Friday, 17 June 2016

Dr Kesorn Pechrach Weaver: Piezoelectrics in Circuit Breakers: Piezoelectric Instrumentation

Dr Kesorn Pechrach Weaver: Piezoelectrics in Circuit Breakers: Piezoelectric Instrumentation: Piezoelectric Instrumentation The Piezo-ceramic used as the actuator in this paper is Lead Zirconate Titanate (PZT). The...

Piezoelectric Instrumentation




Piezoelectric Instrumentation





The Piezo-ceramic used as the actuator in this paper is Lead Zirconate Titanate (PZT). The actuator is designed in a U-shape, as shown in Figure 4.13. The material is constructed in a sandwich fashion with layers of PZT material. This structure and the assembly in the U-shape arrangement provide maximum forward deflection of 4 mm and maximum reverse deflection 1.5 mm.

The full specification of the material used is provided in Table 4.1.
Electrical performance

Nominal voltage
325 Vdc
Max. forward voltage
500Vdc
Max. reverse voltage
75 Vdc
Physical performance

Nominal deflection per volt
10-6 m.
Max. forward deflection
4 mm.
Max. reverse deflection
1.5 mm.
Time to deflect (min)
1.25 ms
Blocking force
0.2 N
Beam release force (max)
2.5 N
Physical data

Ceramic
Lead, Titanium, trace
Substrate
Alloy 42 (Ni,Fe,Si,Mn)

Table 4.1 Characteristics of piezoelectric


A Laser Triangulation Sensor was used to measure the deflection of the piezoelectric. The sensor has a 0.01µm resolution. The power supply for piezoelectric was used dual step up transformers transform from 230Vac to 360 Vdc via variable resistor. More than 200 data and 12 sets were recorded to study the relationship between supply voltage and deflection of the piezoelectric

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Piezoelectrics in Circuit Breakers 

Friday, 27 May 2016

Dr Kesorn Pechrach Weaver: Piezoelectrics in Circuit Breakers: Displacement in Piezoelectric

Dr Kesorn Pechrach Weaver: Piezoelectrics in Circuit Breakers: Displacement in Piezoelectric:   Displacement The deflection of a beam shaped monomorphic bending actuator, the d31 effect, which shortens the lateral dimens...

Displacement in Piezoelectric



 


Displacement

The deflection of a beam shaped monomorphic bending actuator, the d31 effect, which shortens the lateral dimension of the active layer if an electric field is applied in the d33 direction of the polarization.  As the active layer is bonded to a passive layer, this causes bending of the device. More efficient designs, known as bimorph, trimorph and multimorph bending actuators, can create bidirectional deflection. By making use of two or more layered piezoelectric structures, similar to piezoelectric multilayer stack actuators, the operating voltage of the multimorph benders is significantly reduced by the small electrode distance [52].
The movement across the temperature range with the reverse charge system is more than 3 times that for a unipolar drive [31]. Re-poling of the ceramic is successfully avoided. This is all accomplished without the use of a temperature sensor or intermediate temperature values. [32]
In recent years there have been some significant advances in extending the concepts of differential flatness and passivity based control to the infinite-dimension. For applications with large displacements, range of input voltage is available. However, at high electric field strengths, piezoelectric material shows significant hysteretic.
Piezoelectric Trimorph-bending actuators consist of a substrate of metal or carbon fibre and two metalised piezoceramic films [59]. They found that the small structural damping the step-response of the uncontrolled bending actuator has a large overshoot and a large settling time.


Reference:


Piezoelectrics in Circuit Breakers: Design & Test

by Dr Kesorn Pechrach Weaver PhD (Author)



Friday, 20 May 2016

Dr Kesorn Pechrach Weaver: Piezoelectrics in Circuit Breakers: Hysteresis and Non-Linearity

Dr Kesorn Pechrach Weaver: Piezoelectrics in Circuit Breakers: Hysteresis and Non-Linearity: Hysteresis and Non-Linearity Hysteresis is a nonlinear phenomenon that can be found in diverse disciplines such as smart material...

Hysteresis and Non-Linearity





Hysteresis and Non-Linearity

Hysteresis is a nonlinear phenomenon that can be found in diverse disciplines such as smart materials [54], ferromagnetism and superconductivity [55]. The hysteresis refers to a static memory effect rate independent hysteresis is characterized by (output vs. input) hysteresis loops [56]. Practical hysteresis loops often demonstrate rate dependent behaviour due to intimate coupling between hysteresis and traditional dynamics [53].
One of the major obstacles in the application of smart actuators is their hysteretic behaviour and some degree of hysteresis. It has been observed by [53], the hysteresis modelling and compensation methods used for smart actuator devices and compensation is required to provide precision positioning systems.
A typical loop response for a piezoceramic actuator driven by a voltage source is shown in [25]. It was shown the position is multivalued with respect to the input voltage and also it is the response is non-linear.
It is a significant difference between the charging and discharging parts. The repeatability of the loop is good to within a few percent. This fact can be used to achieve highly repeatable open loop operation where the actuation is synchronised to operate on one part of the loop.
The major obstacles in the application of smart actuators are their hysteretic behaviour. If the hysteresis effect is not incorporated into the control system it will act as an unmodelled phase lag whose presence will cause instability in a closed-loop system if sufficient phase margin is not provided in the control design. Integration of actuators with these dynamics into mechatronic systems requires some degree of hysteresis compensation, and also in some cases creep compensation, to provide precision positioning [54].
The degree and severity of hysteresis effects in smart actuators can often be reduced by constraining input levels, or incorporating local control feedback. To improve the control of the hysteresis and the linearity can do by controlling the polarisation (charge) rather than the voltage [26]. The system controls the charge on the actuator to achieve highly linear open loop control.
An alternative strategy for controlling hysteresis is to apply a decaying oscillation to a target DC voltage level. The displacement of the actuator converges to a point removing hysteresis from the system. The hysteresis loop converges to the anhysteric line when applied over a range of dc voltages. The non-linearity can be removed by software compensation [25]. In present scanning tunnelling microscopic (STM) designs, PID or robust control laws are used to reduce hysteresis effects [57, 58].
Reference: