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Where: U Where: t = time to charge piezoto U

Piezo


Nano


Positioning

Dynamic Operation(Switched) Example: To determinewhether a selected amplifier can drive a given piezo actua- tor at 50 Hz with 30 µm peak-to-peak displacement, multiplythe actuator’s DOCC by 50 x 30 and compare the result with the average output current of the selected amplifier. If the current required is less than orequal to the amplifier output,then the amplifier has suffi- cient capacity for the applica- tion. For applications such as shockwave generation or valve con- trol, switched operation (on/ off) may be sufficient. Piezo actuators can provide motion with rapid rise and fall times with accelerations in the thou-sands of g’s. For informationon estimating the forces involved, see “DynamicForces,” p. 4-24).The simplest form of binarydrive electronics for piezo applications would consist of a large capacitor that is slowlycharged and rapidly dis-charged across the PZT ceram- ics.The following equation relatesapplied voltage (which corre- sponds to displacement) to time.(Equation 21)Voltage on the piezo afterswitching event. Dynamic Operating CurrentCoefficient (DOCC)

Piezo Actuators Piezo Actuators

Instead of calculating therequired drive power for a given application, it is easier to calculate the drive current, because it increases linearly with both frequency and volt- age (displacement). For this purpose, the DynamicOperating Current Coefficient(DOCC) has been introduced. The DOCC is the current that must be supplied by the ampli- fier to drive the piezo actuator per unit frequency (Hz) and unit displacement. DOCC val-ues are valid for sinewaveoperation in open-loop mode. In closed-loop operation the current requirement can be up to 50% higher.The peak and long-term aver-age current capacities of the different piezo amplifiers canbe found in the technical datatables for the electronics, the DOCC values in the tables for the piezo actuators.

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= start voltage [V]U

p-p

[s]C = piezo actuator capaci-tance [F]U

p-p

= source output voltage(peak-to-peak) [V]R = source output resist-ance [ohm]C = piezo actuator capaci-tance [F]t = time [s]

p-p

= voltage change(peak-to-peak) [V]i

max

= peak amplifiersource/sink current [A] For fastest settling, switched operation is not the best solu-tion because of the resultingovershoot. Modern techniques The voltage rises or falls expo-nentially with the RC time con- stant. Under quasi-static condi- tions, the expansion of the PZT ceramics is proportional to the voltage. In reality, dynamicpiezo processes cannot bedescribed by a simple equa- tion. If the drive voltage rises too quickly, resonance occurs, causing ringing and overshoot. Furthermore, whenever thepiezo actuator expands or con-tracts, dynamic forces act on the ceramic material. These forces generate a (positive or negative) voltage in the piezo element which is superim-posed on the drive voltage. A piezo actuator can reach itsnominal displacement in approximately 30 % of the peri- od of the resonant frequency, provided the controller can deliver the necessary current. (see p. 4-26). The following equation appliesfor constant-current charging (as with a linear amplifier):(Equation 22)Time to charge a piezoceramicwith constant current. With lower-capacity electronics,amplifier slew rate can be alimiting factor. like InputShaping

®

(see p. 4-33) solve the problem of reso- nances in and around the actu-ator with complex signal pro-cessing algorithms. Note Piezo drives are becomingmore and more popular because they can deliver extremely high accelerations. This property is very important in applications such as beam steering and optics stabiliza-tion. Often, however, the actua-tors can accelerate faster than the mechanics they drive can

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