Cristin-resultat-ID: 1951292
Sist endret: 30. november 2021, 12:28
NVI-rapporteringsår: 2021
Resultat
Vitenskapelig artikkel
2021

Electrical power factor for a single crystal tonpilz versus a plate with matching layers

Bidragsytere:
  • Ellen Katrine Sagaas Røed
  • Martin Bring
  • Frank Tichy
  • Else-Marie Åsjord og
  • Lars Hoff

Tidsskrift

Proceedings - IEEE Ultrasonics Symposium
ISSN 1948-5719
e-ISSN 1948-5727
NVI-nivå 1

Om resultatet

Vitenskapelig artikkel
Publiseringsår: 2021
Publisert online: 2021
Trykket: 2021
Open Access

Beskrivelse Beskrivelse

Tittel

Electrical power factor for a single crystal tonpilz versus a plate with matching layers

Sammendrag

For underwater transducers mounted on small platforms, reactive electrical power can constitute a main restriction on the usable frequency range. The frequency range in which the amount of reactive power is acceptable can be increased by increasing the electromechanical coupling coefficient of the active material. However, to avoid large electrical power factor ripple, the transducer design must also have a low mechanical quality factor, Qm . A ferroelectric single crystal can have electromechanical coupling coefficient k=0.9 . The optimum Qm is then as low as 0.6, which is challenging to achieve. We investigated this challenge for a tonpilz design, by calculating Qm for different combinations of head masses and tonpilz stiffnesses, and by calculating the stiffness to density ratio required in the head material to avoid flexural resonances. The effective coupling coefficient of a real transducer is reduced compared to the material coupling coefficient, and in many applications some power factor ripple can be accepted. Both factors relax the Qm requirement. We calculated the power factor of a tonpilz design with k=0.82 and Qm=1.9 , and showed that the power factor ripple is smaller than 0.2 in a frequency band that is 150 % wide relative to the resonance frequency. The frequency independent matching inherent in the tonpilz gives this design an advantage regarding power factor ripple, and this can weigh up for a large Qm . We showed this by comparing the tonpilz to an air-backed composite plate. Like the tonpilz, the composite plate had k=0.82 , but it was matched to water by two conventional acoustic matching layers. Compared to the tonpilz, the composite design had a larger distance between the −3dB points of the acoustic power. Beyond these points, the acoustic power was however falling off more rapidly, resulting in an electrical power factor ripple of nearly 0.5.

Bidragsytere

Ellen Katrine Sagaas Røed

  • Tilknyttet:
    Forfatter
    ved Kongsberg Maritime AS
  • Tilknyttet:
    Forfatter
    ved Institutt for mikrosystemer ved Universitetet i Sørøst-Norge

Martin Bring

  • Tilknyttet:
    Forfatter
    ved Kongsberg Maritime AS

Frank Tichy

  • Tilknyttet:
    Forfatter
    ved Kongsberg Maritime AS

Else-Marie Åsjord

  • Tilknyttet:
    Forfatter
    ved Kongsberg Maritime AS

Lars Hoff

  • Tilknyttet:
    Forfatter
    ved Institutt for mikrosystemer ved Universitetet i Sørøst-Norge
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