共查询到19条相似文献,搜索用时 203 毫秒
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为掌握浮顶油罐内的温度分布,提高加热效率,进行了浮顶油罐内原油加热过程的传热研究。以某2×10~4m~3的单盘浮顶罐为例,基于对浮顶罐加热过程的分析,结合传热学理论,建立了单盘浮顶油罐二维加热模型,应用FLUENT软件对原油加热过程与流动进行了仿真模拟,得到了原油不同加热时间后的温度分布以及原油流场分布,结果表明:原油加热过程中由于自然对流,在浮顶罐内产生漩涡,在罐壁底部流速较低;浮顶罐中心区域内原油温度分布均匀,加热管、罐壁和浮顶下部温度较高。 相似文献
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用最小二乘法回归罐壁温度计算公式 总被引:1,自引:0,他引:1
一、概述在大容量计量中,对立式非保温金属油罐进行计量的最后结果应是标准温度20℃时的值。因此,在实际计量中应将油罐在某一温度t℃下的值换算到20℃时的值。但油罐的罐壁温度由于设备本身等限制,很难直接测得。罐壁温度主要是由罐内油品温度和罐外大气温度所决定,故通常是通过这两个温度推算得到罐壁温度。到目前为止,国内外尚未能得出罐壁温度 相似文献
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采用频域回归法(FDRM)计算4种船舶围壁的动态传热特性,并分析空气层对船舶围壁动态传热及舱室热环境的影响。计算结果表明:空气层对船舶围壁的传热有明显的阻隔作用,且空气层越厚阻隔作用越明显;船舶围壁空气层与保温层的排列次序对围壁传热有一定的影响,空气层在外、保温层在内的排列方式隔热效果更好,内壁温度波动小。 相似文献
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目的 为了分析液氨储罐纯液体泄漏后的事故影响,探究液氨纯液体泄漏量的计算.方法 针对液氨储罐(卧罐、球罐及立式罐)液体泄漏罐压变化及不同类型储罐结构特征导致液面面积变化的特点,利用范德瓦尔斯方程和流体力学方法,建立液氨储罐液体泄漏模型.利用模型对3种液氨储罐液体泄漏进行数值模拟,对比PHAST计算与模型模拟结果.结论 结果发现液面高度hv,s,h的下降呈现先减缓后增大的趋势,泄漏质量流率Qm-v,s,h的下降幅度及泄漏质量mv,s,h呈现先增加后减缓的趋势.泄漏初始时刻,Qm-v,s,h值最大,分别为0.555,0.553,0.552 kg/s;泄漏停止时,mv,s,h值最大,分别为11.245846,11.084621,7.730932 t.模型计算结果与PHAST模拟结果规律相似,Qm-v,s,h(max)的偏差较小,介于16.577%~16.667%;mv,s,h偏差差别较大,立式罐、球罐及卧罐泄漏液体质量偏差分别为4.565%,5.764%和17.630%.结论 根据各参数的变化规律可得,模型适于计算液氨储罐液体泄漏及风险分析. 相似文献
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在低质量流速条件下,对垂直上升光管内汽水两相流动沸腾传热特性进行了系统的实验研究.实验段采用了Φ22mm×2.5mm的1Cr18Ni9Ti不锈钢管.实验条件为压力p =10~21MPa,管内质量流速G=448 ~ 1233kg/(m2·s),内壁热流密度q =130~541kW/m2.实验得到了不同工况下垂直上升光管的壁温分布特性.分析了压力、热负荷和质量流速变化对光管传热特性的影响,探讨了传热恶化的发生机理,并给出了能用于工程实际的传热实验关联式.结果表明:在亚临界及近临界压力区,垂直上升光管通常会发生两类传热恶化:膜态沸腾和干涸.压力与热负荷的增大以及质量流速的减小,均会导致传热恶化提前发生和传热恶化后的壁温飞升值增大.与亚临界区相比,光管在近临界区的传热特性变差,发生传热恶化的临界干度下降,甚至在过冷区就发生壁温飞升. 相似文献
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Simulation Research of Vaporization and Pressure Variation in a Cryogenic Propellant Tank at the Launch Site 总被引:4,自引:0,他引:4
In order to improve depiction of pressure variation and investigate the interrelation among the physical processes in propellant tanks, a 2D axial symmetry Volume-of-Fluid (VOF) CFD model is established to simulate a large-sized liquid propellant tank when the rocket is preparing for launch with propellant loaded at the launch site. The numerical model is considered with propellant free convection, heat transfer between the tank and the external environment, thermal exchange between propellant and inner tank wall surfaces, gas compressibility, and phase change modeled under the assumption of thermodynamic equilibrium. Vaporization rate of the vented LH2 tank and prediction of pressure change in the tank pressurized with GHe are obtained through simulation. We analysis the distributions of phase, temperature, and velocity vectors to reveal interactions among the propellant’s own convection motion, heat transfer and phase change. The results show that the vaporization rate is mainly affected by heat leaks though the tank wall when the tank is vented, but it does not completely accord with the trend of the leakage because of convection motion and temperature nonuniformity of the liquid propellant in the tank. We also find that the main factors on pressure variation in the pressurized tank are the heat transfer on the tank wall surface bonding the ullage and propellant vaporization which has comparatively less influence. 相似文献
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《低温学》2015
Sufficient knowledge of thermal performance and pressurization behaviors in cryogenic tanks during rocket launching period is of importance to the design and optimization of a pressurization system. In this paper, ground experiments with liquid oxygen (LO2) as the cryogenic propellant, high-temperature helium exceeding 600 K as the pressurant gas, and radial diffuser and anti-cone diffuser respectively at the tank inlet were performed. The pressurant gas requirements, axial and radial temperature distributions, and energy distributions inside the propellant tank were obtained and analyzed to evaluate the comprehensive performance of the pressurization system. It was found that the pressurization system with high-temperature helium as the pressurant gas could work well that the tank pressure was controlled within a specified range and a stable discharging liquid rate was achieved. For the radial diffuser case, the injected gas had a direct impact on the tank inner wall. The severe gas-wall heat transfer resulted in about 59% of the total input energy absorbed by the tank wall. For the pressurization case with anti-cone diffuser, the direct impact of high-temperature gas flowing toward the liquid surface resulted in a greater deal of energy transferred to the liquid propellant, and the percentage even reached up to 38%. Moreover, both of the two cases showed that the proportion of energy left in ullage to the total input energy was quite small, and the percentage was only about 22–24%. This may indicate that a more efficient diffuser should be developed to improve the pressurization effect. Generally, the present experimental results are beneficial to the design and optimization of the pressurization system with high-temperature gas supplying the pressurization effect. 相似文献
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低温推进剂贮箱增压过程的传热传质数学模拟 总被引:1,自引:0,他引:1
针对火箭发动机地面试验中低温液氧贮箱的预增压和增压过程建立了气相空间的传热、传质数学模型.运用实际气体的状态方程、连续性方程、能量守恒方程以及推进剂与气相空间的传热、传质方程等组成了关于气相空间参数的微分方程组,并运用四阶Runge-Kutta算法对其进行求解.获得了气相空间的压力、温度、增压气体流量、液氧挥发速率以及贮箱壁温等参数的变化规律.结果表明,在发动机启动前的预增压过程中,气相空间的温度和压力急剧增加,液氧的挥发速率也增加很快;发动机启动后的保持增压阶段,由于气相空间的体积不断发生变化,气相空间参数的变化趋于平缓,液氧表面向气相空间的传质速率也趋于稳定. 相似文献
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This paper presents a study on fluid flow and heat transfer of liquid hydrogen in a zero boil-off cryogenic storage tank in a microgravity environment. The storage tank is equipped with an active cooling system consisting of a heat pipe and a pump–nozzle unit. The pump collects cryogen at its inlet and discharges it through its nozzle onto the evaporator section of the heat pipe in order to prevent the cryogen from boiling off due to the heat leaking through the tank wall from the surroundings. A three-dimensional (3-D) finite element model is employed in a set of numerical simulations to solve for velocity and temperature fields of liquid hydrogen in steady state. Complex structures of 3-D velocity and temperature distributions determined from the model are presented. Simulations with an axisymmetric model were also performed for comparison. Parametric study results from both models predict that as the speed of the cryogenic fluid discharged from the nozzle increases, the mean or bulk cryogenic fluid speed increases linearly and the maximum temperature within the cryogenic fluid decreases. 相似文献