scholarly journals Predicting the Dynamic Stiffness of a Glove Material using Mechanical Impedance Model

2019 ◽  
Vol 1262 ◽  
pp. 012028
Author(s):  
K. A. Md Razali ◽  
R. Samin ◽  
A. As’arry ◽  
N. A. A. Jalil
2013 ◽  
Vol 6 (1) ◽  
pp. 73-88 ◽  
Author(s):  
Yoshiyuki TANAKA ◽  
Shunsuke FUKUSHIMA ◽  
Masaya YAMASHITA ◽  
Yoshinobu OOTANI ◽  
Toshio TSUJI

1974 ◽  
Vol 96 (3) ◽  
pp. 1000-1005 ◽  
Author(s):  
M. G. Sainsbury ◽  
D. J. Ewins

A detailed dynamic analysis is made of a heavily damped foundation structure designed for the multidirectional isolation of machinery vibrations. The principal components of the structure are damped sandwich beams and complex-shaped rubber blocks. In order to study the complete structure, each component was analyzed for its mechanical impedance data. Where possible, these were obtained theoretically, but in some cases it was necessary to resort to experimental measurement. The individual components were then connected together using the dynamic stiffness coupling technique in order to predict the vibration characteristics of the complete structure. The accuracy of the final results testifies to the feasibility of combining measured and theoretical data in this way in order to analyze a complex mechanical structure.


1999 ◽  
Author(s):  
Victor Giurgiutiu ◽  
Craig A. Rogers

Abstract The electro-mechanical (E/M) impedance method has gained acceptance as an effective technique for structural health monitoring, damage detection, and failure prevention. In spite of extensive experimental validation of this novel method, very little work has been dedicated to its modeling. This paper develops a model of the E/M impedance response of a damaged composite beam interrogated by a PZT wafer active sensor. The electromechanical model for the interaction between the beam and the active sensor is developed from first principles. The effective axial force and bending moments induced by the PZT wafer into the beam are considered. Equations of motion for the flexural vibrations of a composite beam under moment excitation are developed. Solution in terms of normal modes with internal damping is obtained. The resulting response and the applied force are utilized to deduce general expressions for pointwise dynamic stiffness and pointwise dynamic compliance. Effective stiffness of the PZT wafer is also calculated, and the complex stiffness ratio for the PZT-structure interaction is determined. Hence, the complex electro-mechanical impedance and admittance are deduced. A numerical example is given to illustrate the method and test its effectiveness. It is found that the real part of the effective pointwise dynamic stiffness interacts at par with the PZT stiffness at structural resonance frequencies. The imaginary part of the complex stiffness ratio directly reflects the pointwise structural resonances. Consequently, the real part of the electro-mechanical impedance directly reflects the pointwise structural resonances too. The same behavior is also found in the electro-mechanical admittance. Thus, the real part of the E/M impedance and the real part of the E/M admittance are found to be direct measures of the structural response, reflective of damage presence.


Proceedings ◽  
2018 ◽  
Vol 2 (13) ◽  
pp. 921
Author(s):  
Karolina Orłowska ◽  
Wojciech Majstrzyk ◽  
Andrzej Sierakowski ◽  
Tomasz Piasecki ◽  
Teodor Gotszalk

In this work we present how to describe mechanical impedance of a photon force (PF) MEMS sensor dedicated to structures’ optomechanical studies. An actuating force (photon force) is caused by the reflection and absorption of the electromagnetic radiation beam due to the radiation pressure effect. Specially designed very soft (low k-constant, ca 10–150 mN/m) cantilevers are presented. The structures integrate a Lorentz loop, which enables electromagnetic actuation. The construction with two mirrors is proposed so that parasitic thermal actuation can be neglected. The MEMS displacement is measured with the use of a laser vibrometer. The mechanical impedance model is presented using which the stiffness is calculated. As validation measurements: thermal noise and known mass adding methods are used.


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