TWI452267B - Tdr apparatus and method for liquid level and scour measurements - Google Patents
Tdr apparatus and method for liquid level and scour measurements Download PDFInfo
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本發明係有關一種可同時量測液面與刷深行為之裝置與方法,特別是關於一種利用時域反射法(time domain reflectometry,TDR)來量測液面與刷深之量測裝置及其方法,以藉此同時監測液面與沖刷深度變化。The invention relates to a device and a method for simultaneously measuring liquid level and brush depth behavior, in particular to a measuring device for measuring liquid level and brush depth by using time domain reflectometry (TDR) The method is used to simultaneously monitor the change in liquid level and scouring depth.
時域反射法(TDR)為一種電磁波感應技術,電磁波之傳輸系統包括作為延長線的同軸纜線與感測導波器(Waveguide),導波器為同軸纜線之延伸,同時作為訊號傳輸與感測元件,導波器之設計主要在將所需監測之環境變化轉換為感測導波器之傳輸阻抗變化,如此可藉由反射訊號得知環境變化參數。導波器為將電磁波從同軸纜線延伸導入待測介質的導波器。TDR含水量導波器通常是由兩根或三根導體桿所組成,如Yu and Yu(2010)提出三根導體型式,而Yankielun and Zabilansky(1999)提出之TDR沖刷導波器型式,則為利用兩根鋼管形成感測導波器。前述技術與一般TDR含水量導波器雷同,只是尺寸較大,在現地應用時,導波器底部可加裝一鋼管帶動貫入(U.S.Patent # 6,909,669),其他相關美國專利也都基於相同概念,例如,美國專利US 6,541,985、6,121,894、6,100,700及5,784,338等。但上述型式在實務上應用,尤其是在台灣地區,仍存在有下列潛在問題:Time Domain Reflectometry (TDR) is an electromagnetic wave sensing technology. The electromagnetic wave transmission system includes a coaxial cable and a waveguide as an extension cable. The waveguide is an extension of the coaxial cable and serves as a signal transmission and transmission. The sensing component, the waveguide is designed to convert the environmental change of the desired monitoring into the transmission impedance change of the sensing waveguide, so that the environmental variation parameter can be known by the reflected signal. The waveguide is a waveguide that extends electromagnetic waves from the coaxial cable into the medium to be tested. The TDR water content waveguide is usually composed of two or three conductor rods. For example, Yu and Yu (2010) propose three conductor types, while Yankielun and Zabilansky (1999) propose the TDR erosion wave guide type. The root steel tube forms a sensing waveguide. The above technology is similar to the general TDR water content waveguide, but the size is large. When used in the field, a steel pipe can be installed on the bottom of the waveguide (US Patent # 6,909,669). Other related US patents are also based on the same concept. For example, U.S. Patents 6,541,985, 6,121,894, 6,100,700 and 5,784,338, and the like. However, the above-mentioned types are applied in practice, especially in Taiwan, and the following potential problems still exist:
一般河水與河床質均有一定的導電度,導電度將造成電磁波傳遞隨距離而衰減,因此一般土壤含水量的導波器很少超過1公尺,若直接採用類似土壤含水量的導波器,沖刷感測範圍勢必相當有限,不適合台灣許多河 段劇烈沖刷的觀測。以Yankielun and Zabilansky(1999)與Yu and Yu(2010)提出導波器初步測試,可以發現訊號衰減隨水深增加而增加的現象,預計若導波器與水深超過2公尺以上,水土界面以及導波器末端的反射訊號將會難以分辨。Generally, river water and riverbed have a certain degree of electrical conductivity, and the conductivity will cause the electromagnetic wave transmission to decay with distance. Therefore, the general soil water content of the waveguide is rarely more than 1 meter. If a waveguide similar to soil water content is directly used, The scouring sensing range is bound to be quite limited and is not suitable for many rivers in Taiwan. The observation of the violent scouring. Yankielun and Zabilansky (1999) and Yu and Yu (2010) proposed a preliminary test of the waveguide, which can be found that the signal attenuation increases with the increase of water depth. It is expected that if the waveguide and the water depth exceed 2 meters, the water-soil interface and the guide The reflected signal at the end of the wave will be difficult to distinguish.
上述相關類似土壤含水量導波器的型式並不適合現地沖刷監測的安裝,在沖積河床尚可以在導波器底部加裝一鋼管帶動貫入,但並不適合礫石或岩質河床之應用,且當沖刷感測範圍超過3公尺以上時,勢必導波器必須分段在現場連接,這些安裝實務問題都需要考慮。此外,上述之剛性感測器在夾雜塊石與高流速的河川環境下,其耐衝擊性堪虞,特別是當刷深較深時,可能容易變形損壞。The above-mentioned type of soil water-conducting wave guide is not suitable for installation of in-situ flushing monitoring. In the alluvial riverbed, a steel pipe can be installed at the bottom of the wave guide to drive through, but it is not suitable for gravel or rocky riverbed applications, and when scouring When the sensing range is more than 3 meters, the waveguide must be segmented and connected in the field. These installation practical issues need to be considered. In addition, the above-mentioned rigid sensor has an impact resistance in a river environment with a mixed stone and a high flow velocity, and particularly when the brush depth is deep, it may be easily deformed and damaged.
TDR量測由於接頭、水-土界面及導波器末端產生的反射訊號,當水位低於TDR導波器頂部時,尚有空氣-水界面的反射訊號,在如此複雜的反射訊號要決定沖刷深度並非簡易或容易自動化的工作。若電磁波由下往上傳遞,可以確保在水-土界面反射之前沒有空氣-水界面的反射訊號,水-土界面反射訊號較容易分辨,但如此的配置將使得導波器的安裝困難度增加。若電磁波由上往下且當水位低於導波器頂部時,在水-土界面反射發生之前即產生接頭、空氣-水界面反射及之間的多重反射,造成水-土界面反射訊號較難以分辨。基於上述分析複雜度,亦即無法穩定快速地提供一自動化有效的分析演算流程。The TDR measures the reflected signal generated by the joint, the water-soil interface and the end of the waveguide. When the water level is lower than the top of the TDR waveguide, there is still a reflection signal at the air-water interface. In such a complex reflection signal, the scouring signal is determined. Depth is not an easy or easy to automate job. If the electromagnetic wave is transmitted from bottom to top, it can ensure that there is no reflection signal at the air-water interface before the water-soil interface is reflected. The water-soil interface reflection signal is easier to distinguish, but such a configuration will increase the difficulty of installation of the waveguide. . If the electromagnetic wave is from top to bottom and when the water level is lower than the top of the waveguide, the joint, the air-water interface reflection and the multiple reflection between the water-soil interface will cause the water-soil interface to reflect the signal more difficult. Resolve. Based on the above analysis complexity, it is impossible to provide an automated and efficient analysis and calculation process stably and quickly.
有鑑於此,本發明提出一種時域反射式液面與刷深之量測裝置及其方 法,以改善上述缺失。In view of this, the present invention provides a time domain reflective liquid level and brush depth measuring device and a method thereof Law to improve the above-mentioned deficiency.
本發明之主要目的係在提供一種時域反射式液面與刷深量測裝置,其係利用時域反射法同時量測液面與刷深行為,藉以同時監測液面與沖刷深度變化,採用結合類似地錨鋼索的導波器設計,提出符合安裝實務的設計,並考慮導體絕緣處理,解決訊號衰減問題。The main object of the present invention is to provide a time domain reflective liquid level and brush depth measuring device, which simultaneously measures the liquid surface and the brush depth behavior by using the time domain reflection method, thereby simultaneously monitoring the liquid surface and the scouring depth change. Combined with the design of the waveguide of similar anchor cable, the design conforming to the installation practice is proposed, and the conductor insulation treatment is considered to solve the signal attenuation problem.
本發明之另一目的係在提供一種時域反射式液面與刷深量測方法,其係為量測液面與沖刷深度的訊號分析演算法,基於不同介質之電磁波速不同,本發明結合反射訊號辨識與波傳速度標定與分析流程,提出一種較可靠的訊號分析演算法。Another object of the present invention is to provide a time domain reflection type liquid level and brush depth measurement method, which is a signal analysis algorithm for measuring liquid level and scouring depth, and the invention combines different electromagnetic wave speeds based on different media. Reflective signal identification and wave velocity calibration and analysis process, a more reliable signal analysis algorithm is proposed.
為達到上述目的,本發明之時域反射式液面與刷深量測裝置,其係安裝於一待監測環境,以監測其液面與沖刷深度變化,此液面與刷深之量測裝置包括有至少一同軸纜線,其係利用一轉接探頭連接一時域反射式金屬感測導波器,同軸纜線傳送一時域反射儀產生之電磁脈波至金屬感測導波器,其係接收電磁脈波並根據該深度變化產生一反射訊號傳回至同軸纜線,以利用同軸纜線傳輸回時域反射儀;並有至少一錨定器連接金屬感測導波器末端,以固定金屬感測導波器。In order to achieve the above object, the time domain reflective liquid level and brush depth measuring device of the present invention is installed in a environment to be monitored to monitor the change of liquid level and scouring depth, and the measuring device for the liquid surface and the brush depth The invention comprises at least one coaxial cable, which uses a transit probe to connect a time domain reflective metal sensing waveguide, and the coaxial cable transmits an electromagnetic pulse wave generated by a time domain reflectometer to the metal sensing waveguide. Receiving electromagnetic pulse waves and generating a reflection signal according to the depth change and transmitting back to the coaxial cable to transmit back to the time domain reflectometer by using the coaxial cable; and having at least one anchor connected to the metal sensing waveguide end to fix Metal sensing waveguide.
本發明之另一實施態樣則為一種時域反射式液面與刷深量測方法,其係利用前述之液面與刷深量測裝置對待監測環境進行液面與沖刷深度變化的量測,此量測方法包括下列步驟:首先,利用量測裝置量測一已知液面及水深之量測波形作為參考波形,且經過標定步驟得知空氣段波傳速度、清水段波傳速度及淤積土段波傳速度;再利用量測裝置自待監測環境中取 得一量測波形,並量測量測波形之量測水位面走時位置與該參考波形之參考水位面走時位置的走時差,再配合已知的空氣段波傳速度,即可取得量測波形對應的液面位置與液面深度(清水與淤積土加總深度);最後,於量測波形中取得一終點走時位置,並配合量測水位面走時位置、液面深度、清水段波傳速度及淤積土段波傳速度計算出待監測環境中的清水段與淤積土段的介面實際位置,進而取得待監測環境的沖刷變化。Another embodiment of the present invention is a time domain reflective liquid level and brush depth measurement method, which utilizes the aforementioned liquid level and brush depth measuring device to measure the liquid level and the scouring depth of the environment to be monitored. The measuring method comprises the following steps: First, measuring the waveform of a known liquid level and water depth by using a measuring device as a reference waveform, and obtaining a wave velocity of the air segment and a wave velocity of the clear water segment through a calibration step and The velocity of the silt soil; the re-measurement device is taken from the environment to be monitored A measurement waveform is measured, and the time difference between the travel time position of the water level surface and the travel position of the reference water level surface of the reference waveform is measured, and the known air segment wave velocity is used to obtain the amount. The liquid level corresponding to the waveform and the depth of the liquid surface (the total depth of the clear water and the silt); finally, the position of the end point is obtained in the measurement waveform, and the position of the water level surface, the depth of the liquid surface, and the clean water are measured. The segmental wave velocity and the velocity of the silt soil segment calculate the actual position of the interface between the clear water segment and the silt soil in the environment to be monitored, and then obtain the erosion change of the environment to be monitored.
底下藉由具體實施例配合所附的圖式詳加說明,當更容易瞭解本發明之目的、技術內容、特點及其所達成之功效。The purpose, technical contents, features and effects achieved by the present invention will be more readily understood by the detailed description of the embodiments and the accompanying drawings.
本發明提出一種利用時域反射(Time Domain Reflectometry,TDR)量測液面與刷深的量測裝置及方法。TDR技術為一種新興的監測技術,利用其原理可設計不同的導波器(Waveguide,或稱探測器),可監測不同的物理量。本發明針對利用TDR監測沖刷所遭遇之問題提出對策,首先在導波器設計方面,採用結合類似地錨鋼索設計概念,提出符合安裝實務與耐衝擊的設計,並考慮導波器導體絕緣處理,解決訊號衰減問題;在量測方法方面,由於空氣、水及地層之介電係數不同,其電磁波速也明顯不同,本發明將結合反射訊號辨識與電磁波速度標定與分析,提出較可靠的訊號分析演算法。The invention provides a measuring device and a method for measuring liquid level and brush depth by using Time Domain Reflectometry (TDR). TDR technology is an emerging monitoring technology that uses its principles to design different waveguides (Waveguides, or detectors) that can monitor different physical quantities. The invention proposes countermeasures for using TDR to monitor the problems encountered in flushing. Firstly, in the design of the waveguide, a design similar to the anchoring cable design is proposed, and the design conforming to the installation practice and the impact resistance is proposed, and the waveguide insulation treatment is considered. Solving the problem of signal attenuation; in terms of measurement methods, the electromagnetic wave velocity is also significantly different due to the different dielectric coefficients of air, water and formation. The present invention combines the identification of reflected signals and the calibration and analysis of electromagnetic wave speed to provide a more reliable signal analysis. Algorithm.
由於本發明係揭露一種利用時域反射技術的液面與刷深量測裝置及其方法,其中所利用到的一些關於電磁波或導波器等之定義、詳細製造或處理過程,係利用現有技術來達成,故在下述說明中,並不作完整描述。而且下述內文中之圖式,亦並未依據實際之相關尺寸完整繪製,其作用僅在表達與本發明特徵有關之示意圖。The present invention discloses a liquid level and brush depth measuring device using a time domain reflection technique and a method thereof, wherein some of the definitions, detailed manufacturing or processing processes for electromagnetic waves or wave guides and the like are utilized, and the prior art is utilized. To achieve this, it is not fully described in the following description. Moreover, the drawings in the following texts are not completely drawn in accordance with actual relevant dimensions, and their function is only to show a schematic diagram relating to the features of the present invention.
第一圖為本發明之液面與刷深量測裝置的架構示意圖,請參閱第一圖所示,此液面與刷深之量測裝置包括有一時域反射式金屬感測導波器10、TDR擷取系統12、錨定器14以及一固定器16等;時域反射式金屬感測導波器10之頂部係利用固定器16固定於待監測環境之橋梁18之頂部或橋墩基座,時域反射式金屬感測導波器10底部則可配合一般鑽掘設備,於河床預定位置鑽掘一孔洞20,提供時域反射式金屬感測導波器10置入固定使用,且時域反射式金屬感測導波器10於孔洞20底部之末端連接錨定器14,以配合錨定器14固定之,並利用澆置混擬土進行感測導波器10固定,錨定器14係可為金屬、非金屬或複合材料等;既有河床面與錨定器14之孔洞空隙則係以回填料22回填,模擬原河床淤積深度,藉以提供沖刷量測使用。The first figure is a schematic diagram of the structure of the liquid level and brush depth measuring device of the present invention. Please refer to the first figure. The measuring device for the liquid level and the brush depth includes a time domain reflective metal sensing waveguide 10 The TDR extraction system 12, the anchor 14 and a holder 16 and the like; the top of the time domain reflective metal sensing waveguide 10 is fixed to the top of the bridge 18 or the pier base by the fixture 16 to the environment to be monitored. The bottom of the time domain reflective metal sensing waveguide 10 can be matched with the general drilling equipment to drill a hole 20 at a predetermined position of the river bed, and the time domain reflective metal sensing waveguide 10 is placed and fixed for use. The field reflective metal sensing waveguide 10 is connected to the anchor 14 at the end of the bottom of the hole 20 to be fixed with the anchor 14. The sensing waveguide 10 is fixed by the pouring mixed soil, and the anchor is fixed. The 14 series can be metal, non-metal or composite material; the gap between the river bed surface and the anchor 14 is backfilled with the backfill 22 to simulate the sedimentation depth of the original river bed, thereby providing flushing measurement.
其中,TDR擷取系統12之架構請同時參閱第二圖所示,此TDR擷取系統12包括有至少一同軸纜線24,電性連接時域反射式金屬感測導波器10,並利用同軸纜線24連接至一同軸纜線多工器(Coaxial multiplexer)26及一時域反射儀(Time domain reflectometer)28,此時域反射儀28則利用控制線30電性連接同軸纜線多工器26及一資料擷取系統32。The architecture of the TDR capture system 12 is also shown in the second figure. The TDR capture system 12 includes at least one coaxial cable 24 electrically connected to the time domain reflective metal sensing waveguide 10 and utilized. The coaxial cable 24 is connected to a coaxial cable multiplexer 26 and a time domain reflectometer 28, and the domain reflector 28 is electrically connected to the coaxial cable multiplexer by using the control line 30. 26 and a data capture system 32.
再者,在本發明之量測裝置中使用之時域反射式金屬感測導波器10的較佳實施例如第三圖所示,同軸纜線24與時域反射式金屬感測導波器10之間係利用一轉接探頭34相互連接,其係電性連接該同軸纜線,以接收該電磁脈波,並監測該環境變化,並據此產生一反射訊號;時域反射式金屬感測導波器10之結構係為至少二金屬桿之多桿式或是至少二金屬纜線之多纜式,以分別作為傳導電磁脈波或反射電磁脈波的正負極通道,且金屬感測導波器10之末端邊界為斷路式連接或短路式連接,斷面形狀係為圓形、橢圓形或任意多邊形等;並在金屬感測導波器10的至少一通道之外表面更包覆有一絕緣層;如第三圖所示,在此係以二條金屬纜線為例,包括有一多心鋼絞纜線102、一鋼纜線104,並於多心鋼絞纜線102包覆絕緣層106,主要構造乃利用同軸纜線24將其內外導體透過轉接探頭34內之電線342與多心鋼絞纜線102和鋼纜線104電性連結,轉接探頭更包括有一金屬或其他導電材質之外殼344,其內有絕緣或非導電材質之填充材料346固定同軸纜線24與多心鋼絞纜線102和鋼纜線104,此外殼344主要在保護轉換接頭34並將內部外洩電場廠遮蔽,減少漏洩電磁場所造成之干擾。此多心鋼絞纜線102與鋼纜線104提供正、負極通道,以作電磁波傳導使用,另外多心鋼絞纜線102則可依照現場安裝環境,選擇不同尺寸,符合設計張力強度,作為整體時域反射式金屬感測導波器10保護使用;絕緣層106則可保護多心鋼絞纜線102與鋼纜線104,不受鏽蝕影響,且可阻絕水體導電度,減少電磁波能量損耗。Furthermore, a preferred embodiment of the time domain reflective metal sensing waveguide 10 for use in the measuring device of the present invention is shown in the third figure, the coaxial cable 24 and the time domain reflective metal sensing waveguide. 10 is connected to each other by a switching probe 34, which is electrically connected to the coaxial cable to receive the electromagnetic pulse wave, and monitor the environmental change, and thereby generate a reflection signal; the time domain reflective metal sense The structure of the measuring waveguide 10 is a multi-bar type of at least two metal rods or a multi-cable type of at least two metal cables to respectively serve as positive and negative passages for conducting electromagnetic pulse waves or reflecting electromagnetic pulse waves, and metal sensing. The end boundary of the waveguide 10 is a broken-circuit connection or a short-circuit connection, and the cross-sectional shape is a circle, an ellipse or an arbitrary polygon, etc.; and the surface of the metal sensing waveguide 10 is coated on the outer surface of at least one channel. There is an insulating layer; as shown in the third figure, here two metal cables are taken as an example, including a multi-core steel strand cable 102, a steel cable 104, and covered by a multi-core steel strand cable 102. The insulating layer 106 is mainly constructed by transmitting the inner and outer conductors thereof through the coaxial cable 24. The wire 342 in the probe 34 is electrically connected to the multi-core steel cable 102 and the steel cable 104. The adapter further includes a metal or other conductive material casing 344 having an insulating or non-conductive material filling material. 346 fixed coaxial cable 24 and multi-core steel stranded cable 102 and steel cable 104. The outer casing 344 is mainly used to protect the conversion joint 34 and shield the internal leakage electric field factory to reduce the interference caused by leakage electromagnetic field. The multi-core steel stranded cable 102 and the steel cable 104 provide positive and negative passages for electromagnetic wave conduction, and the multi-heart steel stranded cable 102 can be selected according to the installation environment of the site, and the design tension is in accordance with the design tension strength. The integral time domain reflective metal sensing waveguide 10 is protected for use; the insulating layer 106 protects the multi-core steel stranded cable 102 and the steel cable 104 from rust, and can block the conductivity of the water body and reduce the electromagnetic wave energy loss. .
請同時參考第一、二、三圖所示,時域反射式金屬感測導波器10連接至同軸纜線24,再依序連接至同軸纜線多工器26;時域反射儀28係發射電磁脈波並接收時域反射式金屬感測導波器10之反射訊號,此反射訊號可進一步分析電磁波於時域反射式金屬感測導波器10遇到不同外在介質(空氣與水)之反射訊號,經由同軸纜線多工器26之切換,時域反射儀28可以連接複數個不同的時域反射式金屬感測導波器10,以提供TDR一機多點佈設之優勢。Please refer to the first, second and third figures at the same time, the time domain reflective metal sensing waveguide 10 is connected to the coaxial cable 24, and then sequentially connected to the coaxial cable multiplexer 26; the time domain reflectometer 28 is The electromagnetic pulse wave is emitted and receives the reflection signal of the time domain reflective metal sensing waveguide 10, and the reflection signal can further analyze the electromagnetic wave in the time domain reflective metal sensing waveguide 10 to encounter different external media (air and water) The reflection signal is switched by the coaxial cable multiplexer 26, and the time domain reflectometer 28 can be connected to a plurality of different time domain reflective metal sensing waveguides 10 to provide the advantages of TDR multi-point layout.
前述電磁波於時域反射式金屬感測導波器走時之典型波形,其較佳實施例如第四圖所示,第四(a)圖為時域反射式金屬感測導波器於實際量測時之示意圖,由於空氣之介電係數為1,一般水之介電係數為81,因此電磁波在兩者介面有明顯反射訊號,而當電磁波到達金屬感測導波器底部(開放型態),則有明顯之正反射訊號,如第四(b)圖所示。然而,受限於水與水下淤積土介電係數相差不甚明顯狀況下,加上TDR反射波形受到電纜電阻(即延長纜線長度)的影響呈現平滑的特性,或是外在水與淤積土導電度影響下,因此水與淤積土介面不容易清楚判釋,無法由此一位置直接提供淤積土位置,亦即無法反應沖刷變化。The preferred waveform of the electromagnetic wave in the time domain reflective metal sensing waveguide is preferably shown in the fourth figure, and the fourth (a) is the time domain reflective metal sensing waveguide in the actual amount. Schematic diagram of the time measurement, since the dielectric constant of air is 1, the dielectric constant of water is 81, so the electromagnetic wave has obvious reflection signals in the interface between the two, and when the electromagnetic wave reaches the bottom of the metal sensing waveguide (open type) , there is a clear positive reflection signal, as shown in the fourth (b). However, limited by the difference in the dielectric coefficient between water and submerged silt, the TDR reflection waveform is smoothed by the cable resistance (ie, the length of the extension cable), or external water and siltation. Under the influence of soil conductivity, the interface between water and silt soil is not easy to be clearly interpreted, and the location of silt soil cannot be directly provided from this position, that is, it cannot reflect the change of flushing.
因此,為避免此問題,本發明除了上述量測裝置之外,也同時提出一對應沖刷分析的量測方法。在本發明之量測方法中,主要係量測感測裝置在不同材料介面所產生之電磁波反射訊號走時,並利用一已建立之沖刷感測導波器裝置之系統參數標定與量測程序,藉以來分析沖刷變化。因此,在完整說明本發明之方法前,先就標定步驟之流程詳細說明如下:Therefore, in order to avoid this problem, in addition to the above-described measuring device, the present invention also proposes a measuring method corresponding to the flushing analysis. In the measuring method of the present invention, the electromagnetic wave reflection signal generated by the sensing device in different material interfaces is mainly used, and the system parameter calibration and measurement program of the established scouring sensing waveguide device is utilized. After the analysis, wash the changes. Therefore, before the method of the present invention is fully described, the flow of the calibration step is described in detail as follows:
首先,請參閱第五(a)圖所示,利用前述之量測裝置,可於現場或室內得到一已知相關配置之TDR第一量測波形,可設定為參考波形,已知相關配置係包含導波器波形起點走時位置t0 (可為纜線接頭或其他人為定義固定位置)、參考水位面走時位置ta/w,r 以及對應之液面深度(清水與淤積土加總深度)La/w,r 、導波器波形終點走時位置te,r 、清水段深度Lw,r 以及淤積土段深度Ls,r 。First, referring to the fifth (a) diagram, the TDR first measurement waveform of a known correlation configuration can be obtained in the field or indoor by using the above-mentioned measuring device, and can be set as a reference waveform, and the related configuration system is known. Contains the start position of the wave guide waveform t 0 (can be a cable joint or other artificially defined fixed position), the reference water level travel time position t a / w, r and the corresponding liquid level depth (clear water and silt soil total Depth) L a/w,r , the position of the waveguide end point t e,r , the depth of the clear water section L w,r and the depth of the silt section L s,r .
接續,基於前述參考波形,則可以再利用已知另一組至多組不同水位下之二量測波形,如較佳實施例第五(b)圖所示,並計算水位面走時位置
ta/w,m
,在已知與參考波形水位差異△La
,則可以基於下列方程式(1),計算出空氣段波傳速度Va
:
最後,基於前述參考波形,則可以額外再提供至少一組不同水位下之第二量測波形,並計算量測波形之水位面走時位置ta/w,m
、導波器波形終點走時位置te,m
,且需提供對應之清水段深度Lw,m
,以及淤積土段深度Ls,m
,其較佳實施例如第五(b)圖所示,利用參考波形(第一量測波形)與第二量測波形兩組資料,則可以基於下列方程式(2),藉由此聯立方程式,可以計算出清水段波傳速度Vw
以及淤積土段波傳速度Vs
:
至此,即完成整個標定流程,且藉由上述的標定步驟,則可提供量測裝置相關的空氣段波傳速度Va 、清水段波傳速度Vw 以及淤積土段波傳速度Vs 。At this point, the entire calibration process is completed, and by the above calibration step, the air segment wave velocity V a associated with the measuring device, the clear water segment wave velocity V w , and the silt soil segment wave velocity V s can be provided .
在說明完整個標定流程後,接續將本發明之實際沖刷量測方法的詳細流程說明如下:首先,可直接沿用或重新進行上述標定步驟,如第五(a)圖所示,可於現場得到一已知相關配置之TDR量測波形,設定為參考波形,已知相關配置係包含金屬感測導波器波形起點走時位置t0 、參考水位面走時位置ta/w,r 以及對應之液面深度(清水與淤積土加總深度)La/w,r 、金屬感測導波器波形終點走時位置te,r 、清水段深度Lw,r ,以及淤積土段深度Ls,r 。After explaining the complete calibration process, the detailed process of the actual scouring measurement method of the present invention is described as follows: First, the above calibration step can be directly followed or re-executed, as shown in the fifth (a) diagram, which can be obtained on the spot. A TDR measurement waveform of a known related configuration is set as a reference waveform, and the related configuration includes a metal sensing waveguide waveform starting point travel time t 0 , a reference water level surface travel time position t a/w, r, and a corresponding The depth of the liquid surface (the total depth of clear water and silt) L a/w,r , the position of the metal sensing waveguide waver t t , r , the depth of the clear water L W, r , and the depth of the silt s,r .
接續,基於前述參考波形,則可以進行量測波形分析,如第五(b)圖所示,先計算水位面走時位置ta/w,m ,在已知空氣段波傳速度Va ,則可以基於前述方程式(1),計算出與參考波形水位差異ΔLa ,亦即求得量測波形之對應液面深度(水土深度)La/w,m 。Continuation, based on the aforementioned reference waveform, the measurement waveform analysis can be performed. As shown in the fifth (b) diagram, the water level surface travel time t a/w,m is first calculated , and the known air segment wave velocity V a , Then, based on the foregoing equation (1), the water level difference ΔL a from the reference waveform can be calculated, that is, the corresponding liquid surface depth (water and soil depth) L a/w,m of the measured waveform is obtained.
最後,由上述步驟計算取得之量測水位面走時位置ta/w,m 以及對應液面深度La/w,m ,另外則可根據量測波形計算金屬感測導波器波形終點走時位置te,m ,再配合已知清水段波傳速度Vw 以及淤積土段波傳速度Vs ,即可利用下列方程式(3),計算量測時淤積土段深度Ls,m ,對應參考(初始)波形淤積土深度Ls,r ,則可得知於待監測環境中的清水段與淤積土段的介面實際位置,進而求得待監測環境的沖刷變化。Finally, the measured water level surface travel time position t a / w, m and the corresponding liquid surface depth L a / w, m calculated by the above steps, in addition, the metal sensing waveguide waveform end point can be calculated according to the measured waveform When the time position t e,m , together with the known wave velocity V w of the clear water section and the wave velocity V s of the silt section, the following equation (3) can be used to calculate the depth L s,m of the silt section during the measurement. Corresponding to the reference (initial) waveform silt depth L s,r , the actual position of the interface between the clear water section and the silt soil section in the environment to be monitored can be known, and the wash change of the environment to be monitored can be obtained.
綜上所述,本發明之量測裝置及方法主要係利用時域反射法同時量測液面與刷深行為,藉以同時監測液面與沖刷深度變化,配合裝置採用結合類似地錨鋼索的導波器設計,提出符合安裝實務的設計,並考慮導體絕緣處理,解決訊號衰減問題。再加上本發明結合反射訊號辨識與波傳速度標定與分析流程,實為一種相當可靠的訊號量測方法。In summary, the measuring device and method of the present invention mainly uses the time domain reflection method to simultaneously measure the liquid surface and the brush depth behavior, thereby simultaneously monitoring the change of the liquid surface and the scouring depth, and the fitting device adopts a guide which is similar to the anchor cable. Wave filter design, proposed to meet the installation practice design, and consider the conductor insulation treatment to solve the signal attenuation problem. In addition, the invention combines the reflection signal identification and the wave velocity calibration and analysis process, which is a fairly reliable signal measurement method.
以上所述之實施例僅係為說明本發明之技術思想及特點,其目的在使熟習此項技藝之人士能夠瞭解本發明之內容並據以實施,當不能以之限定本發明之專利範圍,即大凡依本發明所揭示之精神所作之均等變化或修飾,仍應涵蓋在本發明之專利範圍內。The embodiments described above are merely illustrative of the technical spirit and the features of the present invention, and the objects of the present invention can be understood by those skilled in the art, and the scope of the present invention cannot be limited thereto. That is, the equivalent variations or modifications made by the spirit of the present invention should still be included in the scope of the present invention.
10...時域反射式金屬感測導波器10. . . Time domain reflective metal sensing waveguide
102...多心鋼絞纜線102. . . Multi-core steel cable
104...鋼纜線104. . . Steel cable
106...絕緣層106. . . Insulation
12...TDR擷取系統12. . . TDR capture system
14...錨定器14. . . Anchor
16...固定器16. . . Holder
18...橋樑18. . . bridge
20...孔洞20. . . Hole
22...回填料twenty two. . . Backfill
24...同軸纜線twenty four. . . Coaxial cable
26...同軸纜線多工器26. . . Coaxial cable multiplexer
28...時域反射儀28. . . Time domain reflectometer
30...控制線30. . . Control line
32‧‧‧資料擷取系統32‧‧‧Information Capture System
34‧‧‧轉接探頭34‧‧‧Transfer probe
342‧‧‧電線342‧‧‧Wire
344‧‧‧外殼344‧‧‧Shell
346‧‧‧填充材料346‧‧‧Filling materials
第一圖為本發明之液面與刷深量測裝置的架構示意圖。The first figure is a schematic diagram of the structure of the liquid level and brush depth measuring device of the present invention.
第二圖為本發明使用之TDR擷取系統的架構示意圖。The second figure is a schematic diagram of the architecture of the TDR capture system used in the present invention.
第三圖為本發明使用之時域反射式金屬感測導波器的結構示意圖。The third figure is a schematic structural view of a time domain reflective metal sensing waveguide used in the present invention.
第四(a)圖為本發明利用時域反射式金屬感測導波器於實際量測時之示意圖。The fourth (a) diagram is a schematic diagram of the present invention using the time domain reflective metal sensing waveguide in actual measurement.
第四(b)圖為本發明利用金屬感測導波器量測到之波形示意圖。The fourth (b) diagram is a schematic diagram of the waveform measured by the metal sensing waveguide in the present invention.
第五(a)圖及第五(b)為本發明分別於不同環境下之量測波形的時域反射式金屬感測導波器之分析標示示意圖。The fifth (a) diagram and the fifth (b) are schematic diagrams of the analysis of the time-domain reflective metal sensing waveguides of the measurement waveforms respectively in different environments.
10...時域反射式金屬感測導波器10. . . Time domain reflective metal sensing waveguide
12...TDR擷取系統12. . . TDR capture system
14...錨定器14. . . Anchor
16...固定器16. . . Holder
18...橋樑18. . . bridge
20...孔洞20. . . Hole
22...回填料twenty two. . . Backfill
Claims (16)
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TWI484209B (en) * | 2013-12-02 | 2015-05-11 | Nat Applied Res Laboratories | Magnetic device for measuring scour depth |
CN108663384B (en) * | 2018-06-08 | 2020-07-31 | 太原理工大学 | Anchor rod nondestructive testing device and method based on TDR |
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Citations (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5784338A (en) * | 1997-09-15 | 1998-07-21 | The United States Of America As Represented By The Secretary Of The Army | Time domain reflectometry system for real-time bridge scour detection and monitoring |
TWI230218B (en) * | 2003-09-02 | 2005-04-01 | China Engineering Consultants | Water monitoring device and monitoring method |
US6909669B1 (en) * | 1999-04-19 | 2005-06-21 | The United States Of America As Represented By The Secretary Of The Army | Scour detection and monitoring apparatus adapted for use in lossy soils and method of employment thereof |
TWM374568U (en) * | 2009-10-16 | 2010-02-21 | Xing-Tai Xiao | Riverbed terrain scour monitoring device |
-
2011
- 2011-04-08 TW TW100112213A patent/TWI452267B/en not_active IP Right Cessation
Patent Citations (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5784338A (en) * | 1997-09-15 | 1998-07-21 | The United States Of America As Represented By The Secretary Of The Army | Time domain reflectometry system for real-time bridge scour detection and monitoring |
US6909669B1 (en) * | 1999-04-19 | 2005-06-21 | The United States Of America As Represented By The Secretary Of The Army | Scour detection and monitoring apparatus adapted for use in lossy soils and method of employment thereof |
TWI230218B (en) * | 2003-09-02 | 2005-04-01 | China Engineering Consultants | Water monitoring device and monitoring method |
TWM374568U (en) * | 2009-10-16 | 2010-02-21 | Xing-Tai Xiao | Riverbed terrain scour monitoring device |
Non-Patent Citations (1)
Title |
---|
楊培熙「TDR水位量測技術在大地與水利工程之應用」,碩士論文,國立交通大學,民92 * |
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