Working-point control technique for the homodyne interferometry in hydrophone calibration

2015 ◽  
Author(s):  
Ping Yang ◽  
Guangzhen Xing
2013 ◽  
Vol 25 (24) ◽  
pp. 2412-2415 ◽  
Author(s):  
Yupeng Li ◽  
Yangan Zhang ◽  
Yongqing Huang

2008 ◽  
Vol 6 (5) ◽  
pp. 381-383 ◽  
Author(s):  
王泽锋 王泽锋 ◽  
Zefeng Wang Zefeng Wang ◽  
胡永明 胡永明 ◽  
Yongming Hu Yongming Hu ◽  
孟洲 孟洲 ◽  
...  

2018 ◽  
Vol 36 (18) ◽  
pp. 3824-3836 ◽  
Author(s):  
Xiaolei Li ◽  
Lei Deng ◽  
Xiaoman Chen ◽  
Haiping Song ◽  
Yahao Liu ◽  
...  

2011 ◽  
Vol 131 (7) ◽  
pp. 536-541 ◽  
Author(s):  
Tarek Hassan Mohamed ◽  
Abdel-Moamen Mohammed Abdel-Rahim ◽  
Ahmed Abd-Eltawwab Hassan ◽  
Takashi Hiyama

2020 ◽  
Vol 15 (3) ◽  
pp. 37-48
Author(s):  
Zubair Rashid Wani ◽  
Manzoor Ahmad Tantray

The present research work is a part of a project was a semi-active structural control technique using magneto-rheological damper has to be performed. Magneto-rheological dampers are an innovative class of semi-active devices that mesh well with the demands and constraints of seismic applications; this includes having very low power requirements and adaptability. A small stroke magneto-rheological damper was mathematically simulated and experimentally tested. The damper was subjected to periodic excitations of different amplitudes and frequencies at varying voltage. The damper was mathematically modeled using parametric Modified Bouc-Wen model of magneto-rheological damper in MATLAB/SIMULINK and the parameters of the model were set as per the prototype available. The variation of mechanical properties of magneto-rheological damper like damping coefficient and damping force with a change in amplitude, frequency and voltage were experimentally verified on INSTRON 8800 testing machine. It was observed that damping force produced by the damper depended on the frequency as well, in addition to the input voltage and amplitude of the excitation. While the damping coefficient (c) is independent of the frequency of excitation it varies with the amplitude of excitation and input voltage. The variation of the damping coefficient with amplitude and input voltage is linear and quadratic respectively. More ever the mathematical model simulated in MATLAB was in agreement with the experimental results obtained.


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