State Primary Standard of the Unit of Liquid Mass Flow Rate

The pressing current problems of increasing the level of the metrological service of instruments for measuring liquid mass flow rate are presented. The action principle, metrological characteristics, results of investigations of the State primary standard of the unit of liquid mass flow rate, and the verification scheme regulating the order of transferring the size of the unit to working measurement standards are presented.     

Assessment of Influence of Flow Diverter on the Metrological Characteristics of Calibration Devices Used for the Units of Mass and Unit of Volume of a Liquid in a Flow and of Mass and Volume Discharges of Liquid

Measurement Techniques - A new approach to the assessment of interfering factors that arise in the process of diversion of a flow of liquid in the weighing device of a calibration device is...     

The Initial Equations and the Equations for Measuring the Mass and Volume Flow Rates of a Gas

A mathematical model of the flow of a gas in Laval nozzles is analyzed. The model is used to obtain equations for measuring the mass and volume flow rates of a gas.__________Translated from Izmeritel’naya Tekhnika, No. 4, pp. 44–48, April, 2005.     

活塞式液体流量标准装置体积校准方法的探讨

对活塞式液体流量标准装置体积校准方法进行了研究,基于理想圆柱体模型建立了活塞装置体积模型,引入修正系数对所建立的体积模型进行修正,并利用质量守恒定律提出采用质量法对活塞装置进行体积校准.对修正系数进行赋值分析和不确定度评定,结果表明5L及以上体积的扩展不确定度优于0.05％.该方法操作简便,可控性好,结果准确可靠.     

高准确度静态质量法液体流量标准装置及其不确定度评价

本文介绍了一种高准确度质量法液体流量标准装置的设计方法,为对市场中出现的高准确度科里奥利质量流量计的量值传递提供了可能。文中介绍了装置设计过程中,为提高装置准确度用到的电动换向、衡器自校准、蒸馏水代替自来水等方法。试验证明,上述方法的应用使装置达到了预期的不确定度水平。文章还着重介绍了高准确度静态质量法液体流量标准装置不确定度的评价要点,对装置的不确定度水平进行了评定。     

科氏质量流量计测量含气液体流量关键技术综述

含气液体流量测量是科氏质量流量计面临的测量难题,对科氏质量流量计的驱动技术、信号处理技术都提出更高的要求.从驱动、信号处理、误差修正这3大核心技术出发对科氏质量流量计测量含气液体流量进行综述,分析含气液体流量下,驱动、信号处理以及误差修正技术的难点,并针对难点总结出含气液体流量下最佳的驱动技术、信号处理技术和误差修正技...     

Fundamental Mass Flow Measurement of Solid Particles

A generic mass flow measurement device was developed as a variation on the theme of counting. In a hypothetical infinitely sparse mass flow, the number of passing particles could be counted in a time frame and multiplied by the mean mass per particle to obtain a mass flow per time unit. In a mass flow of realistic density, however, particles travel in cluster formation and direct counting of individual particles is impossible. If a method could be available that reconstructs the original number of particles in a cluster, the mass flow can be computed for realistic clustered mass flows. This reconstruction algorithm was developed in this research; it uses the measured cluster lengths to reconstruct the total number of particles in each passing cluster. The lengths of the clusters were measured with an optoelectronic device. The reconstruction algorithm was developed using simulation, augmented by clustering theory. For identical diameter particle flow, simulation results showed that the number of particles in a cluster could be reconstructed using a very simple reconstruction formula. This formula uses only the total number of clusters per time frame and the total number of individual particles measured in the same time frame. However, identical diameter flow is not realistic, since even identical particles are measured with a certain error. Reconstruction of the realistic distributed diameter particle flow was approximated using the identical particle method. The optical mass flow sensor has major advantages over traditional methods. It is virtually insensitive to vibrations, contamination, temperature drift, and misalignment and the underlying measurement concept is well understood. But most importantly, the sensor does not require calibration. The mass flow of identical particles (4.5 mm air gun pellets) was measured with an error smaller than 3% even for high density flow rates.     

Fundamental Mass Flow Measurement of Solid Particles

A generic mass flow measurement device was developed as a variation on the theme of counting. In a hypothetical infinitely sparse mass flow, the number of passing particles could be counted in a time frame and multiplied by the mean mass per particle to obtain a mass flow per time unit. In a mass flow of realistic density, however, particles travel in cluster formation and direct counting of individual particles is impossible. If a method could be available that reconstructs the original number of particles in a cluster, the mass flow can be computed for realistic clustered mass flows. This reconstruction algorithm was developed in this research; it uses the measured cluster lengths to reconstruct the total number of particles in each passing cluster. The lengths of the clusters were measured with an optoelectronic device. The reconstruction algorithm was developed using simulation, augmented by clustering theory. For identical diameter particle flow, simulation results showed that the number of particles in a cluster could be reconstructed using a very simple reconstruction formula. This formula uses only the total number of clusters per time frame and the total number of individual particles measured in the same time frame. However, identical diameter flow is not realistic, since even identical particles are measured with a certain error. Reconstruction of the realistic distributed diameter particle flow was approximated using the identical particle method. The optical mass flow sensor has major advantages over traditional methods. It is virtually insensitive to vibrations, contamination, temperature drift, and misalignment and the underlying measurement concept is well understood. But most importantly, the sensor does not require calibration. The mass flow of identical particles (4.5 mm air gun pellets) was measured with an error smaller than 3% even for high density flow rates.     

质量流量计测量高粘度流体流量

介绍了质量流量计的测量原理。举例说明了质量流量计在高粘度流体流量测量中的应用。     

科里奥利质量流量计测得值不确定度评定

本文使用新建立的水流量标准装置,依据JJG 1038-2008《科里奥利质量流量计检定规程》,采用静态质量法,对科里奥利质量流量计示值误差测得值的不确定度进行分析。     

液体容积式流量计的漏流量变化原因分析

本文主要是对液体容积式流量计漏流量发生变化原因的探讨。     

Method of Measuring the Mass Discharge and Consistency of a Flow Carrying A Suspension

A method is developed for determining the mass discharge and consistency of a pipe flow carrying a suspension under pressure. Mass discharge and consistency are determined by using readings of the power used by the hydraulic dredger which moves the flow.     

Method of Measuring the Mass Flow Rate of a Substance by Using Restricting Apertures

A new method is considered for measuring the mass flow rate of a substance in pipelines using restricting apertures, without the use of instruments for measuring the density and temperature of the flow. A structural measurement scheme is given and analytical expressions are obtained for determining the mass flow rate and the density of the substance under working conditions. A calculation is given of the errors of the flow parameters.     

科氏质量流量计数字驱动方法研究与实现

基于DDS和MDAC,研究科氏质量流量计数字驱动方法中的频率、相位、幅值跟踪。采用TMS320F28335芯片,研制科氏质量流量变送器,实现驱动方法。配以CMF025型号传感器进行了气 液两相流实验,实验结果表明,研制的变送器在两相流下能够维持流量管的振动并完成流量测量。     

水流量对空气源热泵热水器性能的影响

通过对空气源热泵热水器的性能进行实验研究,测试了水流量对热泵热水器性能的影响。实验结果表明：水流量对加热时间、能效比等性能有一定的影响,这种影响随着流量偏离正常值而加剧;设计适当的水流量,不但可以适当提高热泵热水器的能效比（COP）,而且降低了冷凝器进出口水的温差值和排气压力。     

科氏质量流量计模拟驱动方法研究

驱动系统是科里奥利质量流量计的重要组成部分之一。它为流量管提供驱动力,使流量管以其固有频率和稳定的振幅振动,并且能够跟随流量管固有频率的变化而变化。目前的驱动系统是基于模拟信号的工作方式。分析了这种驱动系统的工作原理,比较了各种波形的驱动信号,研究了几种驱动电路。     

金属雾化过程气体质量流率的研究

金属雾化过程中颗粒的尺寸大小及统计分布规律是影响粉末冶金和喷射沉积快速凝固材料组织和性能的关键因素。雾化气体的质量流率对金属颗粒的尺寸及分布有很大影响，本文根据热力学第一定律推导出雾化气体质量流率的表达式，气体质量流率主要受雾化器出口面积及气体膨胀比的影响，出口面积愈大，膨胀比愈小，气体质量流率愈大，当临界膨胀比（Ｐ２／Ｐ１）ｃ＝时，气体质量流率达到最大值。     

Three-Dimensional Simulation of Heat and Mass Transfer Processes during SHF Heating of Oil Flow in a Pipeline

Journal of Engineering Physics and Thermophysics - This article considers mathematical simulation of heat and mass transfer processes in the course of SHF heating of flow of a viscous fluid, oil...     

Mass Flow through Solid 4H

We continue our solid ⁴He flow experiments in which we grow solid helium samples at constant temperature in the hcp region of the phase diagram. We exploit the properties of liquid helium in a confined geometry (porous Vycor glass), and induce a mass flow through the solid at pressures higher than the bulk melting pressure. We previously observed flow, but our temperature was limited to T≥350 mK. At T≈400 mK it was found that the flow ceased at P≈27 bar, and no flow was observed for T>550 mK. We have begun to extend our measurements to lower temperatures, and our data show that at lower temperatures we observe flow at higher pressures.