PIEZOELECTRIC TRANSFORMER

Abstract: Piezoelectric transformer comprising a piezoelectric body which is divided into a primary portion (2) and a secondary portion (3), whereby both the primary portion and the secondary portions are able to generate and transform piezoelectric vibrations in accordance with an AC-voltage fed to one portion while a transformed voltage is delivered from the other portion. The piezoelectric body is formed by a substantially oval or annular body which has been polarised substantially perpendicular to the peripheral direction. Therefore the annular transformer can operate at an increased frequency because it employs the thickness vibration instead of the peripheral vibration. As a result an increased field intensity is allowed because the field intensity is substantially proportional to the frequency.

Description: Title: Piezoelectric transformer- Technical Field. The invention relates to a piezoelectric transformer comprising a piezoelectric body which is divided into a primary portion and a secondary portion, whereby both the primary portion and the secondary portion are able to generate and transform piezoelectric vibrations in accordance with an AC-voltage fed to one portion while a transformed voltage can be delivered from the other portion. Background Art A known piezoelectric transformer of this type comprises a piezoelectric body in form of an oblong plate having a mechanical resonance frequency. The transformer is preferably operated at this resonance frequency. However, this transformer is encumbered with the draw-back that further resonance frequencies may have an effect on the mode of operation of the transformer. Furthermore, US-PS No. 3,736,446 discloses an annular transformer. Thepiezoelec- trie material is layered by means of through electrodes along a portion of the periphery of this transformer, said portion utilizing oscillations in the peripheral direction. As an alternative, a ring can be painted on the ceramics. This structure is encumbered with the draw-back that it is relatively expensive to manufacture. In addition, the resonance frequency is relatively low for oscillation types along the periphery. The transformable effect is proportional to the frequency. The effect transformable by means of this annular transformer is therefore relatively insignificant. Brief Description of the Invention The object of the invention is therefore to provide a piezoelectric transformer pre- senting a higher field intensity than hitherto known and which does not involve undesired resonance frequencies. A piezoelectric transformer of the above type is according to the invention characterised in that the piezoelectric body is formed by a substantially oval or annular body which has been polarised substantially perpendicular to the peripheral direction. An annular piezoelectric body presents three basic modes of vibration, viz. the periphery presenting the lowest frequency and a planar and a thickness vibration presenting a comparatively higher frequency due to the reduced extent of the vital dimension. Therefore the annular transformer is according to the invention able to operate at a comparatively higher frequency as it operates on a thickness vibration instead of a peripheral vibration. Moreover, the geometry provides an increased capacity, which together with the increased operation frequency results in a reduced output impedance. Thus the transformer is able to handle increased currents, typically in the range of 0.1 to 5 A. The power in the transformer is transferred as a mechanical vibration. The maximum allowed, transferred power depends on the fatigue strength of the ceramics. For a predetermined maximum mechamcal strain in the ceramics the transferred power is P = f^-e-vol-k eff 2 where P = transferred power f res = resonance frequency vol = volume k eff = efficient piezoelectric coupling coefficient corresponding to the existing mode of vibration e = dielectric permittivity When two annular transformers are made of the same ceramics and with the same volume, the maximum allowable strain and e vol is constant. As previously mentioned, the resonance frequencies are higher for the thickness vibration than for the peripheral vibration, and as far as conventional piezoelectric ceramics of the power type is concerned, the associated coupling coefficients are 0.3 to 0.35 (k 31 , peripheral vibration) and 0.40 to 0.45 (k τ , thickness vibration), respectively. The difference in coupling coefficient results in an increased power density of (0.45/0.35) 2 = 1.65 and the resonance frequency is typically a factor 10 higher. Totally, the power den- sity is increased by 1.65*10 = 16.5. Brief Description of the Drawing The invention is explained in greater detail below with reference to the accompanying drawings, in which Fig. 1 illustrates a piezoelectric transformer with an annular piezoelectric body on each side of an insulating plate, Fig. 2 is a sectional view through the transformer of Fig. 1 and illustrating the vibrations, Fig. 3 is a sectional view through the transformer of Fig. 1 and illustrating the electrode configurations, Fig. 4 is a sectional view corresponding to the sectional view of Fig. 3, where one primary electrode has been moved away from the insulating layer so as to reduce the mechanical stresses due to the polarisation, Fig. 5 is a sectional view corresponding to the sectional view of Fig. 3, but showing an alternative positioning of the primary electrodes, Fig. 6 is a sectional view corresponding to the sectional view of Fig. 5, where the inner electrode has been withdrawn so as to reduce the polarisation stresses, Fig. 7 illustrates an alternative embodiment of a piezoelectric transformer, where the annular piezoelectric body has been slotted, Fig. 8 illustrates an alternative embodiment of a piezoelectric transformer, where the annular piezoelectric body has been wound up like a coil, Fig. 9 illustrates an alternative embodiment of a piezoelectric transformer, where the annular piezoelectric body presents a wavy closed shape, and Fig. 10 illustrates an alternative embodiment of a piezoelectric transformer, where the primary portion is quadrangular and presents a circular opening. Best Mode for Carrying Out the Invention The piezoelectric transformer illustrated in Fig. 1 comprises an annular piezoelectric body on each side of an insulating plate 1. One piezoelectric body 2 serves as primary portion whereas the other piezoelectric body 3 serves as secondary portion. Electrodes are provided both at the primary portion 2 and at the secondary portion 3, and both said primary portion and said secondary portion are able to generate and transform piezoelectric vibrations in response to an AC-voltage fed from one portion while the transformed voltage can be delivered from the other portion. According to the invention each piezoelectric body is formed by a substantially oval or annular body. As a result, an improved uniform distribution of the stresses, an increased coupling coefficient as well as improved cooling conditions are obtained. A vital factor for maxiiriizing the efficient coupling is that b/h is either less than 0.25 or 0.35 < b/h < 0.8 or especially 0.4 < b/h < 0.7, where b represents the width and h represents the height. Fig. 2 illustrates that the transformer operates as a semiwave resonator. Fig. 3 illustrates an example of an electrode structure at both the primary portion and at the secondary portion. A circumferential electrode is provided on the primary portion both at the top side 4 and at the bottom side 5. The secondary portion is formed as a multilayer structure with inner electrodes 69, 66. These inner electrodes 69, 66 are alternately connected to one output terminal 7 and the other output terminal 8. In Fig. 4, one primary electrode 5' has been moved away from the insulating layer 1 so as to reduce the mechamcal stresses during the polarisation. Unlike the insulat- ing layer 1 , the ceramics is subjected to dimensional changes during the polarisation. Fig. 5 illustrates an alternative positioning of the primary electrodes on the inner side and the outer side, respectively, of the annular body 2. The secondary electrodes 6a, 6b are positioned in the same position as in Figs. 3 and 4. Fig. 6 illustrates an alternative positioning of the primary electrodes, where the inner electrode has been withdrawn so as to reduce the polarisation stresses. Figs. 7, 8 and 9 illustrate alternative embodiments of the piezoelectric body, which for instance is split up and wound up like a coil, cf. Fig. 8. The piezoelectric material is preferably a PZT ceramics. PZT is preferred because The transformer can for instance be used for transforming 120 VAC into 12 VAC. The piezoelectric transformer presents a relatively high energy density, viz. up to 0.04 W/cm 3 kHz corresponding to a field intensity of 20 W/cm 3 at 500 kHz. Thus the component is suited for miniaturising. Other things being equal, the latter results in a comparatively smaller component, which in turn involves a reduced cost price. The increased operating frequency has also the effect that filter components (coils, capacitors) of the associated structure can present lower values and consequently a reduced physical size as well as a reduced price. The insulation between the primary and the secondary portions depends no longer on the leakage path along the surface of the transformer, but on the breakdown voltage in the insulating layer. Therefore the reduced dimensions present no hindrance to meet the same or higher requirements to the insulation. The operating frequency is typically 500 kHz. The piezoelectric material can be Navy type 1. The external diameter is 10 mm, whereas the internal diameter is 7 mm. Each part is of a length of 1.8 mm, and the two parts are separated by a round aluminium disk of a thickness of 0.25 mm. The total length of the transformer is 3.85 mm. Nothing but transformers have been discussed until now where one part is a multi- layer component while the other part is a bulk component. It is, however, also possible that both components are either bulk or multilayer components in response to the desired voltage ratio and the impedance conditions to which the transformer is to be adapted. The bulk components are less expensive and it is possible to obtain a voltage ratio of up to 1:3 by employing materials presenting a varying permittivity on the primary and the secondary portions. Furthermore it is possible to use an either triangular or quadrangular blank with a round opening instead of the cylindrical blank, cf. Fig. 10. The opening is asymmetrically positioned so as to further attenuate undesired resonances. Quadrangles can be cut out in a cost-saving manner, and it is easy to drill round openings.

Claims: Claims 1. Piezoelectric transformer comprising a substantially piezoelectric body which is divided into a primary portion and a secondary portion, whereby both the primary portion and the secondary portion are able to generate and transform piezoelectric vibrations in accordance with an AC-voltage fed to one portion while a transformed voltage can be delivered from the other portion, characterised in that the piezoelectric body is formed by a substantially oval or annular body, which has been polarised substantially perpendicular to the peripheral direction. 2. Piezoelectric transformer as claimed in claim 1, characterised in that the primary portion of the piezoelectric transformer has been polarised in the longitudinal direction. 3. Piezoelectric transformer as claimed in claim 1, characterised in that the primary portion of the annular piezoelectric body has been substantially radially polarised. 4. Piezoelectric transformer as claimed in claim 1, characterised in that the piezoelectric body substantially describes a coil. 5. Piezoelectric transformer as claimed in claim 1 or 2, characterised in that the transformer is operated at a resonance frequency, preferably a thickness resonance frequency. 6. Piezoelectric transformer as claimed in claims lto3, characterised in that the secondary portion is provided with a plurality of inner electrodes 6a, 6b). 7. Piezoelectric transformer as claimed in claim 1, characterised in that the piezoelectric body is formed by a polygonal body, preferably a quadrangular body provided with an opening, preferably a circular opening. 8. Piezoelectric transformer as claimed in claim 7, characterised in that the opening is asymmetrically positioned.

Inventors: BREBOEL KLAUS, BREBOEL, KLAUS
Applicants: BREBOEL KLAUS, LIMIEL V KLAUS BREBOEL, BREBOEL, KLAUS, LIMIEL V/KLAUS BREBOEL
Application year: 1999
Main classification: H01L41
IPC codes: H01L41, H02N2