TWI231362B - Method for measuring speed of longitudinal wave and thickness inside concrete plate by using stress wave - Google Patents
Method for measuring speed of longitudinal wave and thickness inside concrete plate by using stress wave Download PDFInfo
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1231362 五、發明說明(/ )【技術領域】 本發明係有關一種以廣六、、士^ 波檢測混凝土版内部縱波ϋ度與厚度之方法’本發明乃利用應力波行經整個混凝土期$厚度至版底之反射原理,可同時精相得㈣土版之内苟縱波速度與厚度。1231362 V. Description of the invention (/) [Technical Field] The present invention relates to a method for detecting the longitudinal wave thickness and thickness of a concrete plate by using waves, waves, and waves. The invention uses stress waves to travel through the entire concrete period. The principle of reflection at the bottom of the plate can be obtained at the same time to obtain the P-wave velocity and thickness of the soil plate.
ο IX 5 1Α 經濟部智慧財產局員工消費合作社印製 ο 2 【先前之技術】 新建完工之混凝土構造物皆須進行尺寸上之驗收且為 合約規範的主要項目之一,例如新建剛性道路之混凝土舖 面厚度、橋樑之混凝土橋面版、水庫工程之溢洪道、混凝 土坡面工· ••等等,皆僅有一面可接觸之構造物,其厚 度之篁測方法傳統上僅能採用鑽心取樣方式,丈量鑽心試 體長度作為驗收依據,此種方法費時昂貴且須在鑽心位置 實施修補’若考慮日後耐磨性及滲水問題,鑽心破壞取樣 方式則不適宜。 因此在1995年由美國之國家科學基金會(National Science Foundation)資助下,研究以敲擊回音法(impact-echo method)之非破 壞性檢 測技術 ,取 代目 前昂貴 費時的 鑽心取樣方法,並且於1998年建立此項技術之美國檢測及 材料協會(American Society for Testing and Materials,以 下簡稱ASTM)標準量測規範(全名為:ASTM C 1383 “Standard Test Method for Measuring the P-Wave Speed and一一:…一ο IX 5 1Α Printed by the Consumer Cooperatives of the Intellectual Property Bureau of the Ministry of Economic Affairs 2 [Previous technology] Newly completed concrete structures must undergo dimensional acceptance and be one of the main items specified in the contract, such as concrete for new rigid roads The thickness of the pavement, the concrete deck of the bridge, the spillway of the reservoir project, the concrete sloper, etc. are all structures that can only be touched on one side, and the method of measuring the thickness can only use the core sampling method. Measuring the length of the core sample as the basis for acceptance. This method is time-consuming and expensive and must be repaired at the core location. 'If the future wear resistance and water seepage are considered, the sampling method of core damage is not suitable. Therefore, in 1995, funded by the National Science Foundation of the United States, the non-destructive detection technology of the impact-echo method was researched to replace the current expensive and time-consuming core sampling method. Established the American Society for Testing and Materials (ASTM) standard measurement specifications (full name: ASTM C 1383 "Standard Test Method for Measuring the P-Wave Speed and one by one": …One
(請先閱讀背面之注意事項再填寫本頁) 本紙張尺度適用中國國家標準(CNS)A4規格(210 X 297公釐) A7 經濟部智慧財產局員工消費合作社印製 1231362 " ..... 11 B7 五、發明說明(1)(Please read the precautions on the back before filling out this page) This paper size applies the Chinese National Standard (CNS) A4 specification (210 X 297 mm) A7 Printed by the Employees' Cooperatives of the Intellectual Property Bureau of the Ministry of Economic Affairs 1231362 " .... . 11 B7 V. Description of the Invention (1)
Method”),如附件一所示。 敲擊回音法係在測試物體表面利用機械性敲擊產生暫 態應力波動,並將其傳入物體内,該應力波動包含有表面 波 R(Rayleigh-wave,簡稱 R-wave或 R波),縱波 p(P-waVe, 5 或P波)及剪力波S(S-wave,或S波),如圖一所示,其中表 面波係沿著物體表面以遠離敲擊點的方式向外擴散,而縱 波及努力波則以球狀的波形方式向前傳動。其中壓力波(P) 速度最快、剪力波(S)次之,而表面波(R)略慢於剪力波。 在敲擊表面以表面波(R)造成之擾動為最大,因此,在敲 10擊表面配置接收器,則接收到之最初擾動訊號為p波到達 所造成,而接收到之最大擾動訊號則為R波到達所造成。 對版狀結構而言,當縱波及剪力波遇到反射介面,如 版的底部時,將被反射回去;當這些反射波回到敲擊面時, 則產生表面的位移。利用表面放置的接收器則可監測到此 15位移反應,如果該接收器被安排在靠近敲擊點時,則監測 到的位移主要是因為縱波所造成。當反射波到達敲擊面 後’將再被反射回版内部。因此敲擊激發之應力波會在版 的頂面及底面間來回傳動,如圖二A所示,而激發出版的 厚度振動模態,如圖二B所示,使得靠近敲擊位置監測到 20 之敲擊反應具有週期性,經由快速傅利葉轉換(fft),可 得此敲擊反應之頻率(f),此頻率與混凝土版内部縱波來 回於版頂與版底所需時間週期之倒數有關稱為厚度頻率 (fT)(thickness frequency),如圖二c所示,可由下列公式 表示: ____ 4 本紙張尺度適用中國國家標準(CNS)A4規格(21G x 297公髮)Method ”), as shown in Annex 1. The percussion echo method uses mechanical impact on the surface of the test object to generate transient stress fluctuations and introduces them into the object. The stress fluctuations include surface waves R (Rayleigh-wave , Referred to as R-wave or R-wave), longitudinal wave p (P-waVe, 5 or P wave) and shear wave S (S-wave, or S wave), as shown in Figure 1, where the surface wave system is along the object The surface diffuses outward away from the impact point, while the longitudinal and effort waves are transmitted forward in a spherical wave form. Among them, the pressure wave (P) is the fastest, followed by the shear wave (S), and the surface wave (R) is slightly slower than the shear wave. The surface wave (R) is the largest disturbance on the striking surface. Therefore, when the receiver is arranged on the 10 striking surface, the initial disturbance signal received is caused by the p-wave arrival. The largest disturbance signal received is caused by the arrival of the R wave. For the plate-like structure, when the longitudinal and shear waves meet the reflection interface, such as the bottom of the plate, they will be reflected back; when these reflected waves return When hitting the surface, surface displacement occurs. The receiver placed on the surface can monitor At this point, the 15 displacement response, if the receiver is arranged near the impact point, the detected displacement is mainly due to longitudinal waves. When the reflected wave reaches the impact surface, it will be reflected back to the interior of the plate. The stress wave excited by the impact will be transmitted back and forth between the top and bottom surfaces of the plate, as shown in Figure 2A, and the thickness vibration mode of the excited publication, as shown in Figure 2B, so that a knock of 20 is detected near the strike position. The strike response has a periodicity. Through the fast Fourier transform (fft), the frequency (f) of the strike response can be obtained. This frequency is related to the inverse of the time period required for the internal longitudinal wave of the concrete plate to go back and forth between the plate top and the plate bottom. The frequency (fT) (thickness frequency), as shown in Figure 2c, can be expressed by the following formula: ____ 4 This paper size applies to China National Standard (CNS) A4 (21G x 297)
tj!? 線 (請先閱讀背面之注意事項再填寫本頁) (1) 五、發明說明(3 ) r Cp.pla IT =--tj !? line (Please read the precautions on the back before filling this page) (1) V. Description of the invention (3) r Cp.pla IT =-
2T 在前述之公式(1)中, T為混凝土版之厚度;2T In the foregoing formula (1), T is the thickness of the concrete plate;
Cp,plate為縱波在版狀結構物内傳播的視波速。 根據經驗法則,由於此視波速(非實際波速)為在無限 體内之實際的波速(Cp)之96〇/〇。因此公式(1)可以可改寫成 下列之公式(2)或(3),即: (2)Cp, plate is the apparent wave velocity of longitudinal waves propagating in the plate-like structure. According to the rule of thumb, this apparent wave velocity (non-actual wave velocity) is 96/0 of the actual wave velocity (Cp) in the infinite body. Therefore, formula (1) can be rewritten as the following formula (2) or (3), namely: (2)
_ 0.96G 一—2T 或混凝土版之厚度(T)可由下列公式表示·· 10 7 = 0.96— 2fT (3) 圖二A為混凝土版之敲擊回音試驗示意圖,其中,混 凝土版之厚度(T),實際版厚〇.3m,敲擊源1〇旁設有一接 收器(在本圖中為第二接收器22,當然也可改用第一接收 器 21)。 15 圖三B為記錄之位移波形。 圖三C即為由位移波形以傅利葉轉換而成之振幅頻 譜。由圖三C中之頻譜可觀察到一個高振幅的尖峰(約 5.86kHz),此尖峰的頻率即為公式(3)中之頻率(卜)。 請參閱圖四A,該敲擊回音試驗系統由三個主要元件 20所組成:一敲擊源1〇、二接收器(即第一接收器21與第二 接收器22)及一台含資料抓取卡之攜帶型電腦(圖中未 1231362 A7 --—------_________ 五、營明蹲日月(呼) " 一~ (請先閱讀背面之注意事項再填寫本頁) 示)°試驗使用直徑3mm〜12mm之鋼球為敲擊源J 〇,而第 一、第二接收器2 1、2 2為一寬頻之位移接收器。剛試之混 凝土表面與該第一、第二接收器21、22之壓電材料間以一 薄錯片(圖中未示)來完成該二接收器21、22之電路及使該 5 二接收器21、22與混凝土表面緊密壓合。含資料抓取卡之 攜帶型電腦則可儲存由接收器輸出之訊號,並進行訊號處 理及分析。 公式(3)即為ASTM C 1383以敲擊回音法量測p波波速 及混滅土版厚度(T)之基本公式。以下對ASTM C 1383法 10 ®測P波波速及混凝土版厚度之檢測步驟加以敘述。 步驟一 :P波波速之量測 經濟部智慧財產局員工消費合作社印製 圖四A及四B分別為P波速度之檢測裝置示意圖及量測 之位移波形圖,在已知之距離L (0.3m)配置兩個接收器 21、22(21為第一接收器、22為第二接收器),並於混凝土 15 版表面距第一接收器21適當距離A (0.15m)處,即敲擊源 10位置,給予一敲擊產生暫態應力波,使三者成一直線, 利用兩個接收器所得之表面行走P波波到時間差(△ t),參 閱圖四B’及已知前述第一與第二接收器21、22之距離L, 利用下列公式(4)可算得行經表面之p波波速。 C -~ 20 Ρ Δί (4) 步驟二:敲擊回音試驗 圖四C及四D分別為敲擊回音檢測之檢測裝置示意圖 及量測之頻譜圖,在混凝土表面給予一敲擊並在距離甚小 6 本紙張尺度適用中國國家標準(CNS)A4規格(21〇 X 297公|| )----- 1231362 A7 Β7 10 15 經濟部智慧財產局員工消費合作社印製 20 〇·4Τ)放置一第-接你势。, , 乐一接收器22,則所監測到的位移波 形主要是因為!>波到達所造成,應力波來回於混凝土版頂 面及底面傳動,因而產生一共振頻率,是^、版厚頻率, (卜)利用FFT技巧將該第二接收器22所量得之數位化波 I轉至頻4領域求得頻譜含量,頻譜圖中之高振幅尖峰值 即導入之應力波遇到版底之邊界多次來回頂底反射造成之 版厚頻率卜’將所得fT值及由步驟-所量得Ρ波波速代 A式(3)汁算,則可求得混凝土版之厚度,即版厚(丁)。 由上述試驗步驟中得知,現行ASTM C 1383之混凝 土版厚度量測,乃利用在混凝土版表面量測到之表面縱波 速度(Cp)及敲擊回音試驗測得來回於版頂與版底之厚度頻 率(fT) ’再代入公式(3)而計算得到混凝土版之厚度(τ)。 兹舉一實例詳細說明如下,假設某一工程之混凝土版 厚(T)為〇.2m。圖五A、B分別為ASTM C 1383法來量測混 凝土版之表面縱波速度之配置俯視圖、示意圖,其中,依 實際之版長(L)、版寬(W)及版厚(T)分別為1.2、1.2及 〇.199m ’其上有七條量測線,線a、線b與線c間距〇.2m, 而線D、線E、線F與線G之間距為〇.l5m。而圖五C及D分 別為量測線A上敲擊後該第一接收器2 1及第二接收器22所 量測之波形圖,表面行走之縱波波到時間分別為(ti)及 (D ’ t1=-3 6.7;/s& t2=43.4//s,二者之時間差為八1 = 1241 = 43.4-(-36·7) = 80·1//8,該第一及第二接收器21、22之間距(L), L = 0.3m,並以公式(4)求出表面之Ρ波波速為3745m/s。縱 波到達第一接收器21之時間(M為負值,此乃因資料擷取_ 0.96G-2T or the thickness of the concrete plate (T) can be expressed by the following formula: 10 7 = 0.96-2fT (3) Figure 2A is a schematic diagram of the tap echo test of the concrete plate, in which the thickness of the concrete plate (T ), The actual version is 0.3m thick, and there is a receiver (the second receiver 22 in this figure, of course, the first receiver 21 can also be used instead). 15 Figure 3B shows the recorded displacement waveform. Figure 3C shows the Fourier transform amplitude spectrum. From the spectrum in Figure 3C, a high-amplitude spike (approximately 5.86 kHz) can be observed, and the frequency of this spike is the frequency (b) in formula (3). Please refer to FIG. 4A. The percussion echo test system is composed of three main components 20: a percussion source 10, two receivers (that is, the first receiver 21 and the second receiver 22), and a data-containing device. Portable computer for grabbing card (1213362 A7 in the picture ---------_________ V. Yingming squatting sun and moon (calling) " a ~ (Please read the precautions on the back before filling this page) (Shown) ° The test uses a steel ball with a diameter of 3mm ~ 12mm as the striking source J 0, and the first and second receivers 21 and 22 are a wide-band displacement receiver. A thin film (not shown) is used between the concrete surface just tested and the piezoelectric materials of the first and second receivers 21 and 22 to complete the circuits of the two receivers 21 and 22 and make the 52 receivers The devices 21 and 22 are tightly pressed against the concrete surface. The portable computer with data capture card can store the signal output by the receiver, and perform signal processing and analysis. Formula (3) is the basic formula of ASTM C 1383 for measuring the p-wave velocity and the thickness (T) of the mixed soil plate by the percussion echo method. The following describes the test procedures of ASTM C 1383 Method 10 ® for measuring P-wave velocity and thickness of concrete plates. Step 1: Measurement of P-wave velocity Printed by the Consumer Cooperatives of the Intellectual Property Bureau of the Ministry of Economic Affairs. Figures 4A and 4B are schematic diagrams of the P-wave velocity detection device and measured displacement waveforms, respectively, at a known distance L (0.3m ) Configure two receivers 21 and 22 (21 is the first receiver and 22 is the second receiver), and the appropriate distance A (0.15m) from the first receiver 21 on the surface of the concrete 15 plate, that is, the source of the strike 10 position, give a hit to generate a transient stress wave, make the three in a straight line, use the surface walking P wave wave obtained by the two receivers to the time difference (△ t), see Figure 4B 'and the aforementioned first and The distance L of the second receivers 21 and 22 can be calculated by using the following formula (4). C-~ 20 Ρ Δί (4) Step 2: Tap echo test chart. Figures 4C and 4D are schematic diagrams of the detection device for the tap echo detection and the measured spectrum chart, respectively. A tap is given on the concrete surface and the distance is very short. Small 6 This paper size applies the Chinese National Standard (CNS) A4 specification (21〇X 297 male ||) ----- 1231362 A7 Β7 10 15 Printed by the Intellectual Property Bureau of the Ministry of Economic Affairs and Consumer Cooperatives (20 〇 · 4Τ) Place one First-pick you up. , Leyi receiver 22, the displacement waveform detected is mainly because! > Caused by the arrival of the wave, the stress wave is transmitted back and forth on the top and bottom surfaces of the concrete plate, so a resonance frequency is generated, which is the thickness of the plate. (b) The digits measured by the second receiver 22 using the FFT technique The converted wave I is turned to the frequency 4 area to obtain the spectrum content. The high amplitude spikes in the spectrum diagram are the imported stress waves that meet the boundary of the bottom of the plate. The thickness of the plate caused by the top and bottom reflection multiple times. From the step-measured P-wave speed instead of formula (3), the thickness of the concrete plate can be obtained, that is, the plate thickness (D). It is known from the above test steps that the current thickness measurement of the concrete plate of ASTM C 1383 is measured by the surface longitudinal wave velocity (Cp) and the tap echo test measured on the surface of the concrete plate. The thickness frequency (fT) 'is then substituted into formula (3) to calculate the thickness (τ) of the concrete plate. Here is an example to explain in detail as follows, suppose the thickness (T) of the concrete version of a project is 0.2m. Figure 5A and B are top views and schematic diagrams of the measurement of the surface longitudinal wave velocity of the concrete plate by the ASTM C 1383 method, respectively. Among them, the actual plate length (L), plate width (W), and plate thickness (T) are respectively 1.2, 1.2 and 0.199m 'There are seven measuring lines on it, the distance between line a, line b and line c is 0.2m, and the distance between line D, line E, line F and line G is 0.15m. Figures 5C and D are the waveforms measured by the first receiver 21 and the second receiver 22 after tapping on the measurement line A, respectively. The time of arrival of the longitudinal waves on the surface is (ti) and ( D 't1 = -3 6.7; / s & t2 = 43.4 // s, the time difference between the two is eight 1 = 1241 = 43.4-(-36 · 7) = 80 · 1 // 8, the first and second The distance (L) between the receivers 21 and 22, L = 0.3m, and the surface P wave velocity is 3745m / s according to formula (4). The time when the longitudinal wave reaches the first receiver 21 (M is negative, this Data retrieval
(請先閱讀背面之注意事項再填寫本頁) 本紙張尺度適用中國國家標準(CNS)A4規格(21〇 X 297公釐) 1231362 經濟部智慧財產局員工消費合作社印製(Please read the precautions on the back before filling out this page) This paper size is applicable to China National Standard (CNS) A4 (21 × X 297 mm) 1231362 Printed by the Consumer Cooperatives of the Intellectual Property Bureau of the Ministry of Economic Affairs
A7 、發明說明(6 ) 系統設定訊號達激發門檻時為〇值,而敲擊產生之有效訊 號通常發生在激發之前,故資料擷取時,會設定成前激發 模式(pre-trigger mode),因此第一接收器21擷取到之波到 訊號時間會出現在負值處,由於只需要q至L間之時間, 只要取其相對時間差即可,並不影響量測之精確性。 接著進行敲擊回音試驗,儀器配置如圖六A,圖六B 為敲擊後該第二接收器22所量測之波形圖,對圖六B波形 圖進行快速傅利葉轉換(FFT),可得圖六〇所示之頻譜圖, 由此頻譜圖很清楚辨識出敲擊反應之版厚頻率為 9334Hz。將量測線A上測得之波速3745m/s與厚度頻率 9334Hz代入公式(3)得版厚為〇.193m與實際厚度〇 2m比較 得量測誤差為-3.5%。若同樣的依前述之ASTM c 1383法 來量測混凝土版其他六條量測線上之表面縱波速度,所求 得之數據及量測誤差均列在此下列之表一中,其最大誤差 高達5.0%,平均誤差亦有2 5%,精確度不佳。 表一以習知方法量測P波波速及版厚之結果 I適用中國國家標準(CNS)A4規格(210 X 297公釐 1231362 A7 —B7 五、發明說明(7 ) 10 然而,習知方法所存在之嚴重誤差,經仔細探討後發 現,這裡存在一個很明顯不一致之處,亦#,公式⑺中 之縱波速度(cp)應為混凝土版内部之縱波速度,而非以表 5面之縱波速度來假設相同,由於混凝土是由水泥、砂、骨 材及水所組合而成之複合材料,屬於不均質材料,因此表 面量測到之表面縱波速度—定不會與内部縱波速度一致, 從實務角度來看,其不-致性有時候可高達10%以上以 表面之縱波速度當作是版内部之縱波速度,必然使後續之 推算均不準確。因此,若套用現行ASTM C】如之混凝土 版波速與厚度量測方法,求得的結果與實際之值存在著明 顯誤差。故,必須克服此一問題。 【目的及功效】 15 20 本發明之主要目的,在於解決上述的問題而提供一種 量測方法同時精確測得混凝土版之内部縱波速度與厚度。 本發明乃利用應力波行經整個混凝土版厚度至版底之反射 原理,可同時測得混凝土版之内部縱波速度與厚度,而奍 現仃ASTM C 1383僅量測混凝土表面之縱波速度來推求混 凝土版之厚度,如此,本發明所取得之結果更接近實際值, 精確度高。 本發明之次一目的,在於解決上述的問題而提供一種 量測方法同時精確測得混凝土版之内部縱波速度與厚度, 其所需設備簡單、成本低、又以不破壞原有結構之方式進 L___一 _ 9 >紙張尺度‘ T關家標準(CNS)A4規格⑵G χ 297公^ I231362 A7 B7 五、赞明說明(?) 仃,故能提昇土木建築結構非破壞檢測技術水平與工程品 質 10 15 經 濟 部 智 慧 財 產 局 員 工 消 費 合 作 社 印 製 20 【技術内容】 本發明係提供一種以應力波檢測混凝土版之内部縱波 速度與厚度之方法,包含下列步驟: 一、 定距步驟: 概略估計待檢測之版厚(T),準備一第一接收器及 一第二接收器,決定適當之第二接收器與敲擊源 間之最小距離(H),並使該敲擊源及該第二接收器 之距離必須大於此最小距離(H),其中,該最小距 離(Η)必須滿足下列公式: ^>2rxtan50.5° 二、 敲擊步驟: 敲擊後讀取該第一接收器之敲擊時間原點 (t〇), 三、 應力波讀取步驟: 讀取該第一接收器之縱波經版底反射到達時門 (tp),並求得内部行走時間ΔίρΆ ; 四、 版厚頻率量測步驟: 設置第一或第二接收器,進行敲擊回音試驗 測得到版厚頻率(fT); 五、 計算步驟: 利用下列二公式: 量 (請先閱讀背面之注意事項再填寫本頁) 本紙張尺度適用中國國家標準(CNS)A4規格(210 X 297公釐) 1231362A7. Explanation of the invention (6) The system sets the signal to zero when the signal reaches the excitation threshold, and the effective signal generated by the tap usually occurs before the excitation. Therefore, when data is acquired, it will be set to the pre-trigger mode. Therefore, the wave-to-signal time captured by the first receiver 21 will appear at a negative value. Since only the time between q and L is required, it only needs to take the relative time difference, which does not affect the accuracy of the measurement. Then perform the tap echo test. The instrument configuration is shown in Figure 6A, and Figure 6B is the waveform measured by the second receiver 22 after the tap. The fast Fourier transform (FFT) is performed on the waveform in Figure 6B. The spectrogram shown in FIG. 60 clearly indicates that the plate thickness frequency of the tap response is 9334 Hz. The wave velocity 3745m / s and thickness frequency 9334Hz measured on the measuring line A were substituted into formula (3) to obtain a plate thickness of 0.193m and a comparison with the actual thickness of 0.2m. The measurement error was -3.5%. If the same method is used to measure the surface longitudinal wave velocities of the other six measurement lines of the concrete version according to the aforementioned ASTM c 1383 method, the obtained data and measurement errors are listed in Table 1 below, with a maximum error of 5.0 %, The average error is also 2 5%, and the accuracy is poor. Table 1 Results of measuring P-wave velocity and plate thickness by conventional methods I Applicable to China National Standard (CNS) A4 (210 X 297 mm 1231362 A7-B7 V. Description of the invention (7) 10 However, conventional methods Existing serious errors, after careful discussion, it is found that there is an obvious inconsistency here. Also, the P-wave velocity (cp) in formula 应 should be the P-wave velocity inside the concrete version, not the P-wave velocity in Table 5. Let ’s assume the same. Because concrete is a composite material composed of cement, sand, aggregate, and water, which is an inhomogeneous material, the surface P-wave velocity measured on the surface will not be consistent with the internal P-wave velocity. From the point of view, its inconsistency can sometimes be as high as 10% or more. Taking the longitudinal P-wave velocity on the surface as the P-wave velocity inside the plate will inevitably make subsequent calculations inaccurate. Therefore, if the current ASTM C is applied, such as concrete There are obvious errors between the measured wave velocity and thickness measurement method and the actual value. Therefore, this problem must be overcome. [Objective and Effect] 15 20 The main purpose of the present invention is to In order to solve the above problems, a measurement method is provided to accurately measure the internal longitudinal wave velocity and thickness of the concrete plate. The invention uses the principle of reflection of the stress wave traveling through the thickness of the entire concrete plate to the bottom of the plate, and can simultaneously measure the inside of the concrete plate P-wave velocity and thickness, but now ASTM C 1383 only measures the P-wave velocity of the concrete surface to estimate the thickness of the concrete plate. In this way, the results obtained by the present invention are closer to the actual value and the accuracy is high. It is to solve the above problems and provide a measurement method to accurately measure the internal longitudinal wave velocity and thickness of the concrete plate. The required equipment is simple, low cost, and L_1_ 9 > Paper scale 'T family standard (CNS) A4 specification ⑵G χ 297 public ^ I231362 A7 B7 V. Explain (?) 仃, so it can improve the level of non-destructive detection technology and engineering quality of civil building structures 10 15 Ministry of Economic Affairs wisdom Printed by the property bureau employee consumer cooperative [Technical content] The present invention provides a method for detecting concrete by stress waves. The method of internal P-wave velocity and thickness includes the following steps: 1. The distance setting step: Estimate the thickness (T) of the plate to be detected, prepare a first receiver and a second receiver, and determine the appropriate second receiver. The minimum distance (H) from the striking source, and the distance between the striking source and the second receiver must be greater than the minimum distance (H), where the minimum distance (该) must satisfy the following formula: ^ > 2rxtan50.5 ° 2. Step of tapping: read the origin of the tapping time (t0) of the first receiver after tapping, 3. Step of reading the stress wave: Read the longitudinal wave of the first receiver The bottom reflection reaches the door (tp), and finds the internal walking time Δίρ 求; Fourth, the thickness measurement step of the plate: Set the first or second receiver, and perform the knock echo test to obtain the plate thickness frequency (fT); V. Calculation steps: Use the following two formulas: Quantities (please read the precautions on the back before filling this page) This paper size is applicable to China National Standard (CNS) A4 (210 X 297 mm) 1231362
五、發明說明( Cp ⑹(々) λ/^χ,)2:0·9216 及 r = 096CpV. Description of the invention (Cp ⑹ (々) λ / ^ χ,) 2: 0 · 9216 and r = 096Cp
Xfi) ❼計算出混凝土内部之内部縱波速度(Cp)與混凝 5 土版之厚度(τ)。 本發明之上述及其他目的與優點,不難從下述所選用 實施例之詳細說明與附圖中,獲得深入了解。 當然,本發明在某些另件上,或另件之安排上容許有 所不同,但所選用之實施例,則於本說明書中,予以詳細 10 說明,並於附圖中展示其構造。 【圖式簡單說明】 圖一係敲擊後各種波之擴散方式示意圖 圖二A係敲擊激發之應力波會在版的頂面及底面來 回傳動示意圖 15 圖二B係版的厚度振動模態示意圖 圖一 C係敲擊反應之頻譜圖 圖三A係混凝土版之敲擊回音試驗示意圖 圖三B及三C分別為所量測之位移波形及頻譜圖 圖四A及四B分別為P波速度之檢測裝置示意圖及量 20 測之位移波形圖 圖四C及四D分別為敲擊回音檢測之檢測裝置示意圖 及量測之頻譜圖 11 本紙張尺度適用中國國家標準(CNS)A4規格(210 X 297公釐) (請先閱讀背面之注意事項再填寫本頁} Η叮· ;線· 經濟部智慧財產局員工消費合作社印製 經 濟 部 智 慧 財 產 局 員 工 消 費 合 作 社 印 製 縱波P 版厚頻率fT 版寬W P波波速Cp 1231362 A7Xfi) ❼ Calculate the internal longitudinal wave velocity (Cp) inside the concrete and the thickness (τ) of the concrete soil plate. The above and other objects and advantages of the present invention can be easily understood from the detailed description and accompanying drawings of the selected embodiments below. Of course, the present invention allows some differences in the arrangement or arrangement of other parts, but the selected embodiment is described in detail in this specification and its structure is shown in the drawings. [Brief description of the diagram] Figure 1 is a schematic diagram of the various wave diffusion modes after striking. Figure 2 A is the stress wave excited by the striking and will drive back and forth between the top and bottom of the plate. 15 Figure 2 B-plate thickness vibration mode Schematic diagram 1C is the spectrum diagram of the tapping response. Fig. 3A is the diagram of the tap echo test of the concrete version. Figs. 3B and 3C are the measured displacement waveforms and spectrum diagrams. 4A and 4B are the P waves. Schematic diagram of speed detection device and displacement waveform diagram of measurement 20 Figures 4C and 4D are schematic diagrams of detection device and measurement spectrum diagram of tap echo detection, respectively. 11 This paper size applies to China National Standard (CNS) A4 specification (210 X 297 mm) (Please read the precautions on the back before filling out this page} Η ding ·; line · printed by the employee consumer cooperative of the Intellectual Property Bureau of the Ministry of Economy Version wide WP wave speed Cp 1231362 A7
五、發明說明(W ) 圖五A、B分別為ASTM C 1383法來量測混凝土版之 表面縱波速度、厚度之配置俯視圖、示意圖 圖五C及D分別該二接收器所量測之波形圖 圖六A、六B及六C分別為發明版厚頻率量測步驟之 5 裝配圖、量測之位移圖及頻譜圖 圖七A及七B分別為混凝土内部縱波反射行為之實驗 裝置圖與波到訊號之圖形 圖八A及八B分別為大於最小距離為〇55m之實驗之 配置圖及量測結果 10圖九A、九B及九C係本發明第一實施例敲擊之裝配 圖及二接收器所量測之波形圖 圖十A、十B及十C間接推求敲擊時間原點表面r波 波速量測之裝配圖及二接收器所量測之波形圖 圖十一 A、十一 B及十一 c係本發明第二實施例敲擊 15 之裝配圖及二接收器所量測之波形圖 圖十二係本發明之流程圖 【圖號說明】V. Description of the invention (W) Figure 5A and B are top views and schematic diagrams of the configuration of measuring the surface longitudinal wave velocity and thickness of the concrete plate according to ASTM C 1383, respectively. Figures 5C and D are the waveforms measured by the two receivers. Figures 6A, 6B, and 6C are respectively the assembly drawing, measured displacement chart, and spectrum diagram of the invention's thick frequency measurement step 5. Figures 7A and 7B are experimental device diagrams and waves of the longitudinal wave reflection behavior inside the concrete, respectively. Figures 8A and 8B of the signal are the configuration diagrams and measurement results of experiments larger than the minimum distance of 055m. 10 Figures 9A, 9B, and 9C are assembly drawings of the first embodiment of the invention and Waveforms measured by the two receivers. Figures 10A, 10B, and 10C indirectly calculate the r-wave velocity measurement of the surface at the origin of the striking time. Waveforms measured by the two receivers. Figures 11A, 10 1B and 11c are the assembly diagram of the second embodiment of the present invention and the waveform diagram measured by the second receiver is shown in FIG. 12. The 12th diagram is the flowchart of the present invention. [Illustration of drawing number]
表面波R 20 剪力波S 版長Y 版厚T 視波速Cp,plate 縱波經版底反射到達時間t 本紙張尺度適用中國國家標準Surface wave R 20 Shear wave S version Long Y version Thick T Apparent wave speed Cp, plate P wave arrival time through plate bottom reflection t This paper size applies Chinese national standard
(請先閱讀背面之注意事項再填寫本頁) I23l362 五 10 15 20 k發明說明(丨1 ) 敲擊時間原點t。 第一接收器測得時間tl 表面行走時間差△t 敲擊源至第一接收器距離A 敲擊源至第二接收器距離Η 兩接收器之間距L 直達之Ρ波之初始擾動時間tps 經版底反射後之P波之擾動時間 直達之S波之初始擾動時間tsh 直達之R波之初始擾動時間tR 敲擊源10 接收器21、22(21為第一接收器;22為第二接收器) 定距步驟51 敲擊步驟52 應力波讀取步驟53 版厚頻率量測步驟54 計算步驟55 【實施例之詳細說明】 圖中所示者為本發明所選用之實施例之結構,此僅供 說明之用,在專利申請上並不受此種結構之限制。 本發明係一種以應力波檢測混凝土版之内部縱波速度 與厚度之方法。關於本發明之技術原理,當物體的表面給 予一個點敲擊源(Impact)時,將產生暫態應力波動並導入 物體内’該應力波動包含有壓力波(p_wave)、剪力波(S_ wave)及表面波(R_wave),其中壓力波及剪力波在物體内 第二接收器測得時間t: 内部行走時間差△t 反射角0 線 13 本紙張尺度適用中國國家標準(CNS)A4規格(210 X 297公釐) 1231362 A7 五、發明說明(/ 2 ) 部依半球狀的波形方式向前傳動,而表面波則沿著物體表 面遠離敲擊點的方式向外擴散出去,如圖一所示,其中壓 力波(P)速度最快、煎力波(S)次之,而表面波(R)略慢於剪 力波。 5 在此凊參閱圖七A及七B ’其分別為混凝土内部縱波 反射行為之儀器裝置圖與理論數值分析所得反射波之波到 訊號圖形’在圖七B中之反射波波到訊號已經將沿著混凝 土表面傳動之P波、S波與R波到達之擾動訊號移除。由此 理論分析可知,當縱波之入射角與反射角0大於5〇5度 時,此反射之P波將由向下之波形反轉為向上之波形,若 反射角0太小’則所測得之訊號無轉向且較不明顯,不易 精確測得。故,可以得到此敲擊源至第二接收器22之最小 距離(H)之限制條件為下列之公式(5) 10 15 H>2T X tan50.5° (5) 20 假设一版厚(T)為〇.2m,依公式(5)計算可得知其最小 距離(H)應大於0.485m。若以距離(H)為〇.55m來實驗,配 置圖如圖八A所示,則可得到圖八b之訊號結果,圖八b中 下方之波形圖為移除沿者混凝土表面傳動之p波、S波與R 波到達之擾動訊號,圖八B中上方之波形圖為實際量測到 之波形圖,將包含沿著混凝土表面傳動之P波、s波與R波 到達之擾動訊號。其中,依時間順序分別可測得·· tps係為沿表面傳動之p波之初始擾動時間; 本紙張尺度適用中國國家標準(CNS)A4規;|各(210 X 297公髮) (請先閱讀背面之注意事項再填寫本頁)(Please read the precautions on the back before filling this page) I23l362 5 10 15 20 k Description of invention (丨 1) Tap the time origin t. Time measured by the first receiver tl Surface walking time difference Δt Distance between the strike source and the first receiver A Distance between the strike source and the second receiver Η The initial perturbation time of the P wave directly from L between the two receivers tps Warp Perturbation time of P wave after bottom reflection Initial perturbation time of direct S wave tsh Initial perturbation time of direct R wave tR Strike source 10 Receiver 21, 22 (21 is the first receiver; 22 is the second receiver ) Fixed distance step 51 Knock step 52 Stress wave reading step 53 Thick plate frequency measurement step 54 Calculation step 55 [Detailed description of the embodiment] The figure shown is the structure of the selected embodiment of the present invention, this is only For illustrative purposes, this structure is not restricted by patent applications. The invention is a method for detecting the internal longitudinal wave velocity and thickness of a concrete plate by a stress wave. Regarding the technical principle of the present invention, when a point impact is given to the surface of an object, a transient stress wave will be generated and introduced into the object. The stress wave includes pressure wave (p_wave) and shear wave (S_ wave). ) And surface wave (R_wave), in which pressure wave and shear wave are measured at the second receiver in the object t: internal walking time difference △ t reflection angle 0 line 13 This paper size applies Chinese National Standard (CNS) A4 specification (210 X 297 mm) 1231362 A7 V. Description of the invention (/ 2) The part is driven forward in a hemispherical waveform, while the surface wave spreads outward along the surface of the object away from the impact point, as shown in Figure 1. Among them, the pressure wave (P) has the fastest speed, the frying force wave (S) is the second, and the surface wave (R) is slightly slower than the shear wave. 5 Here please refer to Figures 7A and 7B 'These are the instrument and equipment diagrams of the longitudinal wave reflection behavior inside the concrete and the wave-to-signal pattern of the reflected wave obtained from the theoretical numerical analysis.' The reflected wave-to-signal in Figure 7B has been Disturbance signals of P-wave, S-wave and R-wave arriving along the concrete surface are removed. From this theoretical analysis, it can be known that when the incident angle and reflection angle 0 of the longitudinal wave is greater than 50.5 degrees, the reflected P wave will be reversed from a downward waveform to an upward waveform. If the reflection angle 0 is too small, then it will be measured. The signal is non-steering and less obvious, which is difficult to measure accurately. Therefore, the limiting condition of the minimum distance (H) from the striking source to the second receiver 22 can be obtained as the following formula (5) 10 15 H > 2T X tan 50.5 ° (5) 20 Assuming a plate thickness (T ) Is 0.2m. According to formula (5), it can be known that the minimum distance (H) should be greater than 0.485m. If the distance (H) is 0.55m for the experiment, the configuration diagram is shown in Figure 8A, the signal result in Figure 8b can be obtained, and the lower waveform diagram in Figure 8b is the removal of the p along the concrete surface. The disturbance signal of the arrival of waves, S waves, and R waves. The upper waveform in Figure 8B is the actual measured waveform. It will include the disturbance signals of P waves, s waves, and R waves transmitted along the concrete surface. Among them, according to the time sequence, tps is the initial perturbation time of the p wave transmitted along the surface; this paper size applies the Chinese National Standard (CNS) A4 regulations; | each (210 X 297 public) (please first (Read the notes on the back and fill out this page)
^31362 A7 ^^—----B7 —__ 五、發明說明⑴) ~—----^ tpb係為經版底反射後之p波之擾動時間; ish係為沿表面傳動之S波之初始擾動時間; 係為沿表面傳動之R波之初始擾動時間。^ 31362 A7 ^^ —---- B7 —__ 5. Description of the invention ⑴) ~ ——---- ^ tpb is the perturbation time of the p wave reflected by the bottom of the plate; ish is the S wave driven along the surface The initial perturbation time is the initial perturbation time of the R wave propagating along the surface.
Γ靖先間讀背面之注意事項再填寫本頁) 而上述之tpb即為本發明所要此反射之p波所經過的時 後面之實施例中,僅以tp來表示該反射p波之到達時 請參閱圖十二,本發明「以應力波檢測混凝土版之内 部縱波速度與厚度之方法」,其主要包含下列步驟·· 一 ·定距步驟51 ; 10 二·敲擊步驟52 ; 三·應力波讀取步驟5 3 ; 四·版厚頻率量測步驟54 ;及 五·計算步驟55。 茲舉前面採用ASTM C 1383量測版厚之同一實例詳 15 細說明如下,該混凝土版厚(T)之為0,2m,此為待量侧之 值。 第一、進行定距步驟: 經濟部智慧財產局員工消費合作社印製 由設計之版厚(T)為0.2m,先代入公式(5),則得知最 小距離(H) ·· 20 Η > 2 X T X tan50.0° > 2 x 0.2 x tan 50.5° > 〇.485m 故,稍後之該敲擊源至該第二接收器22之距離必須 大於此最小距離(H)。 15 本紙張尺度適用中國國家標準(CNS)A4規格(210 X 297公爱" 1231362Γ Jing first read the precautions on the back before filling out this page) and the above tpb is the time when the reflected p wave is required by the present invention. In the following embodiments, only the tp is used to indicate the arrival time of the reflected p wave. Please refer to FIG. 12. The present invention “method for detecting the internal longitudinal wave velocity and thickness of a concrete plate by stress waves” mainly includes the following steps: a. Distance setting step 51; 10 two. Tapping step 52; three. Stress Wave reading step 5 3; 4. Plate thickness frequency measurement step 54; and 5. Calculation step 55. Here is an example of measuring the plate thickness using ASTM C 1383. The detailed description is as follows. The thickness (T) of the concrete plate is 0,2m, which is the value to be measured. First, the distance-setting step is performed: The thickness of the printed version (T) is 0.2m, which is printed by the employee's consumer cooperative of the Intellectual Property Bureau of the Ministry of Economic Affairs, and the formula (5) is substituted into the minimum distance (H). ; 2 XTX tan50.0 ° > 2 x 0.2 x tan 50.5 ° > 〇.485m Therefore, the distance from the strike source to the second receiver 22 later must be greater than the minimum distance (H). 15 This paper size applies to China National Standard (CNS) A4 (210 X 297 Public Love " 1231362
經 濟 部 智 慧 財 產 局 員 工 消 費 合 作 社 印 製 五、發明說明(叫 第二、進行敲擊步驟·· 參閱圖九A、九B及九C,敲擊並決定敲擊時間原點 (t〇),該敲擊源至該第二接收器22之距離(⑴為〇 55m大 於要求之最小距離。採用可感測敲擊時間原點之敲擊器, 該敲擊器内部裝設有感應元件(壓電材料),此一裝置即將 第一接收器21與敲擊源1〇結合成一體,可直接得到敲擊 時間原點,圖九B為敲擊得到之訊號,由圖中得敲擊時 間原點(t0)為-4〇.〇焊,此時間負值乃因資料擷取系統設定 訊號達激發門檻時為〇值,而敲擊產生之有效訊號通常發 生在激發之前,故資料擷取時,會設定成前激發模式 (pr^tdgger mode),因此時間原點會出現在負值處,本發 明只需要t0至tp間之時間,只要取其相對時間差即可, 並不影響本發明之精確性。 第三、應力波讀取步驟: 參閱圖九A、九B及九C,敲擊後,讀取第二接收器 22之縱波經版底反射到達時間(%)為133 2焯如圖九c所 示,並求得縱波内部行走時間(Λν=νΜ為ι33·2-(· 40.0)=173.2//s 〇 第四、版厚頻率量測步驟: 版後頻率量測同前面ASTM C 1383之量測,設置一 第二接收器22(當然也可改用第一接收器21),如圖六a 所示,進行敲擊回音試驗量測得到版厚頻率(心),其量測 之位移波形及頻譜圖分別為圖六B及六C所示,其顯示 出版厚頻率(fT) = 9334Hz。 5 10 15 20 (請先閱讀背面之注意事項再填寫本頁) 訂·· ;線· 16 1231362 A7 B7 五、發明說明(〇 第五、計算步驟: 计算出混凝土内部之平的 厚声m㈣ 之十均縱波速度(cP)與混凝土版之 =。内部縱波速度(Cp)等於實際行走距離除以内部 5 而此實際行走距離為利用畢氏定理中 Α之基本原理來求出的,則得公式(6), 三Printed by the Consumer Cooperative of the Intellectual Property Bureau of the Ministry of Economic Affairs. 5. Description of the invention (called the second step of tapping. Refer to Figures 9A, 9B, and 9C. Tap and decide the tap time origin (t0). The distance from the tapping source to the second receiver 22 (⑴55mm is greater than the required minimum distance. A tapper capable of sensing the origin of the tapping time is used, and a sensing element (press (Electrical material), this device is to combine the first receiver 21 and the tapping source 10, and can directly obtain the origin of the tapping time. Figure 9B shows the signal obtained from the tapping. The point (t0) is -40.0. Welding at this time is negative because the data acquisition system sets the signal to 0 when the signal reaches the excitation threshold, and the effective signal generated by the tap usually occurs before the excitation. , Will be set to the pre-excitation mode (pr ^ tdgger mode), so the time origin will appear at a negative value, the present invention only needs the time between t0 and tp, as long as the relative time difference is taken, it does not affect the invention Accuracy. Third, stress wave reading steps: Figures 9A, 9B, and 9C. After tapping, read that the longitudinal wave reflection arrival time (%) of the second receiver 22 is 133 2 焯, as shown in Figure 9c, and find the internal walking time of the longitudinal wave. (Λν = νΜ is ι33 · 2- (· 40.0) = 173.2 // s 〇 Fourth, the plate thickness frequency measurement steps: frequency measurement after the plate is the same as the previous ASTM C 1383 measurement, a second receiver 22 is set (Of course, the first receiver 21 can also be used instead.) As shown in Fig. 6a, the plate thickness frequency (heart) is obtained by performing a tap echo test. The measured displacement waveforms and spectrum diagrams are shown in Fig. 6B and As shown in Figure 6C, it shows the publishing thickness frequency (fT) = 9334Hz. 5 10 15 20 (Please read the notes on the back before filling this page) Order · ·; Line · 16 1231362 A7 B7 V. Description of the invention (〇 第V. Calculation steps: Calculate the tenth average longitudinal wave velocity (cP) of the flat thick sound m㈣ inside the concrete and the concrete version =. The internal longitudinal wave velocity (Cp) is equal to the actual walking distance divided by the internal 5 and this actual walking distance is used It can be obtained from the basic principle of A in Bishop's theorem, then formula (6), three
Cp (f)2+T2Cp (f) 2 + T2
At, 將公式(3)代入公式(6),得公式 (6)At, substituting formula (3) into formula (6), we get formula (6)
Cp : ⑺ 10 15 由於已知版厚頻率(fT)及内部行走時間差(AtJ,故由 公式⑺即可求得㈣縱波速度(Cpp再將解得之縱波速度 (Cp)代入公式(3)則可得混凝土版之厚度(τ)。 在已知 H = 0.55m’ fT = 9334Hz 及 Atp=173.2//s 之情況下, 代入公式(7),即可得到内部縱波速度(Cp)為3947m/s, 再將此縱波速度(Cp)代入公式(3)求得混凝土版之厚度 為0.203m,量測誤差為ι·5%。 同樣的,再舉本發明之第二實施例,其係以的間接方 式求得敲擊時間原點(t❹)之檢測法,該間接方式乃利用波 傳時間方式反推敲擊時間原點,故在上述量測步驟中,需 增加表面R波波速之量測(此R波波速量測屬於習知技 術)。 表面R波波速之量測請參閱圖十A、十B及十C。 在一敲擊源10旁設置一較接近之第一接收器21及一較遠 17 20 1231362 A7 五、發明說明(A ) 離之第二接收器22,敲擊 w 後該第一接收器21及第二接收 ^之1測到R波波到時間分別為(t〇及(t2),12.0//8 及…"S,該第一及第二接收器之間距(L),L = 〇i5m, 並以習知公式求出表面之R波波速: 5 (CR) = L/h-ti) =0.15/(64-(-2.0)) =0.15/66 =2272(m/s); 一有了 R ;皮波速後,τ進行前述之五個量測步驟。第 一步驟為定距步驟,配置圖如圖十- Α所示,第二接收 器22與敲擊源之距離為H,55m,第一接收器21與敲擊 源10之距離為A=0.15m;第二步驟為敲擊步驟並決定敲 擊時間原點(tQ),敲擊後分別得到第_接收器21與第二接 收器22之波形訊號如圖十一 B及圖十一 c之結果,其中 R波到達第-接收器21之時間為ti==_53·,而敲擊時間 原點應該往前推至R波行經距離A所需之時間,即 10 15 ㈣卜(差)=—53·4 —= —119 伞 經 濟 部 智 慧 財 產 局 員 工 消 費 合 作 社 印 製 20 第二步驟為應力波讀取步驟,參閲圖十一 A、十一 Β 及十一 c,敲擊後,讀取第二接收器22之縱波經版底反 ,到達時間(tp)為55·4^如圖十一 c所示,並求得縱波内 部行走時間(AWt。)為55·4-(_119·4) = 174·8%。第四步驟 為版厚頻率量測步驟,版厚頻率fT同樣為9334Ηζ,再進 行第五計算步驟,將第三與第四步驟得到之 18 |____ 15 林國家標準(CNS)A4規格(210 X 297公釐 1231362 A7Cp: ⑺ 10 15 Because the known thickness frequency (fT) and the internal walking time difference (AtJ), the ㈣ longitudinal wave velocity can be obtained from the formula ((Cpp then substitutes the obtained longitudinal wave velocity (Cp) into the formula (3). The thickness (τ) of the concrete plate can be obtained. When H = 0.55m 'fT = 9334Hz and Atp = 173.2 // s, the formula (7) can be substituted to obtain the internal longitudinal wave velocity (Cp) of 3947m / s, and then substituting this longitudinal wave velocity (Cp) into formula (3) to obtain the thickness of the concrete plate is 0.203m, and the measurement error is ι · 5%. Similarly, the second embodiment of the present invention is described as follows. The indirect method is to obtain the detection method of the tap time origin (t❹). This indirect method uses the wave propagation time method to invert the tap time origin. Therefore, in the above measurement step, the amount of surface R wave velocity needs to be increased. (This R-wave velocity measurement is a conventional technique.) For surface R-wave velocity measurement, please refer to Figures 10A, 10B, and 10C. Set a closer first receiver 21 next to a tapping source 10. And a farther 17 20 1231362 A7 V. Description of the invention (A) The second receiver 22 away, the first receiver 21 after hitting w The R-wave arrival times measured for the second receiver ^ 1 are (t0 and (t2), 12.0 // 8 and ... " S, the distance between the first and second receivers (L), L = 〇 i5m, and determine the surface R wave velocity with a conventional formula: 5 (CR) = L / h-ti) = 0.15 / (64-(-2.0)) = 0.15 / 66 = 2272 (m / s); With R; pico speed, τ performs the aforementioned five measurement steps. The first step is a fixed distance step, the configuration diagram is shown in Figure X-A, and the distance between the second receiver 22 and the striking source is H, 55m, the distance between the first receiver 21 and the tapping source 10 is A = 0.15m; the second step is the tapping step and the tapping time origin (tQ) is determined. After tapping, the _receiver 21 and the The waveform signals of the two receivers 22 are shown in the results of Figure 11B and Figure 11c, where the time when the R wave reaches the -receiver 21 is ti == _ 53 ·, and the origin of the tapping time should be pushed forward to R The time required for the wave to travel through distance A, that is, 10 15 ㈣bu (poor) = — 53 · 4 — = —119 Umbrella Ministry of Economic Affairs Intellectual Property Bureau employee consumer cooperative printing 20 The second step is the stress wave reading step, see Figures 11A, 11B and 11c, after tapping Read the longitudinal wave of the second receiver 22 through the background of the plate. The arrival time (tp) is 55 · 4 ^ as shown in Figure 11c, and the longitudinal travel time (AWt.) Of the longitudinal wave is 55 · 4-(_ 119 · 4) = 174 · 8%. The fourth step is the plate thickness frequency measurement step, and the plate thickness frequency fT is also 9334Ηζ, and then the fifth calculation step is performed, and the 18 and ____ 15 forest countries are obtained in the third and fourth steps. Standard (CNS) A4 size (210 X 297 mm 1231362 A7
五、發明說明() 與fT = 9334 Hz代入公式(7),即可得到 、 4°卩縱波速度(Cp) 為3891m/s,再將此縱波速度(cd)代入八々^ P P;n入公式(3)求得混凝土 版之厚度(T)為0.200m,量測誤差為〇 〇%。 粽上所述,以本發明方法經兩次量測後所得之版厚平 5均為0.2015m,平均誤差只有0·75%,遠低於習知方法之 2.5%,大幅提升其精確度。 探究其原因’由於混凝土内部並非均一材質(混有石 頭、沙等等),其表面與内部之縱波速度並不相同。然而, 因本發法係以内部實際反射之内部縱波速度(Cp)來計算, 而非以表面之表面縱波速度(cp)來推估,自然能具有較高 之精確性,十分合理。 以上僅是藉由較佳實施例詳細說明本發明,對於該實 施例所做的任何簡單修改與變化皆不脫離本發明之精神與 範圍。 由以上詳細說明,可使熟知本項技藝者明瞭本發明的 確可達成刖述目的’實已符合專利法之規定,爰提出發明 專利申請。 10 15 (請先閱讀背面之注意事項再填寫本頁) 訂 經濟部智慧財產局員工消費合作社印製 【附件】 20 附件一:美國檢測及材料協會標準量測規範ASTM C 1383影本一式兩份 19 本紙張尺度適用中國國家標準(CNS)A4規格(210 X 297公釐)V. Description of the invention () and fT = 9334 Hz are substituted into formula (7), then 4 ° 卩 longitudinal wave velocity (Cp) is 3891m / s, and then this longitudinal wave velocity (cd) is substituted into 々 々 PP; n into The thickness (T) of the concrete plate obtained by the formula (3) is 0.200 m, and the measurement error is 0.00%. As mentioned above, the plate thickness and thickness 5 obtained after two measurements by the method of the present invention are all 0.2015m, and the average error is only 0.75%, which is far lower than 2.5% of the conventional method, which greatly improves its accuracy. Investigate the reason ’As the interior of the concrete is not a homogeneous material (mixed with stones, sand, etc.), the P-wave velocity on the surface and inside is not the same. However, because this method of calculation uses the internal longitudinal wave velocity (Cp) of the actual internal reflection instead of the surface longitudinal wave velocity (cp) to estimate, the natural energy has higher accuracy and is very reasonable. The above is only a detailed description of the present invention through a preferred embodiment, and any simple modifications and changes made to the embodiment will not depart from the spirit and scope of the present invention. From the above detailed description, those skilled in the art can understand that the present invention can indeed achieve the stated purpose, and that it has complied with the provisions of the Patent Law, and filed an application for an invention patent. 10 15 (Please read the notes on the back before filling out this page) Order printed by the Consumers ’Cooperative of the Intellectual Property Bureau of the Ministry of Economic Affairs [Annex] 20 Annex 1: American Testing and Materials Association Standard Measurement Specification ASTM C 1383 Photocopy in duplicate 19 This paper size applies to China National Standard (CNS) A4 (210 X 297 mm)
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CN107525577A (en) * | 2017-08-21 | 2017-12-29 | 兰州交通大学 | Attenuation of P-wave measurement apparatus and method |
CN110133114A (en) * | 2019-06-27 | 2019-08-16 | 中国工程物理研究院化工材料研究所 | A kind of solid stress wave propagation rate test device and method suitable for wide temperature range |
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CN111965651A (en) * | 2020-08-06 | 2020-11-20 | 胡新发 | Method for testing plate thickness |
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2002
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CN107525577A (en) * | 2017-08-21 | 2017-12-29 | 兰州交通大学 | Attenuation of P-wave measurement apparatus and method |
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CN110133114A (en) * | 2019-06-27 | 2019-08-16 | 中国工程物理研究院化工材料研究所 | A kind of solid stress wave propagation rate test device and method suitable for wide temperature range |
CN111965651A (en) * | 2020-08-06 | 2020-11-20 | 胡新发 | Method for testing plate thickness |
CN111965651B (en) * | 2020-08-06 | 2022-05-13 | 胡新发 | Method for testing plate thickness |
CN111830136A (en) * | 2020-08-07 | 2020-10-27 | 中铁第一勘察设计院集团有限公司 | Ballastless track concrete structure damage detection method based on stress wave |
CN112902889A (en) * | 2021-04-09 | 2021-06-04 | 湖南芯仪电子科技有限公司 | Double-channel thickness gauge and method for measuring longitudinal wave velocity in concrete through double-channel thickness gauge |
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