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使用激光多谱勒测速仪研究管式反应器中的湍动规律 被引量:1
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作者 陈国 刘代俊 +1 位作者 梁斌 应建康 《四川大学学报(工程科学版)》 EI CAS CSCD 2002年第2期124-126,共3页
采用激光多谱勒测速仪 (LaserDopplerAnemometer)测定一种生产磷铵的管式反应器中流点的velocity -arriv etime序列 ,通过对这一序列的分析 ,研究了管式反应器流向截面上表征流体湍动程度的均方根脉动速度和湍动度的分布情况 ,实验表明... 采用激光多谱勒测速仪 (LaserDopplerAnemometer)测定一种生产磷铵的管式反应器中流点的velocity -arriv etime序列 ,通过对这一序列的分析 ,研究了管式反应器流向截面上表征流体湍动程度的均方根脉动速度和湍动度的分布情况 ,实验表明均方根脉动速度和湍动度在径向上呈现抛物线分布 ,均方根脉动速度随Re呈线形变化 ,而湍动度随雷诺数呈抛物线变化。均方根脉动速度在管式反应器中的分布为u′r2 =kRe +R(r2 ,Rer) =k(DUρ/ μ) +R(r2 ,Rer) ,Re >2 0 0 0。 展开更多
关键词 管式反应器 湍动度分布 LDA 激光多普勒测速仪 规律
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旋流燃烧器冷态模化试验研究 被引量:2
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作者 董永胜 孙保民 +1 位作者 初燕 郭永红 《现代电力》 2006年第3期36-40,共5页
以石嘴山电厂旋流燃烧器为研究对象,分析其存在的在底灰中含有大量未燃尽黑色块状物(约占底灰的10%)这一问题,通过分析石嘴山电厂旋流燃烧器本身结构特点发现在稳燃环处存在台阶结构,在台阶处易造成煤粉热解堆积,这是造成可燃物损失大... 以石嘴山电厂旋流燃烧器为研究对象,分析其存在的在底灰中含有大量未燃尽黑色块状物(约占底灰的10%)这一问题,通过分析石嘴山电厂旋流燃烧器本身结构特点发现在稳燃环处存在台阶结构,在台阶处易造成煤粉热解堆积,这是造成可燃物损失大的原因。因此提出了将原有稳燃环结构改造成稳燃齿结构,从而降低煤粉在稳燃环的台阶处的堆积,加强扰动和输运能力,强化着火和燃烧。依据冷态相似模化的原理搭建气固两相流冷态实验台,利用试验台分别对原有旋流燃烧器模型和3种改进的燃烧器模型进行气相试验。通过对原有旋流燃烧器模型和改进燃烧器模型的一次风气相冷态空气动力场湍动度和时均速度的研究,对3种改造方案及其原有稳燃环进行比较分析,提出了改进的最佳方案。 展开更多
关键词 热能工程 旋流燃烧器 湍动度 冷态模化试验 时均速
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Turbulent boundary layers and hydrodynamic flow analysis of nanofluids over a plate 被引量:4
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作者 AOUINET Hana DHAHRI Maher +2 位作者 SAFAEI Mohammad Reza SAMMOUDA Habib ANQI Ali E. 《Journal of Central South University》 SCIE EI CAS CSCD 2021年第11期3340-3353,共14页
A numerical analysis of the log-law behavior for the turbulent boundary layer of a wall-bounded flow is performed over a flat plate immersed in three nanofluids(Zn O-water,SiO_(2)-water,TiO_(2)-water).Numerical simula... A numerical analysis of the log-law behavior for the turbulent boundary layer of a wall-bounded flow is performed over a flat plate immersed in three nanofluids(Zn O-water,SiO_(2)-water,TiO_(2)-water).Numerical simulations using CFD code are employed to investigate the boundary layer and the hydrodynamic flow.To validate the current numerical model,measurement points from published works were used,and the compared results were in good compliance.Simulations were carried out for the velocity series of 0.04,0.4 and 4 m/s and nanoparticle concentrations0.1% and 5%.The influence of nanoparticles’ concentration on velocity,temperature profiles,wall shear stress,and turbulent intensity was investigated.The obtained results showed that the viscous sub-layer,the buffer layer,and the loglaw layer along the potential-flow layer could be analyzed based on their curving quality in the regions which have just a single wall distance.It was seen that the viscous sub-layer is the biggest area in comparison with other areas.Alternatively,the section where the temperature changes considerably correspond to the thermal boundary layer’s thickness goes a downward trend when the velocity decreases.The thermal boundary layer gets deep away from the leading edge.However,a rise in the volume fraction of nanoparticles indicated a minor impact on the shear stress developed in the wall.In all cases,the thickness of the boundary layer undergoes a downward trend as the velocity increases,whereas increasing the nanoparticle concentrations would enhance the thickness.More precisely,the log layer is closed with log law,and it is minimal between Y^(+)=50 and Y^(+)=95.The temperature for nanoparticle concentration φ=5%is higher than that for φ=0.1%,in boundary layers,for all studied nanofluids.However,it is established that the behavior is inverted from the value of Y^(+)=1 and the temperature for φ =0.1% is more important than the case of φ =5%.For turbulence intensity peak,this peak exists at Y^(+)=100 for v=4 m/s,Y^(+)=10 for v=0.4 m/s and Y^(+)=8 for v=0.04 m/s. 展开更多
关键词 turbulent boundary layers nanofluids hydrodynamic flow wall shear stress turbulent intensity
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