Piezo Stack Amplifier, Single Channel, 300 mA

The dynamic properties of a closed-loop piezo system depends on many factors, most important, the payload and the spring constant of any material the piezo system is pushing against. A servo loop maintains accurate position control, and the settings of the control loop filters have a significant impact on the dynamic performance and stability of the system. Unfortunately, high dynamics and high position stability conflict with each other, particularly when a large load needs to be moved. In general, Newport electronics are optimized for the highest achievable positioning accuracy under static conditions and over a wide load range. Upon request, an optimization of the control loop parameters that is based on the mass, inertia, rigidity of the payload, and an applied external force, can be made according to application's operating bandwidth and stability requirements. The table below summarizes the closed-loop step response times for all Newport NanoPositioning products with strain gauge feedback and standard controller settings. This step response time is adjusted as part of the factory acceptance test. The closed-loop step response time is defined as the maximum time required for any displacement (up to a step equal to the nominal closed-loop range) with a stability of ± 1%, a maximum position overshoot of 10% and damping that ensures better than ± 0.1% stability, measure after 10X the step response time. The step response time is adjusted with the listed test load. For the NanoFocusing Objective stage NPO100SG, for example, a 100 µm step displacement with ± 100 nm stability and a 135 g objective lens can be reached within 80 ms. As mentioned above, considerably different performance may be possible with custom controller settings.

In open-loop, a piezoelectric actuator can reach its nominal displacement in approx. one third of the period of its first resonant frequency. The resonant frequencies for all our devices are provided for different loads, see specifications on the individual product pages. For loads in between, a linear relationship between the load and the resonant frequency can be assumed. Example: With 105 g load, the resonant frequency of the NanoPositioning linear stage NPXYZ100 in z-direction is 250 Hz. It can reach its nominal displacement within 1.3 ms. When the stage is excited with a sharp electrical pulse, the stages resonant frequency will be excited resulting in position overshoots with a damped oscillation. Hence, shorter electrical pulses may result in higher super-elevation, but not in shorter rise times.

Another boundary for fast open-loop operation is the current that can be provided by the piezoelectric amplifier. The diagram displays the max. sinusoidal frequency which can be supplied by the NPC3 and NPC3SG amplifiers as a function of the capacitance of the piezoelectric transducer and the voltage amplitude. For other models please see user manual for drive frequency curves.