Piezo
Ceramics Tutorial 12 of 15
Useful Relationships
Piezoelectric
Equations and Constants
To a good approximation, the interaction between the
electrical and mechanical behaviour of the piezoelectric
medium can be described by the following relationships:
S = sET + dE
D = dT + TE
E = -gT + ( T)-1D
S = sDT + gD
E =
field (Vm-1)
T = Stress (Nm-2)
S = Strain (dimensionless)
D = Dielectric displacement (Cm-2)
and
the superscripted permittivity and compliance s denotes the quantity
kept constant under boundary conditions (e.g T is the permittivity
under constant stress).
"d"
and "g" are piezoelectric constants, related by
the general expression:
d = r og
where:
r = relative permittivity
(or dielectric constant)
o = permittivity of free
space ( 8.85x10-12Fm-1)
The
piezoelectric constants are defined as follows:
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direct
effect |
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reverse
effect |
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| d= |
charge
density developed |
CN-1 |
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d
= |
strain
developed |
mV-1 |
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applied
mechanical stress |
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applied
field |
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| g= |
electric
field developed |
VmN-1 |
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g= |
strain
developed |
m2C-1 |
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applied
mechanical stress |
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applied
charge density |
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As well as the
above there are other parameters to be considered which
characterise a piezoelectric material; of prime importance
are the coupling coefficient, loss factor and the mechanical
quality factor.
The
Coupling Coefficient
This parameter determines the efficiency of energy
conversion in the component (but not the overall efficiency
of the ceramic as a transducer) and is defined as follows:
(i)
For an electrically stressed component
k2
= stored mechanical energy
total stored energy
(ii)
For a mechanically stressed component
k2
= stored electrical energy
total stored energy
The
derivation of k from critical frequencies is complex and
graphical solutions are generally used to facilitate
calculations of k from (fn - fm)/fm. (see IRE Standards on
Piezoelectric Crystals: Measurements of Piezoelectric
Ceramics, 1961.)
An
approximate solution which depends on the shape of the
piece, the mode of vibration as well as the material and is
useful in design is given by:

This expression is often used for thick (1Ot > d) discs
and is then called kD.
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Dielectric
Loss
The efficiency of a transducer depends on the mechanical and
dielectric loss as well as the coupling coefficient. The
dielectric loss is usually the most significant factor and
is the ratio of the effective series resistance to the
effective reactance, or as in the diagram to the right. It
is the tangent of the loss angle 
tan = series resistance
series reactance
Ceramics
with a low tan should be employed for transducers
which are to be run continuously at high power levels.
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Mechanical/
Quality Factor Qm
is defined as the ratio of the energy supplied per cycle to
the energy dissipated per cycle and can be calculated from:

where C is the low frequency (1 kHz) capacitance and Zm the
minimum impedance. QM can also be determined approximately
from the frequency response curve as right:
The
frequency difference fz - f, is the frequency bandwidth at
about 3dB where the amplitude is 1 /SQR(2) of its maximum
value.
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QM = fr
f2 - f1
(only where Q>3) |
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Direction
Dependence
Because poled piezoelectric ceramics are anisotropic and the
direction of polarising may be freely chosen, a method of
identifying the axes of a component is necessary in order to
specify its parameters.
The
direction of polarisation is conventionally taken as the 3
axis, with axes 1 and 2 perpendicular to this. The terms 4,
5 and 6 refer to shear stains associated with the 1, 2 and 3
directions.
This
axis notation is used when specifying mast of the
piezoelectric parameters discussed above.
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Permittivity: ij
i - direction of dielectric displacement.
j - direction of electric field.
E.g. 11T is the
permittivity for a material whose dielectric displacement
and field are in the 1 direction under conditions of
constant stress.
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Compliance:
sii
i - direction of strain.
j - direction of stress.
E.g. s55D
is the shear strain to shear stress ratio at constant
electric displacement, for shear about an axis perpendicular
to the poling direction.
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