Piezo
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Positioning
Note: In positioning applications,
piezo actuators are operated
well below their resonant fre-
quencies. Due to the non-ideal
spring behavior of piezoceram-ics, the theoretical result fromthe above equation does not
necessarily match the real-
world behavior of the piezo
actuator system under large
signal conditions. When
adding a mass M to the actua-
tor, the resonant frequencydrops according to the follow-ing equation:(Equation 11)Resonant frequency withadded mass.m´ Where: Resonant Frequency In general, the resonant fre-quency of any spring/mass sys-
tem is a function of its stiffness
and effective mass (see Fig.
23). Unless otherwise stated,
the resonant frequency given
in the technical data tables for
actuators always refer to theunloaded actuator with oneend rigidly attached. For piezo
positioning systems, the data
refers to the unloaded system
firmly attached to a significant-
ly larger mass.(Equation 10)Resonant frequency of an idealspring/mass system.
Piezo Actuators Piezo Actuators Nanopositioning &
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Where:f
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Solutions >
= phase angle [deg]F
Industrial motion controllers Motion Controllers >
max = resonant frequency [Hz]f = operating frequency[Hz]
Ceramic
Linear motors & Stages Ceramic Linear Motors & Stages Index Index >
eff = additional mass M + m
O = resonant frequency ofunloaded actuator [Hz]k
eff .The above equations show thatto double the resonant fre-
quency of a spring-mass sys-
tem, it is necessary to either
increase the stiffness by a fac-tor of 4 or decrease the effec-tive mass to 25 % of its original
value. As long as the resonant
frequency of a preload spring
is well above that of the actua-tor, forces it introduces do not
significantly affect the actua-
tor’s resonant frequency.The phase response of a piezoactuator system can be approx-
imated by a second order sys-tem and is described by the fol-lowing equation:(Equation 12)
T = piezo actuator stiffness[N/m]m
eff = effective mass (about1/3 of the mass of the
ceramic stack plus any
installed end pieces)
[kg]
Fig. 23. Effective mass of an actuator fixed at one end. 4-25