日益突出,以及空重箱长期独立运输等问题,研究空重箱的协同运输过程,以减少运输资源的浪费。方法在使用折叠式集装箱的情况下,为实现门到门的高效服务,以运输公司总利润最大为目标,建立空重箱协同运输优化模型,并通过LINGO建模求解具体算例。结果通过算例分析,验证了模型的可行性,并与是否使用折叠式集装箱、是否考虑空重箱协同运输等多种模式进行对比。结果发现,在一定条件下相对于传统的运输模式,平均运力利用率提高了15.23%。结论验证了使用折叠式集装箱的空重箱协同运输的经济效益高于其他运输模式。 相似文献
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M. Brzoza E. Specht J. Ohland O. Belkessam Th. Lübben U. Fritsching 《Materialwissenschaft und Werkstofftechnik》2006,37(1):97-102
A coupled gas‐dynamical and thermo‐mechanical model for simulation of the gas flow, gas and specimen temperature, phase, stress, strain, and displacement transient‐fields during quenching of cutting discs and shafts of steel is introduced. The material properties (e. g. density, conductivity, heat capacity, hardness) are obtained by homogenization procedures. The material behaviour is described as an extension of the classical J2‐plasticity theory with the extension of temperature and phase fraction dependent yield criteria. The coupling effects such as dissipation, phase transformation enthalpy, and transformation induced plasticity (TRIP) are considered. Simulations were carried out for cutting discs of knives, and for shafts made of steel SAE 52100 with varying diameter. For the validation of the simulations, these work pieces were heated in a roller hearth kiln up to 850 °C, and than quenched in a field of nozzles in which the heat transfer coefficient was known and could be locally adjusted by the volume flow of each nozzle. The phase fractions, surface hardness, distortion, and residual stresses were measured. The simulated and measured results fit quite well. According to optimization‐simulations the shafts were quenched with a certain heat transfer coefficient distribution. The bigger diameter parts of the shaft were more intensively quenched by an increased gas flow so that the hardness profiles were equalized and the residual stresses at the edges were significantly reduced. 相似文献
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S. Luki? B. BornscheinL. Bornschein G. DrexlinA. Kosmider K. SchlösserA. Windberger 《Vacuum》2012,86(8):1126-1133
The gas-flow reduction factor of the second forward Differential Pumping Section (DPS2-F) for the KATRIN experiment was determined using a dedicated vacuum-measurement setup and by detailed molecular-flow simulation of the DPS2-F beam tube and of the measurement apparatus. In the measurement, non-radioactive test gases deuterium, helium, neon, argon and krypton were used, the input gas flow was provided by a commercial mass-flow controller, and the output flow was measured using a residual gas analyzer, in order to distinguish it from the outgassing background. The measured reduction factor with the empty beam tube at room temperature for gases with mass 4 is 1.8(4) × 104, which is in excellent agreement with the simulated value of 1.6 × 104. The simulated reduction factor for tritium, based on the interpolated value for the capture factor at the turbo-molecular pump inlet flange is 2.5 × 104. The difference with respect to the design value of 1 × 105 is due to the modifications in the beam tube geometry since the initial design, and can be partly recovered by reduction of the effective beam tube diameter. 相似文献
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An inductively coupled plasma (ICP) is analyzed by means of experiments and numerical simulation. Important plasma properties are analyzed, namely, the effective temperature inside the central channel and the mean flow velocity inside the plasma. Furthermore, the effect of torches with different injector diameters is studied by the model. The temperature inside the central channel is determined from the end-on collected line-to-background ratio in dependence of the injector gas flow rates. Within the limits of 3% deviation, the results of the simulation and the experiments are in good agreement in the range of flow rates relevant for the analysis of relatively large droplets, i.e., ~50 μm. The deviation increases for higher gas flow rates but stays below 6% for all flow rates studied. The velocity of the gas inside the coil region was determined by side-on analyte emission measurements with single monodisperse droplet introduction and by the analysis of the injector gas path lines in the simulation. In the downstream region significantly higher velocities were found than in the upstream region in both the simulation and the experiment. The quantitative values show good agreement in the downstream region. In the upstream region, deviations were found in the absolute values which can be attributed to the flow conditions in that region and because the methods used for velocity determination are not fully consistent. Eddy structures are found in the simulated flow lines. These affect strongly the way taken by the path lines of the injector gas and they can explain the very long analytical signals found in the experiments at low flow rates. Simulations were performed for different injector diameters in order to find conditions where good analyte transport and optimum signals can be expected. The results clearly show the existence of a transition flow rate which marks the lower limit for effective analyte transport conditions through the plasma. A rule-of-thumb equation was extracted from the results from which the transition flow rate can be estimated for different injector diameters and different injector gas compositions. 相似文献
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类金刚石膜(Diamond-like Carbon,DLC)具有优异的气体阻隔性能.在PET瓶体内表面制备DLC阻隔涂层时,阻隔涂层的均匀性会受到瓶体内流场结构(气压分布、速度分布等)的显著影响.本文应用格子波耳兹曼方法(Lattice Boltzmann Method/Model,LBM)对PET瓶体内制备DLC阻隔涂层时的流场结构进行模拟,研究了送气速度、气体运动粘度系数和装置结构变化时瓶体内部流场结构的变化.研究结果表明,降低进气速度和提高气体运动粘度系数有利于减弱回流而获得层流结构;装置结构的调整能够改变瓶体内的流场结构,采用恰当的异型装置可以获得较理想的流场结构,对实验工作具有一定的指导意义. 相似文献
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针对水流量标准装置中横板型稳压罐,基于Navier-Stokes方程建立罐体计算流体动力学仿真模型。使用湍流模型、流体体积函数瞬态模型和有限体积法进行离散,并在近壁区采用标准的壁面函数法进行修正,完成横板型稳压罐内部两相流场的数值模拟。数值结果显示空罐充水流态依次经过无水状态-射流-上壅-漫流-稳定状态,同时形成掺气现象和泡状流;气液体积比1:3情况下,满罐充水流场有固定周期的晃荡现象,上侧形成逆时针转动的漩涡气腔,流场湍流粘度较小,分布较均匀,稳定效果最好。 相似文献
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RH真空精炼吹氩参数对循环流动影响的数值分析 总被引:1,自引:1,他引:0
为研究RH真空脱气过程中的流动行为,建立了描述气泡驱动下的RH循环气-液两相流动的数学模型.基于欧拉-欧拉两流体模型,利用计算流体力学(CFD)商业软件FLUENT6.0,对不同充气量条件下的循环流量进行了预测.计算结果与实验数据的比较表明两者具有较好的一致性.应用该模型对充气压强与循环流量、充气量与上升管内气相及液相速度分布关系进行了数值模拟,用以理解其中的流动规律,为工程技术改进提供参考. 相似文献