本論文主旨針對降低橋樑光纖感測系統建置成本進行可行性評估及測試，並提出三種不同光路架構進行討論。實驗首先提出一寬平坦光源與可調式光纖光柵當作濾波器的功率感測系統，觀測端利用Labview自行開發出一訊號擷取程式，並進行單點的橋樑撓曲度感測。在寬頻光源架構底下，波長完全吻合的情況下可得到最大功率-29.66 dBm，光纖光柵受力後會逐漸遞減至最低功率-41.26 dBm，相關係數R^2為0.93，解析度在曲率<12 m-1時為12.29 με，而曲率介於12 m-1到27 m-1時解析度則為37.56 με。而後，在第四章中我們又針對中長距離橋樑導入環形雷射架構，使整體功率上升，當濾波器與光纖光柵波長吻合的情形下最大功率達-9.01 dBm，開始受力後逐漸遞減至最小功率-21.5 dBm，相關係數R^2為0.9412，解析度在曲率< 12 m-1約為12.53 με，而曲率介於12 m-1到27 m-1時解析度約為28.55 με。最後，我們提出了一分佈式光纖感測網路，在系統中加入陣列波導光柵(AWG)，增加主系統的擴充性預期可減少系統佈建數量，進而降低成本。首先取用陣列波導光柵的兩個分別位在1539.76 nm及1540.56 nm的通道。當系統使用摻鉺光纖放大器做光源時，模擬結果在1540.5 nm處有單一波長產生，實驗波長同樣位在約1540.65 nm的位置，此原因為摻鉺光纖放大器的均勻展寬特性。當光源換成半導體放大器時，由模擬結果顯示兩個分別位在1539.8 nm與1540.6 nm位置的波峰產生；實作中，同樣出現兩個位在1539.89 nm與1540.71 nm位置的波峰，此為半導體放大器的非均勻展寬特性所造成的結果。除此之外，頻譜中多波長效應起因於端面間的不規律反射，而功率的不均等現象則與四波混頻效應及元件插入損耗的不同有關。

The purpose of this thesis is to evaluate and test the feasibility of reducing the construction cost of optical fiber sensing system for bridge, and propose three different optical structures. In this thesis, a broadband light source and tunable fiber grating are proposed as a filter for power sensing system. The observation end utilizes Labview to develop a power acquisition program and perform single-point bridge deflection. Under broadband light source structure, in the case of a complete match of the wavelength can obtain a maximum power of -29.66 dBm, followed by a decline to the lowest power at -41.26 dBm while force onto the FBG. The correlation coefficient R^2 is 0.93. Resolution equals 12.29 με while curvature below 12 m-1 and 37.56 με when curvature is between 12 m-1 to 27 m-1. For the long-distance bridge, we proposed the ring laser structure into the system, so that the overall power rise in the case of maximum power of -9.01 dBm, and followed by decline to the lowest power at -22.4 dBm while force onto the FBG. The correlation coefficient R^2 is 0.9412. Resolution equals 12.53 με while curvature below 12 m-1 and 28.55 με when curvature is between 12 m-1 to 27 m-1. To increase extensibility of fiber sensing network, , we designed a distributed fiber optical sensing network and apply a arrayed waveguide grating (AWG) into the system. At the first, we take two AWG channels, which located at 1539.76 nm and 1540.56 nm. When we applied Erbium-doped Optical Fiber Amplifier (EDFA) light source, there is a single peak at 1540.5 nm, the experimental wavelength is also shown at 1540.65 nm. The reason is due to homogeneous broaden characteristics of EDFA. While we applied semiconductor optical amplifier (SOA), the simulation results show that the two peaks appear at 1539.8 nm and 1540.6 nm simultaneously. The experiment also shows two peaks anchored at 1539.89 nm and 1540.71 nm. This is because the inhomogeneous broaden characteristics of a SOA. In addition, the multi-wavelength effect in the spectrum is due to the irregular reflection between the end faces, and the power inequality is due to the effect of four-wave mixing and the difference of the component insertion loss.

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