METHOD AND APPARATUS FOR MEASURING ACCELERATION OR MECHANICAL FORCES

Abstract: A method for measuring acceleration or mechanical forces, the acceleration causing inertial forces, uses a transducer or accelerometer in which at least one piezoelectric element is influenced by a shearing force substantially parallel to the polarization axis of the piezoelectric element, where the shearing force is created by a component of a mechanical or an inertial force substantially perpendicular to the polarization axis. A transducer for measuring acceleration or mechanical forces, the acceleration causing inertial forces, includes at least one piezoelectric element and at least two spaced surfaces abutting the piezoelectric element and arranged so that they are mutually displaced by a component of a mechanical or an inertial force acting substantially in a direction perpendicular to the polarization axis of the piezoelectric element. The piezoelectric element is preferably mounted between the free ends of two arms posiitoned on a supporting base, the arms being deformed or tilted in a direction perpendicular to their longitudinal axis by the force or acceleration. Forces or accelerations in three directions may be measured using a single piezoelectric element with a plurality of electrodes. The principles are also useful for the measurement of force or pressure.

Description: METHOD AND APPARATUS FOR MEASURING ACCELERATION OR MECHANICAL FORCES FIELD OF THE INVENTION This invention relates to transducers employing piezoelectric elements for generating an electrical output in accordance with mechanical influences to which the piezoelectric element is subjected. The invention finds particular application in accelerometer transducers for giving electrical outputs in accordance with acceleration. BACKGROUND OF THE INVENTION Mechanical dynamometers are often used for static and dynamic measurements of mechanical forces. The forces to be measured may cause changes in the electrical charge, voltage, current or impedance in one or more measuring elements. When measuring mechanical vibrations or acceleration it is known to use seismic accelerometers employing piezoelectric material for generating the electrical charges. For such accelerometers it is known to have a seismic mass arranged on the piezoelectric element or material which again is arranged on a base. Thus, when the accelerometer is subjected to acceleration, inertial forces introduce strains in the ceramic element which produces electrical outputs by virtue of the piezoelectric effect. When vibrations having a frequency which is substantially lower than the natural resonant frequency of the total ac¬ celerometer system are acting upon the base, the seismic masε is forced to follow the vibrations thereby acting on the piezoelectric element with a force which is proportional to the seismic mass and the acceleration. Thereby, the inertial force acting on the piezoelectric element generates elec- trical charges on the element which charges are proportional to the acceleration. When the piezoelectric element is subjected to compression forces during vibration, the accelerometer is of the compres- sion type, and when the piezoelectric element is subjected to shear forces during vibration, the accelerometer is of the shear type. The compression type accelerometer is the most simple in its construction, but it is rather sensitive to temperature transients since the ceramic piezoelectric material is pyroelectric in the axis of polarization and the signals is taken from electrodes perpendicular to this axis. In contrast to this, the shear type accelerometer has a low sensitivity to temperature transients as the signal here is taken from electrodes parallel to the axis of polarisation. It is known that a higher sensitivity can be obtained by an accelerometer of the "bender" type. In such an accelerometer, the force from the seismic mass acts to bend a so-called "bender element", which has a layer of an electric conductive material sandwiched between two layers of piezoelectric material being polarized in their direction of thickness. Thus, when the element is bent, then, in a plane perpendicu¬ lar to the longitudinal axis of the element, stresses of compression are generated in one of the two layers and stresses of tension are generated in the remaining layer. When the length of the bender element is considerable larger than the thickness of the element, the electrical charges generated on each of the two layers will be larger than the charges obtained if the same seismic mass is operating di¬ rectly for the purpose of compression or shear of the piezoelectric material. However, a disadvantage of the bender element is that it is pyroelectric, since the electrodes are arranged on surfaces which are perpendicular to the axis of polarization. Another disadvantage of the bender element is that the piezoelectric material constitutes a major part of the mecha¬ nical construction which causes some problems when trying to optimize this construction. SUMMARY OF THE INVENTION It is therefore a principal object of this invention to provide a method and a transducer in which the pyroelectric effects of the piezoelectric material are reduced or avoided. According to the principles of the present invention this is done by using the shear sensitivity of the piezoelectric material while at the same time having the force of the seismic mass amplified. The principle of the present invention is illustrated in Fig. 1. In Fig. 1 two arms 1, 2 are shown both of which are secured in one end to a relatively stiff base 3 by two hinges 4, 5 and in the other end are secured to oppositely positioned surfaces of a piezoelectric element 6 which element is polarized in the longitudinal direction of the arms 1, 2. When the system of Fig. 1 is influenced by a force P perpen¬ dicular to the longitudinal axis of the arms 1, 2 at a dis¬ tance L from the axis of the hinges, a moment M = P x L is generated at the securing points. The hinges 4, 5 are only able to transfer shear or compression forces; thus, the moment M will not be transferred by the hinges, but the result will be a force couple P fl , P f2 with the arm h, where P fl , P f2 and the arm h fulfil the equation: P x L = P fl x h = P f2 x h or P fl = P f2 = P X L / h - Thus, the force P perpendicular to the longitudinal axis of the arms is transformed to a force couple P fl , P f2 acting in the longitudinal direction of the arms. The forces P fl , P f2 are L/h times larger than the force P and impose a mechanical stress on the piezoelectric element. From the above discussion it should be understood that accor- ding to the principles of the present invention, it is pos¬ sible, by arranging a seismic mass with its centre of gravity at a distance L from the axis of the hinges, to produce an accelerometer having a sensitivity which is L/h times larger than for an accelerometer where the same seismic mass is arranged to act directly on the piezoelectric element or elements, while at the same time obtaining the low dynamic temperature sensitivity which is characteristic for ac¬ celerometers of the shear type. It is therefore a principal object of the invention to pro- vide an improved method for measuring acceleration or mecha¬ nical forces, where the acceleration causes inertial forces, using a transducer or an accelerometer in which at least one piezoelectric element is influenced by a shearing force substantially parallel to the polarization axis of the piezoelectric element. In accordance with the principles of the invention this shearing force is created by a component of a mechanical or an inertial force being substantially perpendicular to the polarization axis of the piezoelectric element. When a shearing force or forces acts or act on a piezoelectric element, electrical charges are created on surfaces of the element whereby an electrical voltage may be generated across said piezoelectric element. The charges or voltage may be used in order to determine the component of the mechanical force or the component of the acceleration resulting in the shearing force. Preferably the shearing force is created by a mutual dis¬ placement of at least two spaced surfaces, with the displace¬ ment having a component substantially parallel to the axis of polarization of the piezoelectric element and being caused by the mechanical or inertial force. For the mechanical or inertial force component to create the shearing force it is preferred that the piezoelectric element or elements is or are mounted in an intermediate and abutting relationship with the surfaces. It is preferred that the piezoelectric element or elements is or are mounted between and in shear relationship with a first and a second of two substantially oppositely positioned surfaces, and in a preferred embodiment, a first piezoelectric element and a second piezoelectric element are mounted between and in shear relationship with said first and second substantially oppositely positioned surfaces, respectively. However, more than two piezoelectric elements may be arranged between these surfaces. In order to obtain a good sensitivity to the forces acting on the piezoelectric elements, the polarization axes of the piezoelectric elements should be substantially parallel to each other. However, the polarisation axes may be opposed to each other. In order for the two spaced surfaces to be mutually displaced by the mechanical or inertial force component and thereby creating the shearing force, it is preferred that each of the said two oppositely positioned surfaces are part of one of two arms or uprights positioned on a supporting base. The arms should be fastened to the base so that the arms are deformed or tilted in relation to the supporting base by said force componen . The form of the piezoelectric element or elements may vary, however, in order to maximize the sensitivity of the trans- ducer, it is preferred that the piezoelectric element or elements has or have substantially parallel surfaces extending in the direction of the axis of polarization. Hence, when the piezoelectric element or elements is or are being influenced by said generated shearing force, electrical charges are generated on the surfaces of the piezoelectric element or elements. Thus, the generated charges or a corresponding generated voltage difference may represent a measure of the force component creating the shearing force. The substantially opposite parallel surfaces of the piezoelectric element or elements may be plane surfaces or cylindrical surfaces. It should be understood that according to the principles of the invention it is possible to measure force components having different directions by having different directions of the surfaces of the piezoelectric element or elements. Thus, in a preferred embodiment, a measure of a first mecha¬ nical or inertial force component substantially perpendicular to the polarization axis is obtained from first charges being developed on a first pair of parallel surfaces of the piezoelectric element or elements, and a measure of a second mechanical or inertial force component, which is substan¬ tially perpendicular to the polarization axis and substan¬ tially perpendicular to the direction of the first force component, is obtained from second charges being developed on a second pair of parallel surfaces of the piezoelectric element or elements. Furthermore, a tri-axial measurement may be performed by further measuring a third mechanical or inertial force com¬ ponent substantially parallel to the polarization axis of the piezoelectric element or elements, with a shearing force being created by said third force component. It should be understood that a measurement in two directions may also be performed by combining the measurements of the first and the third force components. Another object of the invention is to provide a transducer or an accelerometer which is able to measure a mechanical force or an acceleration according to the principles of the present invention. Thus, according to the invention, a transducer or an accelerometer is provided comprising at least one piezoelectric element and at least two spaced surfaces abut¬ ting said piezoelectric element. These surfaces are arranged so that they are mutually displaced when a component of a mechanical or an inertial force acts substantially in a direction perpendicular to the polarization axis of the piezoelectric element. In order to obtain mechanical stress within the piezoelectric element or elements and thereby creating a shearing force, it is preferred that the piezoelectric element or elements of the transducer are positioned between and in shearing re¬ lationship with the two spaced surfaces. It is furthermore preferred that the two spaced surfaces are arranged so that they are substantially opposed to each other. Thus, when the spaced surfaces are mutually displaced by the force component, the piezoelectric element or elements will be influenced by a shearing force substantially parallel to the polarization axis of the piezoelectric element or elements, thereby generating an electrical signal which may be output from the piezoelectric element or elements and used for determining the mechanical force component or the acceleration component. It is preferred that the transducer has two ore more piezoelectric elements mounted between and in shear re¬ lationship with said two substantially oppositely positioned surfaces, where the piezoelectric elements have substantially parallel polarization axis. Furthermore it is preferred that the two spaced surfaces of the transducer are part of one or two arms or uprights positioned on a supporting base, the arms being deformed or tilted in relation to the supporting base when the force component is acting on at least one of the arms. In order to obtain an electrical output signal when measuring a mechanical force or an acceleration, it is preferred that the transducer further comprises first electrical output means for outputting a first electrical output signal being developed across a first pair of substantially parallel surfaces of the piezoelectric element or elements, said first output signal representing a measure of a first mechanical or inertial force component substantially perpendicular to the polarization axis. It is furthermore preferred that the transducer comprises second electrical output means for outputting a second elec¬ trical output signal being developed across a second pair of substantially parallel surfaces of the piezoelectric element or elements, said second output signal representing a measure of a second mechanical or inertial force component, which is substantially perpendicular to the polarization axis and substantially perpendicular to the direction of the first force component. In order to obtain a tri-axial transducer it is also pre¬ ferred that the transducer comprises third electrical output means for outputting a third electrical output signal being developed by a shearing force acting on the piezoelectric element or elements, said shearing force being generated by a third mechanical or inertial force component substantially parallel to the polarization axis of the piezoelectric element or elements. It should be understood that the transducer or accelerometer according to the present invention may be constructed to incorporate any of the features presented in this specifi¬ cation and the accompanying drawings. BRIEF DESCRIPTION OF THE DRAWINGS Embodiments and details of the system appear from the claims and the detailed discussion of embodiments of the system given in connection with the accompanying drawings in which: Fig. 1 is a schematic illustration of the principles of the invention, Figs. 2 and 3 show embodiments of a symmetrical transducer according to the invention, Fig. 4 shows an embodiment of a transducer with two piezoelectric elements in accordance with the invention, Fig. 5 shows an embodiment of a transducer with four piezoelectric elements in accordance with the invention, Fig. 6 shows an embodiment of a transducer in accordance with the invention in which the piezoelectric element is formed as a block with a cylindrical hole, Fig. 7 shows an embodiment of a transducer in accordance with the invention having an annular piezoelectric element, and Fig. 8 shows a presently preferred embodiment of a transducer in accordance with the invention having an annular piezoelectric element. DETAILED DESCRIPTION OF THE INVENTION In the example shown in Fig. 1, the arms 1, 2 are secured to the base 3 by use of hinges 4, 5 allowing the arms to be tilted in relation to the supporting base. However, it should be understood that it is not necessary to secure the arms by use of hinges, but it is preferred that the attachment of the arms to the base is performed in such a way that deformation or tilting of the arms in relation to the base by a force perpendicular to the longitudinal axis of the arms is facilitated. Thus, it is preferred that each of the arms themselves is substantially more easily tilted in relation to the supporting base than the combination of the two arms and the piezoelectric element or elements. This is illustrated by the embodiments shown in Figs. 2 and 3. Fig. 2 shows a symmetrical transducer having two pair of arms 21a, 21b and 21c, 21d secured to a base 22 where the tilting of the arms is facilitated by notches 25a, 25b and 25c, 25d. Between each pair of arms 21a, 21b and 21c, 21d, a piezoelectric element 23 and 24, respectively, is sandwiched, and a pair of seismic masses 26a, 26b and 26c, 26d is arranged on the outer surface of the arms 21a, 21b and 21c, 21d, respectively. The axes of polarization of the piezoelectric elements 23 and 24 are indicated by the arrows 27 and 28, respectively. In this embodiment of the invention, the construction of the transducer is symmetrical in order to obtain balance of the system and thereby reduce or avoid transverse movements in the transducer construction. If the electrical signals from the two piezoelectric elements 23 and 24 are added, the transducer will mainly be sensitive to forces or accelerations in a direction given by the arrows 29 and 30, and if the signals from the two elements are subtracted, the transducer will mainly be sensitive to angu- lar forces or angular accelerations around an axis perpen¬ dicular to the plane given by the arrows 27, 28, 29 and 30. Fig. 3 shows another symmetrical transducer similar to the transducer of Fig. 2, but with the seismic masses 36, 37 sandwiched between corresponding pairs of piezoelectric elements 33a, 33b and 33c, 33d, respectively. The reference numerals of Fig. 3 are otherwise similar to the reference numerals of Fig. 2. If the seismic mass 36 equals the sum of the seismic masses 26a and 26b, the arm lengths from the notches 25a and 25b to the centre of gravity of the corre- sponding seismic mass or masses 36 or 26a and 26b are equal, and if the distances between the hinges which may be repre ¬ sented by the notches 25a and 25b in Figs. 2 and 3 are equal, the shearing force acting on the piezoelectric element 23 in Fig. 2 will equal the shearing force acting on the piezoelectric elements 33a and 33b in Fig. 3. Fig. 4 shows a transducer corresponding to one half of the transducer shown in Fig. 3, but turned 90° so that the axis of polarization of the piezoelectric elements is in the direction of the z-axis of the system of co-ordinates. In Fig. 4 the two arms are referred to by 41a and 41b, the two piezoelectric elements are referred to by 42 and 43 with surfaces 42a, 42b and 43a, 43b, respectively, the two notches are referred to by 44a and 44b, the seismic mass is referred to by 45, and the base is referred to by 46. It is preferred that the surfaces 42b and 43a are in con¬ ducting engagement with the seismic mass 45 which should be made from a conductive material with the result that the potential of surface 42b equals the potential of surface 43a. When measuring an acceleration in the z-direction in accor- dance with prior art technique the two piezoelectric elements act in parallel with the substantial same potential dif¬ ference being generated from surface 42a to surface 42b and from surface 43b to surface 43a. This voltage can be obtained by grounding the surfaces 42a and 43b and by measuring the voltage of the seismic mass 45. However, accelera ions in the x-direction may be measured according to tn«- principles of the present invention by having the t . piezoelectric elements 42 and 43 in series. Having the sam~ potential for the surfaces 42b and 43a, the surface 42a may be grounded and the electrical series output may be output from the surface 43b. It should be noted that the electrical output signal may represent the electrical charges generated at the surface 43b. Thus, with the arrangement of a transducer as shown in Fig. 4 it is possible to bring output signals to a combined sum¬ mation and difference amplifier and thereby measure ac¬ celeration in two directions which are perpendicular to each other. If the direction of polarization of the piezoelectric element 43 is turned substantially 180°, the output signals from the elements 42 and 43 should preferably be combined in parallel when measuring accelerations in the x-direction and in series when measuring accelerations in the z-direction. If it is desired to measure accelerations or forces in all three axes of the system of co-ordinates, this can be ac¬ complished by having a second pair of piezoelectric elements arranged on the seismic mass 45. This is illustrated in Fig. 5 which shows a tri-axial accelerometer where the principles of the present invention is used when measuring in the x- direction and the y-direction, whereas the acceleration in the z-direction is measured in accordance with prior art techniques. The transducer of Fig. 5 comprises piezoelectric elements 51, 52, 53 and 54 which are all polarized in the z-direction of the transducer or accelerometer. All four elements 51, 52, 53 and 54 have their inner surfaces in conducting engagement with a seismic mass 55, which is preferably made of a con- ducting material, whereas their outer surfaces are abutting four corresponding arms 58a, 58b and 59a, 59b. The elements may be clamped between the arms and the seismic mass by a clamping ring surrounding the arms. The arms are arranged on a base 57, and it is preferred that the arms have notches 60a, 60b and 61a, 61b (61a and 61b are not shown) in order to facilitate tilting when measuring accelerations or forces in the x-direction or the y-direction. It is preferred that the outer surface of element 51 is connected to ground, and that the two elements 51 and 52 are connected in series in order to feed a signal to an x-output for measuring accelerations or forces in the x-direction. Correspondingly, it is preferred that the outer surface of element 53 is connected to ground, and that the two elements 53 and 54 are connected in series in order to feed a signal to an y-output for measuring accelerations or forces in the y-direction. Both the x-signal and the y-signal may be con¬ nected to charge amplifiers delivering the x-output and the y-output, respectively. When the transducer in Fig. 5 is vibrated in the z-direction, the signals of all four elements 51-54 are summed at the seismic mass 55, since the input at the charge amplifiers of the x-output and the y-output are virtually zero. Thus, when measuring forces or accelerations in the z-direction, the signals from all four elements 51-54 are used in parallel and an output signal for measurements in the z-direction is taken from the seismic mass 55 and fed to a voltage amplifier in order to obtain a z-output. When vibrating the transducer in the x-direction or the y- direction the corresponding pair of elements are connected in series. Each element in such a pair of series connected elements has the substantially same capacity and the same resulting charges, and if the first element in such a pair is connected to ground and the second element is connected to virtually zero at the charge amplifier, the centre of such a pair will also have a voltage of zero. Thus, no or only a small error signal will be generated in the non-vibrating directions, even if all the elements 51-54 are electrically connected to each other at the centre point, which may be represented by the seismic mass 55. It is important to notice that the output signal feeding the z-output is not capacitively loaded, since a vibration in the z-direction otherwise could result in a current being drawn from the centre point to ground. Thus, the voltage amplifier at the z-output should preferably be an amplifier with a low input capacity. Fig. 6 shows a tri-axial transducer or accelerometer mea¬ suring along the same principles discussed in connection with Fig. 5. However, in Fig. 6 the four elements 51-54 of Fig. 5 are replaced by one piezoelectric element formed mainly as a block 62 having a substantially cylindrical hole 63. The outer surfaces 64-67 of the block 62 correspond to the outer surfaces of the elements 51-54 in Fig. 5. The reference numerals in Fig. 6 are otherwise similar to the reference numerals of Fig. 5. There is no separate seismic mass in the transducer of Fig. 6, since the weight of the block 62 will operate as a seismic mass when measuring in the z-direction. Furthermore, when measuring in the x-direction and the y-direction the masses of the arms and the clamping ring will also contribute to the total seismic mass. However, a separate seismic mass may be introduced into the hole 63 in order to obtain a greater sensitivity of the transducer. Another example of a tri-axial transducer or accelerometer is shown in Fig. 7. This transducer corresponds to the trans¬ ducer of Fig. 6, however, the piezoelectric block 62 is now replaced with a piezoelectric element 72 having a substan¬ tially annular cross section with a hole 73. The surfaces 74, 75, 76 and 77 abutting the arms 58a, 58b and 59a, 59b which are formed to engage with these surfaces, correspond to the surfaces 64-67 in Fig. 6. It should be understood that the transducer of Fig. 7 will operate in a way corresponding to the transducer of Fig. 6, but the annular construction may be produced at lower costs. Fig. 8 shows a presently preferred embodiment of a tri-axial transducer or accelerometer operating according to the principles discussed in connection with Fig. 5. A piezoelectric ring 72 is polarized in the axial direction, and a cylindrical seismic mass 55 made of tungsten is soldered into the piezoelectric ring 72. Four arms 58a, 58b, 59a, and 59b (59a and 59b are not shown) are positioned adjacent to the piezoelectric ring 72, and an insulating ring 81 insulates the four arms 58a, 58b, 59a, and 59b from a clamping ring 82 of steel pressing the four arms firmly against the piezoelectric ring 72. Each of the four arms 58a, 58b, 59a, and 59b is supported by a corresponding hinge 60a, 60b, 6la, and 61b (61a and 61b are not shown) that electrically and mechanically interconnects the corresponding arm to a thickfilm circuit board 84 containing three amplifiers. The thickfilm circuit board 84 is glued into a base 57, which is made of titanium and comprises an integrated electrical connector. A wire 86 connects the cylindrical seismic mass 55 to the amplifier for the z- direction. The housing 87 of the transducer is made of titanium, and is externally shaped as a cube. The housing 87 has a cylindrical bore, into which the base 57 is pressed and welded to the housing. The accelerometer shown in fig. 8 has the following specifications: Sensitivity before amplifier (X and Y directions) : 9 pC/g Sensitivity before amplifier (Z direction) : 10 mV/g Resonance frequency (X and Y directions) : 8 kHz Resonance frequency (Z direction) : 10 kHz Weight: 15 gram Although only a limited number of embodiments of the in¬ vention has been specifically disclosed and described herein, it will be obvious that the invention is not limited thereto, but is capable of being embodied in other forms as well. Furthermore, the invention is not limited to the measurements of acceleration, but may for example be employed in instruments that measure force or pressure.

Claims: CLAIMS 1. A method for measuring acceleration or mechanical forces, said acceleration causing inertial forces, using a transducer or an accelerometer in which at least one piezoelectric element is influenced by a shearing force substantially parallel to the polarization axis of the piezoelectric element, c h a r a c t e r i s e d in that the shearing force is created by a component of a mechanical or an inertial force, said mechanical or inertial force component being substan¬ tially perpendicular to said polarization axis. 2. A method according to claim 1, wherein the shearing force is created by a mutual displacement of at least two spaced surfaces, said displacement having a component substantially parallel to said axis of polarization and being caused by said mechanical or said inertial force, and said piezoelectric element or elements being mounted in an inter¬ mediate and abutting relationship with said surfaces. 3. A method according to claim 2, wherein the piezoelectric element or elements is or are mounted between and in shear relationship with a first and a second of two substantially oppositely positioned surfaces. 4. A method according to claim 2, wherein a first piezoelectric element and a second piezoelectric element are mounted between and in shear relationship with a first and a second of two substantially oppositely positioned surfaces, respectively, said first and second piezoelectric elements having substantially parallel polarization axes. 5. A method according to claim 2, wherein two or more piezoelectric elements are mounted between and in shear relationship with a first and a second of two substantially oppositely positioned surfaces, said piezoelectric elements having substantially parallel polarization axes. 6. A method according to any of the claims 3-5, wherein each of said two oppositely positioned surfaces is part of one of two arms or uprights positioned on a supporting base, the arms being deformed or tilted in relation to the supporting base by said force component. 7. A method according to any of the claims 2-6, wherein the piezoelectric element or elements have substantially parallel surfaces extending in the direction of the axis of po¬ larization, with electrical charges being developed on said parallel surfaces when the piezoelectric element or elements is or are being influenced by said generated shearing force, said charges representing a measure of said force component creating the shearing force. 8. A method according to claim 7, wherein the substantially opposite parallel surfaces of the piezoelectric element or elements is or are plane surfaces. 9. A method according to claim 7, wherein the substantially opposite parallel surfaces of the piezoelectric element or elements is or are cylindrical surfaces. 10. A method according to any of the claims 7-9, wherein a measure of a first mechanical or inertial force component substantially perpendicular to the polarization axis is obtained from first charges being developed across a first pair of parallel surfaces of the piezoelectric element or elements, and a measure of a second mechanical or inertial force component, which is substantially perpendicular to the polarization axis and substantially perpendicular to the direction of the first force component, is obtained from second charges being developed on a second pair of parallel surfaces of the piezoelectric element or elements. 11. A method according to any of the claims 1-10, further comprising measuring a third mechanical or inertial force component substantially parallel to the polarization axis of the piezoelectric element or elements, with a shearing force being created by said third force component. 12. A transducer for measuring acceleration or mechanical forces with said acceleration causing inertial forces, said transducer comprising at least one piezoelectric element and at least two spaced surfaces abutting said piezoelectric element, c h a r a c t e r i s e d in that the surfaces are arranged so that they are mutually displaced by a component of a me¬ chanical or an inertial force acting substantially in a direction perpendicular to the polarization axis of said piezoelectric element. 13. A transducer according to claim 12, wherein the piezoelectric element or elements is or are positioned between and in shearing relationship with the two spaced surfaces, so that the piezoelectric element or elements is or are influenced by a shearing force substantially parallel to the polarization axis of the piezoelectric element or elements when the spaced surfaces are mutually displaced by said force component. 14. A transducer according to claim 12 or 13, wherein the spaced surfaces are arranged so that they are substantially opposed to each other. 15. A transducer according to claim 14, wherein two ore more piezoelectric elements are mounted between and in shear relationship with said two substantially oppositely positioned surfaces, said piezoelectric elements having substantially parallel polarization axes. 16. A transducer according to any of the claims 12-15, where¬ in each of said two spaced surfaces are part of one of two arms or uprights positioned on a supporting base, the arms being deformed or tilted in relation to the supporting base by said force component. 17. A transducer according to any of the claims 13-16, where¬ in the piezoelectric element or elements has or have substantially parallel surfaces extending in the direction of the axis of polarization, with electrical charges being de¬ veloped on said parallel surfaces when the piezoelectric element or elements is or are influenced by said shearing force, said charges representing a measure of said force component creating the shearing force by mutually displacing said surfaces. 18. A transducer according to claim 17, wherein the substan¬ tially opposite parallel surfaces of the piezoelectric element or elements is or are plane surfaces. 19. A transducer according to claim 17, wherein the substan¬ tially opposite parallel surfaces of the piezoelectric element or elements is or are cylindrical surfaces. 20. A transducer according to any of the claims 17-19, fur¬ ther comprising first electrical output means for outputting a first electrical output signal being developed across a first pair of substantially parallel surfaces of the piezoelectric element or elements, said first output signal representing a measure of a first mechanical or inertial force component substantially perpendicular to the polarization axis. 21. A transducer according to claim 20, further comprising second electrical output means for outputting a second electrical output signal being developed across a second pair of substantially parallel surfaces of the piezoelectric element or elements, said second output signal representing a measure of a second mechanical or inertial force component, which is substantially perpendicular to the polarization axis and substantially perpendicular to the direction of the first force component. 22. A transducer according to any of the claims 12-20, fur¬ ther comprising third electrical output means for outputting a third electrical output signal being developed by a shearing force acting on the piezoelectric element or elements, said shear¬ ing force being generated by a third mechanical or inertial force component substantially parallel to the polarization axis of the piezoelectric element or elements. 23. A transducer according to any of the claims 16-22, where¬ in the arms are arranged on the supporting base so as to facilitate said deformation or tilting. 24. A transducer according to claim 23, wherein each of the arms themselves are more easily tilted in relation to the supporting base than the combination of the two arms and the piezoelectric element or elements. 25. A transducer according to claim 23 or 24, wherein the arms are arranged on the supporting base by use of hinge means. 26. A transducer according to claim 23 or 24, wherein for each of said arms, a part of the arm, which part is close to the supporting base, is made less stiff than the remaining part of the arm.

Inventors: HANSEN KNUD STYHR, HANSEN, KNUD, STYHR
Applicants: BRUEEL & KJAER AS, HANSEN KNUD STYHR, A/S BRUEEL & KJAER, HANSEN, KNUD, STYHR
Application year: 1996
Main classification: G01P15
IPC codes: G01L5, G01P15