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Abstract
We design the static and dynamic characteristics of a piezoelectric nanomicrotransducer intended for use in nanotechnology
and microelectronic hardware, devise its parametric structural schematic diagram, and determine the influence of its physical
and geometric parameters on its static and dynamic characteristics.
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... By solving the wave equation with allowance methods of mathematical physics for equation electromagnetoelasticity, the boundary conditions on loaded working surfaces of actuators, the strains along the coordinate axes, it is possible to construct the linear structural-parametric model of the actuator for the mechatronics systems [14][15][16][17][18][19][20][21][22][23]. ...
... x = and x δ = , we obtain the following set of the equations for determining stresses in the piezoactuator [15][16][17][18][19][20][21][22][23][24] International Journal of Physics 11 33 3 3 0 33 33 33 3 3 33 33 ...
... After algebraic transformations of the generalized structural-parametric model of the actuator we provided the transfer functions of the actuator in matrix form [14][15][16][17][18][19][20][21][22][23], where the transfer functions are the ratio of the Laplace transforms of the displacement of the face actuator and the corresponding parameter or force at zero initial conditions. ...
... The piezoactuator for the nanomechanics is provided the displacement from nanometers to tens of micrometers, a force to 1000N. The piezoactuator is used for research in the nanomedicine and the nanobiotechnology for the scanning tunneling microscopes, scanning force microscopes and atomic force microscopes [14][15][16][17][18][19][20][21][22][23][24][25][26][27][28][29][30][31][32]. ...
... In [8,27] was used the transfer functions of the piezoactuator for the decision problem absolute stability conditions for a system controlling the deformation of the electro magneto elastic actuator. The elastic compliances and the mechanical and adjusting characteristics of the piezoactuator were found in [18,[21][22][23]28,29] for calculation its transfer functions and the structural-parametric models. The structural-parametric model of the multilayer and compound piezoactuator was determined in [18][19][20]. ...
... The elastic compliances and the mechanical and adjusting characteristics of a piezoactuator were explored in Reference [17][18][19] in order to calculate its transfer functions and create the structural-parametric model. The structural-parametric model of a multilayer and compound piezoactuator was determined in References [17][18][19][20][21][22] with output displacement. ...
... The elastic compliances and the mechanical and adjusting characteristics of a piezoactuator were explored in Reference [17][18][19] in order to calculate its transfer functions and create the structural-parametric model. The structural-parametric model of a multilayer and compound piezoactuator was determined in References [17][18][19][20][21][22] with output displacement. In this paper, we solve the problem of building the generalized structural parametric model and the generalized parametric structural schematic diagram of an electromagnetoelastic actuator for the equation of electromagnetoelasticity in the general form. ...
The generalized parametric structural schematic diagram, the generalized structural-parametric model, and the generalized matrix transfer function of an electromagnetoelastic actuator with output parameters displacements are determined by solving the wave equation with the Laplace transform, using the equation of the electromagnetolasticity in the general form, the boundary conditions on the loaded working surfaces of the actuator, and the strains along the coordinate axes. The parametric structural schematic diagram and the transfer functions of the electromagnetoelastic actuator are obtained for the calculation of the control systems for the nanomechanics. The structural-parametric model of the piezoactuator for the transverse, longitudinal, and shift piezoelectric effects are constructed. The dynamic and static characteristics of the piezoactuator with output parameter displacement are obtained.
... Generalized structural-parametric model and generalized parametric structural schematic diagram of the electromagnetoelastic actuator after algebraic transformations provides the transfer functions of the electromagnetoelastic actuator for nano-and micromanipulators [9][10][11][12][13][14][15][16][17][18][19][20][21][22][23][24][25][26]. ...
... The nano piezoactuator works on the basis of the inverse piezoeffect due to its nano deformation at the electric field strength is applied. [16][17][18][19][20][21][22][23][24][25][26][27][28][29][30][31][32][33][34] On the characteristic of the nano piezoactuator deformation from the electric field strength, the initial curve is observed, on which the vertices of the main hysteresis loops lie. The main hysteresis loops have a symmetric change in the electric field strength relative to zero, and partial loops have an asymmetric change in the strength relative to zero. ...
For the nano piezoactuator with hysteresis in control system its set of equilibrium positions is the segment of line. By applying Yakubovich criterion for system with the nano piezoactuator the condition absolute stability of system is evaluated.
... The equations [27][28][29][30][31][32][33][34][35] of the piezoeffects have form The differential equation of a piezoactuator 12-52 is written ...
The structural scheme of a piezoactuator is obtained for astrophysics. The matrix equation is constructed for a piezoactuator. The characteristics of a piezoactuator are received for astrophysics.
... Piezo drives are used for atomic force microscopy, nanomanipulators, nanotechnology, biotechnology, astronomy, space research, metrology, laser resonator [16][17][18][19][20][21][22][23][24][25][26][27][28][29][30][31][32][33][34][35]. ...
The structural model of the drive for nanobiotechnology is obtained. The structural scheme of the drive is constructed. In nanobiotechnology for the control systems with the drive its deformations are determined.
... In structural schema of an engine its energy transformation is clearly [4][5][6][7][8][9][10][11][12][13][14]. The piezo engine is applied for precise adjustment in scanning microscopy and adaptive optics [11][12][13][14][15][16][17][18][19][20][21][22][23][24][25][26][27][28]. ...
In nanosciences research the structural model of an electro elastic engine is constructed. Its structural scheme of is received. For an engine its matrix equation of the deformations are obtained in the decisions of the precision control systems. The parameters of an engine are determined.
... The piezoactuator uses the inverse piezoeffect and serves for the actuation of mechanisms or the management and converts the electrical signals into the displacement and the force [1][2][3][4][5][6][7][8]. The piezoactuator is applied for the drives of the scanning tunneling microscopes, scanning force microscopes and atomic force microscopes [14][15][16][17][18][19][20][21][22][23][24][25][26][27][28][29][30][31][32]. ...
Background/Aim: With the availability of biosimilars, hospital formulary drug selection among biologics extends beyond clinical and safety considerations when comes to hospital resource management, to factors like human resource allocation and financial sustainability. However, research assessing the time and cost of labor, supplies, and waste disposal of biologics from the standpoint of hospitals remains limited. This study focuses on short-acting granulocyte-colony stimulating factor originators (Granocyte® and Neupogen®) and biosimilar (Nivestim®), comparing them based on mean total handling times per dose and total annual expenses. Materials and Methods: Ten nurses from a Taiwanese cancer center were recruited; they each prepared three doses of each drug. Results: Findings showed that the mean total handling times per dose of Granocyte® and Neupogen® were significantly higher than that of Nivestim®. Handling Nivestim® required the lowest total annual expense. Conclusion: Nivestim® is an advantageous alternative to Granocyte® and Neupogen®, benefiting hospital resource management.
The structural schemes of electroelastic engine micro and nano displacement are determined for applied bionics and biomechanics. The structural scheme of electroelastic engine is constructed by method mathematical physics. The displacement matrix of electroelastic engine micro and nano displacement is determined.
In the work is calculated of the piezoactuator for astrophysics. The structural scheme of the piezoactuator is determined for astrophysics. The matrix equation is constructed for the piezoactuator. The mechanical characteristic is determined. The parameters of the piezoactuator are obtained in nano control systems for astrophysics.
Decision wave equation, structural - parametric model and block diagram of electro magneto elastic actuators are obtained, its transfer functions are bult. Effects of geometric and physical parameters of electro magneto elastic actuators and external load on its dynamic characteristics are determined. For calculation of communications systems with piezoactuators the block diagram and the transfer functions of piezoactuators are obtained.
Structural-parametric models, parametric structural schematic diagrams and transfer functions of electromagnetoelastic actuators are determined. A generalized parametric structural schematic diagram of the electromagnetoelastic actuator is constructed. Effects of geometric and physical parameters of actuators and external load on its dynamic characteristics are determined. For calculations the mechatronic systems with piezoactuators for nano- and microdisplacement the parametric structural schematic diagrams and the transfer functions of piezoactuators are obtained.
The structural model of a nano drive is determined for biomedical research. The structural scheme of the piezo drive is obtained. The matrix equation is constructed for a nano drive.
Structural-parametric models, parametric structural schematic diagrams and transfer functions of electromagnetoelastic actuators are determined. A generalized parametric structural schematic diagram of the electromagnetoelastic actuator is constructed. Effects of geometric and physical parameters of actuators and external load on its dynamic characteristics are determined. For calculations the mechatronic systems with piezoactuators for nano-and microdisplacement the parametric structural schematic diagrams and the transfer functions of piezoactuators are obtained.
The structural model of the nano piezoengine is determined for applied biomechanics and biosciences. The structural scheme of the nano piezoengine is obtained. For calculation nano systems the structural model and scheme of the nano piezoengine are used, which reflect the conversion of electrical energy into mechanical energy of the control object. The matrix equation is constructed for the nano piezoengine in applied biomechanics and biosciences.
The mathematical models of a piezoengine are determined for nanomedicine and applied bionics. The structural scheme of a piezoengine is constructed. The matrix equation is obtained for a piezoengine.
The structural model of an engine for nanochemistry is obtained. The structural scheme of an engine is constructed. For the control systems in nanochemistry with an elecro elastic engine its characteristics are determined.
The transfer function and the transfer coefficient of a precision electromagnetoelastic engine for nanobiomedical research are obtained. The structural diagram of an electromagnetoelastic engine has a difference in the visibility of energy conversion from Cady and Mason electrical equivalent circuits of a piezo vibrator. The structural diagram of an electromagnetoelastic engine is founded. The structural diagram of the piezo engine for nanobiomedical research is written. The transfer functions of the piezo engine or are obtained.
Parametric block diagrams are constructed for the multilayer piezoelectric transducer in longitudinal piezoeffect with the counter-electromotive force taken into account. The transfer functions of the multilayer piezoelectric transducer are obtained with regard to the influence of geometric and physical parameters of the multilayer piezoelectric transducer, counter-electromotive force, and external load.