Adjustable current waveform via altering the damping coefficient: A new way to reduce Joule heating in electromagnetic forming coils

2021 ◽  
Vol 293 ◽  
pp. 117086
Author(s):  
Limeng Du ◽  
Liangyu Xia ◽  
Xian Li ◽  
Li Qiu ◽  
Zhipeng Lai ◽  
...  
2011 ◽  
Vol 131 (4) ◽  
pp. 288-294 ◽  
Author(s):  
Tatsuya Furukawa ◽  
Keita Akagi ◽  
Hisao Fukumoto ◽  
Hideaki Itoh ◽  
Hiroshi Wakuya ◽  
...  

2012 ◽  
Vol 132 (2) ◽  
pp. 187-191 ◽  
Author(s):  
Yoshinobu Murakami ◽  
Takahiro Takino ◽  
Naohiro Hozumi ◽  
Masayuki Nagao

2010 ◽  
Vol 130 (3) ◽  
pp. 265-271 ◽  
Author(s):  
Shuji Sato ◽  
Seisuke Nishimura ◽  
Shingo Seki

2018 ◽  
Vol 138 (5) ◽  
pp. 346-351 ◽  
Author(s):  
Hiroyuki Kaneko ◽  
Naoki Itamoto ◽  
Kazuo Shinjo

2011 ◽  
Vol 131 (7) ◽  
pp. 574-583 ◽  
Author(s):  
Shin-ichi Tanaka ◽  
Tsukasa Miyagi ◽  
Mikimasa Iwata ◽  
Tadashi Amakawa

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.


Equipment ◽  
2006 ◽  
Author(s):  
C. Yang ◽  
G. Y. Tang ◽  
D. G. Yan ◽  
H. Q. Gong ◽  
John C. Chai ◽  
...  

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