What type of flow meter should be used to display the real-time flow rate for crude oil transportation?
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I recently worked on a small design that involved using a material whose viscosity is similar to that of crude oil. There’s a small issue: I want to know the instantaneous flow rate during pumping. When pumping water, we can use a glass rotameter – by observing the position of the float, we can determine the current flow rate. But for materials with such viscosity, a rotameter certainly won’t work. I’m wondering what is used in the petrochemical industry for this purpose; I would appreciate any guidance you could provide. Also, for measuring the total amount such as the overall volume discharged, an LC elliptical rotor flow meter should work fine. Thank you again.High reliability, good repeatability, high measurement accuracy, low pressure loss. No moving parts, wide range, fast response time, no need for temperature or pressure compensation.
**Applications**
· Measurement of gas mass flow rate in industrial pipelines
· Measurement of flue gas velocity emitted from chimneys
· Measurement of flue gas flow rate in calcination furnaces
· Measurement of air flow rate in gas processing systems
· Measurement of compressed air flow rate
· Measurement of gas flow rate during semiconductor chip manufacturing
· Measurement of gas flow rate in wastewater treatment processes
· Measurement of gas flow rate in heating, ventilation, and air conditioning systems
· Measurement of gas flow rate in flux recovery systems
· Measurement of combustion gas flow rate in combustion boilers
· Measurement of gas flow rate for natural gas, flare gas, hydrogen, etc.
· Measurement of carbon dioxide flow rate during beer production
· Measurement of gas mass flow rate during production in cement, cigarette, and glass factories
Examples: In the United States: FCI SIERRA, etc.; in China: Naiside, etc.
**Key Parameters**
Accuracy: 1%±0.5%F.S
Repeatability: ±0.2%
Range: 0.05~90 m/s
Applicable flow range: 0~5000 Nm3/h (for Φ250 air)
Applicable pressures: <2 Mpa, <3 Mpa
Applicable medium temperature ranges: -25~120°C, -25~200°C, -25~500°C
Power supply: 24V DC or 220V AC
Output: 4~20 mA
Communication interface: 232 or 485
On-site display: LED or LCD
Protection rating: IP65
Explosion protection class: ExdllCT4
**Open-channel Flow Meter**
Unlike the previous types, this is a flow meter used to measure the flow rate of free-surface water in open channels that are not completely filled. A waterway with non-full pipe flow is called an open channel, and a device used to measure the flow rate of water in such channels is known as an open channel flowmeter. In addition to circular shapes, open-channel flow meters also come in various other shapes such as U-shaped, trapezoidal, and rectangular. Applications of open-channel flow meters include urban water supply channels; intake and discharge channels in thermal power plants, as well as channels for wastewater treatment input and output ; Water discharge from industrial and mining enterprises, as well as channels used for water conservancy projects and agricultural irrigation. Some estimates put the figure at 1,995 units, accounting for about 1.6% of all flow meters, but there are no estimated figures available for their use in China. Edit this paragraph: Electrostatic flowmeter – The Tokyo Institute of Technology in Japan developed an electrostatic flowmeter suitable for measuring the flow rate of low-conductivity liquids in oil transport pipelines. The metal measuring tube of the electrostatic flowmeter is connected to the piping system in an insulated manner; the charge within the measuring tube can be determined by measuring the static charge on the measuring capacitor. They conducted actual flow tests using measuring tubes made of metals such as copper and stainless steel, as well as plastics, with inner diameters of 4–8 mm. The tests showed that there is a nearly linear relationship between flow rate and charge. Edit this paragraph: Combined effects flow meter – This instrument operates on the principle that the momentum and pressure of the fluid cause deformation in its chamber; by measuring this deformation resulting from the combined effects, the flow rate can be determined. This instrument was developed by the GMI Institute of Engineering and Management in the United States, and two patents have been applied for. Edit this paragraph: Tachometric flowrate sensor. It was developed by the Industrial Instruments Company of the Russian Scientific and Engineering Center, and is based on the theory of the suspension effect. This instrument has been successfully applied in various fields (for example, more than 2,000 units were installed in nuclear power plants to measure hot water flow, with continuous use over 8 years), and it is still being improved to expand its areas of application. Edit this paragraph: Coriolis mass flow meter (CMF) The Coriolis mass flow meter (hereafter referred to as CMF) is a direct-type mass flow measuring instrument that operates on the principle that, as fluid flows through a vibrating tube, a Coriolis force is generated which is proportional to the mass flow rate. The application of CMF in our country started relatively late. In recent years, several manufacturers (such as Taihang Instrument Factory) have developed products on their own to supply the market; other manufacturers have established joint ventures or utilized foreign technology to produce a range of instruments. Abroad, more than 30 series of CMF products have been developed. The technical focus in the development of each series lies in innovative designs for the flow detection tube structure, as well as in improving aspects such as the stability and accuracy of the instrument’s zero point ; Increasing the deflection of the measuring tube improves sensitivity: it enhances the stress distribution within the measuring tube, reduces fatigue damage, and improves resistance to vibration interference. Edit this paragraph: Electromagnetic flowmeter (EMF). Since its introduction into industrial use in the early 1950s, the application areas of EMF have continued to expand; by the late 1980s, it accounted for 16%–20% of the total sales value of flowmeters worldwide. Our country has seen rapid development in recent years; sales in 1994 were estimated to be between 6,500 and 7,500 units. In China, EMFs with a maximum diameter of 2–6 meters have been manufactured, and there is the capability to produce units with a 3-meter diameter that have been tested under actual flow conditions. In 2008, sales reached $77 million, with an estimated sales volume of over 350,000 units. Edit this paragraph: Vortex flow meter (USF). The USF was introduced into industrial use in the late 1960s, and by the late 1980s it accounted for 4% to 6% of the total sales value of flow meters worldwide. The estimated global sales volume in 1992 was 35,400 to 48,000 units, while domestic production during the same period was estimated at 8,000 to 9,000 units. 5.4 Wilo Flow Meters The Wilo flow meters feature an engineering design that fully adheres to aerodynamic principles, making them sensing elements of exceptional quality in terms of accuracy, efficiency, and reliability. 5.5 Elliptical Gear Flow Meters Cast-iron elliptical gear flow meters are widely used for measuring various oils and liquid media that do not corrode cast iron. Cast steel elliptical gear flow meter, used for measuring high-pressure, low-corrosivity media. Cast iron elliptical gear flow meter, with an aluminum rotor, suitable for measuring low-viscosity, low-corrosivity media such as gasoline. ■ Technical Parameters and Selection 1. Materials of main components and nominal pressure 2. Accuracy grades: 0.5 level and 0.2 level (generally at -10°C to +60°C) 3. Temperature range for the medium: LC-A, LC-E: (-20°C to +100°C); LC-Q: (-20°C to +60°C). For LC-A and LC-E, with high-temperature adjustment and the addition of a high-temperature heat dissipation tube, the temperature can reach 200°C. 4. Explosion protection grade for remote display at the installation site: E*aⅡCT5, dⅡBT4 Conclusion As can be seen from the above, although flow meters have become increasingly sophisticated over time, there are still an enormous variety of them. To date, there is no flow meter that is suitable for all applications. Each type of flow meter has its applicable range as well as its limitations. This requires us to: (1) When selecting instruments, it is essential to be familiar with both the instruments themselves and the objects being measured, while also taking other factors into consideration, so that the measurements can be accurate ; (2) Make efforts to develop new types of instruments to improve them further on the existing basis. Edit this paragraph: Differential pressure flow meter. A differential pressure flow meter (hereinafter referred to as DPF or flow meter) is an instrument that measures flow rate based on the differential pressure generated by a flow sensing element installed in a pipeline, along with known fluid properties and the geometric dimensions of the sensing element and the pipeline. The DPF consists of a primary device (sensing element) and a secondary device (differential pressure conversion and flow display instrument). DPFs are usually classified by the type of sensing element, such as orifice plate flowmeters, venturi flowmeters, and average velocity tube flowmeters. Secondary devices include various mechanical, electronic, and mechatronic differential pressure gauges, differential pressure transmitters, as well as flow display and calculation instruments. They have evolved into a large category of instruments with a great variety of models, characterized by a high degree of standardization, serialization, and universalization. Differential pressure gauges can be used to measure flow parameters as well as other parameters such as pressure, level, density, etc. Based on the working principle of their sensing elements, DPFs can be classified into several major types, including throttle type, dynamic head type, hydraulic resistance type, centrifugal type, dynamic pressure gain type, and jet type. Among these, the throttle type and dynamic head type are the most widely used. The sensing elements of throttle-type DPFs are divided into two main categories based on their degree of standardization: standard type and non-standard type. A so-called standard throttling device is one that is designed, manufactured, installed, and used in accordance with standard documents; its flow rate can be determined and its flow measurement error can be estimated without the need for actual flow calibration. Non-standard throttling devices are testing components that are less mature and have not yet been included in standard documents. The development of the standard throttle-type DPF was a lengthy process; as early as the 1920s, the United States and Europe began large-scale experimental research on throttle devices. The most commonly used throttling devices – orifice plates and nozzles – are beginning to be standardized. A type of standard nozzle today is the ISA 1932 nozzle, whose geometry was standardized in the 1930s; the standard orifice plate was also formerly known as the ISA 1932 orifice plate. The standardization of the structural forms of throttling devices is of great significance, as only by standardizing these structures can a wide range of international research findings be brought together. It facilitates the advancement of both the theory and practice related to measuring devices in terms of depth and breadth, an advantage that other flow meters do not possess. In 1980, the ISO (International Organization for Standardization) officially adopted the international standard ISO 5167, marking the birth of the first international standard for flow measurement throttling devices. ISO 5167 summarizes the theoretical and experimental research results from several decades on a limited number of throttling devices (orifice plates, nozzles, and venturi tubes) worldwide, reflecting the current scientific and technical standards in the field of such measuring elements. However, since the official issuance of ISO 5167, it has revealed many urgent problems that need to be addressed, mainly in the following areas. 1) Obsolescence of ISO 5167 test data: The data used in ISO 5167 are mostly test results from the 1930s. Today, there have been significant advancements in throttling device manufacturing technology, as well as in flow testing equipment and experimental methods. It is necessary to conduct systematic tests again in order to obtain more accurate and reliable data. In the 1980s, large-scale tests were conducted in both the United States and Europe, laying the foundation for revising ISO 5167. 2) The issue regarding the specification for the length of straight pipe sections in ISO 5167: When ISO 5167 was voted on, the United States voted against it, mainly due to disagreements over the specifications for the length of straight pipe sections. This issue should be one of the main concerns in the revision of ISO 5167. 3) Scientific issues regarding the provisions in ISO 5167: There are numerous factors that affect the discharge coefficient of throttle devices. These include the ratio β of pore diameter to pipe diameter, the pressure measurement devices used, the Reynolds number, the degree of eccentricity in the installation of the throttling element, the types of flow restrictors before and after it, as well as the length of the straight pipe section. Other factors include the sharpness of the inlet edge of the orifice plate, the roughness of the pipe wall, and the turbulence level of the fluid flow. The interactions among these many factors are complex, and some parameters are difficult to measure directly. As a result, some of the provisions in the standard are not determined on a scientific basis; rather, they are set arbitrarily in order to ensure consistency. The renowned flow expert E.A. Spencer raised a series of issues that should be re-examined, such as the flatness of the orifice plate, its concentricity, the sharpness of the right-angled edges, pipe roughness, the upstream flow velocity distribution, and the role of flow regulators. 4) Regarding the issue of improving the measurement accuracy of throttle-type DPFs: Given the important role of throttle-type DPFs in flow meters, it is highly significant to enhance their measurement accuracy. Previous international academic conferences have concluded that it is necessary for flow measurement specialists, as well as those working in fluid mechanics and computer technology, to work closely together to address this issue. In the 1980s, the United States and Europe began large-scale experimental research on orifice plate flowmeters; in Europe, this was part of the EEC Experimental Program, while in the United States it was part of the API Experimental Program. The purpose of the test is to conduct a new round of extensive experimental research using the latest testing equipment and statistical analysis techniques for test data, in order to lay a technical foundation for revising ISO 5167. In 1999, ISO issued a revised version of ISO 5167 (ISO/CD 5167-1-4). This document was a committee draft that contained significant changes in both its technical content and formatting; it represented a completely new standard. It was originally scheduled to be approved as a DIS (draft standard) at the ISO/TC30/SC2 meeting held in Denver, USA, in July 1999, but the meeting concluded that there were still detailed issues that required further discussion, and it was not approved. It is not yet known when the new ISO 5167 standard will be officially issued. The new ISO 5167 standard introduces substantial changes in both of its core aspects: first, the formula for the discharge coefficient of orifice plates, with the Reader-Harris/Gallagher formula (R-G formula) replacing the Stolz formula; second, the requirements regarding the length of the straight pipe section upstream of the throttling device and the use of flow regulators. We usually refer to the throttling devices listed in ISO 5167 (GB/T2624) as standard throttling devices, while all others are called non-standard throttling devices. It should be noted that non-standard throttling devices refer not only to those with a structure different from that of standard throttling devices; standard throttling devices also qualify as non-standard when operating under conditions other than the standard ones. For example, a standard orifice plate operating in a multiphase flow, or a standard Venturi nozzle operating at critical flow conditions, falls into this category. Currently, the main types of non-standard throttling devices are as follows: 1) Devices for low Reynolds numbers, such as 1/4 circular orifice plates, conical inlet orifice plates, double orifice plates, double inclined orifice plates, and semi-circular orifice plates ; 2) For dirty media: annular orifice plates, eccentric orifice plates, ring-shaped orifice plates, wedge-shaped orifice plates, elbow throttling elements, etc ; 3) Low-pressure loss applications: Lohr tubes, Dal tubes, Dal orifice plates, dual Venturi nozzles, universal Venturi tubes, Vasy tubes, etc ; 4) For small pipe diameters: integral (embedded) orifice plate ; 5) End-thrust throttling devices: end-hole plates, end-nozzles, Borda tubes, etc ; 6) Wide-range throttling device: Elastically loaded variable-area variable-head flow meter (linear orifice plate) ; 7) Capillary throttle element – laminar flow meter ; 8) Pulsating flow throttling device ; 9) Critical flow throttling device – sonic venturi nozzle ; 10) Mixed-flow throttling device. The growing use of throttle-type DPFs in practical applications inevitably leads to the need for the development of non-standard throttle devices. Over the past decade, ISO has been continuously preparing technical documents related to such non-standard throttle devices, publishing them as technical reports until they can be established as official standards. It is foreseeable that in the future, several relatively mature non-standard throttling devices may be upgraded to standard types. In the mid-to-late 1990s, worldwide, various types of DPFs accounted for 50%–60% of the total number of flow meters sold (about one million units per year), and they represented around 30% of the total sales value. In our country, the number of units sold accounts for 35%–42% of the total volume of flow meters (excluding household gas meters, household water meters, and glass tube float flow meters), which amounts to 60,000–70,000 units per year. 2 Working Principle 2.1 Basic Principle When fluid fills a pipe and flows through a throttling element within it, the flow velocity increases at that element due to local constriction, resulting in a decrease in static pressure. Thus, a pressure difference is created before and after the throttling element. The greater the fluid flow rate, the greater the pressure difference generated; thus, the flow rate can be determined based on this pressure difference. This measurement method is based on the continuity equation of flow (the law of mass conservation) and Bernoulli’s equation (the law of energy conservation). The magnitude of the pressure difference is related not only to the flow rate but also to many other factors; for example, when the type of throttling device or the physical properties of the fluid in the pipeline (density, viscosity) vary, the pressure difference generated at the same flow rate will also differ. 2.2 Flow equation Where qm is the mass flow rate, in kg/s; qv is the volume flow rate, in m3/s; C is the discharge coefficient ; ε--expansibility coefficient ; β--diameter ratio, β=d/D; d--diameter of the orifice under operating conditions, m ; D--Inner diameter of the upstream pipeline under operating conditions, m ; △P--differential pressure, Pa ; ρl--density of the upstream fluid, kg/m3. As can be seen from the above equation, the flow rate is a function of six parameters: C, ε, d, ρ, △P, and β(D). These six parameters can be divided into two categories: measured quantities and statistical quantities (C, ε). (1) Measured values: 1) In equations (4.1) for d and D, d is in a quadratic relationship with the flow rate; its accuracy has a significant impact on the overall accuracy of the flow rate measurement. The error value should generally be kept within ±0.05%, and the effect of operating temperature on the thermal expansion of the material must also be taken into account. The standard requires that the inner diameter D of the pipe be measured actually; multiple measurements should be taken at several sections along the upstream pipe section to determine the average value, with the error not exceeding ±0.3%. In addition to the high requirements for the accuracy of logarithmic measurements, it is also necessary to consider the severe impact that inner diameter variations can have on causing abnormal throttling in the channel upstream of the throttle element. Therefore, when the throttle device is not supplied as a set, this issue must be given due attention in on-site piping. 2) In the flow equation, ρ occupies the same position as △P; in other words, when striving for a high precision level in differential pressure transmitters, it is essential not to forget that the measurement accuracy of ρ must also be matched accordingly. Otherwise, the increase in △P will be offset by the decrease in ρ. 3) △P Differential pressure: The accurate measurement of △P should not be limited to simply using a high-precision differential pressure transmitter. In fact, whether a differential pressure transmitter can receive an accurate differential pressure value depends on a series of factors. Among these, the proper manufacturing, installation, and use of the pressure tapping holes and pressure conduits are key to ensuring accurate differential pressure readings. Many of these influencing factors are difficult to determine quantitatively or qualitatively; only by improving the standardization of manufacturing and installation processes can this goal be achieved. (2) Statistics 1) C statistic: The C statistic is a value that cannot be measured directly (it refers to a value obtained when something is designed, manufactured, and installed according to standards without any calibration before use). In practical applications, the most complex situation arises when the actual value of C does not match the value specified by the standards. Their deviations are caused by a series of factors such as design, manufacturing, installation, and use. It should be clear that all the aforementioned steps must strictly adhere to the standard specifications in order for their actual values to match those specified by the standards; it is difficult to meet such requirements in practice. It should be noted that deviations from standard conditions can be quantitatively estimated (and corrected) in some cases, while in others they can only be qualitatively estimated (as for the magnitude and direction of the uncertainty). But in reality, sometimes it is not just one condition that deviates, which leads to very complex situations, because general information only covers the errors caused by deviations in a single condition. If many conditions deviate simultaneously, relevant data is unavailable. 2) The expansibility coefficient ε is a correction for the change in the discharge coefficient caused by changes in the density of the fluid as it passes through the throttle element. Its error consists of two parts: one is the error of ε at normal flow rates, that is, the error of the value determined according to standards ; The second is the error resulting from fluctuations in the flow rate, which in turn cause variations in the ε value. Generally, under conditions of low static pressure and high differential pressure, the ε value exhibits significant errors. When △P/P ≤ 0.04, the error of ε is negligible. 3 Classification The classification of differential pressure flowmeters is shown in Table 4.1. Table 4.1 Classification Table of Differential Pressure Flow Meters Classification Principle Classification Type Classification based on the principle behind the generation of differential pressure: 1) Throttling type ; 2) Dynamic head type ; 3) Hydrodynamic resistance type ; 4) Centrifugal ; 5) Dynamic pressure gain type ; 6) Jet type: Classified by structural form 1) Standard orifice plate ; 2) Standard nozzle ; 3) Classical venturi tube ; 4) Venturi nozzle ; 5) Conical inlet orifice plate ; 6) 1/4 circle orifice plate ; 7) Annular orifice plate ; 8) Eccentric orifice plate ; 9) Wedge-shaped orifice plate ; 10) Overall (embedded) orifice plate ; 11) Linear orifice plate ; 12) Annular orifice plate ; 13) Dowle tube ; 14) Roros tube ; 15) Elbow ; 16) Replaceable orifice plate throttling device ; 17) Critical flow throttling devices classified by purpose 1) Standard throttling devices ; 2) Low Reynolds number throttle device ; 3) Contaminated flow throttling device ; 4) Low-pressure loss throttling device ; 5) Small-diameter throttling device ; 6) Wide-range throttling device ; 7) Critical flow throttling device ; 3.1 Classification by the principle behind the generation of differential pressure 1) Throttling type: It operates on the principle that as the fluid passes through a throttling element, part of its pressure energy is converted into kinetic energy, thereby creating a differential pressure. The component used for detection in this type is called a throttling device, and it represents the most common type of DPF. 2) Dynamic head type: It operates on the principle of the conversion of dynamic pressure into static pressure, such as the average velocity tube flow meter. 3) Hydrodynamic resistance type: It operates on the principle of pressure difference generated by fluid resistance; the sensing element is a capillary bundle, and it is also known as a laminar flow meter. It is generally used for measuring very small flow rates. 4) Centrifugal type: Operates on the principle of differential pressure generated by centrifugal force in curved or annular tubes, such as elbow flow meters and annular tube flow meters. 5) Dynamic pressure gain type: It operates based on the principle of dynamic pressure amplification, such as the Pitot-venturi tube. 6) Jet type: It operates on the principle of fluid jet impact, such as jet differential pressure flow meters. 3.2 Classification by structural form 1) Standard orifice plate, also known as orifice plate with concentric right-angled edges; its axial cross-section is shown in Figure 4.2. A orifice plate is a thin plate shaped into a circular shape with concentric rings and sharp right-angled edges. The upper edge of the orifice in the plate should be a sharp right angle. Standard orifice plates have three pressure tapping methods: corner connection, flange, and D-D/2 pressure tapping ; As shown in Figure 4.3. To measure flow from either direction, a symmetric orifice plate can be used; both edges of the throttling orifice possess the characteristics of the upstream edge of a right-angled edge orifice plate, and the entire thickness of the orifice plate does not exceed that of the throttling orifice. Figure 4.2 Standard orifice plate Figure 4.3 Three pressure extraction methods for orifice plates 2) Standard nozzles come in two structural forms: ISA 1932 nozzles and long-diameter nozzles. a. The ISA 1932 nozzle (Figure 4.4) is a nozzle whose upstream surface consists of a plane perpendicular to the axis, a constricted section defined by two arc segments with a circular profile, a cylindrical throat, and a groove. The pressure tapping method for ISA 1932 nozzles is only corner tapping. Figure 4.4 ISA 1932 nozzle b. Long-diameter nozzle (Figure 4.5): A nozzle whose upstream surface consists of a plane perpendicular to the axis, a converging section with a 1/4 elliptical profile, a cylindrical throat, and possibly grooves or bevels. For long-diameter nozzles, there is only one pressure measurement method: D-D/2. 3) The classic venturi tube consists of an inlet cylindrical section A, a conical contraction section B, a cylindrical throat C, and a conical expansion section E, as shown in Figure 4.6. Depending on the different processing methods, there are the following structural forms: ① Those with a coarse casting shrinkage zone ; ②With mechanically processed shrinkage sections ; ③With iron plate welding shrinkage sections. The relationships between the different structural forms of L1, L2, R1, R2 and D, d are shown in Table 4.2. 4) The venturi nozzle consists of an inlet nozzle, a cylindrical throat, and a diffusion section, as shown in Figure 4.7. 5) Conical inlet orifice plate: The conical inlet orifice plate is similar to a standard orifice plate; it is essentially a standard orifice plate placed in an inverted position. Its structure is shown in Figure 4.8, and the pressure measurement is carried out using corner connection methods. Table 4.2 Relationship between L1, L2, R1, R2 and D, d Note: Thick casting inlet, mechanically processed inlet, thick-welded sheet metal inlet 1 ±0.25D (100mm<D<150mm) L1=0.5D±0.05D L1=0.5D±0.05D 2 L2=the smaller of 1D or 0.25D+250mm L2≥D (inlet diameter) L2≥D (inlet diameter) 3 R1=1.375D+20% R1<0.25D R1=0, except for welds 4 R2=3.625d to 3.8d R2<0.25D R2=0, except for welds Figure 4.6 Classical venturi tube Figure 4.7 Venturi nozzle Figure 4.8 Conical inlet orifice plate 1—Ring gap ; 2-Clamping ring ; 3 – Upstream end face A ; 4-Downstream end face B ; 5-axis ; 6-Flow direction ; 7-Pressure tap ; 8-hole plate ; Clamping ring with X-band gap ; Y – Separate pressure tap. Provided by AirLoo Network HVAC experts. Edit this section: Basic principles and types of ultrasonic flowmeters. Ultrasonic waves carry information about the flow velocity of the fluid as they propagate through it. Therefore, the flow velocity of the fluid can be detected using the received ultrasonic waves, which can then be converted into flow rate. Based on the detection method, ultrasonic flowmeters can be classified into different types such as the velocity difference method, Doppler method, beam deflection method, noise method, and related methods. An acoustic flow meter is a type of non-contact instrument that has come into use over the past decade or so, thanks to the rapid development of integrated circuit technology. It is suitable for measuring fluids that are difficult to access and observe, as well as flow rates in large-diameter pipes. It can be used in conjunction with a water level gauge to measure the flow rate of open-flow water. By using ultrasonic flow measurement, there is no need to install measuring elements in the fluid, which means that the flow pattern of the fluid remains unchanged and no additional resistance is generated. The installation and maintenance of such instruments do not affect the operation of the production pipelines, making it an ideal energy-saving flow meter. As is well known, current industrial flow measurement faces the challenge of measuring large-diameter flows with high volumes. This is because conventional flow meters encounter difficulties in manufacturing and transportation as the diameter of the measurement tube increases, resulting in higher costs, greater energy losses, and other installation-related issues – all of which can be avoided by ultrasonic flow meters. Since various ultrasonic flowmeters can be installed outside the pipeline and perform non-contact flow measurement, their cost is basically independent of the diameter of the pipeline being measured. In contrast, the cost of other types of flowmeters increases significantly as the diameter grows; therefore, for larger diameters, ultrasonic flowmeters offer a better cost-performance ratio compared to other types of flowmeters with similar functions. Considered to be a good flow measurement instrument for large diameters, the Doppler ultrasonic flow meter is capable of measuring the flow rate of two-phase media, making it suitable for measuring dirty flows such as those in sewers and wastewater systems. In power plants, using portable ultrasonic flowmeters to measure large-diameter flow rates such as the water inflow to turbines and the circulating water volume in steam turbines is much more convenient than using Pitot tubes in the past. Ultrasound flow meters can also be used for gas measurement. The applicable range of pipe diameter is from 2 cm to 5 m; it can be used in open channels and buried channels several meters wide, as well as in rivers up to 500 m wide. Furthermore, the flow measurement accuracy of ultrasonic measuring instruments is hardly affected by parameters such as the temperature, pressure, viscosity, and density of the fluid being measured. Moreover, they can be designed as non-contact and portable instruments, which enables them to address the flow measurement challenges associated with highly corrosive, non-conductive, radioactive, and flammable/explosive media, issues that are difficult to handle with other types of instruments. Furthermore, given the characteristics of non-contact measurement and with the aid of appropriate electronic circuits, one instrument can be used for measuring various pipe diameters as well as across a range of flow rates. The adaptability of ultrasonic flowmeters is also incomparable to that of other instruments. Ultrasonic flowmeters possess some of the advantages mentioned above; as a result, they are receiving increasing attention and are evolving toward standardized and universal product lines. Standard, high-temperature, explosion-proof, and wet-type models with different acoustic frequencies have now been developed to meet the needs of flow measurement in various media, applications, and pipeline conditions. The main drawbacks of ultrasonic flowmeters at present are that the temperature range of the fluid that can be measured is limited by the temperature tolerance of the ultrasonic transducer and the coupling material between the transducer and the pipeline, as well as the lack of accurate data regarding the sound propagation speed of the fluid under high temperatures. At present, in our country it can only be used to measure fluids below 200°C. Furthermore, the measurement circuit of an ultrasonic flowmeter is more complex than that of a conventional flowmeter. This is because, in general industrial measurement applications, the flow velocity of liquids is often several meters per second, while the speed of sound in liquids is around 1500 m/s. The maximum change in the speed of sound caused by changes in the flow velocity (or flow rate) of the fluid is on the order of 10^-3. If a precision of 1% is required for measuring the flow velocity, then the precision needed for measuring the speed of sound must be on the order of 10^-5 to 10^-6. Therefore, a sophisticated measurement system is necessary to achieve this, and this is precisely why ultrasonic flowmeters can only be put into practical use with the rapid development of integrated circuit technology. An ultrasonic flow meter consists of an ultrasonic transducer, electronic circuitry, and a flow display and accumulation system. The ultrasonic transmitting transducer converts electrical energy into ultrasonic energy, which is then emitted into the fluid to be measured. The ultrasonic signals received by the receiver are amplified by electronic circuits and converted into electrical signals representing flow rate, which are fed to display and accumulation instruments for display and calculation. This enables the detection and display of traffic. Ultrasonic flowmeters commonly use piezoelectric transducers. It utilizes the piezoelectric effect of piezoelectric materials; an appropriate transmitting circuit is used to apply electrical energy to the piezoelectric elements of the transmitting transducer, causing it to generate ultrasonic vibrations. Ultrasonic waves are transmitted into the fluid at a certain angle, then captured by a receiving transducer, and converted into electrical energy via piezoelectric elements for detection. The transmitting transducer utilizes the inverse piezoelectric effect of piezoelectric elements, while the receiving transducer makes use of the piezoelectric effect. The piezoelectric elements of ultrasonic flowmeter transducers are often made into circular thin sheets that vibrate along their thickness. The diameter of the thin sheet should be more than 10 times its thickness to ensure the directivity of vibration. Lead zirconate titanate is commonly used as the material for piezoelectric elements. To fix the piezoelectric element and direct ultrasonic waves into the fluid at an appropriate angle, the element must be placed in an acoustic wedge to form the entire transducer (also known as the probe). The material of the acoustic wedge is required not only to have high strength and resistance to aging, but also to result in minimal energy loss of ultrasonic waves passing through it, meaning that the transmission coefficient should be close to 1. The commonly used material for acoustic wedges is plexiglass, as it is transparent and allows one to observe the assembly of the piezoelectric elements within the acoustic wedge. Additionally, certain rubbers, plastics, and bakelite can also be used as sound wedge materials. The electronic circuit of an ultrasonic flowmeter includes transmission, reception, signal processing, and display circuits. The measured instantaneous and cumulative flow rates are displayed as digital or analog values. Based on the principles of signal detection, ultrasonic flowmeters can currently be roughly classified into types such as the propagation speed difference method (including direct time difference method, time difference method, phase difference method, and frequency difference method), beam shift method, Doppler method, correlation method, spatial filtering method, and noise method, as shown in the figure. Among them, the method based on noise principles has the simplest structure, is easy to measure and carry, is inexpensive, but has lower accuracy; it is suitable for use in situations where high accuracy in flow measurement is not required. Since the basic principle of each of the direct time-difference method, time-difference method, frequency-difference method, and phase-difference method is to determine the flow velocity of the fluid by measuring the difference in the propagation speeds of ultrasonic pulses in the forward and reverse directions, they are collectively referred to as the propagation speed difference methods. Among them, the frequency difference method and the time difference method overcome the errors caused by changes in sound speed with fluid temperature, offering high accuracy; therefore, they are widely used. Depending on the configuration method of the transducer, the propagation speed differences are further classified into: the Z method (transmission method), the V method (reflection method), the X method (cross method), etc. The beam deflection method relies on the fact that the direction of propagation of the ultrasonic beam in a fluid changes as the flow velocity of the fluid changes, and this change is used to determine the flow velocity. Its sensitivity is very low at low flow velocities, which limits its practical use. The Doppler method utilizes the principle of acoustic Doppler effect; by measuring the Doppler shift of the ultrasonic waves scattered by particles in the fluid, it is possible to determine the flow rate of the fluid. This method is suitable for measuring the flow rate of fluids containing suspended particles or bubbles. The correlation method utilizes correlation techniques to measure flow rate. In principle, the accuracy of measurement using this method is independent of the sound speed in the fluid; as a result, it is unaffected by factors such as fluid temperature or concentration, which ensures high measurement accuracy and a wide range of applicability. But correlators are expensive and have relatively complex circuits. This drawback can be overcome after microprocessors became widely used. The noise method (sound listening method) utilizes the principle that the noise generated by fluid flow within a pipe is related to the flow velocity of the fluid, and it determines the flow velocity or flow rate by detecting this noise. Its method is simple and the equipment is inexpensive, but the accuracy is low. The above methods each have their own characteristics, and the choice should be made based on factors such as the properties of the fluid to be measured, the flow velocity distribution, the location where the pipeline is installed, and the requirements for measurement accuracy. Generally, since the temperature of the working fluid in industrial production often cannot be kept constant, the frequency difference method and the time difference method are commonly used. The direct time difference method is used only when the pipe diameter is very large. The general principle for choosing the transducer installation method is: when the fluid flows parallel to the tube axis, the Z method should be used ; The V-method or X-method is used when the flow direction is not parallel to the pipe axis, or when the location of the piping limits the spacing between the transducers. When the flow field distribution is uneven and the straight pipe section ahead of the sensor is short, multiple channels (such as dual or quad channels) can also be used to overcome the flow measurement errors caused by flow velocity disturbances. The Doppler method is suitable for measuring two-phase flows, and it has seen rapid development as it avoids the problems of blockage, wear, and deposition caused by suspended particles or bubbles in conventional instruments, which can lead to their malfunction. With the development of industry and energy-saving efforts, as well as the use of kerosene-blended (COM) and coal-water blended (CWM) fuels, along with energy-saving methods such as adding water to fuel oils to enhance combustion, these factors all open up broad prospects for the application of Doppler ultrasonic flow meters. There are many types of flowmeters, and those that are commonly used in the market include: electromagnetic flowmeters, vortex flowmeters, turbine flowmeters, orifice plate flowmeters, V-cone flowmeters, metal rotor flowmeters, glass rotor flowmeters, rotameter flowmeters, gear flowmeters, venturi tube flowmeters, and ultrasonic flowmeters. The requirements for straight pipe sections in terms of installation conditions are lowest for V-cone flow meters, while electromagnetic, vortex flow, orifice plate, and other types of flow meters have higher requirements – generally 5D ahead and 3D behind the flow meter. When there are elbows, valves, etc. at the front end of the flow meter, the requirements for a straight pipe section are even higher, with a maximum requirement of 50D ahead and 5D behind. Therefore, when selecting a flow meter, it is essential to take into account factors such as the installation environment and location on-site, in order to choose a flow meter that is more suitable for those specific conditions. Electromagnetic flowmeter. Parameters required for a flowmeter: 1. The medium to be measured; 2. The temperature of the medium being measured; 3. The pressure of the medium being measured; 4. The flow rate of the medium being measured; 5. The desired level of measurement accuracy; 6. The conditions in the installation site. Principles for selecting a flowmeter: A flowmeter is a type of measuring device that follows general economic principles – the higher the precision, the higher the price; the greater the weight, the higher the price; the more functions it has, the higher the price. Imported products are more expensive than domestic ones. Since we are talking about selection principles, it is necessary to consider factors such as functionality and price. For example, if a user needs to measure the instantaneous flow rate of water in a four-inch pipe, most flow meters can meet this requirement; the cheapest ones cost a few hundred yuan, while the most expensive ones can cost hundreds of thousands of yuan – it depends on the user’s choice. For measuring liquids and gases, different flowmeters are suitable for each. Let’s briefly discuss the applicable situations, arranged from lowest to highest in terms of price per unit. For measuring liquids: glass rotameters, orifice plates, elliptical gear flowmeters, turbine flowmeters, metal rotameters, electromagnetic flowmeters, vortex flowmeters, ultrasonic flowmeters, and mass flowmeters. For measuring gases: glass rotameters, orifice plates, metal rotameters, turbine flowmeters, vortex flowmeters. Tower flowmeters: Differential pressure flowmeters such as orifice plates, nozzles, and Venturi tubes (collectively known as standard throttling devices) have dominated the field of flow measurement for nearly a century. Their advantages include standardization, simple and robust structure, ease of manufacturing, low cost, and wide applicability. For nearly a century, research and efforts to improve them have been ongoing, but due to inherent structural defects and their own intrinsic shortcomings, these issues have not yet been properly resolved. For example, an unstable discharge coefficient, poor linearity, and low repeatability affect the accuracy as well. The sharp edge at the inlet of the orifice plate is prone to wear, dirt tends to accumulate in the front section, the range ratio is low, and pressure loss is high; moreover, the extremely strict requirements regarding the straight pipe section make it difficult to meet them in practical use. To overcome these shortcomings, various non-standard throttling elements such as 1/4 circular orifice plates, conical inlet orifice plates, notched orifice plates, eccentric orifice plates, wedge-shaped orifice plates, replaceable orifice plates, and elbow fittings have been developed in an attempt to solve these problems. However, like standard orifice plates, most of these throttling elements fail to break away from the pattern of sudden contraction at the center of the fluid; they merely improve certain local issues to some extent without fundamentally solving all problems. It was not until the mid-1980s that breakthrough progress was made in such improvements: the tower flowmeter emerged, breaking away from the structural pattern that had persisted for nearly a century and enabling a \"qualitative leap\" in throttling differential pressure instruments. The major breakthrough of the tower flowmeter lies in the fact that the fluid contracts from the center of the pipe toward the inner walls of the pipe; that is, a tower-shaped element (throttle element) installed coaxially within the pipe is used to force the fluid to gradually move from the center toward the inner walls of the pipe as it flows past this element. The flow rate of the fluid is determined by measuring the pressure difference before and after the tower-shaped element. It is precisely this structure of converging sidewalls that endows the tower flow meter with a series of advantages that other differential pressure instruments cannot match, completely overcoming the many shortcomings of traditional differential pressure instruments represented by orifice plates. After more than 10 years of use both domestically and internationally, as well as numerous tests, it has been fully proven to be capable of performing more accurate and effective measurements on various fluids, including those that are dirty or flowing at low speeds, within extremely short straight pipe sections, across a wider range of measurements. Thus, a brand-new, epoch-making chapter for differential pressure flow meters was opened. It can be predicted that as people come to know, understand, become familiar with, and master it, it will gradually and completely replace traditional differential pressure instruments represented by orifice plates.