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1.
摇摆运动条件下自然循环复合型脉动的实验研究   总被引:1,自引:1,他引:0  
对摇摆运动条件下的自然循环两相流动不稳定性进行实验研究。实验结果表明:摇摆运动造成的两相流动不稳定性(波谷型两相流动不稳定性)和密度波型脉动相互叠加形成复合型脉动,加剧了系统的两相流动不稳定性。复合型脉动分为不规则的复合型脉动和规则的复合型脉动两部分,复合型脉动仅发生在高欠热度区域。规则的复合型脉动发生边界与相同热工水力参数下的密度波型脉动边界接近且受摇摆参数影响较小。  相似文献   

2.
基于最大Lyapunov指数(λ)对摇摆运动下压降型脉动(PDO)的混沌演化行为进行了实验研究和混沌演化特性分析。研究认为其混沌演化路径可分为3个阶段:热工水力稳定区、频率锁定振荡区和脱离摇摆影响区,并对每个阶段热工水力原理和混沌性特征及成因进行了分析。热工水力稳定区不产生PDO,呈高随机性低振幅轻微振荡。频率锁定振荡区中,PDO周期被迫与摇摆周期保持一致,呈不规则的拟周期运动,λ显著增大。脱离摇摆影响区中PDO产生倒流并以固有频率进行振荡。λ达到极大值,表现出强烈的混沌特性。   相似文献   

3.
针对摇摆条件下自然循环波谷型脉动进行研究,构建了计算波谷型脉动的模型并进行了分析,计算结果和实验值符合较好。分析结果表明:对于摇摆运动下的波谷型脉动,在其整体流动波动过程中起主导作用的是摇摆运动引起的附加压降,而在波谷附近,由于产汽的影响,局部摩擦压降和重位压降交替主导流动,并最终诱发波谷处的流动不稳定性;摇摆振幅和频率越大,即摇摆程度越剧烈时,摇摆附加压降波动越剧烈,流量、壁温等热工参数变化越剧烈,波谷型脉动起始点对应功率也越低。  相似文献   

4.
摇摆运动引起的波动与自然循环密度波型脉动的叠加   总被引:4,自引:1,他引:3  
针对海洋条件(即摇摆工况)下.核动力装置自然循环流动不稳定的特点进行了实验研究结果表明,摇摆引起的流量波动的附加量与自然循环密度波型脉动的流量脉动相叠加.加剧了系统的不稳定.通过频谱分析,分析了叠加效应的强弱。  相似文献   

5.
摇摆运动对自然循环流动不稳定性的影响   总被引:1,自引:0,他引:1  
分析研究了摇摆运动下的自然循环流动不稳定性和摇摆对不稳定性的类型以及不稳定性起始点的影响.结果表明,摇摆使流动不稳定性提前发生,改变了不稳定性的类型,摇摆引起的波动和密度波型脉动发生叠加.摇摆运动下自然循环存在两个稳定区域,在这两个区域中间包含着不稳定区域.  相似文献   

6.
一回路设备在设计时需考虑压力脉动的影响,而在海洋条件下,船体的运动会影响压力脉动,因此需要考虑海洋条件对压力脉动的影响。本文建立了海洋条件下的附加惯性力模型,通过自定义函数将该模型应用于Fluent求解器中,采用大涡数值模拟方法对细长管道进行数值计算,得到不同摇摆频率及雷诺数下的流场结果,并对监测点进行时域与频域分析,获取到监测点处的压力均方根及功率谱密度曲线。分析结果表明:在湍流充分发展区,压力脉动量相对于平均压力而言为小值;湍流压力脉动随着船体摇摆频率/雷诺数的增加而增加;随着雷诺数的增加,其对湍流压力脉动的影响减小,但摇摆条件增大了雷诺数对压力脉动的影响。  相似文献   

7.
采用理论分析与RELAP5/MC程序计算相结合的方法,研究了非对称加热条件下摇摆运动对并联双通道管间脉动特性的影响。结果表明,摇摆运动会引起周期等于摇摆周期以及1/2摇摆周期的流量波动,当摇摆引起的流量波动周期与系统固有热工水力振荡周期接近时,会发生共振效应,从而使密度波振荡提前发生。增大摇摆幅度及通道到摇摆中心的距离可增强流量波动幅度,降低系统稳定性。  相似文献   

8.
对摇摆条件下的单相强迫循环流量脉动特性进行实验研究,并通过受力分析研究影响流量脉动的主要因素。研究表明:摇摆运动能否造成强迫循环流量出现周期性的脉动主要取决于泵驱动压头与附加惯性力的相对大小。摇摆幅度或频率越大,流量脉动幅度越大;循环泵驱动压头越大,流量脉动幅度越小;当驱动压头与附加惯性力的比值达到一定值后,摇摆运动发生前后流量不再出现明显变化。  相似文献   

9.
对摇摆条件下的单相强迫循环流量脉动特性进行实验研究,并通过受力分析研究影响流量脉动的主要因素.研究表明:摇摆运动能否造成强迫循环流量出现周期性的脉动主要取决于泵驱动压头与附加惯性力的相对大小.摇摆幅度或频率越大,流量脉动幅度越大;循环泵驱动压头越大,流量脉动幅度越小;当驱动压头与附加惯性力的比值达到一定值后,摇摆运动发生前后流量不再出现明显变化.  相似文献   

10.
多管平行通道流动不稳定性类型试验研究   总被引:4,自引:0,他引:4  
针对由 7根双层套管单管组成的多管平行通道流动不稳定性试验段 ,进行了流动不稳定性类型试验 ,结果表明 ,试验段的管间脉动主要表现为密度波脉动、不规则脉动和热力型脉动 3类 ,与单通道流动不稳定性、两管平行通道管间脉动 ,均有明显的区别  相似文献   

11.
Two-phase flow instability of natural circulation under a rolling motion condition is experimentally studied. The experimental results show the rolling motion induces a fluid flow fluctuation. At the trough point of the flow fluctuation, rolling motion can cause the early occurrence of natural circulation two-phase flow instability, and this case is defined as trough-type flow oscillation. The system stability decreases with increasing rolling amplitude and effect of rolling frequency is nonlinear. The complex overlap effect of trough-type flow oscillation and density wave oscillation can enhance the system coolant fluctuation; this case is defined as complex flow oscillation. Complex flow oscillation may be divided into two types: regular and irregular complex flow oscillations. Irregular complex flow oscillation is a transition type from trough-type flow oscillation to regular complex flow oscillation. Under the same thermal hydraulic conditions, the marginal stability boundary (MSB) of regular complex flow oscillation is similar to that of density wave oscillation without rolling motion, and the influences of rolling parameters on the MSB are slight.  相似文献   

12.
The local loss coefficient for a 90° bend in rolling motion is investigated with CFD code FLUENT. The calculation results are validated with experimental and theoretical results in steady state. The effect of spanwise and transverse additional forces on the bend loss is significant. The effects of additional forces on the bend loss are mainly embodied in the downstream section. The oscillation of bend loss caused by the spanwise and transverse additional forces is very regular while that caused by velocity oscillation is very irregular. The effect of velocity oscillation on the bend loss is significant in rolling motion with low Reynolds number. But the variation of bend loss coefficient with velocity oscillating period is very limited.  相似文献   

13.
Natural circulation is widely used in nuclear reactor systems as the passive safety system. With the development of the floating nuclear power plant (FNPP), researchers should pay more attention to flow and heat transfer characteristics for the natural circulation under ocean conditions for the safety of FNPP. In this paper, the flow characteristics in a single-phase natural circulation system were investigated and the effects of heaving, rolling and coupled motions were analyzed. The oscillation amplitude of flow rate increases with the increase of period in a certain range and maximum acceleration under heaving motions. With the increase of oscillation intensity (higher frequency and larger maximum rolling angle), the oscillation amplitude increases and the average flow rate decreases under rolling motions. Moreover, the lateral displacement of rolling center changes the oscillation period and induces larger amplitude oscillations. The flow characteristic becomes more complex when the system is subjected to coupled motions. The oscillation period is the least common multiple of two motions’ periods. The oscillation induced by coupled motions makes the system more unstable than that induced by an individual motion. The potential superposition effect exists under coupled motions and needs to be addressed for the operation safety.  相似文献   

14.
In ocean environment, the ship motion significantly affects the natural circulation behavior in ship-based integrated-type reactor. This paper theoretically and experimentally investigated natural circulation characteristics in symmetrical loops under rolling condition. Experiments were carried out on a test loop with a symmetrical configuration by simulating the structure of an accrual reactor. The theoretical results revealed that only angular acceleration contributes to the resultant force under zero power rolling condition. In a closed circuit with a uniform cross-section area, the angular acceleration force integral is proportional to the angular acceleration and the area enclosed by the circuit. The integral value varies over time and causes flow oscillations. However, the angular acceleration force does not influence the flow status in the shared part of the two symmetrical neighbor circuits due to force interactions. Rolling experiments with a zero power load confirmed these results. Full power experiments under rolling condition exhibited observable flow rate and temperature oscillations in each branch of the flow channel. The oscillations in the side flow channels had the same values for both the period and the phase with the variation of rolling angle. The angular acceleration force was the main cause of this. The oscillations in the middle channel had a period half the value of the rolling period. The periodical variation of the vertical component of gravity caused this. The horizontal component of gravity was out-phasing with angular acceleration. Therefore, it alleviated oscillation in the side channels. The experimental results showed that for the same rolling period, as the rolling angle increased, the average flow rate decreased and oscillation amplitudes increased. Also, as the power load increased, the oscillations in the middle channel increased and the oscillation in the side channel decreased.  相似文献   

15.
针对摇摆运动下自然循环流动不稳定性的非线性演化特性进行了分析。应用非线性时间序列分析方法对不同流动状态的时间序列进行幅度谱分析、吸引子重构,并基于相空间重构理论,计算包括关联维数(CD)、Kolmogorov熵(K熵)和最大李雅普诺夫指数(MLE)在内的几何不变量的值,根据计算结果分析了摇摆运动下两相自然循环系统流动不稳定性的非线性演化特性。分析结果表明:随着无量纲功率的增大,系统几何不变量的值先增加后减小,系统由极限环运动经倍周期分岔发展成混沌振荡,最终回到稳定流动;系统非线性特征先增强后减弱,是由于热驱动力、流动阻力和摇摆引起的驱迫外力之间的相互反馈及耦合程度不同所致。  相似文献   

16.
The flow in a tight lattice is strongly affected by the quasi-periodic lateral flow pulsations caused by large scale vortices. This kind of large scale vortices is largely responsible for the momentum and heat exchange across the gaps. In rolling motion, the coherent structure and flow oscillation are affected by an additional force. The coherent structure in rolling motion is more significant than that in no rolling motion. The oscillation period in rolling motion is about 10% bigger than that in no rolling motion. The rolling motion can affect the coherent structure. However, the effect of rolling motion on the thermal hydraulic parameters, i.e. wall temperature and bulk temperature, is very limited. The wall temperature and wall shear stress in rolling motion and no rolling motion are nearly the same. The additional force due to rolling motion can change the moving characteristics of coherent structures, but its effect on the turbulent flow and heat transfer is weak.  相似文献   

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