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In
addition to the coupling coefficient, the total efficiency
of a transducer depends on the mechanical and dielectric
losses. The dielectric losses, tan
The mechanical losses can be determined from the mechanical quality or damping factor, QM, from Formula 21.
QM can also be determined approximately from the frequency response curve as follows:
The frequency difference f2 - f1 is the frequency bandwidth at about 3dB where the amplitude is 1/SQR(2) of its maximum value. Of
these losses, the dielectric losses are usually the most
significant. Therefore it is recommended that materials with
a low dissipation factor be used for high power
applications, particularly since these losses increase with
power. For high intensity transducers, the overall
electroacoustical efficiency
It should be noted that at high drive levels QE and QM are not constants. They are usually lower than the low drive level values. The
dielectric permittivity of the material. and therefore the
dielectric constant and capacitance, decreases as the
applied frequency (mechanical or electrical) exceeds each
resonant frequency of the particular ceramic part. For
static operation, well below the first resonance frequency,
the dielectric permittivity is For
dynamic operation well above all resonance frequencies of
the ceramic part, the material behaves as if it was clamped
(strain = 0), and the electric permittivity is
where k1, kZ and k3 represent the coupling factors for the particular resonance For a thin plate, k1 and k2 are k31 and k'31 (length and width, respectively), and k3 is kt (thickness) For a thin disc, k1 is kp (radial), k2 is Kt (thickness), and there is no third resonance. For a rod, k1 is k33 (length), k2 is k'p, and there is no third resonance. In addition to FA and fr (series and parallel resonance frequencies), there is a frequency, fm at which the transducer's electromechanical transduction is maximized This frequency represents the maximum sensitivity for receivers or the maximum output for drivers This frequency, the bandwidth, and the output are all dependent on the external resistive load, ReX . When k<<1, fm may be calculated using Formula 26.
The maximum bandwidth, B, obtainable by electrical tuning, is approximately equal to the product of the coupling coefficient and the series or parallel resonance frequency. Refer to Formula 27.
If the mechanical quality factor is high (QM>Q), the external Formula 37 resistance Rex for a fairly flat frequency response can be approximated by Formula 28 for parallel inductance, or Formula 29 for series inductance.
Many of the calculated parameters above are interrelated Thus, many useful relationships can be derived A few of the most useful relationships are described in Formulas 30 through 37.
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