JP2007117934A - Bolt tightening langevin-type oscillator - Google Patents

Abstract

<P>PROBLEM TO BE SOLVED: To provide a bolt-tightening Langevin type oscillator providing an amplitude large enough to generate cavitation even in a high frequency. <P>SOLUTION: The bolt-tightening Langevin type oscillator is composed by setting a total thickness formed by thicknesses of first and second metal plates 7, 8 and piezoelectric elements 3 to be one wavelength, by forming the second metal plate 8 as two plate-like state facing large and small plates, holding the piezoelectric elements 3 so that the first metal plate 7 and the larger face of the second metal plate 8 come into contact with each other, and fastening the central part with a bolt 6. By this configuration, an enlarged amplitude is transmitted to a third metal plate 9 set to a half wavelength, to provide a high amplitude of a high frequency having 3/2 wavelength as a whole. <P>COPYRIGHT: (C)2007,JPO&INPIT

Description

  The present invention relates to a piezoelectric element used in a vibration system for high-power ultrasonic applications, and more particularly to a bolt-clamped Langevin type vibrator suitable for a high-frequency ultrasonic cleaner.

  Currently, a piezoelectric element is used as a driving source for generating ultrasonic waves in an ultrasonic cleaning machine. Above all, industrial ultrasonic cleaners used for cleaning products after machining have a strong ultrasonic wave generator called bolt-clamped Langevin type vibrator because of the large ultrasonic output. Is used.

  FIG. 1 is a side view showing an example of a bolted Langevin type vibrator. A general bolted Langevin type vibrator 1 has a pair of disk-shaped piezoelectric elements 3 having a through hole at the center on both sides of an electrode plate 2, and has the same diameter as the piezoelectric element 3 on both sides thereof. A disk-shaped metal plate 4 and a metal plate 5 are arranged and integrally connected by a bolt 6 at the center.

  FIG. 2 is a graph showing the vibration characteristics of a bolted Langevin type vibrator. The horizontal axis represents the distance to the right end face as + L and the distance to the left end face as -L when the center of the bolted Langevin type vibrator 1 shown in FIG. 1 is 0 and the length in the longitudinal direction is 2L. The distance from the center with respect to the longitudinal direction of the bolted Langevin type vibrator 1 is shown. The vertical axis indicates the amplitude generated in the longitudinal direction when the bolted Langevin type vibrator 1 is driven at the resonance frequency, and the amplitude in the right direction from the center of the bolted Langevin type vibrator 1 shown in FIG. Plus), the amplitude in the left direction is shown as-(minus).

  Α shown in FIG. 2 indicates a maximum amplitude value when driven by a certain voltage. Here, when attention is paid only to the amplitude of the right end face of the bolted Langevin type vibrator 1 shown in FIG. 1, the amplitude is proportional to the voltage, and the voltage value changing with time at the resonance frequency is synchronized with the change in amplitude. The horizontal axis of the graph is replaced with time T, and the trajectory is exactly the same as the graph in which + L is + T and -L is -T. At this time, time 2T is a half wavelength of the resonance frequency, and it can be seen that the total length 2L of the bolted Langevin type vibrator is a half wavelength of the resonance frequency.

  Bolt-clamped Langevin type vibrators used in industrial ultrasonic cleaners are generally used with a resonance low frequency of 20 kHz to 50 kHz that is easy to generate cavitation. In order to improve, a high-frequency bolted Langevin type vibrator having a resonance frequency of 50 kHz to 200 kHz has also been used.

  This high-frequency bolt-tightened Langevin type vibrator usually uses a technique for increasing the frequency by shortening the entire length. For example, in a bolt-clamped Langevin type vibrator having a total length of 40 mm at 50 kHz, when the resonance frequency is about 100 kHz, the total length is shortened to about 20 mm.

  However, in this case, not only is it difficult to integrally couple the piezoelectric element and the metal plate with a bolt, but it is also necessary to reduce the thickness of the piezoelectric element. For this reason, there is a problem in that electrical input is also limited and high output cannot be obtained. As a solution to this problem, a proposal has been made to solve the problem by designing the total length to be 1.5 wavelengths, not half-wave, and to make the total length three times longer than the half-wave design. ing. Such a bolt-clamped Langevin type vibrator is disclosed in Patent Document 1.

JP-A-6-254493

FIG. 3 is a graph showing the relationship between the sound intensity and the frequency for generating cavitation in the ultrasonic cleaner. The horizontal axis indicates the frequency (Hz), and the vertical axis indicates the minimum sound intensity (W / cm ² ) necessary for cavitation generation. Further, the graph shows two levels of water as the medium, deaerated water and saturated water. As can be seen from the graph, the higher the frequency, the higher the minimum sound wave intensity required for cavitation generation, and a minimum sound wave intensity of several times is required at 50 kHz to 200 kHz compared to the normally used 20 kHz to 50 kHz. I understand.

  However, in a conventional bolted Langevin type vibrator having a resonance frequency of 50 kHz to 200 kHz, even if the total length is 1.5 wavelengths, the amplitude obtained with the same electrical input is a bolted Langevin resonator having a resonance frequency of 20 kHz to 50 kHz. There is a problem that the minimum sound intensity for obtaining cavitation at a high frequency cannot be obtained as described above.

  Therefore, an object of the present invention is to solve the above-mentioned problems of the prior art. Specifically, an object of the present invention is to provide a bolted Langevin type vibrator capable of obtaining a large amplitude sufficient to cause cavitation even at high frequencies.

  The present invention employs the following means in order to solve the above problems. That is, according to the present invention, the total thickness formed by the thicknesses of the first and second metal plates and the thickness of the piezoelectric element is set to one wavelength, and the amplitude is increased by the second metal plate. The gist is that a large amplitude can be obtained even at higher frequencies.

  According to the present invention, there is provided a bolted Langevin type vibrator comprising a first metal plate, a second metal plate, a third metal plate, a piezoelectric element and a bolt, the first metal plate being an upper surface portion. And a bottom surface portion and a side surface portion, and has a female screw at the top surface portion or the central portion of the bottom surface portion, and the second metal plate is composed of the top surface portion, the bottom surface portion, and the side surface portion. There is a female screw in the center, and the area of the bottom surface of the second metal plate is larger than that of the top surface, and the piezoelectric element is a plate composed of a top surface, a bottom surface, and a side surface, and is 1 or more. The first metal plate is in contact with and sandwiched between the top surface of the first metal plate and the bottom surface of the second metal plate, and has a hole penetrating from the top surface to the bottom surface. The first metal plate and the second metal plate are threaded into the female screw of the first metal plate and the female screw of the second metal plate through the hole of the element. Fastening the metal plate, the third metal plate is composed of an upper surface portion, a bottom surface portion and a side surface portion, the bottom surface portion of the third metal plate abuts on the upper surface portion of the second metal plate, The dimension formed by the sum of the thickness of the first metal plate, the thickness of the second metal plate, and the thickness of all the piezoelectric elements is one wavelength, and the thickness dimension of the third metal plate is a half wavelength. A bolted Langevin type vibrator characterized by being a positive integer multiple is obtained.

  The total thickness formed by the thicknesses of the first and second metal plates and the thickness of all the piezoelectric elements is set to one wavelength, and the area of the bottom surface of the second metal plate is the area of the top surface. A larger plate shape, sandwiching the piezoelectric element so that the bottom surface of the first metal block and the second metal block are in contact, and fastening the central part with the bolt constitutes a bolted Langevin type vibrator By doing so, an enlarged amplitude is transmitted to the third metal block set to a half wavelength, and a high amplitude at a high frequency of 1.5 wavelengths as a whole is obtained. The third metal block may be a positive integer multiple of a half wavelength.

  The outer shapes of the first metal plate and the piezoelectric element are preferably discs having the same diameter. However, the first metal plate has a polygon or a larger surface on which the outer periphery of the piezoelectric element is inscribed. It may be a rectangular plate. Further, the bottom surface of the second metal plate has a circular shape with the same diameter as the outer shape of the piezoelectric element, and preferably has a structure in which the diameter decreases toward the upper surface or a truncated cone shape. It is good also as the shape of the polygon frustum which has the bottom face of the polygon which inscribed or a larger area than it. Furthermore, in the second metal plate, the ridge line connecting the upper surface portion and the bottom surface portion is preferably a curve, but may be a straight line or a ridge line that is a combination of a straight line and a curve.

  According to the present invention, there is obtained a bolted Langevin type vibrator characterized in that the second metal plate and the third metal plate are integrally molded. The second metal plate and the third metal plate may be mechanically coupled by fastening, bonding, welding, or the like using bolts, but may be integrally formed by cutting or casting from a single material. Also good.

  In addition, according to the present invention, there is obtained a bolted Langevin type vibrator having a concave portion that circulates in a side surface portion of the third metal plate.

  In the present invention, it is desirable that the third metal plate is a disk having the same outer diameter as that of the piezoelectric element. Furthermore, the surface on the side facing the surface to be joined to the second metal plate is a vibration radiation surface, and by providing a concave portion around the side surface portion of the third metal plate, the vibration distribution of the entire radiation surface is made uniform. It becomes possible to.

  Furthermore, according to the present invention, there can be obtained a bolted Langevin type vibrator characterized in that there are two or more piezoelectric elements and a fourth metal plate is sandwiched between the piezoelectric elements. When the thickness of the piezoelectric element is reduced in order to reduce the drive voltage, it is necessary to increase the number of piezoelectric elements corresponding to the reduced thickness of the piezoelectric element to supplement the power resistance strength. At this time, it is possible to adjust the frequency and control the vibration mode by inserting a fourth metal plate between the piezoelectric elements.

  As described above, according to the present invention, it is possible to provide a bolted Langevin type vibrator capable of obtaining a large amplitude sufficient to cause cavitation even at high frequencies.

  Hereinafter, embodiments of the present invention will be described in detail with reference to the drawings.

  FIG. 4 is a side view showing the first embodiment. In FIG. 4, the hatched portion indicates a cross section. In the first embodiment, the first metal plate 7, the second metal plate 8, the third metal plate 9, the two piezoelectric elements 3, the bolt 6, and the electrode plate 2 are used as shown in FIG. A bolted Langevin type vibrator was used.

  The first metal plate 7, the second metal plate 8, and the third metal plate 9 were made of an aluminum alloy. The first metal plate 7 is a disc having a diameter of 35 mm and a thickness of 10 mm, and an M10 (ISO standard) female screw is attached so as to penetrate the center of the disc. The second metal plate 8 is composed of a disc portion having a diameter of 35 mm and a thickness of 5 mm, and a horn-shaped portion having a thickness of 15 mm that gradually decreases from 35 mm to 23 mm. The central portion has a diameter of 35 mm. A female screw having a depth of 15 mm from the surface was attached. The third metal plate 9 is a disc having a diameter of 35 mm and a thickness of 23 mm, and the third metal plate 9 and the second metal plate 8 are integrally molded bodies obtained by cutting a single aluminum alloy material. It was.

  As the piezoelectric element 3, lead zirconate titanate-based piezoelectric ceramics was used. Two pieces with an outer diameter of 35 mm, an inner diameter of 15 mm, and a thickness of 5 mm are used, and the two piezoelectric elements 3 face each other with the same polar face, and the electrode plate 2 is sandwiched between them. Arranged. Further, one of the two surfaces of the piezoelectric element 3 not in contact with the electrode plate 2 is disposed so as to contact the first metal plate 7, and the other surface has a diameter of the second metal plate 8. It arrange | positioned so that it may contact | abut on the surface used as 35 mm. Then, a bolt 6 was screwed into the female screw, and the first metal plate 7 and the second metal plate 8 were fastened. A third metal plate 9 is integrated with the second metal plate 8, and in this state, a bolted Langevin type vibrator is formed.

  Here, the thickness (the dimension from A to D shown in FIG. 4) formed by the first metal plate 7, the two piezoelectric elements 3, and the second metal plate 8 is a length of one wavelength at the resonance frequency. The thickness of the third metal plate 9 (dimensions from D to E shown in FIG. 4) is half the wavelength at the resonance frequency, and the thickness is designed and adjusted from the sound speed of the material used for each. The dimensions are not limited to the above.

  FIG. 5 is a graph showing the vibration characteristics of Example 1. In this graph, the vertical axis indicates amplitude, the horizontal axis indicates the position in the longitudinal direction shown in FIG. 4, and the amplitude at each position in the longitudinal direction of the bolted Langevin type vibrator according to the first embodiment. . Further, in the graph, the value of the amplitude when the vibration radiation surface 11 shown in FIG. 4 has the maximum amplitude in the left direction with respect to the longitudinal direction is indicated by − (minus) on the vertical axis. The amplitude at each position is shown. Accordingly, the display of + (plus) on the vertical axis indicates that the amplitude is in the right direction with respect to the longitudinal direction.

  From the vibration characteristics of Example 1 shown in FIG. 5, it can be seen that the absolute value of the amplitude is amplified from β1 to γ1 in the region C to D of the graph, that is, the second metal plate 8 portion. The value of γ1 appears as the amplitude at the vibration radiation surface 11 shown in FIG. The amplification of the amplitude is realized by providing the second metal plate 8 with two large and small surfaces having different areas facing each other. Further, it can be seen that the wavelength is A wavelength in the region A to D, and the half wavelength is in the region D to E.

  In Example 1, when a voltage of 100 Vpp with a frequency of 100 kHz was applied, an amplitude of γ1 = 1.5 μm was obtained. This is a value corresponding to 1.5 to 2 times the amplitude obtained conventionally. Therefore, a large amplitude sufficient to cause cavitation even at high frequencies was obtained during ultrasonic cleaning.

  FIG. 6 is a side view showing the second embodiment. The basic configuration is the same as that of the first embodiment, but in the second embodiment, by using four piezoelectric elements 3 having a thickness of 4 mm, the total volume of the piezoelectric elements 3 is increased compared to the first embodiment, and the input is performed. It has a structure that can increase electric power. For this purpose, two sets of two piezoelectric elements 3 with the same polar face facing each other and an electrode plate 2 sandwiched between them are made into an annular shape having an outer diameter of 35 mm, an inner diameter of 15 mm, and a thickness of 3 mm. Are arranged so as to sandwich the fourth metal plate 10 made of an aluminum alloy, and one of the two surfaces not in contact with the electrode plate 2 of the piezoelectric element 3 is the first one as in the first embodiment. It arrange | positioned so that it might contact | abut with the metal plate 7, and it arrange | positioned so that the other surface might contact | abut the surface where the diameter of the 2nd metal plate 8 is set to 35 mm. Then, the bolt 6 was screwed into the female screw, and the first metal plate 7 and the second metal plate 8 were fastened.

  Here, the thicknesses of the first metal plate 7 and the second metal plate 8 are reduced so as to offset the increase in the total thickness of the piezoelectric elements 3 and the increase in the fourth metal plate 10. did. Moreover, the recessed part 12 of width 5mm and depth 3.5mm was provided in the perimeter of the center part of the side part of a 3rd metal plate.

  FIG. 7 is a graph showing the vibration characteristics of Example 2. In this graph, the vertical axis indicates the amplitude as in FIG. 5, the horizontal axis indicates the position in the longitudinal direction shown in FIG. 6, and the amplitude at each position in the longitudinal direction of the bolted Langevin type vibrator according to the second embodiment. Is shown. Further, in the graph, when the vibration radiation surface 11 shown in FIG. 6 has the maximum amplitude in the left direction with respect to the longitudinal direction, the value of the amplitude is indicated by − (minus) on the vertical axis, and at that time The amplitude at each position is shown. Accordingly, the display of + (plus) on the vertical axis indicates that the amplitude is in the right direction with respect to the longitudinal direction.

  From the vibration characteristics of Example 2 shown in FIG. 7, as in Example 1, the absolute value of the amplitude is amplified from β2 to γ2 in the region C to D of the graph, that is, the second metal plate 8 part. I understand that The value of γ2 appears as the amplitude on the vibration radiation surface 11 shown in FIG. Similar to the first embodiment, this amplitude amplification is also realized by providing the second metal plate 8 with two large and small surfaces with different facing areas.

  In Example 1, when a voltage of 100 Vpp with a frequency of 100 kHz was applied, an amplitude of γ2 = 1.3 μm was obtained. This is a slightly smaller value than that of the first embodiment. This is due to an increase in loss due to a decrease in vibration transmission efficiency due to an increase in the piezoelectric element 3 and the fourth metal plate.

  FIG. 8 is a diagram showing the vibration distribution on the vibration radiation surface. The amplitude distribution in the vibration radiation surface 11 from F to G shown in FIG. 6 is shown. The dotted line indicates the vibration distribution 19 in the first embodiment, and the solid line indicates the vibration distribution 20 in the second embodiment. As can be seen from this figure, the vibration distribution 20 according to the second embodiment has a uniform amplitude over a wide region as compared with the vibration distribution 19 according to the first embodiment. This is because the transmission of vibration is made uniform by the effect of the concave groove provided in the third metal plate.

  Therefore, in the second embodiment, although the amplitude is smaller than that in the first embodiment, the vibration distribution on the vibration radiation surface 11 is uniform, and a large amplitude sufficient to cause cavitation at high frequency is also obtained during ultrasonic cleaning. Obtained.

  In Example 1 and Example 2, the first metal plate, the second metal plate, and the third metal plate are discs, but the same effect can be obtained even if square plates are used. . The material to be used is not limited to an aluminum alloy, but may be other metals such as stainless steel and titanium.

  The bolted Langevin type vibrator according to the present invention can be used not only for an ultrasonic cleaning machine for high frequency but also for an ultrasonic processing machine that requires high output and large amplitude, a medical machine using ultrasonic waves, and the like.

The side view which shows an example of a bolt fastening Langevin type vibrator. The graph which shows the vibration characteristic of a bolted Langevin type vibrator. The graph which shows the relationship between the sound wave intensity and frequency for generating cavitation in an ultrasonic cleaner. FIG. 3 is a side view showing Example 1; 3 is a graph showing vibration characteristics of Example 1. FIG. 6 is a side view showing Example 2. 6 is a graph showing the vibration characteristics of Example 2. The figure which shows the vibration distribution of a vibration radiation surface.

Explanation of symbols

DESCRIPTION OF SYMBOLS 1 Bolt tightening Langevin type vibrator 2 Electrode plate 3 Piezoelectric element 4, 5 Metal plate 6 Bolt 7 First metal plate 8 Second metal plate 9 Third metal plate 10 Fourth metal plate 11 Vibration radiation surface 12 Concavity 19, 20 Vibration distribution

Claims (4)

  A bolt-clamped Langevin type vibrator composed of a first metal plate, a second metal plate, a third metal plate, a piezoelectric element and a bolt, wherein the first metal plate has an upper surface portion, a bottom surface portion, and a side surface portion. And the second metal plate is composed of an upper surface portion, a bottom surface portion, and a side surface portion, and the upper surface portion or the central portion of the bottom surface portion is provided with a female screw. And the area of the bottom surface portion of the second metal plate is larger than that of the top surface portion, and the piezoelectric element is a plate shape composed of a top surface portion, a bottom surface portion, and a side surface portion, and is 1 or more. There is a hole in the central portion that is in contact with and sandwiched between the upper surface portion of the plate and the bottom surface portion of the second metal plate, and penetrates from the upper surface portion to the bottom surface portion, and the bolt passes through the hole of the piezoelectric element. , Screwed into the female screw of the first metal plate and the female screw of the second metal plate, and fastened with the first metal plate and the second metal plate The third metal plate includes an upper surface portion, a bottom surface portion, and a side surface portion, and the bottom surface portion of the third metal plate abuts on the upper surface portion of the second metal plate, and the first metal plate And the thickness of the second metal plate plus the thickness of all the piezoelectric elements is one wavelength, and the thickness of the third metal plate is a positive integer multiple of a half wavelength. Bolt-tightened Langevin type vibrator characterized by   2. The bolted Langevin type vibrator according to claim 1, wherein the second metal plate and the third metal plate are integrally molded. 3.   3. The bolted Langevin type vibrator according to claim 1, further comprising a concave portion that circulates in a side surface portion of the third metal plate.   4. The bolt-clamped Langevin type vibrator according to claim 1, wherein the piezoelectric element has two or more and has a fourth metal plate sandwiched between the piezoelectric elements. 5. .

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