TWI879420B - Ultrasonic flowmeter and flow measurement method - Google Patents
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本揭示有關於流體流量檢測的技術領域,特別是有關於一種超音波流量計以及流量檢測方法。 This disclosure relates to the technical field of fluid flow detection, and in particular to an ultrasonic flow meter and a flow detection method.
流量計是工業測量中重要的儀器之一,在各產業應用、科學研究皆有著密切的關連,在測量精度的要求上也越來越高。流量計廣泛應用在各種領域中,像是半導體的製程:塗佈設備、蝕刻設備、洗淨設備、乾燥設備的製造過程皆會使用到流量計的測定技術。 Flowmeter is one of the important instruments in industrial measurement. It is closely related to various industrial applications and scientific research, and the requirements for measurement accuracy are getting higher and higher. Flowmeters are widely used in various fields, such as semiconductor manufacturing processes: coating equipment, etching equipment, cleaning equipment, and drying equipment manufacturing processes all use flowmeter measurement technology.
經發展到許多產業上的應用,雖然超音波流量計是較晚才出現的測量儀器,但其與量測體為非接觸式,就具有不會對流體產生阻力、延長感應器壽命、避免汙染等特性,近年更獲得許多產業的關注及使用。 After developing applications in many industries, although ultrasonic flowmeters are relatively new measuring instruments, they are non-contact with the measuring body, so they do not produce resistance to the fluid, extend the life of the sensor, and avoid pollution. In recent years, they have attracted the attention and use of many industries.
超音波流量計通常包括一個發射超音波訊號的發射器及一個接收超音波訊號的接收器,此發射器及此接收器分別設置於輸送流體的管線上的兩個位置,以分別發射超音波訊號及接收超音波訊號,並藉由發射與接收的時間差來檢測管線中的流體的流量。然而,當超音波流量計的發射器及接收器的其中之一設置於管線上的套管或是彎折處(即,管線厚度過厚)時,發射器發出 的超音波訊號,將可能會受到影響(所產生額外的時間差無法偵測,或訊號過度衰減)而無法抵達接收器。因此,現有的超音波流量計仍無法動態地適用於量測由任意厚度的管線所輸送的流體的流量。 An ultrasonic flow meter usually includes a transmitter that emits ultrasonic signals and a receiver that receives ultrasonic signals. The transmitter and the receiver are respectively arranged at two positions on the pipeline that transports the fluid to emit ultrasonic signals and receive ultrasonic signals respectively, and the flow rate of the fluid in the pipeline is detected by the time difference between emission and reception. However, when one of the transmitter and the receiver of the ultrasonic flow meter is arranged on the casing or bend of the pipeline (i.e., the thickness of the pipeline is too thick), the ultrasonic signal emitted by the transmitter may be affected (the additional time difference generated cannot be detected, or the signal is excessively attenuated) and cannot reach the receiver. Therefore, the existing ultrasonic flow meter is still not dynamically applicable to measure the flow rate of the fluid transported by the pipeline of any thickness.
本揭示之主要目的,在於提供一種超音波流量計以及流量檢測方法,可防止因為管道的內徑中的沉積造成的差異,或者外徑有套管或轉接管道造成外徑不同厚度,而無法依照標準設定的管道內徑值以及外徑值,尋找到超音波訊號的情況發生(傳輸時間與標準時間之間的時間差無法偵測,或訊號過度衰減)。。 The main purpose of this disclosure is to provide an ultrasonic flowmeter and flow detection method, which can prevent the situation that the ultrasonic signal cannot be found according to the standard set inner diameter and outer diameter values of the pipeline due to differences caused by sedimentation in the inner diameter of the pipeline, or different outer diameter thicknesses caused by sleeves or adapter pipes on the outer diameter (the time difference between the transmission time and the standard time cannot be detected, or the signal is excessively attenuated). .
為了達成上述之目的,本揭示的超音波流量計,設置於一非均勻厚度管道,其中該超音波流量計包括:一種超音波流量計,包括:一第一感測器以及一第二感測器,經配置以發射以及接收一訊號;以及一處理電路,耦接該第一感測器以及該第二感測器,經配置以執行以下步驟:(a)控制該第一感測器以及該第二感測器於一發射時間週期中分別發射一第一發射超音波訊號以及一第二發射超音波訊號;(b)控制該第二感測器接收該第一發射超音波訊號,並控制該第一感測器接收該第二發射超音波訊號; (c)檢測該第二感測器所接收的該第一發射超音波訊號的一第一訊號穩定度以及該第一感測器所接收的該第二發射超音波訊號的一第二訊號穩定度是否大於一穩定度閾值;(d)當該第一訊號穩定度或該第二訊號穩定度不大於該穩定度閾值時,增加該第一發射超音波訊號以及該第二發射超音波訊號各自的一發射次數,並調整指示該第一感測器以及該第二感測器各自的一安裝位置的一位置參數,並回到步驟(a);以及(e)當該第一訊號穩定度以及該第二訊號穩定度大於該穩定度閾值時,根據發射該第一發射超音波訊號的時間、接收該第一發射超音波訊號的時間、發射該第二發射超音波訊號的時間以及接收該第二發射超音波訊號的時間,計算流體的流量。 In order to achieve the above-mentioned purpose, the ultrasonic flowmeter disclosed in the present invention is arranged in a non-uniform thickness pipeline, wherein the ultrasonic flowmeter comprises: an ultrasonic flowmeter, comprising: a first sensor and a second sensor, configured to transmit and receive a signal; and a processing circuit, coupled to the first sensor and the second sensor, configured to perform the following steps: (a) controlling the first sensor and the second sensor to transmit a first transmission ultrasonic signal and a second transmission ultrasonic signal respectively in a transmission time cycle; (b) controlling the second sensor to receive the first transmission ultrasonic signal, and controlling the first sensor to receive the second transmission ultrasonic signal; (c) detecting a first signal stability of the first transmission ultrasonic signal received by the second sensor and whether a second signal stability of the second transmitted ultrasonic signal received by the first sensor is greater than a stability threshold; (d) when the first signal stability or the second signal stability is not greater than the stability threshold, increasing the number of transmissions of the first transmitted ultrasonic signal and the second transmitted ultrasonic signal, and adjusting the indication of the first sensor and the second sensor, respectively; a position parameter of an installation position, and return to step (a); and (e) when the first signal stability and the second signal stability are greater than the stability threshold, the flow rate of the fluid is calculated according to the time of emitting the first ultrasonic signal, the time of receiving the first ultrasonic signal, the time of emitting the second ultrasonic signal, and the time of receiving the second ultrasonic signal.
為了達成上述之目的,本揭示的流量檢測方法,應用於設置於一非均勻厚度管道的一超音波流量計,其中該超音波流量計包括一第一感測器、一第二感測器以及一處理電路,其中該流量檢測方法包括:(a)利用該處理電路控制該第一感測器以及該第二感測器於一發射時間週期中分別發射第一發射超音波訊號以及一第二發射超音波訊號;(b)利用該處理電路控制該第二感測器接收該第一發射超音波訊號,並控制該第一感測器接收該第二發射超音波訊號;(c)利用該處理電路檢測該第二感測器所接收的該第一發射超音波訊號的一第一訊號穩定度以及該第一感測器所接收的該第二發射超音波訊號的一第二訊號穩定度是否大於一穩定度閾值; (d)當該第一訊號穩定度或該第二訊號穩定度不大於該穩定度閾值時,利用該處理電路增加該第一發射超音波訊號以及該第二發射超音波訊號各自的一發射次數,並調整該非均勻厚度管道的一內徑參數以及一外徑參數,進而回到步驟(a);以及(e)當該第一訊號穩定度以及該第二訊號穩定度大於該穩定度閾值時,利用該處理電路根據發射該第一發射超音波訊號的時間、接收該第一發射超音波訊號的時間、發射該第二發射超音波訊號的時間以及接收該第二發射超音波訊號的時間,計算流體的流量。 In order to achieve the above-mentioned purpose, the flow detection method disclosed in the present invention is applied to an ultrasonic flow meter installed in a non-uniform thickness pipeline, wherein the ultrasonic flow meter includes a first sensor, a second sensor and a processing circuit, wherein the flow detection method includes: (a) using the processing circuit to control the first sensor and the second sensor to respectively transmit a first transmission ultrasonic signal and a second transmission ultrasonic signal in a transmission time cycle; (b) using the processing circuit to control the second sensor to receive the first transmission ultrasonic signal, and control the first sensor to receive the second transmission ultrasonic signal; (c) using the processing circuit to detect a first signal stability of the first transmission ultrasonic signal received by the second sensor and a second signal stability of the first transmission ultrasonic signal received by the first sensor (d) when the first signal stability or the second signal stability is not greater than the stability threshold, the processing circuit is used to increase the number of shots of the first ultrasonic signal and the second ultrasonic signal, and adjust an inner diameter parameter and an outer diameter parameter of the non-uniform thickness pipe. number, and then return to step (a); and (e) when the first signal stability and the second signal stability are greater than the stability threshold, the processing circuit is used to calculate the flow rate of the fluid according to the time of transmitting the first ultrasonic signal, the time of receiving the first ultrasonic signal, the time of transmitting the second ultrasonic signal, and the time of receiving the second ultrasonic signal.
相較於相關技術,本揭示可達到的技術效果為利用判斷超音波訊號的傳輸穩定度是否過低的方法增加超音波訊號在固定發射周期內的發射次數,以防止因為管道的管壁以及管道接頭的管壁而無法正確傳輸超音波訊號,進而無法測量管道內的流體的流量。 Compared with the related technologies, the technical effect achieved by the present disclosure is to increase the number of ultrasonic signal emissions within a fixed emission cycle by judging whether the transmission stability of the ultrasonic signal is too low, so as to prevent the ultrasonic signal from being unable to be correctly transmitted due to the pipe wall and the pipe joint wall, thereby preventing the flow rate of the fluid in the pipe from being unable to be measured.
100:超音波流量計 100: Ultrasonic flow meter
110(a):第一感測器 110(a): First sensor
110(b):第二感測器 110(b): Second sensor
120:處理電路 120: Processing circuit
S1~S2:外表面 S1~S2: outer surface
us:第一發射超音波訊號 us:First emission of ultrasonic signal
ds:第二發射超音波訊號 ds: Second ultrasonic signal transmission
PP:管道 PP: Pipeline
PF:管道接頭 PF: Pipe fitting
FD:流動方向 FD: Flow direction
r1:內徑 r1: inner diameter
r2~r3:外徑 r2~r3: outer diameter
RT:發射時間週期 RT: Transmit time cycle
WT:開窗時間週期 WT: window time period
tt1~tt2、tt1’:花費時間 tt1~tt2, tt1’: Spending time
△t:時間差 △t: time difference
△t’:傳輸時間差 △t’: Transmission time difference
S410~S470:步驟 S410~S470: Steps
t1~t2:時間點 t1~t2: time point
DAC1~DAC2:曲線 DAC1~DAC2: curve
LL:下限值 LL: Lower limit
圖1A繪示在一些實施例中的超音波流量計的縱截面示意圖。 FIG. 1A is a schematic diagram of a longitudinal cross-section of an ultrasonic flow meter in some embodiments.
圖1B繪示在一些實施例中的超音波流量計的方塊圖。 FIG. 1B is a block diagram of an ultrasonic flow meter in some embodiments.
圖2A繪示在一些實施例中的第一感測器以及第二感測器的設置方法的示意圖。 FIG2A is a schematic diagram showing a method for setting up the first sensor and the second sensor in some embodiments.
圖2B繪示在一些實施例中的第一感測器以及第二感測器的設置方法的示意圖。 FIG2B is a schematic diagram showing a method for setting up the first sensor and the second sensor in some embodiments.
圖3繪示在一般情況下的超音波訊號的波形的示意圖。 Figure 3 shows a schematic diagram of the waveform of an ultrasonic signal under normal circumstances.
圖4繪示在一些實施例中的流量檢測方法的流程圖。 FIG4 is a flow chart showing a flow detection method in some embodiments.
圖5繪示在一些實施例中的超音波訊號的比較的波形的示意圖。 FIG5 is a schematic diagram showing comparative waveforms of ultrasonic signals in some embodiments.
圖6繪示在一些實施例中的接收的第一發射超音波訊號的波形的細部示意圖。 FIG6 is a detailed schematic diagram showing the waveform of the received first transmitted ultrasonic signal in some embodiments.
圖7繪示在另一些實施例中的超音波訊號的波形的示意圖。 FIG7 is a schematic diagram showing the waveform of an ultrasonic signal in some other embodiments.
圖8繪示在另一些實施例中的接收超音波訊號的波形的細部示意圖。 FIG8 is a detailed schematic diagram of the waveform of the received ultrasonic signal in some other embodiments.
圖9繪示在一些實施例中的流量檢測方法進一步包括的步驟的流程圖。 FIG9 is a flow chart showing the steps further included in the flow detection method in some embodiments.
圖10繪示在一些實施例中的接收超音波訊號的距離波幅曲線的示意圖。 FIG10 is a schematic diagram showing a distance amplitude curve of a received ultrasonic signal in some embodiments.
圖11繪示在一些實施例中的流量檢測方法其中一步驟包括的步驟的流程圖。 FIG11 is a flow chart showing the steps included in one step of a flow detection method in some embodiments.
同時參照圖1A以及圖1B,圖1A繪示在一些實施例中的超音波流量計100的縱截面示意圖,以及圖1B繪示在一些實施例中的超音波流量計100的方塊圖。如圖1A以及圖1B所示,本揭示的超音波流量計100包括第一感測器(transducer)110(a)、第二感測器110(b)以及處理電路120,其中處理電路120耦接第一感測器110(a)以及第二感測器110(b)。
Referring to FIG. 1A and FIG. 1B, FIG. 1A is a schematic diagram of a longitudinal section of an
在一些實施例中,第一感測器110(a)以及第二感測器110(b)可以由任意的超音波感測元件或電路實現。在一些實施例中,處理電路120可以由中央處理單元(central processing unit,CPU)、微控制單元(micro control unit,
MCU)、可程式化邏輯控制器(programmable logic controller,PLC)、系統單晶片(system on chip,SoC)或現場可程式邏輯閘陣列(field programmable gate array,FPGA)等實現,但不以此為限。
In some embodiments, the first sensor 110(a) and the second sensor 110(b) can be implemented by any ultrasonic sensing element or circuit. In some embodiments, the
在一些實施例中,超音波流量計100更可包括輸入介面(未繪示)以及記憶體(未繪示)。在一些實施例中,使用者可藉由輸入介面輸入流體類型、管道(pipe)PP以及管道接頭(pipe fitting)PF的平均外徑、管道的內徑r1、管道PP的管壁的厚度(即,r2-r1)、管道PP的材質、安裝的方式。在一些實施例中,處理電路120可根據上述輸入的資料從記憶體讀取對應的流體類型的聲速以及對應的管道PP的材質的聲速,並根據上述輸入的資料、對應的流體類型的聲速以及對應的管道PP的材質的聲速,計算出第一感測器110(a)與第二感測器110(b)之間的水平安裝距離、發射時間週期(或稱為前期波時間週期)、超音波傳遞時間。接著,處理電路120可根據發射時間週期以及超音波傳遞時間計算開窗時間(receiver window)週期,並在開窗時間週期中檢測出後續描述的時間差,其中開窗時間週期為可接收到超音波訊號的一個時間週期。值得注意的是,上述計算的方法皆為本領域常用的計算方式,因此,對此不進一步贅述。
In some embodiments, the
在本實施例中,第一感測器110(a)以及第二感測器110(b)是成對設置在流通管路的管道PP的外表面S1以及管道接頭PF的外表面S2之同一線的位置上(即,本領域常用的V法)。然而,第一感測器110(a)以及第二感測器110(b)的成對設置並不以圖1A所示為限制,意即在其他的實施例中,第一感測器110(a)以及第二感測器110(b)可採用其他種設置方式(例如,本領域常用的Z法、N法或W法)。值得注意的是,由於管道接頭PF套接於管道PP(即,可視為非均勻厚度管道),這將造成設置第一感測器110(a)的管道PP的外徑r2以及設置第二 感測器110(b)的管道接頭PF的外徑r3並不相同,這時候合理的管道外徑範圍將落在設置第一感測器110(a)的管道PP的外徑r2以及設置第二感測器110(b)的管道接頭PF的外徑r3範圍間。舉例而言,可取對外徑r2以及外徑r3之間的平均值做為上述平均外經,並利用此平均外經進行上述段落的計算,但並不限於此方式設定。 In this embodiment, the first sensor 110 (a) and the second sensor 110 (b) are arranged in pairs on the same line of the outer surface S1 of the pipe PP of the flow pipeline and the outer surface S2 of the pipe joint PF (i.e., the V method commonly used in the art). However, the pair arrangement of the first sensor 110 (a) and the second sensor 110 (b) is not limited to that shown in FIG. 1A, that is, in other embodiments, the first sensor 110 (a) and the second sensor 110 (b) can be arranged in other ways (e.g., the Z method, N method or W method commonly used in the art). It is worth noting that, since the pipe joint PF is sleeved on the pipe PP (i.e., it can be regarded as a pipe of non-uniform thickness), the outer diameter r2 of the pipe PP where the first sensor 110(a) is installed and the outer diameter r3 of the pipe joint PF where the second sensor 110(b) is installed are different. At this time, the reasonable pipe outer diameter range will fall between the outer diameter r2 of the pipe PP where the first sensor 110(a) is installed and the outer diameter r3 of the pipe joint PF where the second sensor 110(b) is installed. For example, the average value between the outer diameter r2 and the outer diameter r3 can be taken as the above average outer diameter, and the calculation in the above paragraph is performed using this average outer diameter, but it is not limited to this setting method.
在此雖以管道接頭PF為套管接頭為例,在其他實施例中,超音波流量計100也可應用於管道接頭PF為彎管接頭的情況。
Although the pipe connector PF is a sleeve connector as an example here, in other embodiments, the
以下以實際的例子說明第一感測器110(a)以及第二感測器110(b)的設置方法以及不同類型的管道接頭PF。一併參照圖2A,圖2A繪示在一些實施例中的第一感測器110(a)以及第二感測器110(b)的設置方法。如圖2A所示,圖2A與圖1A的不同之處在於管道接頭PF為彎管接頭,且第一感測器110(a)以及第二感測器110(b)皆設置於管道接頭PF的外表面S2上之彎折處的兩端。此外,圖2A與圖1A的不同之處更在於第一感測器110(a)會直接將第一發射超音波訊號us傳送至第二感測器110(b),第二感測器110(b)會直接將第二發射超音波訊號ds傳送至第一感測器110(a),其中第一發射超音波訊號us以及第二發射超音波訊號ds皆不會在管道PP產生如圖1A的反射(即,類似於Z法的傳遞方式)。在本實施例中,處理電路120也可利用上述相同的方法計算第一感測器110(a)與第二感測器110(b)之間的水平安裝距離、發射時間週期、超音波傳遞時間以及開窗時間週期。
The following is an actual example to illustrate the installation method of the first sensor 110 (a) and the second sensor 110 (b) and different types of pipe joints PF. Referring to FIG. 2A, FIG. 2A shows the installation method of the first sensor 110 (a) and the second sensor 110 (b) in some embodiments. As shown in FIG. 2A, the difference between FIG. 2A and FIG. 1A is that the pipe joint PF is a curved pipe joint, and the first sensor 110 (a) and the second sensor 110 (b) are both installed at the two ends of the bend on the outer surface S2 of the pipe joint PF. In addition, the difference between FIG. 2A and FIG. 1A is that the first sensor 110 (a) directly transmits the first transmitted ultrasonic signal us to the second sensor 110 (b), and the second sensor 110 (b) directly transmits the second transmitted ultrasonic signal ds to the first sensor 110 (a), wherein the first transmitted ultrasonic signal us and the second transmitted ultrasonic signal ds will not generate reflections in the pipe PP as shown in FIG. 1A (i.e., a transmission method similar to the Z method). In this embodiment, the
一併參照圖2B,圖2B繪示在一些實施例中的第一感測器110(a)以及第二感測器110(b)的設置方法。如圖2B所示,圖2B與圖1A的不同之處在於第一感測器110(a)以及第二感測器110(b)是採用Z法分別設置於管道PP的外表面
S1以及管道接頭PF的外表面S2上之不同一線的位置上。此外,圖2B與圖1A的不同之處更在於第一感測器110(a)會直接將第一發射超音波訊號us傳送至第二感測器110(b),第二感測器110(b)會直接將第二發射超音波訊號ds傳送至第一感測器110(a),其中第一發射超音波訊號us以及第二發射超音波訊號ds皆不會在管道PP產生如圖1A的反射(即,以Z法的傳遞方式)。在本實施例中,處理電路120也可利用上述相同的方法計算第一感測器110(a)與第二感測器110(b)之間的水平安裝距離、發射時間週期、超音波傳遞時間以及開窗時間週期。
Referring to FIG. 2B , FIG. 2B shows a method for setting the first sensor 110 (a) and the second sensor 110 (b) in some embodiments. As shown in FIG. 2B , the difference between FIG. 2B and FIG. 1A is that the first sensor 110 (a) and the second sensor 110 (b) are respectively set at different positions on the outer surface S1 of the pipe PP and the outer surface S2 of the pipe joint PF using the Z method. In addition, the difference between FIG. 2B and FIG. 1A is that the first sensor 110 (a) directly transmits the first transmitted ultrasonic signal us to the second sensor 110 (b), and the second sensor 110 (b) directly transmits the second transmitted ultrasonic signal ds to the first sensor 110 (a), wherein the first transmitted ultrasonic signal us and the second transmitted ultrasonic signal ds will not generate reflections in the pipe PP as shown in FIG. 1A (i.e., in the Z-method transmission mode). In this embodiment, the
再者,在一般情況下,第一感測器110(a)用以發射第一發射超音波訊號(ultrasonic signal)us與接收第二感測器110(b)所發射的第二發射超音波訊號ds,第二感測器110(b)用以發射第二發射超音波訊號ds與接收第一感測器110(a)所發射的第一發射超音波訊號us。第一感測器110(a)於相對於流通管路中之流體的流動方向FD(例如,從左而右流動的方向)斜向地發射第一發射超音波訊號us,且由第二感測器110(b)所接收。與此同時,第二感測器110(b)於相對於流通管路中之流體的相反流動方向(即,與流動方向FD相反的方向)斜向地發射第二發射超音波訊號ds,且由第一感測器110(a)所接收,如此便可從第一發射超音波訊號us以及第二發射超音波訊號ds在流體中之傳輸時間差來測量流量。 Furthermore, in general, the first sensor 110(a) is used to emit a first ultrasonic signal us and receive a second ultrasonic signal ds emitted by the second sensor 110(b), and the second sensor 110(b) is used to emit the second ultrasonic signal ds and receive the first ultrasonic signal us emitted by the first sensor 110(a). The first sensor 110(a) emits the first ultrasonic signal us obliquely relative to the flow direction FD of the fluid in the flow pipe (for example, the direction of flow from left to right), and the first ultrasonic signal us is received by the second sensor 110(b). At the same time, the second sensor 110(b) obliquely emits a second ultrasonic signal ds in the opposite flow direction of the fluid in the flow pipe (i.e., the direction opposite to the flow direction FD), and is received by the first sensor 110(a), so that the flow rate can be measured from the transmission time difference between the first ultrasonic signal us and the second ultrasonic signal ds in the fluid.
詳細而言,一併參照圖3,圖3繪示在一般情況下的第一發射超音波訊號us的波形以及第二發射超音波訊號ds的波形的示意圖。如圖1A以及圖3所示,第一感測器110(a)以及第二感測器110(b)會在發射時間週期RT中同時發出相同頻率(例如,3MHz)的訊號。第一感測器110(a)所發出的第一發射超音波訊號us會在管道PP中傳播,並經過一段時間之後,第二感測器110(b)會接收到第一感測器110(a)發出的第一發射超音波訊號us。相似地,第二感測器110(b)所 發出的發射超音波訊號ds也會在管道PP中傳播,並且第一感測器110(a)也會於一段時間之後接收到第二感測器110(b)發出的第二發射超音波訊號ds。由於液體的流動速度及流動方向FD與第一感測器110(a)所發出的第一發射超音波訊號us的傳播方向呈順向傳播(例如都是朝向管道PP的右側),因此第二感測器110(b)收到第一發射超音波訊號us的時間會早於第一感測器110(a)收到第二發射超音波訊號ds的時間。相對地,液體的流動速度及流動方向FD與第二感測器110(b)所發出的第二發射超音波訊號ds的傳播方向呈逆向傳播,因此第一感測器110(a)收到第二發射超音波訊號ds的時間會晚於第二感測器110(b)收到第一發射超音波訊號us的時間。 In detail, refer to FIG. 3 , which shows a waveform of the first transmitted ultrasonic signal us and a waveform of the second transmitted ultrasonic signal ds under normal circumstances. As shown in FIG. 1A and FIG. 3 , the first sensor 110 (a) and the second sensor 110 (b) simultaneously transmit signals of the same frequency (e.g., 3 MHz) in the transmission time period RT. The first transmitted ultrasonic signal us emitted by the first sensor 110 (a) propagates in the pipe PP, and after a period of time, the second sensor 110 (b) receives the first transmitted ultrasonic signal us emitted by the first sensor 110 (a). Similarly, the ultrasonic signal ds emitted by the second sensor 110(b) will also propagate in the pipe PP, and the first sensor 110(a) will also receive the second ultrasonic signal ds emitted by the second sensor 110(b) after a period of time. Since the flow velocity and flow direction FD of the liquid are in the same direction as the propagation direction of the first ultrasonic signal us emitted by the first sensor 110(a) (for example, both are toward the right side of the pipe PP), the time when the second sensor 110(b) receives the first ultrasonic signal us will be earlier than the time when the first sensor 110(a) receives the second ultrasonic signal ds. In contrast, the flow velocity and flow direction FD of the liquid are in the opposite direction to the propagation direction of the second ultrasonic signal ds emitted by the second sensor 110 (b), so the time when the first sensor 110 (a) receives the second ultrasonic signal ds will be later than the time when the second sensor 110 (b) receives the first ultrasonic signal us.
基於此,處理電路120在開窗時間週期WT中檢測第二感測器110(b)收到第一發射超音波訊號us的花費時間tt1以及第一感測器110(a)收到第二發射超音波訊號ds的花費時間tt2,並計算花費時間tt1以及花費時間tt2之間的時間差△t。接著,處理電路120採用時間差法(time of flight,TOF)以基於第一感測器110(a)以及第二感測器110(b)分別收到第二發射超音波訊號ds以及第一發射超音波訊號us之間的時間差△t來計算液體在管道PP中的流速及流量(即,超音波流量計100使用頻率3MHz所得到的測量值)。值得注意的是,本揭示不限制使用時間差法的原則所設計的計算流速及流量的公式。
Based on this, the
然而,由於第二感測器110(b)設置於管道接頭PF的外表面S2上,且第一發射超音波訊號us以及第二發射超音波訊號ds皆需要穿過管道PP的管壁以及管道接頭PF的管壁,過厚的管壁可能會導致第二感測器110(b)接收不到第一感測器110(a)發出的第一發射超音波訊號us或導致第一感測器110(a)接收不到第二感測器110(b)發出的第二發射超音波訊號ds,也可能導致第二感測器110(b) 接收到的第一發射超音波訊號us或第一感測器110(a)接收到的第二發射超音波訊號ds的訊號穩定度不佳(即,訊雜比(signal-to-noise ratio,SNR)過低)。此外,與一般設置方式相比,管道接頭PF更可能造成傳輸時間差(後續段落將進一步說明此傳輸時間差)。因此,流體的流速以及流量將無法藉由時間差法被計算出來。基於此,本揭示提出一種流量檢測方法以解決第二感測器110(b)以及第一感測器110(a)可能無法分別接收第一發射超音波訊號us以及第二發射超音波訊號ds或是訊號穩定度不佳的問題。此外,本揭示的流量檢測方法更藉由調整內徑參數以及外徑參數以消除上述傳輸時間差(即,適當的管道PP的內徑以及管道PP與管道接頭PF的平均外徑可修正傳輸時間差)。在一些實施例中,內徑參數包括管道PP的內徑,外徑參數包括管道PP以及管道接頭PF的平均外徑。詳細步驟將在後續段落說明,在此不進一步贅述。 However, since the second sensor 110(b) is disposed on the outer surface S2 of the pipe joint PF, and both the first transmitted ultrasonic signal us and the second transmitted ultrasonic signal ds need to pass through the pipe wall of the pipe PP and the pipe wall of the pipe joint PF, an excessively thick pipe wall may cause the second sensor 110(b) to fail to receive the first transmitted ultrasonic signal us emitted by the first sensor 110(a) or cause the first sensor 110(a) to fail to receive the second transmitted ultrasonic signal ds emitted by the second sensor 110(b), and may also cause the first transmitted ultrasonic signal us received by the second sensor 110(b) or the second transmitted ultrasonic signal ds received by the first sensor 110(a) to have poor signal stability (i.e., the signal-to-noise ratio (SNR) is too low). In addition, compared with the general setting method, the pipe joint PF is more likely to cause a transmission time difference (the subsequent paragraphs will further explain this transmission time difference). Therefore, the flow velocity and flow rate of the fluid cannot be calculated by the time difference method. Based on this, the present disclosure proposes a flow detection method to solve the problem that the second sensor 110 (b) and the first sensor 110 (a) may not be able to receive the first transmitted ultrasonic signal us and the second transmitted ultrasonic signal ds respectively or the signal stability is poor. In addition, the flow detection method disclosed in the present disclosure further eliminates the above-mentioned transmission time difference by adjusting the inner diameter parameters and the outer diameter parameters (that is, the appropriate inner diameter of the pipe PP and the average outer diameter of the pipe PP and the pipe joint PF can correct the transmission time difference). In some embodiments, the inner diameter parameter includes the inner diameter of the pipe PP, and the outer diameter parameter includes the average outer diameter of the pipe PP and the pipe joint PF. The detailed steps will be described in the subsequent paragraphs and will not be further elaborated here.
一併參照圖4,圖4繪示在一些實施例中的流量檢測方法的流程圖,此流量檢測方法適用於圖1A至圖1B所示的超音波流量計100。如圖4所示,首先,於步驟S410中,處理電路120控制第一感測器110(a)以及第二感測器110(b)於發射時間週期RT中發射第一發射超音波訊號us以及第二發射超音波訊號ds。在一些實施例中,在初始狀態(initial state)中,處理電路120可將第一發射超音波訊號us以及第二發射超音波訊號ds各自的發射次數設定為1。換言之,在初始狀態中,處理電路120可控制第一感測器110(a)於發射時間週期RT中發射一個順向傳播的第一發射超音波訊號us以及一個逆向傳播的第二發射超音波訊號ds。在其他實施例中,在初始狀態中,處理電路120也可將第一發射超音波訊號us以及第二發射超音波訊號ds各自的發射次數設定為其他正整數,並沒有特別的限制。
Referring to FIG. 4 , FIG. 4 is a flow chart of a flow detection method in some embodiments, and the flow detection method is applicable to the
於步驟S420中,處理電路120控制第二感測器110(b)接收第一發射超音波訊號us,並控制第一感測器110(a)接收第二發射超音波訊號ds。於步驟S430中,處理電路120檢測第二感測器110(b)所接收的第一發射超音波訊號us的第一訊號穩定度以及第一感測器110(a)所接收的第二發射超音波訊號ds的第二訊號穩定度是否大於穩定度閾值。當所接收的第一發射超音波訊號us的第一訊號穩定度或所接收的第二發射超音波訊號ds的第二訊號穩定度不大於穩定度閾值時,處理電路120執行步驟S440。反之,當所接收的第一發射次數的第一發射超音波訊號us的第一訊號穩定度以及所接收的第二發射超音波訊號ds的第二訊號穩定度大於穩定度閾值時,處理電路120執行步驟S450。
In step S420, the
在一些實施例中,訊雜比的閾值可預先被設定以及儲存於超音波流量計100的記憶體中。在一些實施例中,所述第一發射超音波訊號us的第一訊號穩定度為所接收的第一發射超音波訊號us的波形的訊雜比,其中穩定度閾值為訊雜比的閾值。在一些實施例中,處理電路120可從所接收的第一發射超音波訊號us計算出雜訊的平均值以及標準差。接著,處理電路120可採樣(sample)所接收的第一發射超音波訊號us的多個波峰值,並根據多個波峰值、雜訊的平均值以及雜訊的標準差計算所接收的第一發射超音波訊號us的波形的訊雜比。類似地,第二訊號穩定度也是以相似的方式從第二發射超音波訊號ds計算出來的,在此不進一步贅述。
In some embodiments, the threshold of the signal-to-noise ratio may be pre-set and stored in the memory of the
值得注意的是,由於從第一感測器110(a)所發送的第一發射超音波訊號us的頻率是已知的(例如,3MHz),處理電路120可根據所接收的第一發射超音波訊號us的頻率從所接收的第一發射超音波訊號us的波形辨識出雜訊,
並進一步地計算雜訊的大小的平均值以及標準差,其中此計算方式也是本領域習知的計算方式,因此,在此不進一步贅述。
It is worth noting that, since the frequency of the first transmitted ultrasonic signal us transmitted from the first sensor 110 (a) is known (e.g., 3 MHz), the
以下以實際的例子說明第一訊號穩定度以及穩定度閾值之間的比對。一併參照圖5,圖5繪示在一些實施例中的第一發射超音波訊號us的波形的比較的示意圖。如圖5所示,當存在管道接頭PF時,第一感測器110(a)於發射時間週期RT中發射特定頻率的一個第一發射超音波訊號us,且第二感測器110(b)於開窗時間週期WT中接收到第一感測器110(a)所發射的第一發射超音波訊號us。 The comparison between the stability of the first signal and the stability threshold is described below with an actual example. Referring to FIG. 5 , FIG. 5 is a schematic diagram showing a comparison of the waveform of the first transmitted ultrasonic signal us in some embodiments. As shown in FIG. 5 , when there is a pipe joint PF, the first sensor 110 (a) transmits a first transmitted ultrasonic signal us of a specific frequency in the transmission time period RT, and the second sensor 110 (b) receives the first transmitted ultrasonic signal us transmitted by the first sensor 110 (a) in the window time period WT.
值得注意的是,傳送第一發射超音波訊號us與接收第一發射超音波訊號us的時間之間存在花費時間tt1’。相較於圖3的不存在管道接頭PF的例子,花費時間tt1’與花費時間tt1之間存在一個傳輸時間差△t’。此傳輸時間差△t’是由管壁的厚度不平均而造成的。在後續段落的步驟S440中,處理電路120就可調整內徑參數以及外徑參數以讓使用者調整管道PP的內徑以及管道PP與管道接頭PF的平均外徑(例如,選用較薄的管道PP的內徑或較薄的平均外徑的管道PP與管道接頭PF以消除傳輸時間差△t’),進而根據內徑參數以及外徑參數改變管道PP的內徑以及管道PP與管道接頭PF的平均外徑。
It is worth noting that there is a time tt1' between the time of transmitting the first transmitted ultrasonic signal us and the time of receiving the first transmitted ultrasonic signal us. Compared with the example of FIG. 3 without the pipe joint PF, there is a transmission time difference △t' between the time tt1' and the time tt1. This transmission time difference △t' is caused by the uneven thickness of the pipe wall. In the subsequent step S440, the
接著,處理電路120檢測第二感測器110(b)所接收的第一發射超音波訊號us的訊雜比。進一步而言,一併參照圖6,圖6繪示在一些實施例中的接收第一發射超音波訊號us的波形的細部示意圖。如圖6所示,處理電路120根據特定頻率從第一發射超音波訊號us中辨識出在時間點t1之前以及時間點t2之後所接收到的訊號為雜訊,並根據雜訊的波峰值計算平均值以及標準差。接
著,處理電路120根據雜訊的平均值、雜訊的標準差以及時間點t1~t2之間的訊號的波峰值,計算第一發射超音波訊號us的訊雜比不大於穩定度閾值。
Next, the
回到圖4,於步驟S440中,處理電路120增加第一發射超音波訊號us以及第二發射超音波訊號ds各自的發射次數,並調整非均勻厚度管道的內徑參數以及外徑參數(即,如上述段落所述),進而回到步驟S410。換言之,一旦處理電路120發現第一訊號穩定度或第二訊號穩定度不大於穩定度閾值,處理電路120就會於步驟S410中控制第一感測器110(a)以及第二感測器110(b)於下一個發射時間週期RT中多發射一次第一發射超音波訊號us,並同步地提高第二感測器110(b)於下一個發射時間週期RT中發射第二發射超音波訊號ds的發射次數。此時,處理電路120會進一步調整非均勻厚度管道的內徑參數以及外徑參數(即,稍微降低參數數值(例如,降低10%)),進而繼續執行步驟S420~S430以繼續判斷第二感測器110(b)所接收的所有第一發射超音波訊號us的第一訊號穩定度以及第一感測器110(a)所接收的所有第二發射超音波訊號ds的第二訊號穩定度是否大於穩定度閾值。與此同時,管道PP的內徑以及管道PP與管道接頭PF的平均外徑會根據內徑參數以及外徑參數被調整(即,內徑以及平均外徑的數值會被調整為內徑參數以及外徑參數的數值)以消除不均勻管壁厚度造成的時間差以及增加第一訊號穩定度以及第二訊號穩定度。由此可知,當處理電路120檢測到第一訊號穩定度或第二訊號穩定度不大於穩定度閾值時,處理電路120就會同時增加第一發射超音波訊號us以及第二發射超音波訊號ds各自的發射次數以及調整非均勻厚度管道的內徑參數以及外徑參數。本揭示中,處理電路120會一直執行步驟S410到步驟S440,直到第一訊號穩定度以及第二訊號穩定度已經大於穩定度閾值時,處理電路120才會執行步驟S450。
Returning to FIG. 4 , in step S440 , the
以下以實際的例子說明在處理電路120增加了第一發射超音波訊號us的發射次數(以增加一次為例)後,第一訊號穩定度以及穩定度閾值之間的比對。一併參照圖7,圖7繪示在另一些實施例中的第一發射超音波訊號us的波形的示意圖。如圖7所示,第一感測器110(a)於發射時間週期RT中發射特定頻率的兩個第一發射超音波訊號us(此時,第一感測器110(a)於發射時間週期RT中也會發射特定頻率的兩個第二發射超音波訊號ds),且第二感測器110(b)於開窗時間週期WT中接收到第一感測器110(a)所發射的第一發射超音波訊號us。接著,處理電路120檢測第二感測器110(b)所接收的第一發射超音波訊號us的訊雜比。進一步而言,一併參照圖8,圖8繪示在另一些實施例中的接收第一發射超音波訊號us的波形的細部示意圖。如圖8所示,處理電路120根據特定頻率從第一發射超音波訊號us中辨識出在時間點t1之前以及時間點t2之後所接收到的訊號為雜訊,並根據雜訊的波峰值計算平均值以及標準差。接著,處理電路120根據雜訊的平均值、雜訊的標準差以及時間點t1~t2之間的訊號的波峰值,計算第一發射超音波訊號us的訊雜比大於穩定度閾值。此時,處理電路120開始執行上述步驟S450。值得注意的是,第二發射超音波訊號ds的訊雜比也是以相似方式從第二發射超音波訊號ds計算來的。第二發射超音波訊號ds的訊雜比也是以相似方式與穩定度閾值進行比較。因此,在此不進一步贅述。
The following is an actual example to illustrate the comparison between the stability of the first signal and the stability threshold after the
基於上述,處理電路120藉由判斷第一訊號穩定度以及第二訊號穩定度是否大於穩定度閾值的方法,將可辨識出所接收到的第一發射超音波訊號us的波峰值會不會過低(即,管道PP的管壁以及管道接頭PF的管壁阻擋掉第一發射超音波訊號us的大部分的能量),或者是辨識出所接收到的第二發射超音波訊號ds的波峰值會不會過低(即,管道PP的管壁以及管道接頭PF的管壁阻擋
掉第二發射超音波訊號ds的大部分的能量),進而判斷是否要提高發射第一發射超音波訊號us的次數以及第二發射超音波訊號ds的次數(即,進一步提高第一發射超音波訊號us的發射能量以及第二發射超音波訊號ds的發射能量)。
Based on the above, the
在一些實施例中,處理電路120可判斷第一發射超音波訊號us的增加後的發射次數是否大於次數閾值。當第一發射超音波訊號us的增加後的發射次數不大於預設的次數閾值時,處理電路120可繼續執行步驟S410。反之,當第一發射超音波訊號us的增加後的發射次數大於次數閾值時,處理電路120可產生警告訊息。在一些實施例中,警告訊息指示目前設置的第一感測器110(a)以及第二感測器110(b)的類型,或是第一感測器110(a)以及第二感測器110(b)的設置方法或設置位置,無法檢測到超音波在流體中的第一傳輸時間。值得注意的是,本揭示的流量檢測方法也會根據第二發射超音波訊號ds的增加後的發射次數以相似的方法判斷是否產生警告訊息。
In some embodiments, the
基於上述,處理電路120藉由判斷第一發射超音波訊號us的增加後的發射次數或第二發射超音波訊號ds的增加後的發射次數是否大於次數閾值的方法,將可避免因為過多的發射次而造成超音波流量計100的耗能過大。於一實施例中,所述次數閾值係與超音波流量計100的類型相關,但不以此為限。
Based on the above, the
回到圖4,於步驟S450中,處理電路120根據發射第一發射超音波訊號us的時間、接收第一發射超音波訊號us的時間、發射第二發射超音波訊號ds的時間以及接收第二發射超音波訊號ds的時間,計算流體的流量(即,流體在管道PP中的流量)。
Returning to FIG. 4 , in step S450 , the
一併參照圖9,圖9繪示在一些實施例中的流量檢測方法進一步包括的步驟S460~S470的流程圖。如圖9所示,首先,當第一訊號穩定度大於穩定度閾值時,處理電路120更可執行步驟S460。於步驟S460中,處理電路120檢測第二感測器110(b)所接收的第一發射超音波訊號us的距離波幅曲線(distance amplitude curve,DAC)的數值。於步驟S470中,處理電路120根據第一發射超音波訊號us的距離波幅曲線的數值、下限值以及第一發射超音波訊號us的發射次數,調整第一發射超音波訊號us的發射次數,並回到步驟S410。
Referring to FIG. 9 , FIG. 9 is a flow chart showing steps S460 to S470 further included in the flow detection method in some embodiments. As shown in FIG. 9 , first, when the stability of the first signal is greater than the stability threshold, the
在一些實施例中,處理電路120可檢測第二感測器110(b)所接收的第一發射超音波訊號us的距離波幅曲線的數值是否皆大於預設的下限值。當所接收的第一發射超音波訊號us的距離波幅曲線的數值中的至少一者不大於下限值時,處理電路120可繼續執行步驟S410。當所接收的第一發射超音波訊號us的距離波幅曲線的數值皆大於下限值時,處理電路120可判斷第一發射超音波訊號us的發射次數是否大於一。在一些實施例中,當判斷第一發射超音波訊號us的發射次數不大於一時,處理電路120可繼續執行步驟S410。當判斷第一發射超音波訊號us的發射次數大於一時,處理電路120可減少第一發射超音波訊號us的發射次數(例如減一),並依據第一發射超音波訊號us的減少後的發射次數繼續執行步驟S410。值得注意的是,本揭示流量檢測方法也會以相似的方法根據第二發射超音波訊號ds的距離波幅曲線調整第二發射超音波訊號ds的發射次數,因此,在此不進一步贅述。
In some embodiments, the
基於上述,處理電路120藉由判斷波幅距離曲線的數值是否大於下限值的方法,將可避免因為過多的發射次數造成波幅距離曲線的數值過大的問題,進而降低超音波流量計100的耗能。
Based on the above, the
以下以實際的例子說明距離波幅曲線的數值與下限值的比較。一併參照圖10,圖10繪示在一些實施例中的接收第一發射超音波訊號us的距離波幅曲線的示意圖。如圖10所示,假設第二感測器110(b)接收的第一發射超音波訊號us的距離波幅曲線為曲線DAC1,則處理電路120在判斷曲線DAC1上的數值皆大於下限值LL時,會進一步判斷第一感測器110(a)的第一發射超音波訊號us的發射次數是否大於一。假設第二感測器110(b)接收的第一發射超音波訊號us的距離波幅曲線為曲線DAC2,則處理電路120會判斷曲線DAC2上的數值未皆大於下限值LL,並且直接繼續執行上述步驟S410。
The following is an actual example to illustrate the comparison between the numerical value of the distance amplitude curve and the lower limit value. Referring to FIG. 10 , FIG. 10 is a schematic diagram of the distance amplitude curve of the first transmitted ultrasonic signal us in some embodiments. As shown in FIG. 10 , assuming that the distance amplitude curve of the first transmitted ultrasonic signal us received by the second sensor 110 (b) is the curve DAC1, when the
一併參照圖11,圖11繪示在一些實施例中的流量檢測方法的其中一步驟S450進一步包括的步驟S451~S453的流程圖,此流量檢測方法的其中一步驟S450包括的步驟也適用於圖1A至圖1B所示的超音波流量計100。如圖11所示,首先,於步驟S451中,處理電路120根據發射第一發射超音波訊號us的時間以及接收第一發射超音波訊號us的時間,測量超音波在流體中的第一傳輸時間(即,順向傳播時間)。
Referring to FIG. 11 , FIG. 11 is a flow chart showing steps S451 to S453 further included in one step S450 of the flow detection method in some embodiments. The steps included in one step S450 of the flow detection method are also applicable to the
於步驟S452中,處理電路120根據發射第二超音波訊號ds的時間以及接收第二超音波訊號ds的時間,測量超音波在流體中的第二傳輸時間(即,逆向傳播時間)。於步驟S453中,處理電路120根據第一傳輸時間以及第二傳輸時間計算流體的流量在一些實施例中,處理電路120可計算第一傳輸時間以及第二傳輸時間之間的時間差,進而根據此時間差利用上述的時間差法計算出流體的流速及流量。
In step S452, the
舉例而言,以圖3的例子來看,如圖3所示,處理電路120計算第一感測器110(a)發射第一發射超音波訊號us的第一個波峰值的時間與第二感測
器110(b)接收第一發射超音波訊號us的第一個波峰值的時間之間的差值(即,花費時間tt1)。接著,處理電路120計算第二感測器110(b)發射第二發射超音波訊號ds的第一個波峰值的時間與第一感測器110(a)接收第二發射超音波訊號ds的第一個波峰值的時間之間的差值(即,花費時間tt2)。接著,處理電路120根據花費時間tt1以及花費時間tt2之間的時間差計算流體的流量。
For example, in the example of FIG. 3, as shown in FIG. 3, the
綜上所述,本揭示提出的超音波流量計以及流量檢測方法根據所接收的發射超音波訊號的穩定度判斷要不要增加發射超音波訊號在固定的發射時間週期內的發射次數,以測量出發射超音波訊號在流體中的順向傳播以及逆向傳播所花費的時間。藉此,可防止因為管道的管壁以及管道接頭的管壁阻擋掉發射超音波訊號的大部分的能量,而無法有效測量流體的流量。此外,本揭示提出的超音波流量計以及流量檢測方法更判斷發射超音波訊號的發射次數是否大於次數閾值,以避免因為過多的發射次數而造成耗能過大。另一方面而言,本揭示提出的超音波流量計以及流量檢測方法還判斷波幅距離曲線的數值是否大於下限值以避免因為過多的發射次數而造成波幅距離曲線的數值過大的問題。 In summary, the ultrasonic flowmeter and flow detection method proposed in the present disclosure determine whether to increase the number of transmissions of the ultrasonic signal within a fixed transmission time period according to the stability of the received transmission ultrasonic signal, so as to measure the time taken for the transmission ultrasonic signal to propagate forward and backward in the fluid. In this way, it is possible to prevent the flow of the fluid from being effectively measured due to the pipe wall and the pipe wall of the pipe joint blocking most of the energy of the transmission ultrasonic signal. In addition, the ultrasonic flowmeter and flow detection method proposed in the present disclosure further determine whether the number of transmissions of the ultrasonic signal is greater than the number threshold, so as to avoid excessive energy consumption due to too many transmissions. On the other hand, the ultrasonic flow meter and flow detection method proposed in this disclosure also determine whether the value of the amplitude-distance curve is greater than the lower limit value to avoid the problem of the amplitude-distance curve value being too large due to too many transmission times.
以上所述僅為本揭示之較佳具體實例,非因此即侷限本揭示之專利範圍,故舉凡運用本揭示內容所為之等效變化,均同理皆包含於本揭示之範圍內,合予陳明。 The above is only a preferred specific example of this disclosure, and does not limit the patent scope of this disclosure. Therefore, all equivalent changes made by applying the content of this disclosure are also included in the scope of this disclosure and are hereby stated.
100:超音波流量計 100: Ultrasonic flow meter
110(a):第一感測器 110(a): First sensor
110(b):第二感測器 110(b): Second sensor
120:處理電路 120: Processing circuit
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| TW523580B (en) * | 2001-02-05 | 2003-03-11 | Surpass Ind Co Ltd | Ultrasonic flow meter |
| CN1643346A (en) * | 2002-03-14 | 2005-07-20 | 恩德斯+豪斯流量技术股份有限公司 | Coriolis mass flow meter with vortex generator |
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