TW202001624A - Analytical method for estimating stress change of tunnel lining through displacements providing substantial suggestions for the optimization of tunnel maintenance and management - Google Patents
Analytical method for estimating stress change of tunnel lining through displacements providing substantial suggestions for the optimization of tunnel maintenance and management Download PDFInfo
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本發明係關於一種土木工程的模擬方法,尤其適用於模擬變位量導致隧道壁面的應力變化。The invention relates to a method for simulating civil engineering, and is especially suitable for simulating the change of stress on the tunnel wall surface caused by displacement.
隧道襯砌為隧道表面以磚、石、混凝土或混凝土與鋼線網、鋼筋、鋼纖維等材料構成之人工結構,近代隧道工法在隧道施工時持續監測隧道變形,待變形趨於穩定後方施作襯砌,因此襯砌原為美觀及提供額外防護而施作,理論上不會承受過多應力。然台灣近2/3以上隧道在營運後襯砌出現異常狀況,其中最常見類型即為變形及裂縫,故近年研究開始關注襯砌變位與裂縫,並將其視為隧道結構劣化和協助研判劣化肇因的重要指標。Tunnel lining is an artificial structure made of brick, stone, concrete or concrete with steel wire net, steel bar, steel fiber and other materials on the surface of the tunnel. The modern tunnel construction method continuously monitors the tunnel deformation during tunnel construction and applies the lining after the deformation becomes stable. Therefore, the lining was originally designed for aesthetics and to provide additional protection, in theory it will not withstand excessive stress. Although nearly two-thirds of tunnels in Taiwan have abnormal lining after operation, the most common type is deformation and cracks, so in recent years, research has begun to pay attention to lining displacement and cracks, and regard it as the deterioration of the tunnel structure and assist in the judgment of deterioration. Important indicators.
已知隧道變位解析方法大多針對監測斷面自身變形行為,然而近年隧道三維絕對變位監測資料的解析成果顯示除單一監測斷面上可見之向內擠壓或向外突出之二維變形行為外,監測斷面之間尚存在可觀之三維變形,以往考慮的斷面變形僅影響局部範圍內之襯砌裂縫,現地所觀察到延續數公尺至數十公尺的斜向、縱向等裂縫型態係由相鄰監測斷面的相對變位所引致。The known methods of tunnel displacement analysis are mostly aimed at monitoring the deformation behavior of the cross section itself. However, in recent years, the analytical results of the three-dimensional absolute displacement monitoring data show that in addition to the inward squeezing or outward protruding 2D deformation behavior seen on a single monitoring cross section In addition, there are still considerable three-dimensional deformations between the monitoring sections. The section deformations considered in the past only affect the lining cracks in the local area. Oblique and longitudinal crack types extending from several meters to tens of meters are observed on the spot. The state is caused by the relative displacement of adjacent monitoring sections.
已知隧道襯砌裂縫型態模擬係建立二維或三維的隧道數值模型,給予外力或變位條件,獲得隧道應變與應力分布。其採用連續體分析,以塑性組成率描述隧道襯砌,將進入塑性的部分視為襯砌材料破壞裂縫產生。模擬結果可與現地隧道監測的地表沉陷量、隧道內空變位比較,或與室內隧道縮尺試驗監測的應力-應變曲線相比,以進行數值模型驗證。換言之,已知技術多係透過隧道內複數點位在加載過程的應力-應變曲線,或位於隧道內或隧道上方幾處位置的變位來確認數值模型的正確性,發生隧道裂縫的位置則以數值模型中進入塑性區之網格代表,鮮少將其模擬結果與實際隧道之裂縫型態直接比對。It is known that the tunnel lining crack pattern simulation system establishes a two-dimensional or three-dimensional tunnel numerical model, gives external force or displacement conditions, and obtains the tunnel strain and stress distribution. It uses continuum analysis to describe the tunnel lining with a plastic composition rate, and the part that enters the plastic is regarded as the lining material damage crack. The simulation results can be compared with the amount of ground subsidence monitored by the existing tunnel, the empty displacement in the tunnel, or compared with the stress-strain curve monitored by the indoor tunnel scale test to verify the numerical model. In other words, the known technology mostly confirms the correctness of the numerical model through the stress-strain curve of the multiple points in the tunnel during the loading process, or the displacement of several positions in or above the tunnel, and the location of the tunnel crack occurs with In the numerical model, the grids that enter the plastic zone are rarely compared with the actual tunnel crack patterns.
本發明之主要目的在於提供一種變位量導致壁面的應力變化之模擬方法,其包括以下步驟:(S1)提供模擬模型,包含三維隧道單元、做為模型邊界之不同的複數個斷面,及其測量變數與變位模態;(S2) 根據該些斷面之變位量測量值計算該隧道單元的相對變位量及該變位模態之組成量且得到該壁面的應力變化之值;(S3) 比對壁面應力變化與該壁面的裂縫分布,視情況修正該相對變位量之計算值以獲得與該裂縫分布相符之應力變化。The main object of the present invention is to provide a method for simulating the stress change of a wall caused by a displacement, which includes the following steps: (S1) providing a simulation model including a three-dimensional tunnel element, a plurality of different cross sections as model boundaries, and Its measurement variables and displacement modes; (S2) Calculate the relative displacement of the tunnel element and the composition of the displacement mode based on the measured displacement values of these sections and obtain the stress change of the wall surface Value; (S3) Compare the stress change on the wall surface with the crack distribution on the wall surface, and modify the calculated value of the relative displacement as appropriate to obtain the stress change consistent with the crack distribution.
本發明之一種變位量導致壁面的應力變化之模擬方法,其中,該壁面係襯砌壁面,該變位量係該襯砌壁面在不同時間之空間位置變化,斷面為隧道中做為變位量測標的之監測橫斷面,該斷面包含數量足以偵測隧道變形現象之複數個監測點,該隧道單元係以二隧道監測斷面為邊界之隧道範圍,該斷面之所有監測點在不同時間之空間位置變化的集合為斷面變位量,特定斷面變化量係變位模態,其為斷面剛體運動與斷面變形,該變位模態對應已知的變位量及壁面應力變化,斷面剛體運動包含所有該監測點一致等量移動為平移變位模態,所有該監測點對斷面形心一致等量旋轉為旋轉變位模態,斷面變形變位模態包含斷面監測點相對於該斷面形心放大或縮小之均勻變形變位模態,及相對於該斷面形心之變形為橢圓形變形變位模態,相對於該斷面形心之變形為三角形變形變位模態,相對於該斷面形心之變形為四邊形變形變位模態,相對於該斷面形心之變形為五邊形變形變位模態,乃至相對於該斷面形心之變形為多邊形變形變位模態之複數種變位模態,且三維空間中隧道內通行方向為軸向,重力方向為垂直向,另一與軸向和垂直向正交之方向為側向,該三維空間中斷面剛體運動包含軸向平移,側向平移,垂直向平移與相對軸向旋轉,相對側向軸旋轉和相對垂直軸旋轉。A method for simulating the stress change of a wall surface caused by a displacement amount of the present invention, wherein the wall surface is a lining wall surface, the displacement amount is a spatial position change of the lining wall surface at different times, and the cross section is a displacement amount in a tunnel The monitoring cross-section of the target, the cross-section contains a number of monitoring points sufficient to detect the deformation of the tunnel. The tunnel unit is a tunnel area bordered by the second tunnel monitoring cross-section. All the monitoring points of the cross-section are different. The set of spatial position changes in time is the cross-section displacement, and the specific cross-section displacement is the displacement mode, which is the rigid body motion and cross-section deformation. The displacement mode corresponds to the known displacement and wall surface. Stress change, the rigid body motion of the cross section includes all the monitoring points that are uniformly moved to the translational displacement mode, and all the monitoring points are uniformly rotated to the centroid of the cross section to the rotational displacement mode, and the cross section deformation displacement mode Including the uniform deformation displacement mode of the cross section monitoring point enlarged or reduced relative to the cross section centroid, and the deformation relative to the cross section centroid is elliptical deformation displacement mode, relative to the cross section centroid The deformation is a triangle deformation displacement mode, the deformation relative to the centroid of the cross section is the quadrilateral deformation displacement mode, and the deformation relative to the cross section centroid is the pentagonal deformation displacement mode, and even relative to the fracture The deformation of the face centroid is a plurality of displacement modes of the polygon deformation displacement mode, and the passage direction in the three-dimensional space is the axial direction, the gravity direction is the vertical direction, and the other direction is orthogonal to the axial direction and the vertical direction For the lateral direction, the three-dimensional space interruption rigid body motion includes axial translation, lateral translation, vertical translation and relative axial rotation, relative lateral axis rotation and relative vertical axis rotation.
本發明之一種變位量導致壁面的應力變化之模擬方法,步驟S1包含以下步驟:(S10) 建立初始模擬模型,且該模擬模型包含三維隧道單元,做為模型邊界之不同的複數個斷面,及其測量變數與變位模態;(S11) 分別施加剛體運動變位模態之斷面變位量於該模擬模型邊界,得到該隧道單元相對剛體運動之應力變化;(S12) 判斷該初始模擬模型之測量變數及應力變化是否均勻,若否,進入步驟S10,若是,進行步驟S13;(S13) 分別施加變形變位模態之斷面變位量於該模擬模型邊界,得到隧道單元變形之應力變化;(S14) 判斷該初始模擬模型之測量變數及應力變化是否均勻,若否,進入步驟S10,若是,進行步驟S15;及(S15) 基於變位模態模擬結果建立模擬模型。A method for simulating the stress change of a wall surface caused by displacement of the present invention. Step S1 includes the following steps: (S10) Establish an initial simulation model, and the simulation model includes a three-dimensional tunnel element as a plurality of different cross sections of the model boundary , And its measurement variables and displacement modes; (S11) Apply the displacement of the rigid body motion displacement mode to the boundary of the simulation model to obtain the stress change of the tunnel element relative to the rigid body motion; (S12) Whether the measured variables and stress changes of the initial simulation model are uniform, if not, proceed to step S10, and if so, proceed to step S13; (S13) Apply the cross-sectional displacement of the deformation displacement mode to the boundary of the simulation model to obtain the tunnel element Deformation stress change; (S14) determine whether the measured variables and stress changes of the initial simulation model are uniform, if not, go to step S10, if yes, proceed to step S15; and (S15) establish a simulation model based on the displacement modal simulation results.
本發明之一種變位量導致壁面的應力變化之模擬方法,步驟S2包含以下步驟:(S20) 取得該些斷面的變位之測量值;(S21) 得到該些斷面的變位之測量值的變位模態組成量;(S22a) 基於該變位模態組成量得到屬於斷面剛體運動的變位模態之組成量;(S23a) 基於作為隧道單元邊界之該斷面剛體運動而得到該隧道單元之相對剛體運動組成量,且基於該組成量排序該相對剛體運動種類;(S24a) 歸零該模擬模型之測量變數,且施加該相對剛體運動之值於該模擬模型邊界,得到該隧道單元相對剛體運動之應力變化;及(S22b) 基於該變位模態組成量得到屬於斷面變形的變位模態之組成量;(S23b) 基於作為隧道單元邊界之斷面變形得到該隧道單元之變形組成量,且基於該組成量排序變形模態;(S24b) 歸零該模擬模型之測量變數,且同時施加該變形模態之值於該模擬模型邊界,得到隧道單元變形之應力變化;(S25) 判斷步驟S24a中該模擬模型之測量變數及應力變化是否均勻,若是,進行步驟S3,若否,進行步驟S24a,及判斷步驟S24b中該模擬模型之測量變數及應力變化是否均勻,若是,進行步驟S3,若否,進行步驟S24b。A method for simulating the stress change of a wall surface caused by a displacement amount of the present invention, step S2 includes the following steps: (S20) obtaining the measured values of the displacements of the sections; (S21) obtaining the measured displacements of the sections The value of the displacement modal composition; (S22a) Based on the displacement modal composition, obtain the displacement modal composition of the section rigid body movement; (S23a) Based on the section rigid body movement as the boundary of the tunnel element Obtain the relative rigid body motion composition of the tunnel element, and sort the relative rigid body motion types based on the composition; (S24a) Zero the measurement variable of the simulation model, and apply the value of the relative rigid body motion to the simulation model boundary to obtain The stress change of the tunnel element relative to the rigid body movement; and (S22b) Based on the displacement mode composition amount, the displacement mode composition amount that belongs to the section deformation is obtained; (S23b) Based on the section deformation that is the boundary of the tunnel element, the Deformation composition of the tunnel element, and sort the deformation modes based on the composition; (S24b) Zero the measurement variables of the simulation model, and simultaneously apply the value of the deformation mode to the boundary of the simulation model to obtain the stress of the deformation of the tunnel element Change; (S25) Determine whether the measurement variables and stress changes of the simulation model in step S24a are uniform, if so, proceed to step S3, if not, proceed to step S24a, and determine whether the measurement variables and stress changes of the simulation model in step S24b are uniform If yes, go to step S3, if no, go to step S24b.
本發明之一種變位量導致壁面的應力變化之模擬方法,步驟S3包含以下步驟:(S30) 歸零該模擬模型之測量變數,施加該隧道單元邊界斷面變位之測量值於該模擬模型邊界,得到該隧道單元因斷面變位測量值引致之應力變化總量;(S31) 判斷該初始模擬模型之測量變數及應力變化是否均勻,若是,進行步驟S32,若否,進行步驟S34;(S32) 判斷襯砌應力超出強度位置與襯砌裂縫位置是否相符,若是,進行步驟S34,若否,進行步驟S33;(S33) 取得分析結果襯砌應力接近強度且未超過者,折減六種相對剛體運動量值及多種變形模態對應之邊界變位量、變形量輸入順序,迄襯砌應力超出強度位置與襯砌裂縫位置相符,之後進行步驟S30;及(S34) 得到分析隧道單元襯砌應力增量及變位量。A method for simulating the stress change of the wall surface caused by the displacement of the present invention. Step S3 includes the following steps: (S30) Zeroing the measurement variable of the simulation model, applying the measurement value of the displacement of the boundary section of the tunnel element to the simulation model The boundary to obtain the total stress change of the tunnel unit due to the measurement of the displacement of the section; (S31) determine whether the measured variables and stress changes of the initial simulation model are uniform, if so, proceed to step S32, if not, proceed to step S34; (S32) Determine whether the position where the lining stress exceeds the strength is consistent with the lining crack position. If so, proceed to step S34; if not, proceed to step S33; The input sequence of boundary displacement and deformation corresponding to the amount of motion and various deformation modes, until the position where the stress of the lining exceeds the strength corresponds to the position of the crack of the lining, then proceed to step S30; Bit amount.
上述「發明內容」並非用以限制所主張標的之範疇,本發明的各種分析檢定作業詳細概觀,在下述實施方式段落會做更進一步描述。The above "invention content" is not intended to limit the scope of the claimed subject matter. A detailed overview of various analysis and verification operations of the present invention will be further described in the following embodiment paragraphs.
為詳細說明本發明之技術內容、所達成的目的及功效,以下茲例舉實施例並配合圖式詳予說明。In order to explain the technical content, objectives and effects of the present invention in detail, the following examples are given in combination with the drawings for detailed description.
圖1係本發明之三維坐標定義與隧道空間關係的示意圖。FIG. 1 is a schematic diagram of the relationship between the three-dimensional coordinate definition and the tunnel space of the present invention.
圖2係本發明之變位量導致壁面的應力變化之模擬方法的流程圖,其包括步驟S1至步驟S3。步驟S1中,提供模擬模型,且該模擬模型包含三維隧道單元、做為模型邊界之不同的複數個斷面及其測量變數與變位模態。特定而言,步驟S1可建立與調整數值試驗模型,該三維模形可為隧道單元,且該壁面可為隧道的襯砌壁面。測量變數可為斷面變位量,進一步而言可為各種變位模態之變位量。圖3係取得不同之複數個監測斷面以供建立模擬模型、斷面變位量測量值等的示意圖。FIG. 2 is a flowchart of a simulation method of the wall surface stress change caused by the displacement amount of the present invention, which includes steps S1 to S3. In step S1, a simulation model is provided, and the simulation model includes a three-dimensional tunnel unit, a plurality of different cross sections as model boundaries, and measurement variables and displacement modes. Specifically, in step S1, a numerical test model can be established and adjusted, the three-dimensional model can be a tunnel unit, and the wall surface can be the lining wall surface of the tunnel. The measurement variable can be the amount of cross-sectional displacement, and further can be the displacement of various displacement modes. Fig. 3 is a schematic diagram of obtaining a plurality of different monitoring sections for the establishment of a simulation model, measurement values of section displacement, etc.
步驟S2中,根據該些斷面之變位量測量值計算該隧道單元的相對變位量及該變位模態之組成量且得到該壁面的應力變化之值。特定而言,步驟S2可解算該些監測斷面變位量之變位模態組成量,並根據該些變位模態組成量解算介於該些監測斷面間的隧道單元之相對變位量,進一步於該模擬模型邊界施加該變位量測量值及得到因該些相對變位量產生之應力變化。In step S2, the relative displacement amount of the tunnel element and the composition amount of the displacement mode are calculated according to the measured displacement values of the cross sections, and the value of the stress change of the wall surface is obtained. Specifically, in step S2, the displacement modality components of the monitoring cross-section displacements can be calculated, and the relative tunnel elements between the monitoring cross-sections can be solved according to the displacement modality components. The displacement amount is further applied to the displacement measurement value at the boundary of the simulation model and the stress change due to the relative displacement amounts is obtained.
步驟S3中,比對壁面應力變化與該壁面的裂縫分布,視情況修正該相對變位量之計算值以獲得與該裂縫分布相符之應力變化。特定而言,步驟S3可根據壁面應力變化均勻與否與隧道實際裂縫分布調整模擬模型,且求解得與裂縫分布相符之襯砌應力變化量。In step S3, the stress change on the wall surface and the crack distribution on the wall surface are compared, and the calculated value of the relative displacement is corrected as appropriate to obtain a stress change that is consistent with the crack distribution. Specifically, in step S3, the simulation model can be adjusted according to whether the wall stress change is uniform or not and the actual crack distribution of the tunnel, and the lining stress change amount that matches the crack distribution can be obtained.
圖4係步驟S1包含之進一步步驟的流程圖。如圖4所示,步驟S1包含步驟S10至步驟S15。步驟S10中,可建立初始模擬模型,且該模擬模型包含三維隧道單元、做為模型邊界之不同的複數個斷面及其測量變數與變位模態。特定而言,數值模型之建立/調整應至少考慮隧道幾何形狀、結構及監測斷面佈置位置、網格尺寸等。測量變數及變位模態可例如為圖5中之相對軸向平移、相對側向平移、相對垂直向平移、相對軸向旋轉、相對側向軸旋轉、相對垂直軸旋轉、均勻變形變位模態、橢圓變形變位模態、三角變形變位模態、四邊變形變位模態、五邊變形變位模態等。FIG. 4 is a flowchart of further steps included in step S1. As shown in FIG. 4, step S1 includes steps S10 to S15. In step S10, an initial simulation model can be established, and the simulation model includes a three-dimensional tunnel unit, a plurality of different sections as boundary of the model, and measurement variables and displacement modes. In particular, the establishment/adjustment of the numerical model should at least take into account the tunnel geometry, structure and location of the monitoring section, grid size, etc. Measurement variables and displacement modes can be, for example, relative axial translation, relative lateral translation, relative vertical translation, relative axial rotation, relative lateral axis rotation, relative vertical axis rotation, uniform deformation displacement mode in FIG. 5 State, elliptical deformation displacement mode, triangular deformation displacement mode, four-sided deformation displacement mode, five-sided deformation displacement mode, etc.
步驟S11中,可分別施加剛體運動變位模態之斷面變位量於該模擬模型邊界,得到該隧道單元相對剛體運動之應力變化。特定而言,可於模型邊界施加變位模態之變位量,即將數值模型邊界之一(遠)端固定,另一(近)端施加模擬的單位變位值,之後讀取隧道襯砌變位的結果。詳細而言,本發明可取相鄰監測斷面為一隧道單元,將其中一端視為固定端強制使變位為零,即可計算該相鄰監測斷面之相對變位,並假設兩監測斷面間變位呈線性分布(圖5及圖7)。將隧道單元前後監測斷面之相對運動輸入數值模型以模擬襯砌裂縫,如已有多期變位與裂縫監測,則可利用前期監測結果再次檢核並修正數值模型,並用於預測未來變位與裂縫之發展趨勢(圖10及圖11)。In step S11, the cross-sectional displacement of the rigid body motion displacement mode can be applied to the boundary of the simulation model to obtain the stress change of the tunnel element relative to the rigid body motion. Specifically, the displacement amount of the displacement mode can be applied to the model boundary, that is, one (far) end of the numerical model boundary is fixed, and the simulated unit displacement value is applied to the other (near) end, and then the tunnel lining deformation is read Bit results. In detail, in the present invention, the adjacent monitoring section can be regarded as a tunnel unit, one end is regarded as a fixed end and the displacement is forced to zero, the relative displacement of the adjacent monitoring section can be calculated, and it is assumed that the two monitoring sections The displacement between the surfaces is linearly distributed (Figure 5 and Figure 7). The relative movement of the monitoring section of the tunnel unit is input into the numerical model to simulate the lining cracks. If there are multiple stages of displacement and crack monitoring, the previous monitoring results can be used to recheck and revise the numerical model and used to predict the future displacement and The development trend of cracks (Figure 10 and Figure 11).
步驟S12中,可判斷該初始模擬模型之測量變數及應力變化是否均勻,若否,進入步驟S10,若是,進行步驟S13。特定而言,可對數值模型檢核隧道壁面變位及隧道壁面與圍岩應力變化是否均勻。In step S12, it can be determined whether the measurement variables and stress changes of the initial simulation model are uniform. If not, proceed to step S10, and if yes, proceed to step S13. In particular, the numerical model can be used to check whether the tunnel wall displacement and the tunnel wall and surrounding rock stress changes are uniform.
步驟S13中,可施加變形變位模態之變位值於該模擬模型邊界,得到隧道單元變形之應力變化。特定而言,可將數值模型邊界的遠端以需求方式固定,且於近端施加例如均勻壓縮、橢圓、三角、四邊等變形變位模態之變位量,且讀取隧道壁面變位與應力變化的情況。In step S13, the displacement value of the deformation displacement mode can be applied to the boundary of the simulation model to obtain the stress change of the tunnel element deformation. In particular, the distal end of the numerical model boundary can be fixed as required, and the displacement amount such as uniform compression, ellipse, triangle, and four-sided deformation displacement modes can be applied at the proximal end, and the tunnel wall displacement and Changes in stress.
步驟S14中,可判斷該變形模態與施加於模擬模型邊界的條件是否吻合,若否,進入步驟S10,若是,進行步驟S2。特定而言,可對數值模型檢核隧道壁面變位及隧道壁面與圍岩應力變化是否均勻。In step S14, it can be determined whether the deformation mode matches the conditions applied to the boundary of the simulation model. If not, proceed to step S10, and if so, proceed to step S2. In particular, the numerical model can be used to check whether the tunnel wall displacement and the tunnel wall and surrounding rock stress changes are uniform.
圖8係步驟S2包含之進一步步驟的流程圖。如圖8所示,步驟S2包含步驟S20至步驟S21、步驟S22a至步驟S24a及步驟S22b至步驟S24b。步驟S20中,可取得該些斷面的變位之測量值,進一步而言,可基於高精度的隧道變位監測技術得到該些斷面變位之測量值。特定而言,可依據隧道監測斷面三維空間坐標測量值計算該隧道斷面變位測量值。FIG. 8 is a flowchart of further steps included in step S2. As shown in FIG. 8, step S2 includes steps S20 to S21, steps S22a to S24a, and steps S22b to S24b. In step S20, the measured values of the displacements of the cross sections can be obtained. Further, the measured values of the displacements of the cross sections can be obtained based on a high-precision tunnel displacement monitoring technology. In particular, the measured value of the tunnel section displacement can be calculated based on the measured values of the three-dimensional coordinate of the tunnel monitoring section.
步驟S21中,可得到該些斷面的變位之測量值的變位模態組成量,進一步而言,可基於該斷面變位測量值得到變位模態組成量。特定而言,可依據監測斷面監測到的變位測量值而計算變位模態之組成量。In step S21, the displacement modal composition of the measured values of the displacement of the cross-sections can be obtained. Further, the displacement modal composition can be obtained based on the measurement of the displacement of the cross-section. In particular, the composition of the displacement mode can be calculated based on the displacement measurement value monitored by the monitoring section.
步驟S22a中,可基於該變位模態組成量得到屬於斷面剛體運動的變位模態之組成量。特定而言,可得到斷面變位測量值的變位模態組成中軸向平移,側向平移,垂直向平移與相對軸向旋轉,相對側向軸旋轉和相對垂直軸旋轉等六種變位模態對應的組成量之數值大小。In step S22a, the composition amount of the displacement mode belonging to the movement of the rigid body of the cross section can be obtained based on the composition amount of the displacement mode. In particular, the displacement modal components that can obtain the measured value of the cross-section displacement include six types of changes: axial translation, lateral translation, vertical translation and relative axial rotation, relative lateral axis rotation and relative vertical axis rotation The numerical value of the component quantity corresponding to the bit mode.
步驟S23a中,可基於作為隧道單元邊界之該斷面剛體運動而得到該隧道單元之相對剛體運動組成量,且基於該組成量排序該相對剛體運動種類,進一步而言,可基於隧道單元邊界兩個斷面之剛體運動變位模態組成量得到該隧道單元之相對剛體運動模態組成量,且基於該組成量大小排序該相對剛體運動種類。特定而言,可得到以其中一斷面為基準之剛體運動量值,且將隧道單元之六個相對剛體運動變位之值依據大小排序。In step S23a, the relative rigid body motion composition of the tunnel element can be obtained based on the section rigid body motion as the boundary of the tunnel element, and the relative rigid body motion types can be sorted based on the composition amount. The constitutive quantities of the rigid body motion displacement modal components of each section are obtained as the relative rigid body motion modal components of the tunnel element, and the relative rigid body motion types are sorted based on the size of the constituent components. In particular, the magnitude of rigid body motion based on one of the cross-sections can be obtained, and the six relative rigid body motion displacement values of the tunnel unit are sorted according to size.
步驟S24a中,可歸零該模擬模型之測量變數,且施加該相對剛體運動之值於該模擬模型邊界,得到該隧道單元相對剛體運動之應力變化,進一步而言,可歸零該模擬模型之測量變數,且施加該隧道單元相對剛體運動模態組成量對應之變位值於該模擬模型邊界。特定而言,可歸零數值模型之變位,且於數值模型邊界施加相對剛體運動變位模態對應之變位值。即依據剛體運動變位模態的組成量,自佔有斷面變位測量值最大組成量之剛體運動變位模態開始,依序於數值模型邊界施加對應之變位值。In step S24a, the measurement variable of the simulation model can be zeroed, and the value of the relative rigid body motion is applied to the boundary of the simulation model to obtain the stress change of the tunnel element relative to the rigid body motion. Further, the simulation model can be zeroed. The variable is measured, and the displacement value corresponding to the composition amount of the tunnel element relative to the rigid body motion modal is applied to the boundary of the simulation model. In particular, the displacement of the numerical model can be reset to zero, and the displacement value corresponding to the displacement mode of the rigid body motion is applied to the boundary of the numerical model. That is, according to the composition of the rigid body motion displacement mode, starting from the rigid body motion displacement mode that occupies the largest component of the cross-sectional displacement measurement value, the corresponding displacement value is applied in sequence at the boundary of the numerical model.
而於步驟S22b中,可基於該變位模態組成量得到屬於斷面變形的變位模態之組成量。特定而言,可得到斷面變位測量值的變位模態組成中相對於斷面形心放大或縮小之均勻變形變位模態,及相對於斷面形心之變形為橢圓形變位模態,相對於斷面形心之變形為三角形變位模態,相對於斷面形心之變形為四邊形變位模態,相對於斷面形心之變形為五邊形變位模態,乃至相對於斷面形心之變形為多邊形變位模態之複數種變位模態對應的組成量之數值大小。In step S22b, the composition amount of the displacement mode belonging to the cross-sectional deformation can be obtained based on the displacement mode composition amount. In particular, in the composition of the displacement mode that can obtain the measurement value of the displacement of the cross section, the uniform deformation displacement mode is enlarged or reduced relative to the centroid of the cross section, and the deformation relative to the centroid of the cross section is the elliptical displacement mode. Mode, the deformation relative to the centroid of the cross section is the triangle displacement mode, the deformation relative to the centroid of the cross section is the quadrangular displacement mode, and the deformation relative to the centroid of the cross section is the pentagon displacement mode, or even relative The deformation at the centroid of the cross section is the numerical value of the composition of the plural displacement modes of the polygon displacement mode.
步驟S23b中,可基於作為隧道單元邊界之斷面變形得到該隧道單元之變形組成量,且基於該組成量排序變形模態,進一步而言,可基於隧道單元邊界兩個斷面之變形變位模態組成量得到該隧道單元之變形組成量,且基於該組成量大小排序該變形模態。特定而言,可得到該隧道單元複數種變形模態依據大小排序之成果。In step S23b, the deformation composition amount of the tunnel element can be obtained based on the deformation of the section as the boundary of the tunnel element, and the deformation modes can be sorted based on the composition amount. Further, the deformation displacement of the two sections of the tunnel element boundary can be based on The modal composition quantity obtains the deformation composition quantity of the tunnel element, and the deformation modalities are sorted based on the composition quantity magnitude. In particular, the results of sorting multiple deformation modes of the tunnel element according to size can be obtained.
步驟S24b中,可歸零該模擬模型之測量變數,且同時施加該變形模態之值於該模擬模型邊界,得到隧道單元變形之應力變化,進一步而言,可歸零該模擬模型之測量變數,且施加該隧道單元變形模態組成量對應之變位值於該模擬模型邊界。特定而言,可歸零數值模型之變位,且基於該模擬模型邊界與該變形模態之組成量大小於該模擬模型邊界而施加對應該變形模態的變位量,從組成量最大之該變形模態開始,且向比例最小之該變形模態依序施加對應該變形模態的變位量於該模擬模型邊界。特定而言,可依據邊界與襯砌變形模態組成量於模型邊界施加對應變形模態之變位量,自現成比例最大變形模態開始,依序於模型邊界施加對應模態之變位量。In step S24b, the measurement variable of the simulation model can be zeroed, and the value of the deformation mode is applied to the boundary of the simulation model at the same time to obtain the stress change of the tunnel element deformation. Further, the measurement variable of the simulation model can be zeroed , And the displacement value corresponding to the deformation mode composition of the tunnel element is applied to the boundary of the simulation model. In particular, the displacement of the numerical model can be reset to zero, and the displacement corresponding to the deformation mode is applied based on the composition of the boundary of the simulation model and the deformation mode at the boundary of the simulation model, from the largest The deformation mode starts, and the displacement corresponding to the deformation mode is sequentially applied to the deformation mode with the smallest ratio at the boundary of the simulation model. In particular, the displacement of the corresponding deformation mode can be applied to the model boundary according to the composition of the boundary and the lining deformation mode, and the displacement of the corresponding mode can be applied in sequence from the model boundary starting from the ready-made maximum deformation mode.
以圓形隧道為例,進行第一次量測時,得到 A、B兩斷面各監測點的絕對座標,斷面皆可藉由監測點的絕對座標計算出該斷面形心位置,並將第二期量測得到之監測值與一次之值相減,再將A斷面之監測值與B斷面之值相減,如此可獲得此兩次量測期間A斷面各監測點相對於B斷面各監測點之變位情形,表示為 (𝑢𝑖 ,𝑣𝑖 ,𝑤𝑖 )AB,12 。斷面變位可分離為剛體運動與變形,其中剛體運動又可分離為剛體平移運動與剛體旋轉運動兩類。Taking the circular tunnel as an example, when the first measurement is performed, the absolute coordinates of each monitoring point of the A and B cross sections are obtained. The cross-sectional centroid position can be calculated by the absolute coordinates of the monitoring points, and Subtract the monitoring value obtained from the second phase measurement with the first value, and then subtract the monitoring value of section A from the value of section B, so as to obtain the relative monitoring points of section A during these two measurements The displacement of each monitoring point on Section B is expressed as (𝑢𝑖,𝑣𝑖,𝑤𝑖 ) AB,12 . The cross-section displacement can be separated into rigid body motion and deformation, of which rigid body motion can be separated into rigid body translational motion and rigid body rotational motion.
詳細而言,由分解變位之概念衍生出軸向單位平移,側向單位平移,垂直向平移與相對軸向旋轉,相對側向軸旋轉和相對垂直軸旋轉等六種剛體運動,加上均勻變形變位模態、橢圓變形變位模態、三邊變形變位模態、四邊變形變位模態、五邊變形變位模態等複數種相對於斷面形心之多邊變形等複數種變形,針對此複數種變位型態分別給予不同的邊界條件,探討個別導致之隧道壁面應力變化及裂縫型態。剛體平移係在圍岩模型的前斷面均勻施加 1單位長度的強制變位,即強制前斷面均勻地沿軸向(Y軸)、側向(X軸)或垂直向(Z軸)移動,側面假設線性漸變,使前、後兩斷面間變位連續分佈 (圖7(a)以側向平移為例);剛體旋轉是前斷面分別繞X軸、Y軸及Z軸旋轉,側面亦假設線性漸變,連結前、後兩斷面(圖7(b)以繞Z軸旋轉為例);變形則是使前後兩斷面皆施加強制變位,側面變位均勻分佈(圖7(c)以橢圓變形為例),以及使前斷面施加強制變位,側面假設線性漸變,連結前、後兩斷面。邊界條件則設置於襯砌及圍岩模型之前、後斷面上。簡而言之,該壁面係襯砌壁面,該變位量係該襯砌壁面在不同時間之空間位置變化,斷面為隧道中做為變位量測標的之監測橫斷面,該斷面包含數量足以偵測隧道變形現象之複數個監測點,該隧道單元係以二隧道監測斷面為邊界之隧道範圍,該斷面之所有監測點在不同時間之空間位置變化的集合為斷面變位量,特定斷面變化量係變位模態,其為斷面剛體運動與斷面變形,該變位模態對應已知的變位量及壁面應力變化,斷面剛體運動包含所有該監測點一致等量移動為平移變位模態,所有該監測點對斷面形心一致等量旋轉為旋轉變位模態,斷面變形變位模態包含斷面監測點相對於該斷面形心放大或縮小之均勻變形變位模態,及相對於該斷面形心之變形為橢圓形變形變位模態,相對於該斷面形心之變形為三角形變形變位模態,相對於該斷面形心之變形為四邊形變形變位模態,相對於該斷面形心之變形為五邊形變形變位模態,乃至相對於該斷面形心之變形為多邊形變形變位模態之複數種變位模態,且三維空間中隧道內通行方向為軸向,重力方向為垂直向,另一與軸向和垂直向正交之方向為側向,該三維空間中斷面剛體運動包含軸向平移,側向平移,垂直向平移與相對軸向旋轉,相對側向軸旋轉和相對垂直軸旋轉。In detail, six rigid body motions, such as axial unit translation, lateral unit translation, vertical translation and relative axial rotation, relative lateral axis rotation and relative vertical axis rotation, plus uniform Deformation displacement mode, ellipse deformation displacement mode, three-sided deformation displacement mode, four-sided deformation displacement mode, five-sided deformation displacement mode, etc. For the deformation, different boundary conditions are given for the multiple displacement patterns, and the stress changes and crack patterns of the tunnel wall caused by individual are discussed. The rigid body translation system applies a forced displacement of 1 unit length uniformly on the front section of the surrounding rock model, that is, the front section is forced to move uniformly in the axial direction (Y axis), lateral (X axis), or vertical direction (Z axis) Assuming a linear gradation on the side, the displacement between the front and back sections is continuously distributed (Figure 7(a) uses lateral translation as an example); rigid body rotation is the rotation of the front section around the X axis, Y axis and Z axis, respectively. The side also assumes a linear gradient, connecting the front and rear sections (Figure 7(b) takes the rotation around the Z axis as an example); the deformation is to force displacements on both the front and rear sections, and the side displacements are evenly distributed (Figure 7 (c) Take the elliptical deformation as an example), and apply a forced displacement to the front section. The side is assumed to have a linear gradient, connecting the front and back sections. The boundary conditions are set on the front and rear sections of the lining and surrounding rock models. In short, the wall is a lining wall, and the displacement is the spatial position of the lining wall at different times. The cross section is a monitoring cross section used as a displacement measurement target in the tunnel. A plurality of monitoring points sufficient to detect tunnel deformation. The tunnel unit is a tunnel area with the monitoring cross section of the second tunnel as the boundary. The set of all the monitoring points of the cross section changing in space at different times is the displacement of the cross section. , The change amount of a specific section is the displacement mode, which is the movement of the rigid body and the deformation of the section. The displacement mode corresponds to the known displacement and the change of the wall stress. The movement of the rigid body of the section includes all the monitoring points The equivalent movement is the translational displacement mode, and all the monitoring points are consistent with the centroid of the section. The equivalent rotation is the rotational displacement mode. The section deformation displacement mode includes the section monitoring point enlarged relative to the centroid of the section. Or reduced uniform deformation deformation mode, and the deformation relative to the centroid of the section is elliptical deformation displacement mode, and the deformation relative to the centroid of the section is triangular deformation displacement mode, relative to the fracture The deformation of the face centroid is the quadrilateral deformation displacement mode, the deformation with respect to the section centroid is the pentagonal deformation displacement mode, and the deformation with respect to the section centroid is the polygonal deformation displacement mode There are multiple displacement modes, and the passage direction in the three-dimensional space is the axial direction, the gravity direction is the vertical direction, and the other direction orthogonal to the axial direction and the vertical direction is the lateral direction. Pan translation, lateral translation, vertical translation and relative axial rotation, relative lateral axis rotation and relative vertical axis rotation.
於步驟S25中,可判斷步驟S24a中該模擬模型之測量變數及應力變化是否均勻,若是,進行步驟S3,若否,進行步驟S24a,及判斷步驟S24b中該模擬模型之測量變數及應力變化是否均勻,若是,進行步驟S3,若否,進行步驟S24b。In step S25, it can be determined whether the measurement variables and stress changes of the simulation model in step S24a are uniform. If so, proceed to step S3, if not, proceed to step S24a, and determine whether the measurement variables and stress changes of the simulation model in step S24b Uniform, if yes, go to step S3, if no, go to step S24b.
於步驟S30中,可歸零該模擬模型之測量變數,施加該隧道單元邊界斷面變位之測量值於該模擬模型邊界,得到該隧道單元因斷面變位測量值引致之應力變化總量。特定而言,可計算該斷面變位測量值造成的壁面應力變化量值。In step S30, the measurement variable of the simulation model can be reset to zero, and the measurement value of the displacement of the tunnel unit boundary section is applied to the boundary of the simulation model to obtain the total stress change of the tunnel unit due to the measurement value of the section displacement . In particular, the amount of change in wall stress caused by the measurement of the displacement of the cross-section can be calculated.
於步驟S31中,可判斷該初始模擬模型之測量變數及應力變化是否均勻,若是,進行步驟S32,若否,進行步驟S34。In step S31, it can be determined whether the measurement variables and stress changes of the initial simulation model are uniform. If so, proceed to step S32, if not, proceed to step S34.
如上所述步驟S3可在不同情況中達到步驟S34。第一種情況,若步驟S31之結果為否,得到分析隧道單元襯砌應力增量及變位量結果。第二種情況,若步驟S31之結果為是,且步驟S32之襯砌壁面應力超出強度位置與襯砌裂縫位置相符,得到分析隧道單元襯砌應力增量及變位量結果。第三種情況,若步驟S31之結果為是且步驟S32之結果為否,進行步驟S33,即可取得分析結果襯砌應力接近強度且未超過者,折減六種相對剛體運動量值及多種變形模態對應之邊界變位量、變形量輸入順序,迄襯砌應力超出強度位置與襯砌裂縫位置相符,之後進行步驟S30。進一步而言,可取得應力超過該襯砌壁面強度、接近或等於該壁面材料的強度之壁面的空間位置,且折減複數個相對之該測量變數及對應該變位模態之斷面變位量的值,以折減過之變位模態斷面變位量施加於該模擬模型邊界,至壁面應力小於該壁面材料強度或壁面應力大於該壁面材料強度位置與襯砌裂縫位置相符為止。特定而言,可取得分析結果襯砌應力接近該壁面材料的強度且未超過者,減少六個相對單位變位分量及變形模態對應之邊界變位量、變形量輸入數值,迄壁面應力小於該壁面材料強度或襯砌應力超出該壁面材料的強度位置與襯砌裂縫位置相符。而測量變數導致襯砌裂縫型態之範例係如圖10所示。隧道單元因前後監測斷面相對運動引致之襯砌裂縫的模擬範例與實際案例比較結果係如圖11所示。Step S3 as described above can reach step S34 in different situations. In the first case, if the result of step S31 is no, the result of analyzing the stress increment and displacement of the tunnel unit lining is obtained. In the second case, if the result of step S31 is YES, and the position where the stress exceeds the strength of the lining wall in step S32 is consistent with the position of the lining crack, the result of analyzing the stress increment and displacement of the lining of the tunnel element is obtained. In the third case, if the result of step S31 is yes and the result of step S32 is no, proceed to step S33 to obtain the analysis result. If the lining stress is close to the strength and does not exceed it, the six relative rigid body motion values and multiple deformation modes are reduced. The input sequence of boundary displacement and deformation corresponding to the state corresponds to the location where the stress of the lining exceeds the strength and the location of the crack of the lining, and then step S30 is performed. Further, the spatial position of the wall with a stress exceeding the strength of the lining wall, close to or equal to the strength of the wall material can be obtained, and a plurality of relative measurement variables and cross-sectional displacements corresponding to the displacement modes can be reduced The value of, is applied to the boundary of the simulation model with the reduced displacement mode cross-sectional displacement until the wall stress is less than the wall material strength or the wall stress is greater than the wall material strength and the lining crack position matches. In particular, the analysis result can be obtained that the lining stress is close to the strength of the wall material and does not exceed the input value of the boundary displacement and deformation corresponding to the six relative unit displacement components and deformation modes, and the wall stress is less than this The position where the strength of the wall material or the stress of the lining exceeds the strength of the wall material is consistent with the position of the crack of the lining. An example of measurement variables leading to lining crack patterns is shown in Figure 10. The simulation results of the lining cracks caused by the relative movement of the cross section of the tunnel unit before and after monitoring the cross section and the actual case are shown in Figure 11.
綜上所述,本發明能協助釐清隧道劣化的兩個重要指標即變位與裂縫的交互影響,輸入變位監測結果獲得引致之隧道襯砌應力、應變分布與裂縫型態,經實際監測資料檢核校正後,得到可描述案例隧道變位-裂縫機制的數值模型,可用於在長期監測下預測裂縫發展趨勢、模擬補強工法成效、評估隧道健全度和安全性等,對隧道維護管理最佳化提供實質建議。In summary, the present invention can help to clarify the two important indicators of tunnel deterioration, namely the interaction between displacement and cracks. Input the displacement monitoring results to obtain the tunnel lining stress, strain distribution and crack pattern, which are checked by actual monitoring data. After the nuclear correction, a numerical model that can describe the tunnel displacement-crack mechanism of the case can be obtained, which can be used to predict the crack development trend under long-term monitoring, simulate the effectiveness of the reinforcement method, evaluate the tunnel health and safety, etc., and optimize the maintenance and management of the tunnel. Provide substantive suggestions.
雖然本發明以具體實施例揭示如上,然其所揭示的具體實施例並非用以限定本發明,任何熟悉此技藝者,在不脫離本發明之精神和範圍內,當可作各種之更動與潤飾,其所作之更動與潤飾皆屬於本發明之範疇,本發明之保護範圍當視後附之申請專利範圍所界定者為準。Although the present invention is disclosed as above with specific embodiments, the disclosed specific embodiments are not intended to limit the present invention. Anyone who is familiar with this art can make various changes and modifications without departing from the spirit and scope of the present invention. The changes and retouching made by it belong to the scope of the present invention, and the scope of protection of the present invention shall be subject to the scope defined in the appended patent application.
S1、S2、S3、S10、S11、S12、S13、S14、S15、S20、S21、S22a、S23a、S24a、S22b、S23b、S24b、S25、S30、S31、S32、S33、S34‧‧‧步驟S1, S2, S3, S10, S11, S12, S13, S14, S15, S20, S21, S22a, S23a, S24a, S22b, S23b, S24b, S25, S30, S31, S32, S33, S34
圖1係本發明之三維坐標定義與隧道空間關係的示意圖。 圖2係本發明之變位量導致壁面的應力變化之模擬方法的流程圖。 圖3係任意隧道內複數個斷面變位量及隧道單元相對變位的示意圖。 圖4係步驟S1包含之進一步步驟的流程圖。 圖5係隧道單元前後監測斷面的建構示意圖。 圖6係各種變位模態的示意圖,包含六種剛體運動變位模態及部分變形變位模態。 圖7係模擬模型中強制變位分佈的示意圖。 圖8係步驟S2包含之進一步步驟的流程圖。 圖9係步驟S3包含之進一步步驟的流程圖。 圖10係各種變位模態之測量變數導致襯砌裂縫型態之範例的示意圖。 圖11係隧道單元因前後監測斷面相對運動引致之襯砌裂縫的模擬與實際結果範例。FIG. 1 is a schematic diagram of the relationship between the three-dimensional coordinate definition and the tunnel space of the present invention. FIG. 2 is a flowchart of a simulation method of the wall surface stress change caused by the displacement amount of the present invention. Figure 3 is a schematic diagram of the displacement of a plurality of cross sections and the relative displacement of tunnel units in any tunnel. FIG. 4 is a flowchart of further steps included in step S1. Figure 5 is a schematic diagram of the construction of the monitoring section before and after the tunnel unit. Figure 6 is a schematic diagram of various displacement modes, including six rigid body movement displacement modes and partial deformation displacement modes. Fig. 7 is a schematic diagram of the forced displacement distribution in the simulation model. FIG. 8 is a flowchart of further steps included in step S2. 9 is a flowchart of further steps included in step S3. FIG. 10 is a schematic diagram of an example in which the measurement variables of various displacement modes result in the cracking pattern of the lining. Figure 11 is an example of the simulation and actual results of the lining cracks caused by the relative movement of the monitoring section of the tunnel unit before and after monitoring.
S1、S2、S3‧‧‧步驟 S1, S2, S3 ‧‧‧ steps
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Families Citing this family (13)
Publication number | Priority date | Publication date | Assignee | Title |
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CN112417542A (en) * | 2020-07-31 | 2021-02-26 | 中电建路桥集团有限公司 | Numerical simulation method for verifying reasonability of tunnel construction excavation scheme |
CN112528360B (en) * | 2020-08-14 | 2024-02-02 | 中铁十六局集团有限公司 | Calculation method for deformation of cross section of underlying tunnel caused by construction of building structure |
CN111985028B (en) * | 2020-08-14 | 2024-02-02 | 中铁十六局集团有限公司 | Calculation method for cross section deformation of adjacent tunnel segment caused by engineering precipitation |
CN112197743B (en) * | 2020-10-10 | 2022-05-17 | 北京工商大学 | Subway tunnel contour-envelope shortest distance analysis method |
CN113532903B (en) * | 2021-08-20 | 2023-03-17 | 中铁隧道局集团有限公司 | Freezing and thawing cycle environment cold region tunnel simulation test platform |
CN114033433B (en) * | 2021-11-16 | 2023-07-25 | 中铁十二局集团有限公司 | Plateau high-ground stress tunnel secondary lining crack monitoring construction method |
CN114969902B (en) * | 2022-03-04 | 2024-06-25 | 西南交通大学 | Active support design method for high-altitude railway high-ground-stress hard rock tunnel |
CN114910626B (en) * | 2022-05-13 | 2023-08-15 | 山东科技大学 | Model test device and method based on basic mosaic unit |
CN115200540B (en) * | 2022-07-08 | 2023-07-28 | 安徽省皖北煤电集团有限责任公司 | Mine roadway deformation monitoring and early warning method and system |
CN115929408B (en) * | 2023-01-17 | 2023-09-19 | 河南理工大学 | Real-time monitoring system and method for coal mine roof fracture in tunneling process |
US12031436B1 (en) | 2023-01-17 | 2024-07-09 | Henan Polytechnic University | Real-time monitoring system and method for coal mine roof fractures during roadway tunneling process |
CN116067333B (en) * | 2023-03-14 | 2023-06-16 | 山东省物化探勘查院 | Method and system for determining deformation of foundation pit support pile by adopting comprehensive theory |
CN117870629B (en) * | 2024-03-13 | 2024-05-10 | 中铁七局集团广州工程有限公司 | Intelligent tunnel rock mass monitoring method |
Family Cites Families (10)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2003065755A (en) * | 2001-08-21 | 2003-03-05 | Taisei Corp | Displacement measuring method for tunnel shape |
KR100457244B1 (en) * | 2002-04-11 | 2004-11-16 | 에스케이건설 주식회사 | A method for forecasting soft ground may be fit face ahead in case of tunneling |
KR100765973B1 (en) * | 2005-11-09 | 2007-10-15 | 주식회사 동호 | instrument measuring underground stress and method measuring of ground movements in case of build in tunnel |
TW200940791A (en) * | 2008-03-19 | 2009-10-01 | Tech Internat Co Ltd E | Conductive concrete heating technology pavement surface and deicingmethod |
JP2010001633A (en) * | 2008-06-19 | 2010-01-07 | Maeda Corp | Tunnel, tunnel construction method, and device for suppressing cracking of lining concrete |
JP2013047629A (en) * | 2011-08-29 | 2013-03-07 | Mie Univ | Method for measuring structure inner space displacement and apparatus thereof |
CN104819702B (en) * | 2015-04-21 | 2017-07-11 | 同济大学 | A kind of segment deformation transmits the modification method of influence on static level elevation |
CN205300520U (en) * | 2015-12-07 | 2016-06-08 | 中国石油天然气股份有限公司 | Tunnel engineering deformation monitoring system |
CN105651226B (en) * | 2015-12-29 | 2018-11-02 | 上海隧道工程有限公司 | The section of jurisdiction monitoring method of class rectangle shield tunnel |
CN107830812B (en) * | 2017-09-14 | 2019-10-18 | 同济大学 | A kind of laser reflection piece implementation method suitable for positioning in tunnel with deformation analysis |
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