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Chun-Min Su, Win-Ti Lin, Sutham Masri
Bilateral Comparison of Primary Low-Pressure Gas Flow Standards Between NIMT and CMS

To verify the measurement capability and performance of the newly established primary low-pressure gas flow standard, a mercury-sealed piston prover, at the National Institute of Metrology of Thailand (NIMT), a bilateral comparison with the piston prover at the Center for Measurement Standards (CMS, Taiwan) was conducted. The piston prover at NIMT has a measurement capability of 5 mL/min to 24 L/min flow range with a relative expanded uncertainty smaller than 0.13 %, whereas that of the system at CMS is 2 mL/min to 24 L/min with 0.10 % expanded uncertainty. The transfer standard (TS) used was a set of three critical flow venturis (CFV’s) with dedicated thermometers. The TS was used at eight flow rates of dry air ranging from 42 mL/min to 14.5 L/min at 0 ℃ and 101.325 kPa (0.055 g/min to 18.87 g/min). Comparison showed that the differences in the normalized average discharge coefficient between NIMT’s measurements and the reference values based on CMS’s results were smaller than 0.06 % throughout the range of flow tested. The En values for the flow measurements at NIMT with reference to CMS were all well less than unity. The equivalence between the two participants was thus demonstrated.

Sutham Masri, Win-Ti Lin , Chun-Min Su
New Primary Low-Pressure Gas Flow Standard at NIMT

To establish the traceability chain of low-pressure gas flow measurement within Thailand, a primary standard with the capacity of 0.005 L/min to 24 L/min (at 296.15 K and 101.325 kPa) was established at National Institute of Metrology (Thailand); NIMT. The standard facility is a mercury-sealed piston prover consisting of three precision- machined glass cylinders. With the positive displacement technique, the facility measures gas flowrate by determining the displaced volume, time, and pressure and temperature of the gas. Flow measurement can be carried out manually or semi-automatically. The electronics were installed in a separate console to minimize the heating effect on the gas temperature. Furthermore, special care was taken in designing the facility to ensure that gas pressure and temperature can be measured as accurate and representative as possible. The relative expanded uncertainty of gas mass flow measurement, evaluated according to ISO GUM, was less than 0.13 % of reading.

Jerker Delsing, Kristoffer Karlsson
Low-Pressure Gap Discharge Ultrasonic Gas Flowmeter

Low-pressure gas measurements are of increasing interest in the process industry for both control purposes and emission measurements. Industrial measurement environments include some very challenging components, such as:
• Dust, particles, vapor, water droplets, etc.
• Temperatures up to 1200 °C
• Pipe diameters of 1 to 10 m
Ultrasound flow measurement techniques have many advantages for such industrial measurement problems. Currently, a major problem is the lack of transducer technology that is sufficiently robust to operate in the presence of the above given industrial components. For the purpose of producing more robust technology, a gap discharge sound transmitter has been developed. Theoretical and experimental studies of the gap discharge transmitter indicate that flow measurement performances in the range of 1-2 % of the actual flow is achievable.
Based on this gap discharge transmitter, an experimental ultrasound gas flowmeter was designed. The design features a gap discharge transmitter and piezo-based receivers. The design was tested in a real industrial environment. The test environment included heavy dust and water vapor in an exhaust pipe at a pelletization plant at LKAB, Kiruna, Sweden. The pipe diameter is 3 m, the pressure is ambient, and the gas flow speed is in the range of 5-20 m/s. The flow conditions were highly turbulent, using a straight pipe length ten times the pipe diameter in front of the experimental flowmeter. This paper presents the experimental gap discharge ultrasonic flowmeter design, the experimental setup and some measurement data. These data indicate that the gap discharge transmitter is feasible for operation in an industrial environment. Further preliminary flow measurement data demonstrate the feasibility of using a gap discharge transmitter as the sound-emitting source in an ultrasonic gas flowmeter.

Carlos Eduardo Jeronymo, Valter Yoshihiko Aibe
Implementation of Quadruple-Timing Pulse Interpolation Applied to Compact Piston Provers

This work presents an electronic circuit for quadruple-timing pulse interpolation applied to compact piston provers. Compact provers are usually employed to prove meters with pulsed outputs. API and ISO standards recommend a minimum of 10000 pulses per run to obtain a resolution better than ±0.01 %. Since the volume of fluid displaced by a compact prover is relatively small, the number of pulses produced during a proving run is often considerably less than 10000 pulses. Pulse interpolation techniques are commonly used to increase resolution and to diminish uncertainty during a proving run by estimating the fractional part of meter pulses within the time interval of the calibration. In this way, pulse interpolation techniques are essential to obtain accurate flow measurements and to allow the calibration of meters with compact provers.

Michael Reader-Harris, Neil Barton, David Hodges
The Effect of Contaminated Orifice Plates on the Discharge Coefficient

Orifice plates can be contaminated by oil, grease, pipeline sludge or other liquids or solids. Experience shows that sometimes the contamination extends to the sharp edge of the orifice plate, but that on many occasions any possible contamination near the edge is cleaned by the flow. The latter case is investigated here. In some of the existing sets of data the contamination in the form of soft deposits used to gather the data means that interpretation is not straightforward; so Computational Fluid Dynamics (CFD) was used to assist in the interpretation.
In the experimental work the contamination was simulated by sticking circular metal discs of defined thickness and radius to the plates so as to leave an untouched region in the neighbourhood of the sharp edge. The effect of this contamination was measured in nitrogen at 63 bar absolute. CFD was used to investigate similar contaminated plates.
A contamination angle was defined, and the CFD predictions were plotted against the contamination angle. The simulations for a diameter ratio, β, equal to 0.6, almost lie on a single curve. The β = 0.2 and β = 0.4 points lie above this curve and the β = 0.75 points lie below the curve. The new NEL experimental data are compared with the CFD and the Advantica data on coated plates with a clean ring as in ISO/TR 12767.
It is clear from the experimental data, as indeed from the CFD, that although the ratio of the thickness of the contamination to the distance from the orifice edge is the most important effect on the shift it is not the only effect. An equation for the percentage shift in discharge coefficient was derived to fit the experimental data: this has an uncertainty of 0.28 % based on 2 standard deviations. The CFD are in remarkably good agreement with the experiments and support the inclusion of the new model in a revision of ISO/TR 12767.

Richard Steven, Charlie Britton, Joshua Kinney
4”, 0.63 Beta Ratio Cone DP Meter Wet Gas Performance

Cone DP meters are often used for unprocessed natural gas flow metering applications. Unprocessed natural gas flows can have entrained water and light hydrocarbon liquids. Hence, it is important to fully understand the wet gas flow response of cone DP meters. One method of metering the gas flow rate of a wet natural gas flow is to estimate the liquid flow rate (usually a mixture of hydrocarbon liquid and water) from an independent source (such as a tracer dilution technique or test separator histories) and then use a wet gas correction factor or "correlation" to correct for the liquid induced gas flow rate error. It is therefore necessary to have a reliable cone DP meter wet gas correlation for wet natural gas flows where the liquid component is a water and / or a light hydrocarbon liquid mixture.

R. Mascomani , S. Saseendran, BVSSS Prasad
Metrological Comparison of Metering Characteristics of Differential Pressure Meters

It is often difficult to realize calibrated accuracy of a flow metering system over measurement range when it is installed under hostile and perturbed flow conditions. Though widespread studies are reported in literature on individual characteristics of meters, comparative evaluation of the performance of these devices under real life installation situations is relatively inadequate. Present study compares classical venturi, cone, standard orifice and new slotted orifice and four hole orifice meters. Experiments are carried out to investigate the effects of single elbow, double elbow in and out of plane, reducer, and expander on the response characteristics of these devices. Discharge coefficients and pressure loss characteristics are analyzed and compared. Pressure and velocity variations created by the flow element restrictions with adjacent meter tubing are also analyzed with computational fluid dynamic simulations. Minimum upstream straight pipe lengths to suppress the effects for each of these tested flow meters are proposed.

Casey Hodges, Charles Britton, William Johansen, Richard Steven
Cone DP Meter Calibration Issues

Cone DP flow meters are becoming increasingly popular for natural gas flow metering. A cond DP meter operates according to the same physical principles as other DP meters but it is not as yet included in the ISO 5167 report on DP meters. In this paper, thirty one cone DP meter single phase data sets from CEESI independent research, a wet gas research Joint Industry Project, and multiple third party cone DP meter calibrations are reviewed. The meters discussed have diameters ranging from 2” to 14”, beta ratios ranging from 0.45 to 0.85, Reynolds numbers ranging between 5e4 and 5e6, and pressures up to 75 bars. This paper discusses:
Performance comparisons between pairs of nominally identical cone DP meters built to the same specifications. These include pairs of meters built by to same manufacturer and built by different manufacturers. Conclusions are drawn on the prospects of similar meters having the same performance.
The discharge coefficient vs. Reynolds number relationship. The potential for exposure to biases, caused by calibrating cone DP meters with low Reynolds number water flows and then extrapolating the resulting data fit for high Reynolds number gas flow applications, will be explained. Multiple meter data sets logged from various test facilities will be used in this discussion.
The practice of periodic re-calibration of cone DP meters will be discussed. Conclusions will be drawn on whether this practice is necessary after examining the repeat calibration data sets of several different meters.
All data sets are plotted on one graph to view the discharge coefficient spread.
There is potential for cone assemblies to suffer some plastic deformation in service (e.g. due to slug strikes, excessive flow rates, etc). Therefore, the effect on a 4” 0.75 beta ratio cone DP meter’s calibration of shifting the cone alignment by 1° off the calibration position has been investigated. The experimental results showed some surprising and important conclusions.
A potential serious flaw in a common meter sizing methodology will be discussed that can leave a cone DP meter not fit for its purpose. A detailed worked example is given. The simple remedy is also given.
Comments are made on the prospects of cone DP meters being eligible for inclusion in ISO 5167.

Casey Hodges
New Differential Producing Meters - Ideas, Implementation, and Issues

There are several relatively new differential producing meters that are available for end users. Each meter claims to have advantages over other meter types, specifically orifice meters. Meter types discussed include; cone meters, Venturi meters, multi-ported averaging pitot tubes, multi-holed orifice plates, and diagnostic differential meters. This paper is intended to be used by purchasers of these meters to help them obtain the best meter for their application. The operating principles of these meters will be explored. This paper will look at the claims that the manufacturers of these meters make in terms of accuracy, required upstream lengths, and diagnostic capabilities. Another important aspect of these meters is industry’s reaction to these meters. Should these meters be included in standards documentation? What data needs to be collected to properly develop standards, and what standards exist to help develop these meters? Additionally, the implementation of these meters and metering systems is discussed with the intent of developing system uncertainties. From a calibration facility perspective, many issues have been observed with differential metering systems. Several of these issues will be discussed in detail along with their associated implications.

Lei Sui, Toan H. Nguyen, James E. Matson, Peter Espina, IvanTew
Ultrasonic Flowmeter for Accurately Measuring Flare Gas over A Wide Velocity Range

Flare gas ultrasonic flow measurement has now been well established with more than 3000 units installed worldwide in process plants and refineries. One of the remaining technical challenges in flare gas ultrasonic flowmetering is to deal with extremely high flare flows (greater than 80 m/s) during emergency flaring. High flare flows introduce soaring flow noise, cause ultrasonic beam drift and thus deteriorate ultrasonic signal quality, leading to an ultimate failure of the flare gas flow measurement. In this paper, the ultrasonic propagation in flare gas has been studied, the beam drift due to gas flow has been investigated and improvements from both mechanical and transducer perspectives have been made. An improved flare gas ultrasonic flow meter has been developed to demonstrate the accurate measurement of air flow up to 123.7 m/s. Testing data have been presented for two typical configurations, Bias 90 and Diagonal 45, in comparison with a Venturi reference meter. The overall accuracy of the new flare meter is demonstrated to be 3-4 %, and the relative standard deviation of the meter readings is within 1.2 %. This new development could translate into higher flow-velocity flare gas measurement and monitoring, depending on the flare gas composition in an actual application.

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