Actuator &
Sensory Devices
                               based on HBLS
                               Smart Materials
Bishakh Bhattacharya
Department of Mechanical Engineering
Indian Institute of Technology, Kanpur
                      What is a Transducer?
Fundamental mechanism for both sensing and actuation is energy
transduction – conversion of signal/energy. Primary forms are grouped into two
categories:
Multicomponent transduction, utilizes “action at a distance” behavior
between multiple bodies.
eg:
Electromagnetic transduction, typically based upon the Lorentz equation and
Faraday’s law, and electrostatic interaction, typically based upon Coulomb’s
law.
Deformation-based / Solid-state transduction, mechanics-of-material
phenomena: crystalline phase changes or molecular dipole alignment.
Piezoelectric effects, shape memory alloys, and magnetostrictive,
electrostrictive materials.
Micro-scale systems currently dominated by electrostatic and electromagnetic
interactions.
Relative position of Actuators and Sensors
in an Intelligent System
Two Important Components: Energy Controller
and Energy Converter
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 The first Piezoelectric Device!
• In a modern quartz
  watch, the crystal
  resonator is
  shaped as a small
  tuning fork that
  vibrates at the
  frequency of
  32,768 Hz!
Follow up: two very common smart actuators
• Thin Disk Buzzer
• Amplified Piezo
  Actuator
       Smarter Actuators for
          Automobiles
• Current trend in Automotive Electronics is to
  use actuators for functions which require
  faster, more powerful and highly precise
  motion.
• Initiated application of Piezoelectric
  Actuators and Rheological Fluids for the
  control of Fuel Injection and Vibration
  control.
• Simple Unimorph/Bimorph/Discs are not
  popular in the industrial scale due to lack of
  efficiency, displacement and safety.
                            Piezo Diesel Injectors were developed to
                            reduce emissions by making the
                            combustion of fuel within the cylinder
                            more efficient (specially for Diesel
                            Engines)
As a Piezo injector performs faster, it can carry out
more injections per cylinder stroke and allows for higher
fuel system pressures. This improves the atomisation of
the diesel, giving improved spray momentum and
greater accuracy. Furthermore, the technology allows
for greater flexibility with regard to the start of injection
and the relevant time interval between individual
injection events. In addition, the new piezo injectors
developed are found to be smaller in size and lower in
weight compared to the traditional injectors
improved combustion control, less fuel consumption,
reduced noise, improved engine performance, and a
considerable reduction in emissions.
 Cut-out of a Piezoelectric Fuel Injector from EPCOS
 (TDK) [Ref. Sealand-Turbo-Diesel Asia]
Comparison of Different Actuation Speeds
   Type             Device       Accuracy   Response
   Pneumatic        Motor        Degrees    10 secs
   Hydraulic        Motor        Degrees    1 sec
   Electro-magnet   Stepper      10 µm      0.1 sec
   Piezoelectric    Actuator     0.01µm     0.0001 sec
   Magnetostrictive Actuator     0.01µm     0.001 sec
   Piezoelectric    Ultrasonic   minutes    0.001 sec
            Issues with PZT
• A relatively high electric field is necessary
  to develop an equivalent system with
  associated high voltage requirement to
  generate appreciable or useful strain.
• Example: PZT block of height 1mm, apply
  1KV field, d33 = 600 m/pV, strain 6x10-4
  and corresponding displacement is the
  same magnitude in mm.
     How can we Maximize the
         Displacement?
Consider a multilayered piezoelectric stack of
length l and number of layers n, which is subjected
to a voltage V.
Neglecting elastic deformation, total displacement
available from a ‘n’ layered stack will be:
Δ = ( l x d X V/(l/n)) = d x V x n
Total displacement is directly proportional to the
number of layers n!
        Multilayer Actuators
• Typical layer thickness is about 50µm
• Typical strain available 0.1%
• Hence, for a 100 mm stack actuator with
  2000 piezo-eletcric layers and an applied
  voltage of about 100V, the displacement
  will be: 10 x 10-9 x 100 x 2000 = 200 µm
• Blocking force = 100 kgf
• Lifetime = 1011 cycles
Major Applications of Multilayers
• Precision Positioners (order of 0.1 !")
• Miniature Ultrasonic Motors (USMs)
 (< 1cm)
• Adaptive Mechanical Dampers
     Advantages of Multilayered
       Piezoelectric Actuators
•   Requires less voltage
•   Produces larger deformation/displacement
•   Safer to use
•   High Life Cycle
•   Lighter and More Compact
•   Concurrent engineering – advantages
    from the development of multi-layered
    capacitors
A Typical Multilayer Configuration
Mechanically Series Connection
Mechanically Parallel
   Connection
Series Modelling of the
  Electrical System
Parallel Connection of the
    Electrical System
            Governing Criteria
• The PZT actuators showing higher mechanical
  compliance should be modelled as a series assembly of
  springs;
• those with higher stiffness can be modelled with a
  parallel assembly of springs.
• In the electrical domain, PZ actuators having faster
  response time should be modelled with a series
  assembly of the capacitors;
• those showing higher robustness to electrical
  disturbances can be modelled with a parallel circuit
Comparison of Mechanical and
     Electrical Models
    Other important properties
• The resonating frequency of a fixed-free
  multilayer actuator is given by:
            1                               #
   fn =
                  and  response  time !" = $ %
                                              &
        2 l r S33
               D
• Where, ρ is the density and S33 denotes
  the compliance modulus
• For example, one 1 cm sample will have
  resonating frequency about 100 kHz and
  response time in milli seconds.
How multi-layers are developed?
• Two common techniques – Cut and Bond
  and Tape-Casting
• In cut and bond technique PZT wafers are
  cut (typical thickness 0.2mm) and bond with
  intermittent metal foils. Major draw back is
  that this is a labor intensive process.
• In tape-casting method, ceramic green
  sheets are printed with electrodes and
  cofired. There are various ways of
  electrically connecting such layers.
Reference:
J. Pritchard, C. R. Bowen,
and F. Lowrie, 2000
Various electrode configurations
Inter-digital   Plate Through
Configuration   Configuration
    Some more configurations
Inter-digital             Electrode with
configuration with slit   Gap
     Design Issues: Electrode
          Configuration
• Inter-digital Configuration is the most
  common and best suitable for mass
  production. However, due to non-uniform
  electric field present towards the edges –
  stress concentration can occur which may
  lead to failure.
• All other configurations are developed to
  make the electric field more uniform and
  hence reduce the stress concentration.
Acoustic Emission Test
  Design Issues: Inactive Area
• Limited Strain is developed at the edge of
  the inter-digitated pattern
                              d 31bulk
               d 31eff   =
                                 S e te
                           [1 +         ]
                                  St
• Where, d31eff is the effective coupling
  constant, S and t are the compliance
  modulus and thickness of piezo while the
  ones with e-subscript denote that of
  electrode.
  Design Issues: Delamination
• Delamination can occur between the
  electrodes and the piezo layers due to
  binder burn-out, inadequate adhesion
  between the electrode and the ceramics
  and thermal expansion mismatch during
  sintering.
• Solution:
  – Control of Organic Binder
  – Decreasing the Metal Powder Surface Area
      Design Issues: Effect of
           Composition
• Increase in Grain size increases
  piezoelectric effect but reduces the
  fracture toughness, also increases
  hysteresis and dielectric loss
• For electrodes – Ag-Pd alloy or Copper-
  Nickel Alloy are better as they have less
  thermal mismatch.
Design Issues: Heat Generation
• Heat Generation during operation of such
  actuator could be expressed as:
                   U f vactuator
              DT =
                    k (T ) A
• ΔT – change in temperature, U dielectric
  loss per driving cycle per volume fraction, f
  – driving frequency, v – actuator volume,
  k- conduction coefficient and A – CS area
Further Amplification of Force?
Cymbals
Range of Derivatives of APA
A Comparison of Piezo Actuators
 Device    Driving   Displaceme   Force   Cost
           Voltage   nt (µm)      (N)
           (V)
 MLA       100       10           900     High
 Bimorph   100       35           1       Low
 Rainbow   450       20           3       Medium
 Cymbal    100       40           15      Low
 Moonie    100       20           3       Medium
Types of Wafer based PZT Devices
                    A Comparison
Actual Market Demand: 100 μm displacement, 100 N force, and
100 μs response.
For multilayer: About 100 thin piezoelectric ceramic sheets are
stacked together, has the advantages of low driving voltage (100
V), quick response (10 μs), high generative force (1 kN), and high
electromechanical coupling.
However, the displacement, on the order of 10 μm, is not
sufficient for some applications.
For Benders: large bending displacement of several hundred μm is
possible, but it has relatively low response time (1 ms) and
generative force (1 N)
  Even more for Electrostrictors
Consider a multilayered electrostrictive stack of
length l and number of layers n, which is subjected
to a voltage V.
Neglecting elastic deformation, total displacement
available from a ‘n’ layered electrostrictor will be:
Δ = [ l x d X (V /(l/n))2 ] = (d/l )x V2 x n2
Total displacement is directly proportional to the
number of layers n2 !
      Types of USM Devices based on Drives
• Rigid Displacement Devices
 - the strain is induced unidirectionally along the direction of the applied
DC field
•   Resonating Displacement Devices
-   the alternating strain is excited by an AC field at the mechanical
    resonance frequency (USMs).
The Rigid Displacement device can be further divided into two types:
servo displacement transducers (positioners), controlled by a feedback
system through a position-detection signal, and pulse drive motors
operated in a simple on/off switching mode, exemplified by inkjet
printers.
                Material Requirements
• The material requirements for these classes of devices
  are somewhat different, and certain compounds will be
  better suited to particular applications.
• The USM, for instance, requires a very hard piezoelectric
  with a high mechanical quality factor QM, to suppress
  heat generation.
• The servo displacement transducer suffers most from
  strain hysteresis and, therefore, a PMN electrostrictor is
  used for this purpose.
• The pulse drive motor requires a low permittivity material
  aimed at quick response with a certain power supply (a
  high-power supply is expensive from the practical device
  application viewpoint!) rather than a small hysteresis,
  hence, soft PZT piezoelectrics are preferred.
    Better Piezoelectric Material
                             Lead Magnesium Niobate / Lead
                             Titanate (PMN-PT)
     A Piezo and an Electrostrictor [Uchino, 2003]
Perovskite Lead Lanthanum Zirconate Titanate (PLZT) ceramic
is actually Lanthanum doped PZT and typically known as
PLZT (100x/100y/100(1-y)).
Special reference for this lecture
• Micro-mechatronics by Uchino &
  Giniewicz, Marcel, Dekker
• Kato, Fine Ceramics Technology
• Pritchard, Bowen, Lowrie; Multilayer
  Actuators: A Review, British Ceramic
  Transactions, 2001
Acknowledgement: Mr. G. Tripathi of the SMSS Lab for the experiment