Electroelastic Deformation of a Piezoelectric FGM Coated Half-Plane Caused by an Electrostatic Potential Difference Applied to the Strip Electrode on the Surface

Author(s):  
Sergey S. Volkov ◽  
Andrey S. Vasiliev ◽  
Sergei M. Aizikovich ◽  
Alexandr N. Litvinenko
IEEE Access ◽  
2019 ◽  
Vol 7 ◽  
pp. 79455-79462 ◽  
Author(s):  
Kaihao Tang ◽  
Hongli Hu ◽  
Lin Li ◽  
Yong Qin ◽  
Xiaoxin Wang

2007 ◽  
Vol 441 (1-3) ◽  
pp. 148-151 ◽  
Author(s):  
Mario Carrasco ◽  
Raquel Coca ◽  
Isabel Cruz ◽  
Silvia Daza ◽  
Manuela Espina ◽  
...  

CrystEngComm ◽  
2016 ◽  
Vol 18 (44) ◽  
pp. 8631-8636 ◽  
Author(s):  
M. D. Perera ◽  
J. Desper ◽  
A. S. Sinha ◽  
C. B. Aakeröy

Calculated molecular electrostatic potential difference (ΔMEP) of acceptor atoms in a multi component system will lead to different supramolecular architectures.


2021 ◽  
Vol 69 (1) ◽  
Author(s):  
Christian Seidl ◽  
Johannes L. Hörmann ◽  
Lars Pastewka

AbstractWe study the frictional response of water-lubricated gold electrodes subject to an electrostatic potential difference using molecular dynamics simulations. Contrary to previous studies on electrotunable lubrication that were carried out by fixing the charges, our simulations keep electrodes at fixed electrostatic potential using a variable charge method. For pure water and NaCl solutions, viscosity is independent of the polarization of the electrodes, but wall slip depends on the potential difference. Our findings are in agreement with previous analytical theories of how wall slip is affected by interatomic interactions. The simulations shed light on the role of electrode polarization for wall slip and illustrate a mechanism for controlling friction and nanoscale flow in simple aqueous lubricants.


1994 ◽  
Vol 133 ◽  
pp. 85-125 ◽  
Author(s):  
Mitsuru Nakai

Divide the ideal boundary of a noncompact Riemannian manifold M into two parts δ0 and δ1 Viewing that M is surrounded by two conducting electrodes δ0 and δ1 we ask whether (M; δ0, δ1) functions as a condenser in the sense that the unit electrostatic potential difference between two electrodes is produced by putting a charge of finite energy on one electrode when the other is grounded. The generalized condenser problem asks whether there exists a subdivision δ0 ∪ δ1 of the ideal boundary of M such that (M; δ0, δ1 functions as a condenser.


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