• Title/Summary/Keyword: HYSTERESIS INDEX

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FBG Sensor Signal Processing System using SLD Tunable Light Source and Etalon Filter (SLD동조 광원과 에탈론 필터를 이용한 FBG 센서 신호처리 시스템)

  • Chung, Chul;Lee, Ho-Joon;Kim, Ki-Soo
    • Journal of the Institute of Electronics Engineers of Korea SD
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    • v.41 no.3
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    • pp.39-44
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    • 2004
  • Fiber Bragg grating sensors are fabricated by core index modulation using UV laser and phasemask. Bragg wavelength of the grating is changed by the external strain. In this paper, a signal processing system of fiber Bragg grating sensor has studied in the optical wavelength domain. The system is based on the sweep semiconductor light source that consists of SLD, F-P tunable filter and etalon filter. The hysteresis effects of PZT in the F-P tunable filter are compensated. The long term measurement stability is obtained by controlling the temperature of F-P tunable filter and the SLD. We compare the strain data from fiber Bragg grating sensor and that from strain gauge at concrete hume pipe. We also get very good results for the long gauge displacement using fiber Bragg grating sensor which are identical to the data with short gauge length ordinary displacement sensor.

Experimental and numerical analysis of seismic behaviour for recycled aggregate concrete filled circular steel tube frames

  • Xianggang Zhang;Gaoqiang Zhou;Xuyan Liu;Yuhui Fan;Ercong Meng;Junna Yang;Yajun Huang
    • Computers and Concrete
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    • v.31 no.6
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    • pp.537-543
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    • 2023
  • To study the seismic behavior of recycled aggregate concrete filled circular steel tube (RACFCST) frames, the seismic behavior experiment of RACFCST frame was carried out to measure the hysteresis curve, skeleton curve and other seismic behavior indexes. Moreover, based on the experimental study, a feasible numerical analysis model was established to analyze the finite element parameters of 8 RACFCST frame specimens, and the influence of different variation parameters on the seismic behavior index for RACFCST frame was revealed. The results showed that the skeleton curve of specimens under different axial compression ratios were divided into three stages: elastic stage, elastic-plastic stage and descending stage, and the descending stage was relatively stable, indicating that the specimen had stronger deformation capacity in the descending stage. With the increase of axial compression ratio, the peak bearing capacity of all specimens reduced gradually, and the reduction was less than 5%. With the decrease of beam-column linear stiffness ratio, the peak bearing capacity decreased gradually. With the decrease of yield bending moment ratio of beam-column, the peak bearing capacity decreased gradually, and the decreasing rate of peak bearing capacity gradually accelerated. In addition, compared with the axial compression ratio, the beam-column linear stiffness ratio and the yield bending moment ratio of beam-column had a more significant influence on the peak bearing capacity of RACFCST frame.

Pyroelectricity of BaTiO3-doped PMNT ferroelectric system for pyroelectric sensor

  • Yeon Jung Kim
    • Journal of the Korean institute of surface engineering
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    • v.56 no.6
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    • pp.380-385
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    • 2023
  • In this study, an MPB PMNT system containing 0.05 to 0.10 wt.% BaTiO3 was synthesized using a traditional chemical method and its pyroelectricity was investigated. Pyroelectricity, dielectricity, and ferroelectricity of the synthesized BaTiO3-PMNT system were analyzed by heat treatment at 1240~1280 ℃ for 4 hours to evaluate its applicability as a pyroelectric sensor. Unlike the simple ABO3 ferroelectric, the BaTiO3-doped PMNT system exhibited phase transition characteristics over a wide temperature range typical of complex perovskite structures. Although no dramatic change could be confirmed depending on the amount of BaTiO3 added, stable pyroelectricity was maintained near room temperature and over a wide temperature range. When the amount of BaTiO3 added increased from 0.05BaTiO3-PMNT to 0.10BaTiO3-PMNT, the electric field slightly increased from 5.00×103 kV/m to 6.75×103 kV/m, and the maximum value of remanent polarization slightly increased from 0.223 C/m2 to 0.234 C/m2. The pyroelectric coefficients of 0.05BaTiO3-PMNT and 0.10BaTiO3- PMNT at room temperature were measured to be ~0.0084 C/m2K and ~0.0043 C/m2K, respectively. The relaxor ferroelectric properties of the BaTiO3-PMNT system were confirmed by analyzing the plot of Kmax/K versus (T-Tmax)γ. The BaTiO3-doped MPB PMNT system showed a distinct pyroelectric performance index at room temperature, and the values were Fv ~ 0.0362 m2/C, Fd ~ 0.575×10-4 Pa-1/2.