TWI317304B - - Google Patents

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TWI317304B
TWI317304B TW95133830A TW95133830A TWI317304B TW I317304 B TWI317304 B TW I317304B TW 95133830 A TW95133830 A TW 95133830A TW 95133830 A TW95133830 A TW 95133830A TW I317304 B TWI317304 B TW I317304B
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Taiwan
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frequency
impedance
ultrasonic
load
vibrator
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TW95133830A
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Chinese (zh)
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TW200714376A (en
Inventor
Saida Itaru
Nunomura Mahito
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Panasonic Elec Works Co Ltd
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Publication of TWI317304B publication Critical patent/TWI317304B/zh

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  • Apparatuses For Generation Of Mechanical Vibrations (AREA)
  • Surgical Instruments (AREA)
  • Orthopedics, Nursing, And Contraception (AREA)
  • Dental Tools And Instruments Or Auxiliary Dental Instruments (AREA)

Description

v 1317304 九、發明說明: 【發明所屬之技術領域】 本發明係有關於能穩定地以目標驅動頻率發生超音波 的超曰波產生裝置及使用該超音波產生裝置的超音波美容 裝置。 【先前技術】 近年來,超音波由於其具有的性質,被應用於促進藥 劑浸透、美容、霧化、乳化、分散、攪拌、清洗、接合、 加工等夕種領域’並開發出了發生超音波的超音波產生裝 置。 圖1 〇及圖11是表示背景技術有關的超音波產生裝置 的、’、。構的圖。圖1 0是將振子接合到喇叭上的超音波產生裝 置,圖11疋使用螺栓將振子固定到喇〇八上的超音波產生裝 置圖1 0及圖11中,(Α )表示整體結構,(β )是八 部分的放大圖。[Technical Field] The present invention relates to an ultrasonic wave generating device capable of stably generating ultrasonic waves at a target driving frequency and an ultrasonic cosmetic device using the ultrasonic generating device. [Prior Art] In recent years, due to its properties, ultrasonic waves have been used to promote the penetration of chemicals, beauty, atomization, emulsification, dispersion, agitation, cleaning, bonding, processing, etc. and to develop ultrasonic waves. Ultrasonic generating device. Fig. 1 and Fig. 11 are diagrams showing an ultrasonic wave generating apparatus according to the background art. Structured map. Fig. 10 is an ultrasonic generating device for joining a vibrator to a horn, and Fig. 11 is an ultrasonic generating device for fixing a vibrator to a slap by using a bolt, Fig. 10 and Fig. 11, (Α) indicates the overall structure, ( β) is an enlarged view of eight parts.

圖10及圖11中,昔旦4士 + > _ 月,Τ、技術有關的超音波產生裝置 50 0Α、500Β結構包括:生成雷柩 王风電振盪的驅動部51丨A、511 β ; 將驅動部511A、511B生成的雷袒、甚姑μ , 取的電振盪轉換成超音波的機械振 盪的超音波振子512A、512B ; Λ甘士 , β,在其中一個接合面513-1Α、 513-1Β上接合超音波振子512Α、时+ 、512Β,將來自超音波振子 512A、512B的超音波的機械振 硒振盪傳輸到另一個放射面 513-2A、513-2B的一種傳輪播姓± 勒構件的喇叭513Α、513Β。 超音波振子512Α、512Β知& .In Fig. 10 and Fig. 11, the structure of the ultrasonic wave generating device 50 Α, 500 Β of the 旦, technology, and the 包括 技术 Β Β 生成 生成 生成 生成 生成 生成 生成 生成 生成 生成 生成 生成 生成 生成 生成 生成 生成 生成 生成 生成 生成 生成 生成 生成 生成 生成 生成 生成 生成 生成 生成 生成 生成 生成 ; The electric oscillations obtained by the driving units 511A and 511B are converted into ultrasonic ultrasonic transducers 512A and 512B of ultrasonic vibrations, and the β, at one of the joint surfaces 513-1Α, 513 -1Β 超 supersonic vibrator 512Α, Hz+, 512Β, the mechanical vibration selenium oscillation of the ultrasonic waves from the ultrasonic vibrators 512A, 512B is transmitted to another radial surface 513-2A, 513-2B The horns of the components are 513 Α and 513 Β. Ultrasonic vibrator 512Α, 512Β知&

和刺队513A、513B的接合類 2014-8318-PF 5 1317304 型大體上可分別a + ^ 一 j為兩類。弟1種接合類型,如圖10(B)The joint type of the squad 513A, 513B 2014-8318-PF 5 1317304 can be roughly two types of a + ^ a j respectively. Brother 1 type of joint, as shown in Figure 10 (B)

所不’超音波振子512A通過粘接劑514A被粘接到喇叭513A 、接口面512 1A上的粘接型。第2種接合類型,如圖工】 (B)所示,由重疊的2個振子5ΐ2_ΐβ構成的超音波振子The ultrasonic vibrator 512A is bonded to the horn 513A and the interface surface 512 1A by the adhesive 514A. The second type of joint, as shown in (B), the ultrasonic vibrator consisting of two overlapping vibrators 5ΐ2_ΐβ

L過累栓51被緊固到喇0八51 3B的接合面51 3-1B 的螺权緊固型。螺栓緊固型中,在螺栓5⑽和超音波振 12B之間、振子512_1B之間、超音波振子和喇口八 51 3B之間’夾緊有導電性薄板51 2-2B。粘接型主要用於數 百咖以上的高頻率型;螺栓緊固型主要用於100kHz以下 低頻率型。 人圖1 2及圖1 3是介紹超音波振盪塊特性的圖。圖丨4是 介紹超音波振i塊的振m模式的圖。圖12是將振子枯㈣The L over-tightening bolt 51 is fastened to the screw fastening type of the joint surface 51 3-1B of the La 0 851 3B. In the bolt fastening type, the conductive thin plates 51 2 - 2B are clamped between the bolt 5 (10) and the ultrasonic vibration 12B, between the vibrator 512_1B, and between the ultrasonic vibrator and the slider 511 3B. The bonding type is mainly used for high frequency type of several hundred or more coffee; the bolt fastening type is mainly used for low frequency type below 100 kHz. Figure 1 2 and Figure 13 are diagrams showing the characteristics of the ultrasonic oscillation block. Figure 4 is a diagram showing the oscillation mode of the ultrasonic vibration block i. Figure 12 is the vibrator dry (four)

喇叭上的超音波產生裝置;圖13是使用螺栓將振子固定到 :刺叭上的超音波產生裝置。s 12⑴、圖13⑴及圖 4(B)是表示超音波振盈塊和超音波振盡的振幅位元相位 置之間關係的圖;® 12(B)、圖13(B)及圖14⑴是 表不超音波振盪塊的阻抗頻率特性的圖,其橫軸為頻率厂 縱轴為顯示常用對數的阻抗z。而且,超音波是縱波,但 = (Α)、圖13(A)及圖14(B)中,出於方便,圖示 為檢波。另外,由於(波長(音速v)/(頻率f), ::?,超音波的波長“因傳播媒質的音速不同而出現變Ultrasonic wave generating device on the horn; Fig. 13 is an ultrasonic generating device for fixing the vibrator to the burr using a bolt. s 12(1), Fig. 13(1), and Fig. 4(B) are graphs showing the relationship between the ultrasonic vibration block and the position of the amplitude bit phase of the ultrasonic vibration; ® 12(B), Fig. 13(B), and Fig. 14(1) are A graph showing the impedance frequency characteristics of the ultrasonic oscillating block, whose horizontal axis is the frequency factory vertical axis is the impedance z showing the common logarithm. Further, the ultrasonic wave is a longitudinal wave, but = (Α), Fig. 13 (A), and Fig. 14 (B) are shown as detection for convenience. In addition, due to (wavelength (sonic v) / (frequency f), ::?, the wavelength of the ultrasonic wave "changes due to the difference in the speed of sound of the propagation medium

由超音波振子512A、512B 件構成的超音波振盪塊5〇1 A 、喇°八513A、513B和接合 501B的尺寸,如圖^(A)The dimensions of the ultrasonic oscillating blocks 5〇1 A , λ° 513A, 513B and the joint 501B composed of the ultrasonic vibrators 512A and 512B are as shown in Fig. 2(A).

2014-8318-PF 6 v1317304 及圖13(A)所示,設計為喇叭513Α、513β的接合面513_1A、 513-1B至放射面513_2A、513_2B之間的厚度u、u (圖 10(B)、圖Π (a))及超音波振盪塊5〇1人、501B的整 體長度L2、L4 (圖1〇 ( A)、圖U ( A)),以便駐波的 波腹位於超音波振盪塊501A、501B的兩端面501_u、 • 501 —2A ( 513-2A) 、5(U-1B、5(U-2B ( 513-2B)。而且, ' 接合到喇n八51、51 3B狀態下的超音波振子51 2A、51 2B, 如圖12(B)及圖13(B)所示,具有針對頻率f的變化, •阻抗z發生變化的固有阻抗頻率特性CA、CB。 該阻抗頻率特性CA、CB,是一種隨著頻率f升高,阻 抗Z變小,在頻率frA、frB下,變成極小ZrA、zrB,之 後’阻抗變大,在頻率faA、faB下,變成極大ZaA、ZaB, 然後再變小的規範。該規範如圖14 ( A )所示,每次振盡 模式時都會重複。該阻抗Z變成極小ZrA、ZrB時的點為諧 振點’阻抗Z變成極大ZaA、ZaB的點為反諧振點。在諧振 修點’由於阻抗Z變成極小ZrA、ZrB,因此,流入超音波振 子512 A、512 B的電流會增加;相反,在反諧振點,由於阻 抗Z變成極大ZaA、ZaB,因此,流入超音波振子5i2A、512B 的電流減小。 如圖14 ( B)所示,粘接型超音波振盪塊5〇ia中的超 音波’設計為駐波的波腹位於其兩端面5 〇 1 — 1 a、5 01 — 2 A (513 — 2A),所以,變為半波長λ/2的整數倍的駐波。 振盛模式表示超音波振盪塊5 〇 1Α中生成的駐波的差異。比 如超θ波振蘯塊5 01A中生成的駐波為半波長的1倍時的2014-8318-PF 6 v1317304 and FIG. 13(A) are designed to have thicknesses u and u between the joint faces 513_1A and 513-1B of the horns 513 Α and 513β to the radiation faces 513_2A and 513_2B (FIG. 10(B), Figure Π (a)) and the ultrasonic wave oscillating block 5 〇 1 person, 501B overall length L2, L4 (Figure 1 〇 (A), Figure U (A)), so that the antinode of the standing wave is located in the ultrasonic oscillation block 501A 501B, both ends 501_u, • 501-2A ( 513-2A), 5 (U-1B, 5 (U-2B ( 513-2B). Moreover, 'extended to the super n51, 51 3B state super As shown in Figs. 12(B) and 13(B), the acoustic transducers 51 2A and 51 2B have inherent impedance frequency characteristics CA and CB which change with respect to the frequency f and the impedance z. The impedance frequency characteristics CA, CB is a type in which the impedance Z becomes smaller as the frequency f increases, and becomes very small ZrA, zrB at the frequencies frA and frB, after which the 'impedance becomes large, and under the frequencies faA and faB, becomes the maximum ZaA, ZaB, and then The specification is reduced as shown in Fig. 14 (A), and is repeated every time the oscillation mode is reached. The point at which the impedance Z becomes extremely small ZrA, ZrB is the resonance point 'The point at which the impedance Z becomes the maximum ZaA, ZaB is Anti-resonance point At the resonance repair point 'Because the impedance Z becomes extremely small ZrA, ZrB, the current flowing into the ultrasonic vibrators 512 A, 512 B increases; on the contrary, at the anti-resonance point, since the impedance Z becomes extremely large ZaA, ZaB, therefore, the inflow The current of the ultrasonic vibrator 5i2A, 512B is reduced. As shown in Fig. 14 (B), the ultrasonic wave in the bonded ultrasonic oscillating block 5〇ia is designed such that the antinode of the standing wave is located at both end faces 5 〇 1 — 1 a, 5 01 — 2 A (513 — 2A), so it becomes a standing wave of an integral multiple of a half wavelength λ/2. The oscillation mode indicates the difference of standing waves generated in the ultrasonic oscillation block 5 〇1Α. When the standing wave generated in the super-theta wave ring block 5 01A is half the half wavelength

2014-8318-PF 7 1317304 振I模式為基本模式,超音 A 0 皮振羞塊501A中生成的駐波為 +波長的3倍時的振盪模式 湯油以一 武為3倍杈式,再有,超音波振 ^塊^中生成的駐波為半波長的5倍時的録模式為5 二核式。此外’圖14通過點接型超音波㈣塊5〇u介紹 :羞模式。對於螺栓緊固型超音波振盤塊MU ,其振盪 才吴式也相同。 、裏超曰波振盈塊5〇1A的接合構件為枯接劑 曰’超音波«塊5〇1B的接合構件為螺检5ΐ4β。另外, 超音波振盪塊5G1A的—個端面5Q1_u是與超音波振子 512A上的剩叭513A接合的面相對的面(不與制叭“Μ接 合的面)’另一端面5(Π-2Α是心⑽的放射面513_2a。 位於超音波振蘆塊5G1B的一個端面5Qhb是與螺栓514B 上的超音波振子512B相接面相對的—面(不與超音波振子 512B相接),另—端面5()卜2β是心5ΐ3β的放射面 513-2B 〇 以上結構的超音波產生裝置500A、500B中,驅動部 11A 511B生成的電振盈ev被施加到超音波振子51 2a、 512B上,通過超音波振子51以、512β被轉換成超音波的 機械振盪,然後被從接合面51 3-1A、513-1B傳輸到喇叭 513A、513B ;然後,從喇队513Α、513β的放射面513_2a、2014-8318-PF 7 1317304 The vibration mode is the basic mode, and the oscillation mode of the supersonic A 0 skin shivering block 501A is 3 times the + wavelength. Yes, the recording mode when the standing wave generated in the ultrasonic vibration block is 5 times the half wavelength is 5 binary mode. In addition, Figure 14 is introduced by the point-contact type ultrasonic (four) block 5〇u: shy mode. For the bolt-on type ultrasonic diaphragm block MU, the oscillation is the same. The joint member of the 曰 super-wave vibrating block 5〇1A is the abutting agent 曰' Ultrasonic «The joint member of the block 5〇1B is a screw test 5ΐ4β. Further, the end surface 5Q1_u of the ultrasonic oscillation block 5G1A is a surface opposite to the surface joined to the remaining horn 513A on the ultrasonic vibrator 512A (the surface not joined to the slap ")"), and the other end surface 5 (Π-2Α is The radiating surface 513_2a of the core (10). One end surface 5Qhb of the ultrasonic vibrating reed 5G1B is a surface opposite to the surface of the ultrasonic vibrator 512B on the bolt 514B (not connected to the ultrasonic vibrator 512B), and the other end surface 5 (2) The ultrasonic vibration ev generated by the drive unit 11A 511B is applied to the ultrasonic transducers 51 2a and 512B, and the ultrasonic vibration ev generated by the drive unit 11A 511B is applied to the supersonic wave generating devices 500A and 500B having the above-described structure. The acoustic vibrator 51 is converted into a mechanical oscillation of the ultrasonic wave by 512β, and then transmitted from the joint faces 51 3-1A, 513-1B to the horns 513A, 513B; and then, from the radiating surface 513_2a of the squad 513 Α, 513β,

513 2B上發射出超音波的機械振盪。上述藥劑滲透促進及 美谷專細以超音波處理的物件〇直接或通過水、朦滯體等 超音波傳播媒介接觸喇叭513A、513B的放射面513-2A、 513 2B ’放射面513-2A、513-2B放射出的超音波被傳輸到 2014-8318-PF 8513 2B emits a mechanical oscillation of the ultrasonic wave. The above-mentioned agent permeation promotion and the ultra-sonic processing of the object, the radiation surface 513-2A, 513 2B 'radiation surface 513-2A of the horns 513A, 513B are directly or through the ultrasonic propagation medium such as water or stagnation. The ultrasonic wave emitted by 513-2B is transmitted to 2014-8318-PF 8

V 1317304 物件物ο ’用於超音波處理。 然後’如圖12(Β)及圖13⑻所示,超音波振盪塊 501A、501Β以諧振點至反讀振點之間的振堡範圍證、腿 中某一頻率f,如驅動頻率fdA、fdB控制超音波產生裝置 500A、500B,使盆進杆拍立'士把、基 便-進仃超曰波振盪。該超音波產生裝置 白_的控制方法有,自激«方式和他激振盈方式。 自激振盛方式,是指通過將超音波振子5m、5i2B的頻率 貝J駆動。p 511A、511B,以目標驅動頻率fdA、f =Γ5、:1Β生成的_EV進行調整,使超音波 12B振動的方式。他激振盤方式,是指預先對 1Τ=:Α、511β進行設定’使得超音波振子5m、5ΐ2β 成目“區動頻率fdA、⑽振盪的電振盪EV 。 所述自激振盪方式及他激振盪方 》 號公報f糞刺令把7、 在如特開2002-2491 53 ^報(專利文獻U及特開1 999_114 文獻2)中已有說明。 就A報(專利 但是,由於在自激振盪方式 的阻抗Z來檢測超音波振子的頻率卜=測,音波振子 標驅動頻率則《模式不同的㈣模式t在=含有目 動部的電振堡EV作出調整’因此 了此會對驅 會存在超音波振子以不同於目標驅動振中,可能 誤的頻率,)進行摄蓋的情況。另外的頻率f (錯 因此,自激振盪方式中可能# ;疋自激振盪, 在恒定的水平。而且,的輪_ 因此,自激垢湯士 4 勒出控制到恒定水平, … 適用於輸出較低阻抗Z的兆赫波段V 1317304 Object ο ' for ultrasonic processing. Then, as shown in Fig. 12 (Β) and Fig. 13 (8), the ultrasonic oscillating blocks 501A, 501 Β are in the range of the vibration range from the resonance point to the anti-reading vibration point, a certain frequency f in the leg, such as the driving frequency fdA, fdB The ultrasonic generating devices 500A and 500B are controlled to make the bowls erect, and the cymbals are erected. The method of controlling the ultrasonic generating device white_ has a self-excited mode and a mode of vibration. The self-excited vibration mode means that the frequency of the ultrasonic vibrators 5m and 5i2B is shifted. p 511A and 511B are modes in which the _EV generated by the target drive frequencies fdA, f = Γ5, and 1Β are adjusted to vibrate the ultrasonic wave 12B. In the case of the excitation mode, the electric oscillation EV is set such that the ultrasonic oscillators 5m and 5ΐ2β are caused to oscillate by the oscillations of the ultrasonic transducers 5m and 5ΐ2β. The oscillating side bulletin f sputum spurs 7 has been described in, for example, JP-A-2002-2491 53 (Patent Document U and JP-A-1999-114 Document 2). The impedance Z of the oscillating mode is used to detect the frequency of the ultrasonic vibrator. The sound frequency of the ultrasonic vibrator is “the mode of the (4) mode t is adjusted in the electric shock EV containing the moving part. Therefore, this will drive the meeting. There is a case where the ultrasonic vibrator is different from the target driving vibration, which may be erroneous.) The other frequency f (wrong, therefore, the self-oscillation mode may be #; 疋 self-oscillation, at a constant level. Moreover, the wheel _ therefore, the self-priming soup 4 is controlled to a constant level, ... suitable for outputting the lower impedance Z megahertz band

2014-8318-PF 9 1317304 的超音波產生裝置。 另-方面,他激振逢方式下,由於受周圍環境變 超音波振子自身發熱等引起的溫度變化等的作用,超Ultrasonic generator for 2014-8318-PF 9 1317304. On the other hand, he is excited by the temperature change caused by the surrounding environment changing the ultrasonic oscillator itself, etc.

振子的輸出特性會出現變化,因此,他激振盪方式中X 使以目標驅動頻率fd使超音波振子進行㈣,也 ^ 目標輸出。 判 而且,由於受周圍環境變化及超音波振子自身發 引起的溫度變化及外部應力等引起的老化等作用,气 率fr及反譜振頻率ia出現移頻的情況較多,因此,自^ 振盧方式下會出現超音波振子以不同於目標驅動頻率 的頻率f振盈,以及他激振盈方式下輸出會出現變化 況’問題比較嚴重。特別是,在以兆赫以上的頻率進行= 出的超音波產生步罟φ,μμ L , m 生展置中it如,由於使用3倍模式及 模式等較高模式,因此’上述問題會變得更嚴重。 。 【發明内容】 本發明繁於以上問題,目的在於提供—種能夠以 驅動頻率穩定地發生超音波的超音波產生裝置。另外 供一種使用該超音波產生裝置的超音波美容裝置。 本發明的超音波產生裝置,包括··生成電振i的驅動 部,將上述驅動部生成的上述電振盈轉換成超音波 振 的超音 -Z- . jlrn T- I LA Λ 、立θ /皮振子,一個面上接合上述超音波振子,將上The output characteristics of the vibrator will change. Therefore, in the excitation mode, X causes the ultrasonic oscillator to perform (4) and ^ target output at the target drive frequency fd. In addition, due to changes in the surrounding environment and temperature changes caused by the ultrasonic transducer itself, and aging caused by external stress, etc., the gas rate fr and the anti-spectral frequency ia are frequently shifted, so the self-vibration In the Lu mode, there will be a supersonic oscillator with a frequency f different from the target driving frequency, and the output will change when he is excited. The problem is more serious. In particular, in the case of megahertz or higher, the ultrasonic generation step φ, μμ L , m is in the middle of the display, and since the higher mode such as the 3x mode and the mode is used, the above problem becomes more serious. . SUMMARY OF THE INVENTION The present invention has been made in view of the above problems, and an object thereof is to provide an ultrasonic generating device capable of stably generating ultrasonic waves at a driving frequency. Further, an ultrasonic cosmetic device using the ultrasonic generating device is provided. The ultrasonic generating device according to the present invention includes: a driving unit that generates the electric vibration i, and converts the electric vibration generated by the driving unit into a supersonic-Z- of the ultrasonic vibration. jlrn T- I LA Λ , 立 θ /Pi Zhenzi, one surface of the above-mentioned ultrasonic vibrator, will be on

述超音波振子轉換的上述超音波的機械振堡傳輸到另〜個 面放射面的傳輪構件;測定上述超音波振子阻抗的剛定 2014-8318-PF ‘ 1317304 部;基於應傳輸上述超音波的機械振盪的對象物接觸上述 傳輸構件的負載時上述超音波振子的阻抗頻率特性和應傳 輸上述超音波的機械振盪的物件物不接觸上述傳輸構件的 無負載時上述超音波振子的阻抗頻率特性的交點上的阻抗 以及上述測定部測定的阻抗,計算應驅動上述超音波振子 的目標驅動頻率,控制上述驅動部,使得上述超音波振子 以该計算出的目標驅動頻率振盪的控制部。此外,本發明 的超曰波美容裝置使用上述超音波產生裝置。 X上”Ό構的超音波產生裝置及超音波美容裝置能夠以 目標‘驅動頻率穩定地發生超音波。^,超音波產生裝置 =有效地對物件物實施超音波處理。另外,超音波美容 裝置旎夠有效地對物件物給予美容效果。 【實施方式】The mechanical vibration of the ultrasonic wave converted by the ultrasonic oscillator is transmitted to another transmitting member of the surface of the surface; the impedance of the ultrasonic transducer is determined to be 2014-8318-PF ' 1317304; the ultrasonic wave is transmitted based on The impedance frequency characteristic of the ultrasonic vibrator when the object of the mechanical oscillation is in contact with the load of the transmission member, and the impedance frequency characteristic of the ultrasonic vibrator when the object to be transmitted by the mechanical oscillation of the ultrasonic wave does not contact the transmission member The impedance at the intersection and the impedance measured by the measuring unit are calculated as a control unit that controls the target drive frequency of the ultrasonic transducer to control the drive unit so that the ultrasonic transducer oscillates at the calculated target drive frequency. Further, the super-wave cosmetic apparatus of the present invention uses the above-described ultrasonic generating apparatus. The ultrasonic generating device and the ultrasonic cosmetic device on the X can stably generate ultrasonic waves at the target 'drive frequency. ^, Ultrasonic generating device = effectively performing ultrasonic processing on the object. In addition, the ultrasonic cosmetic device It is effective enough to give a cosmetic effect to the object.

下面,基於附圖介紹本發 附圖中使用相同符號的結構表 行介紹。 明有關的實施例。此外,各 示其結構相同,在此不再進 首先’ 紹本發明的其士达 本情況的圖。圖!⑴表:::況。® 1是介紹本發明基 卜縱轴為顯示常㈣㈣頻=性,其料為頻率 阻==不:觸傳輪構件的無負載時超音波振子的 〇接觸傳輸構件的負超音波機械振盪的對象物 ⑷表示無負载料合到的阻抗頻率特性。圖1 專傳輸構件狀態下的超音波In the following, the description of the structure table using the same symbols in the drawings will be described based on the drawings. The relevant embodiments are described. Further, the structures are the same, and the drawings of the case of the present invention are not described here. Figure! (1) Table::: Condition. ® 1 is the introduction of the basic axis of the present invention to show the usual (four) (four) frequency = sex, which is the frequency resistance == no: the negative ultrasonic mechanical oscillation of the 〇 contact transmission member of the ultrasonic oscillator when the carrier member is unloaded The object (4) represents the impedance frequency characteristic to which no load is applied. Figure 1 Ultrasonic wave in the state of the transmission component

2014-8318-PF 11 1317304 2子的等價電路;圖1(〇表示負載時接合_等傳輸 構件狀態下的超音波振子的等價電路。 如圖1 (A)所示,無負載時的阻抗頻率特性c壯,是 :旨在某振動模式中,如背景技術中介紹的那樣,隨著頻率 :二,阻抗Z變小,在頻率圩時,變成最小Zr卜之後 變大’在頻率fa時,變成畏士 r 曼成最大Zal ’然後’再次變小的規 他。而且,負載時阻抗頻率特性⑽規範大致與益負载時 :抗頻率特性⑽相同。但有負載時阻抗頻率特性CL中的 最^抗zr2比無負載時阻抗頻率特性肌中的最小阻抗 二#二且1負載時阻抗頻率特性CL中的最大阻抗Za2 L阻抗頻率特性CNL中最大阻抗如變小。 圖1(B)*(C)分別所示,無負载情況下,接人 到傳輸構件狀態下的超音波振接σ 並聯連接到串聯連接的線^、電容H路疋將電谷器C2 电办器Cl及電阻W μ 的電路;有負載情況下’接合到傳輸元件 ° 振子的等僧雷政3 下的超音波 振子的“電路疋指將電容器C2 線圈L、電容…電阻…的電路 與無負載時相比,相當於物件物〇接觸傳、、 電阻的電阻器R2還被串聯連接到電阻器以上、、的 因二::頻率特性中無負载時的最 在有負載的情況下, 抗 最小頻率fi·至最大頻率 斤述。而且,在 的阻抗頻率特性和有負二間的振盪範圍内’無負载時 相交。 負載時的阻抗頻率特性在-個點P處2014-8318-PF 11 1317304 2 equivalent circuit; Figure 1 (〇 shows the equivalent circuit of the ultrasonic oscillator in the state of the transmission member such as the joint _ during load. As shown in Fig. 1 (A), when there is no load The impedance frequency characteristic c is strong: it is intended to be in a certain vibration mode, as described in the background art, with the frequency: two, the impedance Z becomes smaller, and at the frequency 圩, becomes the minimum Zr and becomes larger after the frequency fa At the time, it becomes the maximum Zal 'then' and then becomes smaller again. Moreover, the impedance frequency characteristic (10) of the load is roughly the same as the load-resistance: the anti-frequency characteristic (10), but the impedance frequency characteristic CL in the load The most resistance to zr2 is the minimum impedance in the muscle when there is no load. The minimum impedance in the muscle is #2 and the maximum impedance in the impedance frequency characteristic CL is the load impedance CL2. The maximum impedance in the CNL is reduced. Figure 1(B) *(C) respectively, under no load, the ultrasonic vibration connection σ connected to the transmission member is connected in parallel to the series connected line ^, the capacitor H path, the electric grid C2 electric device Cl and the resistor W μ circuit; 'bonded to the transmission element under load°° The circuit of the ultrasonic oscillator under the Lei Zheng 3 of the sub-equipment refers to the circuit of the capacitor C2 coil L, capacitor...resistor...the resistor R2 corresponding to the object contact and the resistance. It is also connected in series to the resistor, and the second:: the frequency characteristic is the most load-free, the minimum frequency fi· to the maximum frequency, and the impedance frequency characteristics and In the range of the negative two oscillations, 'intersection without load. The impedance frequency characteristic at load is at - point P

2014-8318-PF 12 1317304 無負載時的阻抗頻率特性和有負載時的阻抗頻率特 性在一點P處相交,背景技術介紹的專利文獻i中也有記 載,但這裏發明人發現,即使是施加到傳輸構件上的負載 的作用情況發生變化,只有電阻器R2的電阻大小發生變 化,因此,無負載時的阻抗頻率特性和有負載時的阻抗頻 率特性時常在一個點p處相交’而且,交點P的頻率和 阻抗Zm不變。而且’本發明的一種實施例有關的超音波產 生裝置及使用該產生裝置的超音波美容裝置包括:以該盈 負載時的阻抗頻率特性和有負載時的阻抗頻率特性的交點 p為基準,確定應對超音波振子進行驅動的目標驅動頻率 η的控制部。上述超音波產生裝置及使用了該產生裝置的 =音波美容裝置能夠以目標驅動頻率定地發生超音 (實施例的結構) 圖2是表示實施例有關的超音波產生裝置的結構的方 框圖。圖2中,超音波產生裝置包括:驅動部u、超音波 振子12 K 13、測定部14、控制部15和存餘部。 .¾動部11是生成驅動超音波振子12的電振堡的部 件。驅動部H,比如,包括發生正弦波等特定頻率的交流 ^的振盛電路113和以特定放大率對交流信號進行放大 的放大電路U2。振盪電路113能夠利用科爾皮兹振蘯電 路及哈托萊式振盪電路等眾所周知的振蓋電路。但從能夠 很容易地更改振盪頻率的觀點看,本實施例中,比如,是 使用了 PLL (phase lQcked 1〇〇p)電路的頻率合成器。頻2014-8318-PF 12 1317304 The impedance frequency characteristic at no load and the impedance frequency characteristic at the time of load intersect at a point P, which is also described in the patent document i of the background art, but the inventors here find that even the application to the transmission The action of the load on the component changes, and only the resistance of the resistor R2 changes. Therefore, the impedance frequency characteristic at no load and the impedance frequency characteristic at the time of load often intersect at a point p' and the intersection point P The frequency and impedance Zm are unchanged. Further, the ultrasonic generating device according to an embodiment of the present invention and the ultrasonic cosmetic device using the same include: determining the intersection frequency p of the impedance frequency characteristic at the time of the load and the impedance frequency characteristic at the time of the load as a reference A control unit for the target drive frequency η that drives the ultrasonic oscillator. The above-described ultrasonic generating device and the ?-sound wave cosmetic device using the same can generate a supersonic sound at a target driving frequency (Configuration of the embodiment) Fig. 2 is a block diagram showing the configuration of the ultrasonic generating device according to the embodiment. In Fig. 2, the ultrasonic generating device includes a driving unit u, an ultrasonic transducer 12 K 13 , a measuring unit 14, a control unit 15, and a spare unit. The movable portion 11 is a component that generates an electric shock train that drives the ultrasonic vibrator 12. The drive unit H includes, for example, a vibrating circuit 113 that generates an alternating current of a specific frequency such as a sine wave, and an amplifying circuit U2 that amplifies the alternating current signal at a specific amplification factor. The oscillation circuit 113 can utilize a well-known vibrating circuit such as a Colpitz vibrating circuit and a Hartley-type oscillating circuit. However, from the viewpoint of being able to easily change the oscillation frequency, in the present embodiment, for example, a frequency synthesizer using a PLL (phase lQcked 1〇〇p) circuit. frequency

2014-8318-PF 13 1317304 率合成器,比如,包括基準 波器、電壓控制振盪器和… 位相比較器、低通濾、 令,電壓控制振盪器的輸出, 貝手《成益 之後被轉換成特定的頻率, 貝次倍私 F對八…“ 到位相比較器。位相比較 ^ # , .... 羞斋的輸出的位相進行比較, …… 低通濾波益。低通濾波器基於位相比2014-8318-PF 13 1317304 rate synthesizer, for example, including reference wave, voltage controlled oscillator and... phase comparator, low pass filter, command, voltage controlled oscillator output, beibei The specific frequency, Beibei times private F to eight..." In-phase comparator. Phase comparison ^ #, .... Comparison of the phase of the output of the shy, ... low-pass filter benefits. Low-pass filter based on bit

二:,出生成修正值電應,輸出到電麼控制振蘆器。接 者1壓控制振^根據修正值電壓改變振㈣率,使分 頻後的頻率和基準振盪器的 苗“ 盈益的頻率-致。頻率合成器,通過 刀頻或倍增的分頻器的倍率來獲得想得到的頻率。 超音波振子12是將通過敎部14從驅動#ιι傳來的 電振盪轉換成超音波的機械振盪的部件。比如,通過電極 夹住水晶#壓電材料這種結構的壓電振子。tA 13是一個 面接合有超音波振+ 12,將超音波振子12發生的超音波 的機械振盪傳輸到另—面的放射面的部件,是-種傳輸構 件0 起曰波振子1 2、味卜八13和符合接合類型的接合構件 (圖中未標注)構成超音波振錢2,與背景技術中介紹 的圖10及圖11所示的部件相同。枯著類型中,如圖1〇所 不,喇叭51 3A是呈短高有底的圓筒狀的,如鋁及輕合金等 =金屬構件。比如,’水晶振子等的超音波振子5m通過魅 著劑514A被粘著到喇叭513A的内底面上,進行固定。螺 栓緊固型中,如圖丨丨所示,喇叭5丨3β是朝向放射面—側, 呈尖端細的圓錐梯形的,比如鋁及輕合金等的金屬構件。Two:, the generation of the correction value should be output, and the output to the electric control of the vibrator. The receiver 1 voltage control vibration ^ according to the correction value voltage changes the vibration (four) rate, so that the frequency after the frequency division and the reference oscillator's seedling "profit frequency - the frequency synthesizer, through the knife frequency or multiplication of the frequency divider The frequency is obtained by the magnification. The ultrasonic vibrator 12 is a component that converts the electrical oscillation transmitted from the drive #ιι into the ultrasonic vibration by the cymbal 14. For example, the structure of the piezoelectric material is sandwiched by the electrode. The piezoelectric vibrator. tA 13 is a member in which a supersonic vibration + 12 is superimposed on the surface, and the mechanical oscillation of the ultrasonic wave generated by the ultrasonic vibrator 12 is transmitted to the radiating surface of the other surface, and the transmission member 0 is chopped. The vibrator 1 2, the taste plate 8 and the joint member (not shown) conforming to the joint type constitute the ultrasonic vibration 2, which is the same as the components shown in Figs. 10 and 11 introduced in the background art. As shown in Fig. 1, the horn 51 3A is a short, high-bottomed cylindrical shape, such as aluminum and light alloys, etc. = metal members. For example, the ultrasonic vibrator 5m of the crystal vibrator is viscous by the charm agent 514A. On the inner bottom surface of the horn 513A, and solidify . Fastening bolt type, as shown in Shu Shu, Shu 3β horn 5 towards the radiation surface - the side, a conical shape tapering trapezoidal shape, such as a metal member like aluminum and light alloy.

2014-8318-PF 14 1317304 在大直徑的接合面的接近中間的位置内部面對放射面一侧 形成用於連接螺栓514B的螺絲槽。由接近中央位置存在貫 通孔的多個(圖1 1中是2個)括工cn 個)振子512-1B重疊形成的超 音波振子512B通過貫通孔,力并λ从加 札在插入的螺栓514Β的作用下, 被連接到喇叭51 3Β上,進杆囡令 二 遲仃固疋。而且,在螺栓514Β和 超音波振子512Β之間、各振子5彳?〗 娠于bl2~1B之間、超音波振子 51 2B和喇叭51 3B之間,分別冰豎古道雨 刀別夾緊有導電性薄板512-2B。 枯接型,適合用於如發生兆絲2014-8318-PF 14 1317304 A screw groove for connecting the bolt 514B is formed on the side facing the radiation surface at a position close to the middle of the large-diameter joint surface. The ultrasonic vibrator 512B formed by the overlap of the plurality of vibrators 512-1B in which the through holes are present near the center position (through the cn in FIG. 1) passes through the through holes, and the force λ is pulled from the inserted bolts 514. Under the action, it is connected to the speaker 51 3Β, and the entry is delayed. Further, between the bolt 514 Β and the ultrasonic vibrator 512 、, each of the vibrators 5 彳? 〗 Pregnancy between bl2~1B, between the ultrasonic vibrator 51 2B and the horn 51 3B, respectively, the ice plate is clamped with a conductive sheet 512-2B. Dry type, suitable for use in the occurrence of

戈土死称波#又#數百kHz以上的高頻 率超音波的超音波產生裝置,由 田於疋间頻率,所以,適合 用於如美容、清洗粒子及霧化等 粉儿寻用述。另一方面,螺栓緊 固型’適合用於如發生千赫、、古 诚土丁鄉疚奴4的l〇0kHz以下的低頻率 超音波的超音波產生裝置,由於是低頻率,所以,適合用 於如斷開、接合、分散、液體噴霧等用途。 〜敎部14是測定超音波振子12的阻抗z的部件。測 _ 比如匕括具備檢測超音波振子12 _ f流的檢測 電阻器等的電流檢測電路⑷、通過控制振i電路ιΐ3的 ,盪頻率來控制來自驅動部i i #電振盪頻率的頻率控制 _從頻率控制部j 4 3接收驅動部】工的電振盪頻率通 知,同時基於電流檢測電路141通知的檢測電流值,對收 J頻率控制部143發出通知的頻率中的阻抗z進行運算的 阻抗運算部14 2。 控制部15,是基於應傳輸超音波的機械振盈的對象物 (圖中未標出)接觸^ 13的貞載狀態下超音波振子Μ 、柷頻率特性和應傳輸超音波的機械振盪的物件物〇不It is suitable for use in such as beauty, cleaning particles and atomization. On the other hand, the bolt-on type is suitable for use in ultrasonic generating devices of low-frequency ultrasonic waves such as kilohertz and Gucheng Tudingxiangnu 4, which are low frequency, so it is suitable for low frequency. For applications such as breaking, joining, dispersing, liquid spray, etc. The dam portion 14 is a member that measures the impedance z of the ultrasonic vibrator 12. The measurement _ includes, for example, a current detecting circuit (4) having a detecting resistor for detecting the supersonic vibrator 12 _ f flow, and controlling the frequency control from the driving portion ii # electric oscillating frequency by controlling the oscillating frequency of the oscillating circuit i _ 3 The frequency control unit j 4 3 receives the electric oscillation frequency notification of the drive unit and the impedance calculation unit that calculates the impedance z at the frequency notified by the J-frequency control unit 143 based on the detected current value notified by the current detection circuit 141. 14 2. The control unit 15 is an object that is based on the mechanical vibration of the ultrasonic wave (not shown) and the ultrasonic oscillator Μ in the load state, the frequency characteristic of the 和, and the mechanical oscillation of the ultrasonic wave to be transmitted. Object not

2〇14-8318^PF 15 1317304 接觸喇叭13的無負载狀 性交點P的阻抗z及測定二波振”2的阻抗頻率特 ^ ,, m w ^ 邛14測定到的阻抗Z ,如後面介 ^ ^ -+ α, Λ. , /皮振子12的目標驅動頻率fd, 以3亥叶鼻出的目標驅動頻 振子12垢i π ,控制驅動部11,使超音波 電”: 控制部15,比如包括頻率運算部15〗、 控制°"52和驅動頻率控制部153。 該負載狀態下的超音、、古 g 4s jk / 、子12的阻抗頻率特性和益 負载狀態下的超音波振子 k Zm ’在本實施例中, ^ 1〇 過事先對上述負载狀態中的超音 波振子12的阻抗頻率特 1 2的阳> a 寻生和無負載狀態中的超音波振子 12的阻抗頻率特性進行 贫于 、十-i 夏不’則疋,利用該測定結果計算上 述阻抗頻率特性的交點p, T异上 生F詈1 Φ . 仃事先计箅,用於超音波產 収立U 際測定的超音波振子12最好是已組裝 到超音波產生裝置丨中 衣 的超音波耜湯μ 〇 貫物,但也可以是與實物同規格 产 二4。另外’為保證交點Ρ的阻抗Zm計算精 是利用多個同規格的超音波議2使用平 先法進行統計上的計算。如上所述,由於事 生穿f 乂’』p的阻杬Zm,因此能夠以適合該超音波產 f1的目標驅動頻率…穩定在發生超音波。 率料:二率運算部151基於有負载時超音波振子12的阻抗頻 =寺生和無負载時超音波振子12的阻抗 的阻抗“以及測定部14 :二:點p 波振子12的目標驅動頻率fd,、广D r ’超音 it ^ m ^ -¾ t* + ,將异出的目標驅動頻率Μ 化動頻率控制部153。2〇14-8318^PF 15 1317304 The impedance z of the unloaded intersection P of the contact horn 13 and the impedance frequency of the two-wave vibration "2", mw ^ 邛14 measured impedance Z, as described later ^ ^ - + α, Λ. , / The target drive frequency fd of the pico-brain 12, the target drive frequency element 12 scale i π with 3 hay nose, control the drive unit 11 to make the ultrasonic electricity": the control unit 15, for example The frequency calculation unit 15 and the control unit " 52 and the drive frequency control unit 153 are included. In the load state, the supersonic, the ancient g 4s jk / , the impedance frequency characteristic of the sub 12 and the ultrasonic vibrator k Zm ' in the load state are in the present embodiment, The impedance frequency of the ultrasonic vibrator 12 is 1 >2> a The impedance frequency characteristics of the ultrasonic vibrator 12 in the state of no-load and no-load are depleted, and the result is calculated by using the measurement result. The intersection point p of the impedance frequency characteristic, T is different from the upper generation F詈1 Φ. 仃 In advance, the ultrasonic vibrator 12 for ultrasonic measurement is preferably assembled into the ultrasonic generating device. Ultrasonic soup is a sputum, but it can also be produced in the same specifications as the real product. In addition, the calculation of the impedance Zm for ensuring the intersection point is statistically calculated using a plurality of ultrasonic waves of the same specification. As described above, since the resistance Zm of the f 乂' 』p is generated, it is possible to stabilize the supersonic wave with the target driving frequency suitable for the ultrasonic generation f1. Rate: The second-rate calculation unit 151 is based on the impedance frequency of the ultrasonic vibrator 12 when there is a load = the impedance of the impedance of the ultrasonic vibrator 12 at the time of the temple and the no-load, and the target drive of the measurement unit 14: two: point p-wave oscillator 12 The frequency fd, the width D r 'supersonic it ^ m ^ -3⁄4 t* + , and the target drive frequency of the difference Μ are subjected to the frequency control unit 153.

2014-8318-PF 16 '1317304 电壓控制部1 52是通過控 控制驅動部"…a 電路112的放大率來 在趙立、 、雨出電麼的部件。驅動頻率控制部1 53是 :波產生裝置!的通常使用狀態了,通過以頻率 頻 運算出的目標驅動頻㈣控制振I電路113的振盈 12据叙1制來自驅動冑11❸電振盈頻帛,使超音波振子 i Z振動的部件。 曾立此時,上述阻抗運算部142、頻率控制部143、頻率運 r IM 5卜電壓控制部i 52及驅動頻率控制部⑸,比如包 括微處理器及其周邊電路等(以下稱“_,,),從功能上 構成上述各部件。存儲部! 6是存儲為了運算目標驅動頻率 而對超曰波產生裝置1的各部進行控制的目標驅動頻率 =算程式及在超音波產生裝4!的通f使用狀態下控制超 、產生哀置1各部的控制程式等各種程式、以及測定部 14測出的阻彳几z、測定該阻抗z時的頻率f、各種程式運 行所而的=貝料、運行過程中生成的資料等各種資料的部 件。存儲部1 6,比如包括成為上述MPU的所謂工作記憶體2014-8318-PF 16 '1317304 The voltage control unit 1 52 is a component that controls the drive unit "...a circuit 112 to increase the power in the battery. The drive frequency control unit 1 53 is: a wave generating device! In the normal use state, the vibration of the vibration I circuit 113 is controlled by the target drive frequency (4) calculated at the frequency frequency. 12 The component that drives the 振11❸ electric oscillation frequency 帛 to vibrate the ultrasonic vibrator i Z is described. At this time, the impedance calculation unit 142, the frequency control unit 143, the frequency operation unit, the voltage control unit i52, and the drive frequency control unit (5) include, for example, a microprocessor and its peripheral circuits (hereinafter referred to as "_," The storage unit is configured to store the target drive frequency = calculation program and the ultrasonic generation device 4! for controlling the respective components of the super-hybrid wave generating device 1 in order to calculate the target drive frequency. Various programs such as a control program for controlling the super-use and generating a part of the singularity, and a number of z, which are measured by the measuring unit 14, a frequency f when the impedance z is measured, and a program for operating the various types of the program a component of various materials such as data generated during operation, and the storage unit 1 6 includes, for example, a so-called working memory that becomes the MPU described above.

的 RAM( Random Access Memory )等揮發性記憶元件、EEpR〇M (Electrically Erasable Programmable Read OnlyVolatile memory components such as RAM (Random Access Memory), EEpR〇M (Electrically Erasable Programmable Read Only)

Mem〇ry)等可讀寫非揮發性記憶元件以及ROM ( Read Only Memory)等非揮發性記憶元件等。 下面介紹本實施例的運作。 圖3是表示實施例有關的超音波產生裝置的目標驅動 頻率運算處理中動作的流程圖。圖4是介紹目標驅動頻率 的圖。圖4的橫軸為頻率f,縱軸為常用對數顯示的阻抗z。Mem〇ry) and other non-volatile memory elements such as readable and writable non-volatile memory elements and ROM (Read Only Memory). The operation of this embodiment will be described below. Fig. 3 is a flowchart showing the operation of the target drive frequency calculation processing of the ultrasonic generating device according to the embodiment. Figure 4 is a diagram showing the target drive frequency. The horizontal axis of Fig. 4 is the frequency f, and the vertical axis is the impedance z of the common logarithm.

2014-8318-PF 17 1317304 表:無負載時的阻抗頻率特性;一點鏈線表示有負載 夺的阻抗頻率特性。 、 向超音波產生裝置i供電的電源開關(圖 矛使超音波產生裝置開始超音波發生動# μ # ^ 中 &曰^動作的起動開關(圖 ^ )安裝在超音波產生裝置1±。比如,打開該電 向超音波產生裝置1供電’則運行目標驅動頻率 運算始執行運算目標驅動頻率㈣目標驅動頻率 圖3中,控制部15的電壓控制部152通過調整放大電 路⑴的放大率,將驅動部11要輸出的交流信號的電壓大 小设定成用於目標驅動頻率運算處理的數值,將電壓設定 結:通知頻率控制部143(su)。該目標驅動頻率運;所 =討任意大小’但採用的電壓值能保證運行目標驅動 頻率運f處理時所需功率較小,而且,能夠得到以要求的 精度運鼻目標I®動頻率fd的阻抗ζ。該電壓值,比如,在 本實施例中,可根據阻抗運算部142在後述的處理S13中 測定的電流很容易運算出阻抗,因此,交流信號的最大峰 值時的電壓值為lv,最小峰值時的電壓值為—1¥的lvp_p。 在電壓控制部152通知電壓設定結束時,測定部14的 頻率_ 143通過調整振盪電路113的頻率,即本實施 例中調整分頻器的倍率,在應測定阻抗Z的頻率範圍中特 定頻率f中設定驅動部n輸出的交流信號的頻率f,將窄 設定頻率f及頻率f的設定結束資訊通知阻抗運算; (S12)。2014-8318-PF 17 1317304 Table: Impedance frequency characteristics at no load; a little chain line indicates the impedance frequency characteristics of the load. The power switch that supplies power to the ultrasonic generating device i (the spear causes the ultrasonic generating device to start the ultrasonic generating action # μ # ^ and the start switch (Fig. 2) of the operation of the ultrasonic device is mounted on the ultrasonic generating device 1±. For example, when the electric power is turned on to the ultrasonic generating device 1, the operation target driving frequency is calculated and the operation target driving frequency is executed. (4) Target driving frequency. In FIG. 3, the voltage control unit 152 of the control unit 15 adjusts the amplification factor of the amplifying circuit (1). The voltage level of the AC signal to be outputted by the drive unit 11 is set to a value for the target drive frequency calculation process, and the voltage setting is notified to the frequency control unit 143 (su). The target drive frequency is transmitted; 'But the voltage value used can ensure that the power required for the operation of the target drive frequency is small, and the impedance of the target I® dynamic frequency fd can be obtained with the required accuracy. For example, in this In the embodiment, the impedance can be easily calculated from the current measured by the impedance calculation unit 142 in the processing S13 to be described later. Therefore, the voltage at the maximum peak value of the AC signal can be obtained. In the case of lv, the voltage value at the minimum peak value is lvp_p of -1¥. When the voltage control unit 152 notifies that the voltage setting is completed, the frequency _143 of the measuring unit 14 adjusts the frequency of the oscillation circuit 113, that is, the frequency division in the present embodiment. In the magnification of the device, the frequency f of the AC signal output from the drive unit n is set in the specific frequency f in the frequency range in which the impedance Z is to be measured, and the impedance calculation is performed on the setting end information of the narrow set frequency f and the frequency f (S12).

2014-8318-PF 18 1317304 上述設定結束後,與設定相應的電壓及頻率f的交流 4號經測定部14的電流檢測電路141,從驅動部u被輸 出到超音波振子12。 測定部14的電流檢測電路141以實效值測定驅動部 U流向超音波振子12的電流,將測定的電流通知阻抗運 算部 142 ( S13)。 、測定部14的阻抗運算部142在收到電流檢測電路1412014-8318-PF 18 1317304 After the above-described setting is completed, the current detecting circuit 141 of the measuring unit 14 of the AC No. 4 corresponding to the set voltage and frequency f is output from the driving unit u to the ultrasonic vibrator 12. The current detecting circuit 141 of the measuring unit 14 measures the current flowing from the driving unit U to the ultrasonic transducer 12 by the effective value, and notifies the impedance calculating unit 142 of the measured current (S13). The impedance calculation unit 142 of the measurement unit 14 receives the current detection circuit 141.

通知的測定電流時,利用(阻抗)二(電壓)/(電流) 的關係,根據該測定電流運算阻抗z,將運算出的阻抗z 頻率㈣冑143收到通知的頻率f對應起來,存 存儲部16 ( S14)。 接著,阻抗運算部142根據應測 中的所有頻率f ’判斷是否已測定阻抗Z ( SI5 j。 根據處理S15中的判斷結果、特定頻率範圍中的所有 頻率f測定阻抗7日專「v 、 寺(Yes),阻抗運算部142將存儲部 ^中存儲的阻抗z和頻率f, ' f構成的各組存館部16中以 (或阻抗Z和頻率 中的存儲位置及阻抗Z測定結束通 知頻率運算部151 ( S16)。 逋 ,父:方面’不根據處理S15中的判斷結果、特定頻率 範圍中的所有頻率" ▲一 應根據特定頻率範圍巾 、Q ’阻&運异部142 尸7、目… 圍中應測定阻抗Z的下一頻率f運行阻 抗z測疋,通過將從 中的阻抗2測定結束甬I制部143接收到通知的頻率f 處理S12。 D頻率控制部143,將處理返回到When the measured current is measured, the impedance z is calculated from the measured current using the relationship of (impedance) two (voltage) / (current), and the calculated impedance z frequency (four) 胄 143 is notified of the frequency f received, and stored. Part 16 (S14). Next, the impedance calculation unit 142 determines whether or not the impedance Z (SI5j) has been measured based on all the frequencies f' to be measured. According to the determination result in the processing S15, the impedance is measured for all the frequencies f in the specific frequency range. (Yes), the impedance calculation unit 142 sets the frequency of the impedance z and the frequency f, 'f stored in the storage unit to each of the storage units 16 (or the storage position of the impedance Z and the frequency and the end of the measurement of the impedance Z). The calculation unit 151 (S16). 逋, parent: aspect 'does not according to the judgment result in the processing S15, all the frequencies in the specific frequency range" ▲ should be based on the specific frequency range, Q 'resistance & 7. In the middle, the next frequency f of the impedance Z is measured, and the operating impedance z is measured. The frequency f is received from the measurement of the impedance 2 after the measurement is completed. The frequency f is processed S12. The D frequency control unit 143 Processing returns to

2014-8318-PF 19 1317304 ± p抗運算部142通知相應頻率中阻抗z的測定έ士束 頻率控制部143與上述相同運行處理si2;電流檢測 路141與上述相同運行處理S13;阻抗運算们42愈上 ^目同運行處理S14及處理S15。如上所述,在以特定頻 率範圍中的所有頻率f測 ’ 疋|且抗ζ 束别,反復運行處理 至仍,頻率控制部143在處理犯中每設定一次驅動 11輸出的交流信號的瓶盘 率在應測定阻抗2的頻率範 «更㈣Μ頻率f,在應測定該㈣z的頻率2014-8318-PF 19 1317304 The ±p-resistance calculation unit 142 notifies the measurement of the impedance z in the corresponding frequency that the gentleman beam frequency control unit 143 is the same operation process si2 as described above; the current detection path 141 is the same operation process S13 as described above; the impedance calculations 42 The processing is performed in the same manner as the processing S14 and the processing S15. As described above, when the frequency '| is detected at all the frequencies f in the specific frequency range, and the ζ bundle is resisted, the processing is repeated until the frequency control unit 143 sets the ac signal of the AC signal outputted by the drive 11 every time. The rate at which the frequency of the impedance 2 should be measured «more (four) Μ frequency f, the frequency of the (four) z should be determined

範圍中的所有頻率,中,測定阻抗z。即,在應測定阻抗Z 的頻率範圍内,在掃描頻率f的同時,敎阻抗Z。 該應測定阻抗Z的頻率範圍最好是,以位於有負載時The impedance z is measured for all frequencies in the range. That is, in the frequency range in which the impedance Z should be measured, the impedance Z is the same as the scanning frequency f. The frequency range in which the impedance Z should be measured is preferably such that when it is under load

超音波振子12的阻抗瓶査4i αA 抗頻率特性和無負載時超音波振子12 ^阻抗頻率=性的交點p的頻率&為中心的固^的頻率範 该應测疋阻抗Z的頻率範圍,比如,是位於該交點p 的頻率fra的±1〇% (即,〇 , 〇 ^即,〇 . 9xfm〜1 . lxim)及位於該交 點p的頻率&的±15% (即,0.85xfm〜ii5x⑷等。 如上Μ,通過採用位於該交點p的頻率^ Μ心的固定 頻率範圍’就不會出現錯誤選擇其他振盈模式,能夠選定 應驅動超音波振子1 9 m , * ,、 勺特疋振盪模式中的目標驅動頻率 fd ° •二ΐ ’Λ處理S12中每次設定驅動部11輪出的交流信 號的頻η時的特定頻率f的更改,由於 給予與交點P的阻抗Zm_致的阻抗2的頻率f,因此,按 考慮目標驅動頻率fd大小的適#間隔進行更改。比如,目The impedance bottle of the ultrasonic vibrator 12 checks the frequency characteristic of the 4i αA anti-frequency characteristic and the ultrasonic vibration of the ultrasonic vibrator 12 ^ impedance frequency = no load. The frequency of the center of the solid frequency should be measured. For example, it is ±1〇% of the frequency fra at the intersection p (ie, 〇, 〇^ ie, 〇. 9xfm~1. lxim) and ±15% of the frequency & at the intersection p (ie, 0.85) Xfm~ii5x(4), etc. As above, by using the fixed frequency range of the frequency of the intersection point p, there is no erroneous selection of other oscillation modes, and it is possible to select the ultrasonic transducer to be driven 1 9 m , * , , , The target drive frequency fd ° in the characteristic oscillation mode • The change of the specific frequency f when the frequency η of the alternating current signal that the drive unit 11 rotates is set every time in the process S12, due to the impedance Zm_ given to the intersection point P The frequency f of the impedance 2 is, therefore, changed according to the appropriate interval of the target drive frequency fd. For example,

2014-8318-PF 20 1317304 標驅動頻率fd是3MHz及5MHz等兆赫波段時, 及⑽z #的間隔進行更改。另外,叙咖 f, B x 曰%驅動頻率 疋l〇〇kHZ及500kHz等千赫波段時,按1〇Hz及5〇Hz 的間1¾進行更改。 接著’在阻抗運算部142通知阻抗2測定結束時,控 =5的頻率運算部151選擇存儲部16中預先存儲的: 、負載時超音波振子12的阻抗頻率特性和無負 ,音波振子12的阻抗頻率特性交點p中阻抗& 一致,或 取接近的,測定部14測定的阻抗z,獲得與該選擇阻抗 對應的頻率f ( S17;)。 —接著’頻率運异部i 51根據獲取的該頻率丨,使用 定公式計算目標驅動頻率fd’將計算出的目標驅動頻率Η 通知驅動頻率控㈣153,同時,將目標驅動頻率 理結束通知電壓控制部152(S18)。該特定公式是表示位 於有負載時超音波振子1 2的阻枋斗皇 町I且柷頻率特性和無負載時超 曰波振子12的阻抗頻率特點交點ρ㈣率和目標驅動 頻率fd之間關係的函數’如fd=axi…那樣,按線性 函數給予。如上所述,目標驅動頻率fd表述為與交點p的 頻率^相關的線性函數’因此,計算目標驅動 運算處理就變得簡單’可在短時間内運算目標驅動頻率… 目標驅動頻率fd如圖4所示,如果是在諳振點的頻率 fr到反諧振點的頻率fa之間的咖圍RR内,可以是任 一頻率f。正是由於考#至丨]了由m 到了周圍環境變化及老化等外部 因素導致的阻抗頻率特性變動這-事實,最好是距離反譜2014-8318-PF 20 1317304 When the standard drive frequency fd is a megahertz band such as 3MHz or 5MHz, the interval of (10)z # is changed. In addition, when the gamma f, B x 曰% drive frequency 疋l〇〇kHZ and 500 kHz and other kilohertz bands, the change is made between 1 Hz and 5 Hz. Then, when the impedance calculation unit 142 notifies that the measurement of the impedance 2 is completed, the frequency calculation unit 151 of the control unit 5 selects the impedance frequency characteristic of the ultrasonic vibrator 12 and the non-negative stored in the storage unit 16 in advance, and the acoustic vibrator 12 The impedance & in the intersection point p of the impedance frequency characteristic is identical, or the impedance z measured by the measuring unit 14 is obtained, and the frequency f corresponding to the selected impedance is obtained (S17;). - Then the 'frequency shifting unit i 51 calculates the target driving frequency fd' using the formula to calculate the target driving frequency Η to notify the driving frequency control (4) 153 according to the obtained frequency 丨, and at the same time, the target driving frequency ends the notification voltage control Part 152 (S18). The specific formula is the relationship between the intersection frequency ρ(four) rate and the target drive frequency fd of the impedance frequency characteristic of the super-wave oscillator 12 when the ultrasonic frequency oscillator is located at a load and the ultrasonic oscillator is at a load. The function 'as fd=axi... is given as a linear function. As described above, the target drive frequency fd is expressed as a linear function related to the frequency of the intersection p. Therefore, the calculation of the target drive operation becomes simple. The target drive frequency can be calculated in a short time... The target drive frequency fd is as shown in FIG. As shown, if it is within the coffee circle RR between the frequency fr of the resonance point and the frequency fa of the anti-resonance point, it may be any frequency f. It is precisely because of the test #至丨] that the change in impedance frequency characteristics caused by external factors such as changes in the surrounding environment and aging - the fact is preferably the distance inverse spectrum

2014-8318-PF 21 1317304 =或諧振點較遠的頻率fdi、fd2。換言之, 周圍環境變介& $慮、了 化等會導致阻抗頻率特性變動,設定目 才示驅動頻率fd時,畀疋目 z的差最大。比如,“载時阻抗2和有負載時阻抗 父點P的頻率f m至反諧振點頻率f a 之間,設定目標驅動頻率2014-8318-PF 21 1317304 = or the frequencies fdi, fd2 which are farther from the resonance point. In other words, the ambient environment & $ considerations, etc. will cause the impedance frequency characteristics to change, and when the drive frequency fd is set, the difference of the target z is the largest. For example, "between the impedance of load 2 and the frequency f m of the impedance of the parent point P to the anti-resonant point frequency f a, the target drive frequency is set.

Zdi和有于敢好疋無負载時的阻抗 .和有負載時的阻抗Zdl,的差(丨Zdl_Zd 大,在交點P頻率fm至反諧振點fr之間,設定目標驅動 時’最好是無負«的阻抗Zd2和有負载時的阻 抗Zd2的差(|泌―泌,丨)最大。另外, ^ X的絕對值。外部因素導致阻抗頻率特性變動,包括比2 ==、反譜振點的偏移以及阻抗頻率特性中的错振 ‘,近及反谐振點附近的profile的變形等。如上所述, ,而要通過設定目標驅動頻率fd,判斷是無負载的情況還 疋有負載的情況時,可通過目標驅動頻率fd來測定正 動的超音波振子12的阻抗2很.容易地對是有負 還 是無負載的情況作出判別。 度定 而且’從無負載時消耗功率較小,可抑制發熱的觀點 來看,目標驅動頻率fd最好是振盪範圍RR中,從交點p 的頻率比至反譜振點頻率fa之間的範圍;從該觀點1看, 最好是距離反譜振點上述Margin的頻率如。上述㈣^ 按統計學或經驗進行設定。 頻率運算部151通知目標驅動頻率運算處理結束時, 電壓控制部152設定放大電路U2,按超音波產I裝置} 的通常動作中的放大率對振盪電路113發出的交流信號進 2014-8318-PF 22 1317304 :放大’將目標驅動頻率運算處理結束通知頻率控制部 在收到„亥通知後,頻率控制部^ 43結束振盈電路j j 3 的頻率控制(S19)。通過以上動作,目標驅動頻率運算處 束肖曰波產生裝置1的通常動作被設定成可能的狀 態0 後打開啟動開關,驅動頻率控制部工Μ通過調整 振盪電路⑴的頻率,以頻率運算部i5i通知的目標驅動 、 輸出的父流信號的頻率f,使得超 音波振子12驅動。 由於上述動作’超音波產生裴置ι能夠以目標驅動頻 率Μ敎地發生超音波。因此,超音波產生裝置i能夠有 政地對物件物〇實施超音波處理。 另外’上述實施例的結構是,通過電流檢測電路141 檢測各頻率下驅動部U在超音波振子12上施加固定振幅 ^壓(^面溝到的1Vp _ P )時流向超音波振子U的電 流’阻抗運算部142根據該檢測出的電流測定阻抗 為了更精確地測定阻抗z,也可以更改施加到超音波振= 12上的電壓。 x 另外,上述實施例的結構是’通過電流檢測電 檢測各頻率f下驅動部u在超音波振 ^上她力σ固令 幅電壓(前面講到的i V Ρ — Ρ )時流向超音波振子 、 電流,阻抗運算部142根據該檢測出的電流測定卩且^12的 當然,並不局限於上述情況,也可採用眾 抗Ζ。 1 ’知的Ρ且γ :目1 定方法。比如,也可以通過測定固定值的 几d L v入超音波 2014-8318-PF 23 1317304 振子12時的電壓來測定阻抗。 而且,上述實施例的結構是,測定部14以應測定阻抗 ^的頻率範圍中的所有頻率ί測定阻抗Z後,選擇與存儲 部16中預先存儲的位於有負載時超音波振子12的阻抗頻 率特性和無負載時超音波振子12的阻抗頻率特性的交點ρ 的阻抗Z m -致或最接近的,由測定部i 4測定到的阻抗ζ, 二1 Ρ 1 5根據4選擇的阻抗ζ對應的頻率f來計算目標驅 2頻率fd。但也可採用以下結構,測定部14每次測定阻 二:時,測定到的阻抗2和此次測定時的頻率f會被通知 2制部在該通知的阻抗2與存儲部16中預先存儲 時2有負載時超音波振子12的阻抗頻率特性和無負載 特ΪΓΪΓ12的阻抗頻率特性的交點p上的阻抗^在 所選料,選擇該通知的阻抗ζ,控制部15根據 "ζ所對應的頻率f計算目標驅動頻率fde通過 構,無f在應測定阻抗2的頻率範圍中所有頻 因此,可在短她運行目標驅動頻 計Γ外’上述實施例中,位於有負載時超音波振子12的 的交性和無負載時超音波振子心阻抗頻率特性 預::的:抗Zm,先預先實際測量兩個阻抗頻率特性, 基於位於該預先計算出的交點P的阻抗 =:二Γ广阻抗z,計算應驅動超音波振子心 下結構,計算,振點… 頻率fr及反譜振點頻♦ da和交點Zdi and the difference between the impedance when there is no load and the impedance Zdl when there is load (丨Zdl_Zd is large, between the intersection point P frequency fm and the anti-resonance point fr, when setting the target drive), it is better The difference between the negative Z's impedance Zd2 and the loaded impedance Zd2 is the largest. In addition, the absolute value of ^ X. External factors cause changes in impedance frequency characteristics, including ratio 2 ==, anti-spectral point The offset and the vibration of the impedance frequency characteristic, the deformation of the profile near the near and anti-resonance point, etc. As described above, by setting the target drive frequency fd, it is judged that there is no load and there is load. In the case, the impedance 2 of the forward-moving ultrasonic vibrator 12 can be measured by the target driving frequency fd. It is easy to discriminate whether there is a negative or no load. It is determined and 'the power consumption from no load is small, From the viewpoint of suppressing heat generation, the target driving frequency fd is preferably a range between the frequency ratio of the intersection point p and the frequency of the inverse spectral point fa in the oscillation range RR; from this viewpoint 1, it is preferable that the distance inverse spectrum The frequency of the above Margin is as follows. (4) ^ Set according to statistics or experience. When the frequency calculation unit 151 notifies that the target drive frequency calculation processing is completed, the voltage control unit 152 sets the amplification circuit U2 to the oscillation circuit in the normal operation of the ultrasonic generation device}. The AC signal sent from 113 into 2014-8318-PF 22 1317304: Amplification 'The target drive frequency calculation processing ends the notification frequency control unit. After receiving the notification, the frequency control unit 43 ends the frequency control of the oscillation circuit jj 3 ( S19). Through the above operation, the normal operation of the beam oscillating wave generating device 1 at the target driving frequency calculation is set to a possible state 0, and then the start switch is turned on, and the driving frequency control unit works by adjusting the frequency of the oscillating circuit (1) to the frequency. The frequency f of the target drive signal output by the calculation unit i5i and the output of the parent stream signal is caused to drive the ultrasonic vibrator 12. The above-described action 'ultrasonic generation set ι can generate ultrasonic waves at the target drive frequency. Therefore, the ultrasonic wave The generating device i can perform ultrasonic processing on the object object in a political manner. Further, the structure of the above embodiment is that the current is passed. The measuring circuit 141 detects the current flowing to the ultrasonic transducer U when the driving unit U applies a fixed amplitude to the ultrasonic transducer 12 at each frequency (the 1Vp_P to the surface groove). The impedance calculating unit 142 determines the current based on the detected current. Measuring the impedance In order to measure the impedance z more accurately, the voltage applied to the ultrasonic vibration = 12 can also be changed. x In addition, the structure of the above embodiment is 'electrical detection by electric detection of each frequency f under the driving portion u in the ultrasonic vibration When the voltage is applied to the ultrasonic oscillator and the current, the impedance calculation unit 142 determines the current based on the detected current and is not limited to In the above case, public resistance can also be used. 1 ' knowing Ρ and γ: aiming method. For example, the impedance can also be measured by measuring the voltage at a fixed value of several dl into the ultrasonic transducer 2014-8318-PF 23 1317304. Further, in the above-described embodiment, the measuring unit 14 measures the impedance Z of all the frequencies ί in the frequency range in which the impedance is to be measured, and selects the impedance frequency of the ultrasonic vibrator 12 which is stored in advance in the storage unit 16 at a load. The impedance Z m of the intersection point ρ of the impedance frequency characteristic of the ultrasonic vibrator 12 at the time of no load is the closest or the impedance ζ measured by the measuring unit i 4 , and the impedance ζ corresponding to the selected impedance 4 according to 4 The frequency f is used to calculate the target drive 2 frequency fd. However, the following configuration may be adopted. When the measurement unit 14 measures the resistance 2, the measured impedance 2 and the frequency f at the time of the measurement are notified to the 2nd part to store in advance in the notified impedance 2 and the storage unit 16. At the time of the load 2, the impedance frequency characteristic of the ultrasonic vibrator 12 and the impedance at the intersection p of the impedance characteristic of the no-load characteristic 12 are selected, and the impedance of the notification is selected, and the control unit 15 corresponds to the " The frequency f is calculated by the target drive frequency fde, and f is not all frequency in the frequency range in which the impedance 2 should be measured. Therefore, the target drive frequency meter can be shorted. In the above embodiment, the ultrasonic oscillator is located under load. The ferromagnetic core impedance frequency characteristic of the cross-talk and no-load at 12: Pre-: ZZ, the two impedance frequency characteristics are measured in advance, based on the impedance at the pre-calculated intersection point P: Impedance z, the calculation should drive the subsonic structure of the ultrasonic oscillator, calculate, the vibration point... Frequency fr and anti-spectral frequency ♦ da and intersection

2014-8318-PF 24 A 7304 P的頻率fm之間關係的函數f 計算夺 Si r> T xg ^ tr) + ^ xh ( 算曰‘’㈣率fm’根據計算出的交點P的頻率f 异目標驅動頻率f d。+ ^ ^ 的頻率fm計 撫2 羊d比如’在超音波振盪塊2中沾和a、 、12中,由於交點Ρ的頻率f 、 17曰波 頻率f Γ和 、 車又夕也存在於諧振點的 . 洋反拍振點的頻率fa的中間,闵 率fm按h 。 〒間因此,交點P的頻 . fm= (fr+fa) 進行計算。 頭 圖5疋表不基於諧振點及反諧振點 率,真斗曾„ 70 DT异父點的頻 _ D异目k驅動頻率的流程圖。 基於該諧振點及反諧振點,計 計I曰4® β τ异又點Ρ的頻率f m,再 目禚驅動頻率f d時,超音 所述進行動作^產生裝置1的各部分如下 r的頻率fm計算目椁 丨丹乂點 .處理中以 動頻率心夺的目標驅動頻率運算 中的處理S21到處理S26,除為了 ,、M 6 的頻率銘m L 除為了劍疋阻抗Z而掃描 羊祀圍不同外,與使用圖3介奶的 理⑽相同,在此省略說明。“的上述處理⑴到處 為了測定阻抗Z而掃描的頻率範圍,在 到處理S16中,目的甚押各,人, , '、、’Ό予父點P的頻率fm的阻抗 & ’因此,是以交點ρ ,,^ 扪笼羊fm為中心的固定的頻率範圍。 旦在該處理S21到處理S26中,目的县押 ,E T 0的疋探索諧振點及反諧 振點’因此需要是包括如 义σ自振點的頻率fr及批諧振點 的頻率fa的較大範圍的頻率範圍。 在處理S27中,阻抗運算部142通知阻抗2測定結束 時’控制部1 5的頻率運|ς ~ 士 & ^ 手連异151從存儲部16中存儲的阻 矛頻率f的各經中提取譜振點及反譜振點,運算該提2014-8318-PF 24 A 7304 The function f of the relationship between the frequencies fm of P is calculated as Si r > T xg ^ tr) + ^ xh (calculated 曰 '' (four) rate fm' according to the calculated frequency f of the intersection point The target drive frequency fd. + ^ ^ The frequency fm counts 2 sheep d such as 'in the ultrasonic oscillation block 2 and a, 12, due to the intersection point Ρ frequency f, 17 曰 wave frequency f Γ and, the car again The eve also exists at the resonance point. In the middle of the frequency fa of the ocean back-shooting point, the f rate fm is h. Therefore, the frequency of the intersection point P. fm= (fr+fa) is calculated. Based on the resonance point and the anti-resonance point rate, the flow chart of the frequency of the frequency _ D 异 k 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 。 When the frequency fm of the point is clicked and the driving frequency fd is witnessed, the parts of the generating device 1 are operated by the supersonics, and the frequency fm of the r is calculated as the target point of the target. In the frequency calculation, the processing S21 to the processing S26, in addition to, the frequency M M of the M 6 is divided by the scorpion impedance Z and the scanning of the scorpion circumference is different, and the use of FIG. 3 The principle of milk (10) is the same, and the description is omitted here. "The above-mentioned processing (1) is used to measure the impedance Z to measure the frequency range. In the process S16, the purpose is to hold each other, and the person, ',, ' is given to the parent point P. The impedance of the frequency fm & ', therefore, is a fixed frequency range centered on the intersection point ρ , , ^ 扪 羊 f f f f f f f f f f f 。 。 。 。 。 该 该 该 该 该 该 该 该 该 该 该 疋 疋 疋 疋 疋 疋 疋 疋 疋 疋 疋 疋 疋 疋 疋 疋 疋And the anti-resonance point' therefore needs to be a wide frequency range including the frequency fr of the self-vibration point and the frequency fa of the batch resonance point. In the process S27, the impedance calculation unit 142 notifies the end of the measurement of the impedance 2 'control The frequency of the portion 1 5 is used to extract the spectral point and the anti-spectral point from each of the obstruction frequency f stored in the storage unit 16, and the calculation is performed.

2014-8318-PF 25 ‘1317304 :㈣振點的頻率fr及該提取的譜振點fa,根據表示諧 '黑頻率fr及反譜振點頻率fa和交點p的頻率^的關係 、函數’如fm= (fr+fa)/H算交點p的頻率^諧 振點是阻㈣⑽性的最小,反諧振點是阻抗頻率特性的 =口此此夠很簡單地高精度地提取諧振點及反諧振 點。 接者,頻率運算部151根據該運算出的頻帛fm,使用 特定公式計算目標驅動頻率fd,將計算出的目標驅動頻率 fd通知驅動頻率控制部153’同時,將目標驅動頻率運算 處理結束通知電壓控制部丨52 ( S28 )。 頻率運算部151通知目標驅動頻率運算處理結束時, 電Μ控制冑152設定放大電路112,按超音波產生裝置丄 的通常動作中的放大率對振盪電㉟113發出的交流信號進 打放大’將目標驅動頻率運算處理結束通知頻率控制部 143 ’在收到該通知後,頻率控制部143結束振盈電路ιΐ3 的頻率控制(S29 )。通過以上動作,目標驅動頻率運算處 理、,。束#曰波產生裝置j的通常動作被設定成可能的狀 態。 如上所述,通過先基於諧振點及反諧振點計算交點p 的頻率fni,再計算目標驅動頻率fd,來降低超音波振子 12及超音波產生裝置i的製造偏差對目標驅動頻率^的 影響。 或者,上述實施例中,位於有負載時超音波振子12的 阻抗頻率特性和無負載時超音波振子丨2的阻抗頻率特性2014-8318-PF 25 '1317304 : (4) The frequency fr of the vibration point and the extracted spectral point fa, according to the relationship between the harmonic frequency 'black frequency fr and the inverse spectral point frequency fa and the frequency of the intersection point ^, function ' Fm= (fr+fa)/H Calculate the frequency of the intersection point p. The resonance point is the minimum of the resistance (4) (10), and the anti-resonance point is the impedance frequency characteristic = the mouth is very simple and highly accurate to extract the resonance point and the anti-resonance point. . The frequency calculation unit 151 calculates the target drive frequency fd using the specific formula based on the calculated frequency 帛fm, notifies the drive frequency control unit 153' of the calculated target drive frequency fd, and notifies the target drive frequency calculation process. Voltage control unit 丨52 (S28). When the frequency calculation unit 151 notifies that the target drive frequency calculation processing is completed, the power control unit 152 sets the amplification circuit 112 to amplify the AC signal from the oscillation power 35113 in accordance with the amplification factor in the normal operation of the ultrasonic generation device '. The drive frequency calculation processing end notification frequency control unit 143', after receiving the notification, the frequency control unit 143 ends the frequency control of the oscillation circuit ι3 (S29). Through the above actions, the target drive frequency is calculated and processed. The normal operation of the beam #曰 wave generating device j is set to a possible state. As described above, the influence of the manufacturing deviation of the ultrasonic vibrator 12 and the ultrasonic generating device i on the target driving frequency ^ is reduced by calculating the frequency fni of the intersection point p based on the resonance point and the anti-resonance point, and then calculating the target driving frequency fd. Alternatively, in the above embodiment, the impedance frequency characteristic of the ultrasonic vibrator 12 at the time of load and the impedance frequency characteristic of the ultrasonic vibrator 丨2 when there is no load

2014-8318-PF 26 1317304 的交點P上的阻抗Zm,通過事先對兩個阻抗頻率特性進行 實際測定,來㈣計算。也可採用以下結構,計算譜振點 及反諧振點,根據表示諧振點的頻率fr及反諧振點的頻率 fa和交點P的頻率fm的關係的函數計算交點p的頻率化, 根據計算出的交點P的頻率f m計算交點p的阻抗&。 圖6是表示基於譜振點及反諧振點,計算交點的阻抗 時的流程圖。The impedance Zm at the intersection P of 2014-8318-PF 26 1317304 is calculated by (4) by actually measuring the two impedance frequency characteristics in advance. The following structure can also be used to calculate the spectral vibration point and the anti-resonance point, and calculate the frequency of the intersection point p according to a function of the relationship between the frequency fr of the resonance point and the frequency fa of the anti-resonance point and the frequency fm of the intersection point P, according to the calculated The frequency fm of the intersection point P is used to calculate the impedance & Fig. 6 is a flow chart showing the calculation of the impedance of the intersection based on the spectral point and the anti-resonance point.

基於該諧振點及反諧振點,計算交點p的阻抗&時, 超音波產生裝f 1的各部進行如下所述的動作。圖6中, 基於諧振點及反譜振點計算交點p的阻抗&的處理中處理 S31至處理S37與圖5介紹的上述處s S2I至處理s 同,在此省略介紹。 在處理S 3 8中,頻率運笪立β ί ^w > 馮手連异邛151從存儲部16中存儲的 s:::出14二二出的阻抗Ζ和頻率f和各組,選擇與處理 運异出的頻率fm 一致或最接近,測定部14測定出的 頻率卜獲取該所選頻h對應的阻抗z,作為交點p的阻 杬“存储到存儲部16中,同時’將本處理結束資訊通知 電壓控制部152。 貝孔通知 頻率運异4 151通知本處理結束時,電壓控制部 =大電路m’按超音波產生⑴的通常 放大率對㈣電路113發出的交流信號進行放纟,將本卢 理結束通知頻率控制部143,在收到該通知 率= 部143結束振堡電路m的頻率控制(S39)。车 上所述通過先基於諸振點及反譜振點計算交點pWhen the impedance & of the intersection p is calculated based on the resonance point and the anti-resonance point, each unit of the ultrasonic generation device f1 performs the following operation. In Fig. 6, the processing S31 to S37 in the processing of calculating the impedance & of the intersection point p based on the resonance point and the inverse spectral point are the same as the above-described processing s S2I to s described in Fig. 5, and the description is omitted here. In the processing S 3 8 , the frequency is set to β ί ^w > von 连 邛 邛 151 from the s::: 14 stored in the storage unit 16 out of the impedance Ζ and frequency f and each group, select The frequency fm measured by the measuring unit 14 is obtained by the frequency fm measured by the measuring unit 14 and the impedance z corresponding to the selected frequency h is obtained, and the resistance of the intersection point p is stored in the storage unit 16 and simultaneously The processing end information notification voltage control unit 152. The hole notification frequency difference 4 151 is notified that the processing ends, the voltage control unit = the large circuit m' releases the AC signal from the (four) circuit 113 at the normal amplification factor of the ultrasonic generation (1). Then, the frequency control unit 143 is notified of the termination of the present Luna, and the frequency control of the Zhenbao circuit m is terminated by the notification rate = unit 143 (S39). The above-mentioned passage is calculated based on the vibration point and the anti-spectral point. Intersection point p

2014-8318-PF 27 1317304 的頻率fm,再計算交點p的 心超音波產生裝置二:夂來降低超音波振子 影響。 以、偏差對目標驅動頻率fd的 而掃二=在圖5及圖6所示的動作中1 了測定阻抗Z 因=?率範圍,由於目的是探索諧振點及反譜振點, =吏疋以諸振點的頻…中心的固 T振點的頻率^為中心的固定頻率範圍即可。另外 以4振點的頻率f r為中心的面〜 ^ f . . , ra 、疋頻率範圍及以反諧振點 頻率fa為中心的固定頻率範 其他範圍時,可加大頻率間隔。心小頻率間隔’ 而且’上述實施財,有貞载時超音波振子12的阻抗 頻率特性和無負載時超音波振子 的阻虹頻率特性的交 P的阻抗&,通過預先對兩個阻抗頻率特性進行實際測 :,來預先計算,基於該計算出的交點p的阻抗二二 …測定出的阻抗Z計算應驅動超音波振子12的目把 驢動頻率fd。也可以採用以下結構,預先計算阻抗頻率: :生的傾斜a和交點P的頻率fm之間的對應關係,通過測定 測定以多個頻率f的電振盪驅動超音波振子12時的 多個阻抗Z’根據多個頻率f和多個阻抗z計算阻抗頻率 輕的傾斜a ,基於計算出的阻抗頻率特性的傾斜a,計 算目標驅動頻率fd。包括盔倉哉,j±VAAF1 …、員載情況的同-負載時的阻抗 頻率特性,由於諧振點的頻率圩和反諧振點的頻率“之 1’其間的阻抗z *差大致相同,因&,根據諧振點和反 4振點之間的阻抗頻率特性的傾斜3計算交點p的頻率仏。The frequency fm of 2014-8318-PF 27 1317304, and then calculate the ultrasonic ultrasonic generating device of the intersection point p: 夂 to reduce the influence of the ultrasonic oscillator. In the operation shown in Figs. 5 and 6, the impedance Z is measured in the range of the frequency of the target drive frequency fd. The purpose is to find the resonance point and the anti-spectral point, =吏疋The fixed frequency range centered on the frequency ^ of the solid T-point of the center of the vibration point can be used. In addition, the frequency interval can be increased by the surface of the four-vibration point f r ~ ^ f . . , ra , the frequency range of the 及 and the fixed frequency range centered on the anti-resonance frequency fa. The small frequency interval 'and' the above implementation, the impedance frequency characteristic of the ultrasonic vibrator 12 at the time of the load and the impedance & the impedance of the ultrasonic characteristic of the ultrasonic oscillator at the time of no load, by pre-aligning the two impedance frequencies The characteristic is actually measured: by pre-calculation, based on the calculated impedance of the intersection point p... The measured impedance Z is calculated to drive the target pulsation frequency fd of the ultrasonic vibrator 12. It is also possible to calculate the impedance frequency in advance by using the following structure: a correspondence relationship between the inclination a of the raw and the frequency fm of the intersection P, and measuring the plurality of impedances Z when the ultrasonic transducer 12 is driven by the electric oscillation of the plurality of frequencies f by measurement 'The inclination a of the impedance frequency is calculated from the plurality of frequencies f and the plurality of impedances z, and the target drive frequency fd is calculated based on the calculated inclination a of the impedance frequency characteristic. Including the helmet 哉, j±VAAF1 ..., the impedance frequency characteristics of the same-load condition of the load, because the frequency of the resonance point 圩 and the frequency of the anti-resonance point "1" during which the impedance z * difference is approximately the same, due to &;, the frequency 仏 of the intersection point p is calculated from the inclination 3 of the impedance frequency characteristic between the resonance point and the inverse 4 vibration point.

2014-8318-PF 28 !317304 圖7是表示基於阻抗頻率特性的傾 頻率,再钟首n^ 元鼻父點的 D十算目軚驅動頻率時的流程圖。2014-8318-PF 28 !317304 Fig. 7 is a flow chart showing the tilting frequency based on the impedance frequency characteristic, and then the D-time counting target driving frequency of the first n^ element.

的頻實際測定阻抗頻率特性的傾斜a和交點P 16。" 對應關係,將該對應關係存儲到存儲邱 i以後,基於阻抗頻率特性的傾斜a,計算交點p 率f m,再計算目户 P的頻 异目‘驅動頻率fd時’超音波產生裝 各部的動作如下。圖7由展置1的 算交點…、, 阻抗頻率特性的傾斜a計 、、率f m,再計算目標驅動頻率fd 0 g # 手運鼻處理中的處理⑷到處理s.The frequency actually measures the slope a of the impedance frequency characteristic and the intersection point P16. " Correspondence relationship, after storing the correspondence relationship to store Qiu i, based on the inclination a of the impedance frequency characteristic, calculate the intersection point p rate fm, and then calculate the frequency difference of the target P' drive frequency fd 'ultrasonic generation assembly The action is as follows. Fig. 7 is the intersection point of the expansion 1 ..., the inclination of the impedance frequency characteristic, the rate f m , and then the calculation of the target drive frequency fd 0 g # in the handling of the nose (4) to the processing s.

而掃描的頻率範圍不π k ' /、疋阻抗Z 十乾圍不同外,與使用圖3介紹 到處理S16相鬥+ L 圃^丨、, 口的上述處理S11 lb相冋,在此省略說明。 為了測定阻抗Z而掃描的頻率範圍 到虛理山 肩千祀固在上述處理S11 中,目的是探索給予交點P的 z”此,是以交點P的頻率fm/::頻率fm的阻抗 但。 料fm為中心的固定的頻率範圍。 在該處理S41到虚理ς/β + 反⑽點… 由於目的是探索諧振點到 反咱振點的阻抗頻率特性的傾斜a, :=⑽振點的頻率fa的範圍,至少包== 頻=率範圍即可。通過增加測定點,提高要計算 頻率特性的傾斜a的精度。 抗 在處理S47中,阻抗運糞邱 .oi t 逆异。卩142通知阻抗Z的測定妗 束寸,控制部1 5的頻率運算邮 ° 的測定部Μ測定出的# z/151根據存儲部16中存儲 …μ 和頻率'的各_阻抗頻率 特性的傾斜a,從存儲部丨6中 傾斜a和交點P的頻率^存储的阻抗頻率特性的 間對應關係中的阻抗頻率特性However, the scanning frequency range is not π k ' /, and the 疋 impedance Z is different from the dry circumference, and is the same as the above-mentioned processing S11 lb of the processing of S16, which is described in FIG. . In order to measure the impedance Z, the frequency range of the scan is fixed to the virtual process in the above-mentioned process S11, and the purpose is to explore the z" given to the intersection point P, which is the impedance of the frequency fm/:: frequency fm of the intersection point P. The material fm is the center of the fixed frequency range. In this process S41 to the imaginary ς/β + inverse (10) point... Since the purpose is to explore the inclination a of the impedance frequency characteristic of the resonance point to the anti-shock point, :=(10) The range of the frequency fa, at least the package == frequency = rate range. By increasing the measurement point, the accuracy of the slope a to calculate the frequency characteristic is improved. In the process S47, the impedance is transported, and the impedance is 逆. The measurement impedance Z is measured, and the #z/151 measured by the measurement unit 频率 of the frequency calculation unit of the control unit 15 stores the inclination a of each of the _ impedance frequency characteristics of the ... μ and the frequency ' in the storage unit 16 . Impedance frequency characteristics in the correspondence between the impedance frequency characteristics of the frequency a and the intersection point P stored in the storage unit 丨6

2014-8318-PF 29 * 1317304 * 的傾斜a中選擇與計算出的阻抗頻率特性的傾斜& 一致或 最接近的阻抗頻率特性的傾斜a,獲取與所選阻抗頻率特 性的傾斜a對應的頻率f m。 接著,頻率運算部1 51根據獲取的該頻率fin,使用特 疋公式計算目標驅動頻率f d,將計算出的目標驅動頻率Μ . 通知驅動頻率控制部1 53,同時,將目標驅動頻率運算處 . 理結束通知電壓控制部1 52 ( S48 )。 頻率運算部1 51通知目標驅動頻率運算處理結束時, ♦電壓控制部152設定放大電路112,按超音波產生裝置i 的通常動作中的放大率對振盪電路113發出的交流信號進 行放大,將目標驅動頻率運算處理結束通知頻率控制部 .143,在收到該通知後,頻率控制部143結束振盪電路113 •的頻率控制(S49)。通過以上動作,目標驅動頻率運算處 理、口束超曰波產生裝置1的通常動作被設定成可能的狀 態。 •,採用以上結構,在數點,最小情況下在2點測定 ^卩可因此,此夠更快速地運行目標驅動頻率運算處 理。 而且,上述實施例中,目標驅動頻率運算處理在打開 超曰波產生裝置1的電源時運行,但並不局限於此。如,2014-8318-PF 29 * 1317304 * Select the slope a corresponding to or the closest impedance frequency characteristic of the slope of the calculated impedance frequency characteristic, and obtain the frequency corresponding to the inclination a of the selected impedance frequency characteristic. Fm. Next, the frequency calculation unit 1 51 calculates the target drive frequency fd using the characteristic formula based on the acquired frequency fin, and notifies the calculated target drive frequency Μ to the drive frequency control unit 1 53, and simultaneously calculates the target drive frequency. The control ends the voltage control unit 1 52 (S48). When the frequency calculation unit 1 51 notifies that the target drive frequency calculation processing is completed, the voltage control unit 152 sets the amplification circuit 112 to amplify the AC signal from the oscillation circuit 113 at the amplification factor in the normal operation of the ultrasonic generation device i, and the target is obtained. The drive frequency calculation processing end notification frequency control unit 143 receives the notification, and the frequency control unit 143 ends the frequency control of the oscillation circuit 113 (S49). By the above operation, the normal operation of the target drive frequency calculation processing and the mouth-beam super-chopping device 1 is set to a possible state. • With the above structure, at a few points and at the minimum, it is measured at 2 points. Therefore, it is enough to run the target drive frequency calculation process more quickly. Further, in the above embodiment, the target drive frequency calculation processing operates when the power of the super chopping apparatus 1 is turned on, but is not limited thereto. Such as,

也可以是打開啟動開關,超音波產生裝置i發生超音波的 通過動作過私狀態下運行目標驅動頻率運算處理。或者, 也可以在打開電源開關’接通電源後’啟動開關處理附 的待機狀態下運行目標驅動頻率運算處理。或者,在超音 2014-8318-PF 30 1317304 波產生裝置1安裝有供電源的二次電池,具備充電功能 時’在充電過程中也可以運行目標驅動頻率運算處理。在 上述動作狀態、待機狀態以及充電狀態下的目標驅動頻率 運算處理可以是1次,也可以按特定的時間(比如,啟動 後5分鐘間隔、啟動後1 〇分鐘間隔、啟動後分鐘間隔 等)反復運行。而且,目標驅動頻率運算處理運行結束後, .也可以轉到通常的動作。也可以採用以下結構,為了計算 目標驅動頻率fd,測^所需阻抗z,之後,轉到通常的動 作’在通常的動作過程中使用該測定的阻抗Z運算計算目 標驅動頻率fd的運算。 另外,在上述實施例中,也可以 運算處理後,在存儲邱1R由六妙 丁目心駆動頻率 超音波振子12時=存儲以目標驅動頻…動 汉淑于U ¥無負載狀態下阻 抗Z,在無負载或有 或有負载狀態下的阻 一 負载狀態下通過測定邱Η 振子12的驅動過程中 邛14測定超音波 抗Z和存儲部16中存儲的阻抗 對該測定的阻 判斷是否運算目標驅動頻率:算處仃比較’根據比較結果 行目標驅動頻率運算處理。 ,根據該判斷結果運 圖8是表示基於 々々士 抗偏移判斷是π> 鼻處理動作的流程圖。圖8 運行目標驅動頻率 的流程圖;圖8⑴是表θ 是表示阻抗的存儲動作 在圖 斷動作的流程圖。 ’、 動頻率運算處理運行判Alternatively, the activation switch may be turned on, and the ultrasonic generating device i may generate a supersonic wave. Alternatively, the target drive frequency calculation processing may be executed in the standby state in which the start switch is turned on after the power switch is turned "on". Alternatively, in the supersonic 2014-8318-PF 30 1317304, the wave generating device 1 is equipped with a secondary battery for supplying power, and when the charging function is provided, the target driving frequency calculation processing can also be performed during the charging process. The target drive frequency calculation processing in the above-described operation state, standby state, and charge state may be one time, or may be performed for a specific time (for example, a 5-minute interval after startup, a 1-minute interval after startup, a minute interval after startup, etc.) Run it repeatedly. Moreover, after the target drive frequency operation processing is finished, it is also possible to go to the normal operation. It is also possible to adopt the following configuration, in order to calculate the target drive frequency fd, measure the required impedance z, and then go to the normal operation 'The operation of calculating the target drive frequency fd using the measured impedance Z operation during the normal operation. In addition, in the above embodiment, after the arithmetic processing, when storing the Qiu 1R by the Liu Miao eye-moving frequency ultrasonic vibrator 12 = storing the target driving frequency ... moving Han Shu in U ¥ no load state impedance Z, The measurement of the resistance of the measurement by the ultrasonic impedance Z and the impedance stored in the storage unit 16 is determined by measuring the impedance of the Η 14 during the driving process of the Η 振 vibrator 12 under no load or with or under load. Drive frequency: Calculate 仃 Compare 'According to the comparison result line target drive frequency operation processing. According to the result of the judgment, Fig. 8 is a flowchart showing the nasal processing operation based on the gentleman anti-offset determination. Fig. 8 is a flow chart showing the operation target driving frequency; Fig. 8 (1) is a flow chart showing the storage operation of the impedance in the graph θ. ', dynamic frequency operation processing

(A )中,营皮 自无,控制部 7 田 、I 頻率運算處理中計复 炫刺°卩1 5以最近的目;I:® β W异出的目標驅動頻率fd /目“區動 手Μ由驅動部U來(A), the camp skin is self-existing, the control department 7 field, I frequency calculation processing in the calculation of the spurs °卩1 5 to the nearest target; I:® β W different target drive frequency fd / target "area hands Μ by the drive unit U

2014-8318-PF 31 1317304 動狀t9波振子12 (S51)。接著’測定部14測定處於驅 下的超音波振子12的阻抗Z,存儲到存儲部16 立運行目標驅動頻率運算處理時,纟圖8 (B)中,控制 P 15在有負載時或無負載情況下,按最近—次的目 頻率運算處理計算出的目標驅動頻率fd由驅動部 =音波振112(S61)。接著,測定部14測定處於驅動 1二:的超音波振子12的阻抗z’將測定結果通知存儲部 。接著,控制部15對存儲部16中存儲的2014-8318-PF 31 1317304 Dynamic t9 wave vibrator 12 (S51). Next, the measurement unit 14 measures the impedance Z of the ultrasonic transducer 12 that is being driven, and stores it in the storage unit 16 for the vertical operation target drive frequency calculation processing. In Fig. 8(B), the control P 15 is under load or no load. In this case, the target drive frequency fd calculated by the most recent-order eye frequency calculation process is driven by the drive unit = sound wave 112 (S61). Next, the measuring unit 14 measures the impedance z' of the ultrasonic transducer 12 that is driving the first two: and notifies the storage unit of the measurement result. Next, the control unit 15 stores the storage in the storage unit 16.

和該測定的阻;^ 7, L 町!5抗Z進行比較,判斷比較結果、上 否在特定的範圍以内(S63)。 疋 κ该判斷結果、差在特定範圍以内日夺(Yes ),控制部 、,’口束本處理,不運行目標驅動頻率運算處理。即, =二M:驅動頻率運算處理中計算出的目 來驅動超音波產生裴置工。 初馮半f d 另方面在该判斷結果、差不在特定筋 時,控制部15運杆曰彿 在特疋把圍以内(No) 運仃目標驅動頻率運算處理(s 以本次目標驅動頻率s Μ)。即, 來驅動超音波產生裝置丨。 知艇動頻率fd 這裏,圖8 (A)及⑷所示的 載的情況下運行。所浐B 乍在…負載或有負 況,可通過圖4進行理\疋'”、、的情況還是有負載的情 逆仃理解,無負載眛 J 1月 波振子12的電流不 、、σ有負載時流向超音 12的電流就能夠作出判斷因此’通過測定流向超音波振子And the resistance of the measurement; ^ 7, L town! 5 Anti-Z is compared, and the comparison result is judged to be within a specific range (S63).疋 κ This judgment result and the difference are within a specific range (Yes), the control unit, and the 'mouth group processing, and the target drive frequency calculation processing is not executed. That is, = two M: The purpose of the drive frequency calculation processing is to drive the ultrasonic generation. In addition, when the result of the judgment is that the difference is not at the specific rib, the control unit 15 operates as a target drive frequency calculation process (s with the target drive frequency s Μ ). That is, the ultrasonic generating device 驱动 is driven. The boat movement frequency fd is operated in the case of the load shown in Fig. 8 (A) and (4). If there is a load or a negative condition, it can be understood by the figure in Figure 4, or the situation of the load is reversed. The current flowing to the supersonic 12 when there is a load can make a judgment, so 'measuring the flow to the ultrasonic vibrator

2014-8318-PF 32 •1317304 周圍環境變化,諧振點 超音波產生裝置1無需 通過如上所述的動作,在沒有 及反諧振點大致固定較為穩定時, 運行目標驅動頻率運算處理。 而且也可將種超音波產生裝置1應用于超音波美 容裝置。® 9是表示超音波產生裝置用於超音波美容裝置 例子的局部剖視圖。2014-8318-PF 32 •1317304 Surrounding environment change, resonance point The ultrasonic wave generator 1 does not need to operate as described above. When the anti-resonance point is not substantially fixed and stable, the target drive frequency calculation processing is executed. Further, the ultrasonic generating device 1 can be applied to an ultrasonic beauty device. ® 9 is a partial cross-sectional view showing an example of an ultrasonic generating device for an ultrasonic cosmetic device.

圖9中,超音波美容裝置20包括:機殼(收容容器) 〃備上述驅動部! i、測定部i 4、控制部工5及存儲部 16的電路塊22、具備上述超音波振子12及喇叭13的粘接 型超音波振盪《23。機殼21比如由合成樹脂等構成,包 括使用時手握的把手2H、安裝在把手2H其中一端的 振盈部2卜2。機殼21内部,特別是把手2H内部安裝有 電路塊22,振盤部2卜2的一個面(正面)上安裝有超音 波振蘆塊23 ’需保證剩队13的放射面直接或通過超音波In Fig. 9, the ultrasonic cosmetic device 20 includes a casing (storage container) for preparing the above-described driving portion! i, the measuring unit i 4, the control unit 5, and the circuit block 22 of the storage unit 16, and the bonding type ultrasonic oscillation "23" including the ultrasonic transducer 12 and the horn 13. The casing 21 is made of, for example, synthetic resin, and includes a handle 2H that is held by the hand, and a vibration portion 2 that is attached to one end of the handle 2H. Inside the casing 21, in particular, the circuit block 22 is mounted inside the handle 2H, and an ultrasonic vibration block 23 is mounted on one surface (front surface) of the vibration plate portion 2' 2 to ensure that the radiation surface of the remaining team 13 is directly or through Sound wave

傳輸構件31接觸到肌膚等對象物〇。 由於上述超音波美容裝置2〇中組裝有上述超音波產 生裝置,因此,能夠穩定地以目標驅動頻率f d發生超音 波。因此,超音波美容裝置20能夠有效地對物件物〇給予 美容效果。特別是通過使用藥物有效地作用於肌膚,實現 美麗肌膚。 這畏’阻抗如上所述處於(阻抗(電塵)/(電 流)的關係中,因此,已知電壓時的電流以及已知電流時 的電壓與阻抗是等價的,從該意思上講,包括在阻抗中。 即’取代阻抗’在電麈已知的情況下可以利用電流。另外, 2014-8318-PF 33 ‘1317304 取代阻抗’在電流已知的情況 如上所述,本說明書介紹 明匯總如下。 下,可以利用電壓。 了各種發明。其中的主要發 本發明其中一種實施例有關的超音波產生裝置的特徵 是,包括:生成電振蘯的驅動部;將上述驅動部生成的上 述電振盈轉換成超音波的機械振盧的超音波振子;一個面 上接合上述超音波振子,將上述超音波振子轉換的上述超 音波的機械《傳輸到另—個面放射面的傳輸構件;測定 上述超音波振子阻抗的測定部;基於應傳輸上述超音波的 機械振里的對象物接觸上述傳輸構件的負載時上述超音波 振子的阻抗頻率特性和應傳輸上述超音波的機械振堡的物 件物不接觸上述傳輸構件的無負載時上述超音波振子的阻 抗頻率特性的交點上的阻抗以及上述測定部測定的阻抗, 計算應驅動上述超音波振子的目標驅動頻率,控制上述驅 動邵,使侍上述超音波振子以該計算出的目標驅動頻 盪的控制部。 x 以上結構的超音波產生裝置能夠以目標驅動頻率穩定 地發士超音波。因此,超音波產生裝置能夠有效地對物件 物〇貫施超音波處理。 上述超音波產生裝置的特徵是,上述測定部基 :上述驅動部在上述超音波振子上施加固定振幅的電壓二 流入上述超音波振子的電流值來測定上述阻抗。The transport member 31 comes into contact with an object such as the skin. Since the ultrasonic generating device is incorporated in the ultrasonic cosmetic device 2, the ultrasonic wave can be stably generated at the target driving frequency fd. Therefore, the ultrasonic cosmetic device 20 can effectively impart a cosmetic effect to the object. In particular, by using drugs to effectively act on the skin, beautiful skin is achieved. This impedance is in the relationship of (impedance (electric dust) / (current) as described above, and therefore, the current at the time of the known voltage and the voltage at the known current are equivalent to the impedance, in this sense, It is included in the impedance. That is, the 'substitute impedance' can be used in the case where the electric raft is known. In addition, 2014-8318-PF 33 '1317304 replaces the impedance 'in the case where the current is known as described above, this specification describes the summary The present invention is characterized in that the ultrasonic generating device according to one embodiment of the present invention is characterized in that it comprises: a driving portion for generating an electric vibration; and the electric power generated by the driving portion a supersonic vibrator in which a vibration is converted into a mechanical vibration of a supersonic wave; a transmission member that transmits the supersonic wave that converts the supersonic vibrator on one surface to a surface of another surface; The ultrasonic transducer impedance measuring unit; the ultrasonic vibration when the object in the mechanical vibration transmitting the ultrasonic wave contacts the load of the transmission member The impedance frequency characteristic of the sub-substance and the impedance of the impedance frequency characteristic of the ultrasonic vibrator when the object to be transmitted by the mechanical transmission of the ultrasonic wave is not in contact with the transmission member, and the impedance measured by the measuring unit are calculated. The target driving frequency of the ultrasonic transducer is driven to control the driving direction so that the ultrasonic transducer is driven by the calculated target driving frequency. x The ultrasonic generating device of the above configuration can be stably transmitted at the target driving frequency. Therefore, the ultrasonic generating device can effectively perform ultrasonic processing on the object. The ultrasonic generating device is characterized in that the measuring unit base: the driving unit applies a fixed amplitude to the ultrasonic vibrator. The voltage is applied to the current value of the ultrasonic transducer to measure the impedance.

,通過上述結構的超音波產生裝置’使用(阻抗)==(電 堅)/(電流)的關係,很容易地測定阻抗.。 2014-8318-PF 34 1317304 外’上述超音波產生裝置的特徵是,上述交點的阻 說疋預先測定應傳輸上述超音波的機械振盪的對象 上述傳輸構件的有負載時上述超音波振子的阻抗頻率特性 及應傳輸上述超音波的機械振盪的物件物不接觸上 構件的無負載時上述超音波振子的阻抗頻率特#,根據二 測定結果預先計算出的值。 上述結構的超音波產生裝置,由於事先計算出交點的 阻抗:因此能狗以適合該超音波產生裝置的目標驅動頻率 f d ’穩定地發生超音波。 而且,上述超音波產生裝置中,上述控制部還具有如 下特徵,上述測定部測定上述超音波振子的阻抗頻率特性 中的為振頻率及反諧振頻率’基於該測定到㈣振頻率及 反譜振頻率計算上述交點的阻抗。 在上述結構的超音波產生裝置中,由於基於實際測量 的错振頻率及反諧振頻率計算交點的阻抗,因此,降低$ 因超音波振子及超音波產生裝置的製造偏差對目標驅動 率的影響。 而且,上述超音波產生裝置中,上述目標驅動頻率以 與上述交點的頻率相關的線性函數進行表述,上述控制部 的特徵是,使用上述線性函數計算上述目標驅動頻率。 ,以上結構的超音波產生裝置中,目標驅動頻率fd表述 為與交點P的頻率fm相關的線性函數,因此,計算目標驅The impedance is easily measured by the relationship of (impedance) == (electrode) / (current) by the ultrasonic generating device of the above configuration. 2014-8318-PF 34 1317304 The above-mentioned ultrasonic generating device is characterized in that the impedance of the intersection is measured in advance, and the impedance frequency of the ultrasonic vibrator when the transmission member is loaded with the mechanical oscillation of the ultrasonic wave is measured in advance. The characteristic and the object to be transmitted by the mechanical oscillation of the ultrasonic wave are not in contact with the impedance of the ultrasonic vibrator when the upper member is not loaded, and the value calculated in advance based on the second measurement result. In the ultrasonic generating device of the above configuration, since the impedance of the intersection point is calculated in advance, the ultrasonic wave can be stably generated by the dog at the target driving frequency f d ' suitable for the ultrasonic generating device. Further, in the above-described ultrasonic generating device, the control unit further has a feature that the measuring unit measures the vibration frequency and the anti-resonance frequency in the impedance frequency characteristic of the ultrasonic transducer based on the measured (four) vibration frequency and the inverse spectral oscillation. The frequency calculates the impedance of the above intersection. In the ultrasonic generating device having the above configuration, since the impedance of the intersection is calculated based on the actually measured wobble frequency and the antiresonant frequency, the influence of the manufacturing variation of the ultrasonic vibrator and the ultrasonic generating device on the target driving rate is reduced. Further, in the above-described ultrasonic generating apparatus, the target driving frequency is expressed by a linear function relating to the frequency of the intersection, and the control unit is characterized in that the target driving frequency is calculated using the linear function. In the ultrasonic generating device of the above structure, the target driving frequency fd is expressed as a linear function related to the frequency fm of the intersection point P, and therefore, the target drive is calculated.

動頻率fd的運算處理就變得簡單,可在短時間内運算^標 驅動頻率f d。 * 2014-8318-PF 35 1317304 ^外’上述超音波產生裝置中’上述目標驅動頻率的 、4疋,该頻率是距離諧振點或反諧振點考慮到外部因夸 影響阻抗頻率特性變動幅度的頻率。 ” 述結構的超音波產生裝置,如上所述,纟需要通過 »又疋γ %驅動頻率fd,判斷是無負载的情況還是有負载的 障況%•,可通過目標驅動頻率fd來測定正在驅動的超音 振子的阻^ z,很容易地對是有負載的情 情況作出判別。 疋',,、員載的 3 ’在上述超音波產生裝置中,上述控制部的特徵 疋述測疋部以多個頻率的電振盪對驅動上述超音 =情況時的多個阻抗進行測定,根據上述多個頻率和: 特十算阻抗頻率的傾斜,基於計算出的阻抗頻率 特性的傾斜,計算上述目標驅動頻率。 丰 牲2上述結構的超音波產生裝置中,由於基於阻抗頻率 特性的傾斜計算目標驅動頻率 # , . ^ 貝半13此,只需測定數個點, 兄時,是2個點的阻抗z即可,因此,能夠更 地運行目標驅動頻率運算處理。 、、 另外’上述超音波產生裝置的特徵是,還具備存儲以 上述目標驅動頻率驅動上述 ,, , , ,+. ^ A $ a波振子時上述無負載時的 抗或上逑有負載時的阻抗的存儲 無負載時或上述有負載時, ,ε ^ ^ 乂上逃測定部測定上述超音祕 振子在驅動狀態下的阻抗, 江超曰波 部中存儲的阻抗進行比較,根^疋出的阻抗和上述存儲 算上述目標驅動頻率,根據較結果,判斷是否計 I亥判斷結果計算上述目標驅動The arithmetic processing of the dynamic frequency fd becomes simple, and the driving frequency f d can be calculated in a short time. * 2014-8318-PF 35 1317304 ^External 'in the above-mentioned ultrasonic generating device', the above target driving frequency, 4疋, the frequency is the distance from the resonance point or the anti-resonance point considering the external variation due to the variation of the impedance frequency characteristic . The ultrasonic generating device of the structure, as described above, needs to pass the » 疋 γ % driving frequency fd to determine whether there is no load or a load failure %•, which can be measured by the target driving frequency fd. The resistance of the supersonic oscillator is easy to discriminate against the condition of the load. 疋',,, 3' in the above-mentioned ultrasonic generating device, the characteristics of the above-mentioned control unit The plurality of impedances at the time of driving the supersonic=the case are measured by electrical oscillations at a plurality of frequencies, and the target is calculated based on the inclination of the calculated impedance frequency characteristic based on the inclination of the plurality of frequencies and the tenth impedance frequency. Driving frequency. In the ultrasonic generating device of the above structure, the target driving frequency is calculated based on the tilt of the impedance frequency characteristic # , . . . , and only a few points are measured, and the brother is 2 points. Since the impedance z is sufficient, the target drive frequency calculation processing can be further operated. Further, the above-described ultrasonic generation device is characterized in that it is further provided with the drive at the target drive frequency. In the above,, , , , +. ^ A $ a wave oscillator when the above-mentioned no-load resistance or the impedance at the time of load on the load is stored without load or when the load is present, the ε ^ ^ 乂 escape measurement unit is measured. The impedance of the above-mentioned supersonic vibrator in the driving state is compared with the impedance stored in the super-wave section of the Jiangchao, and the impedance of the root is extracted and the target driving frequency is calculated as described above, and based on the comparison result, it is judged whether or not the result of the judgment is calculated. Calculate the above target drive

2014-8318-PF 36 1317304 頻率 上述結構的超音波產生裝置,在沒有周圍環境變化, 谐振點及反諧振點大致固定較為穩定時,無 _ 句3¾订目標艇 動頻率運算處理。 ^ 而且,本發明其他實施例有關的超音波美容裝置 徵是使用了上述超音波產生裝置中的其中之一。 、特 以上結構的料波美容裝置能肖以目標驅動 地發生超音波。因,匕,超音波美容裝置能夠有效地對:: 物0給予美容效果。 牛 為了介紹本申請發明,前面參照附圖,通過實施 订了恰當、充分地說明。作為同行應認識到能夠 =述實施例進行更改及/或改進。因此,由同行實二更也 2=或;:進方案只要沒有超出申請專利範圍書中的 岸nfiL可讀料該更改方案或改進方案包括在相 應申明專利靶圍書的權利範圍内。 【圖式簡單說明】 :;(A)〜(c)是說明本發明的基本内容的示意圖。 方2 示實施例所有關的超音波產生裝置的結構的 動頻示實施例所有關的超音波產生裝置的目標驅 動頻革運异處理中的操作的流程圖。 圖4是說明目標驅動頻率的示意圖。 圖5是表示基於諸振點及反譜振點,先計算交點的頻2014-8318-PF 36 1317304 Frequency The ultrasonic generating device of the above configuration does not have a _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ _ Further, the ultrasonic cosmetic device according to another embodiment of the present invention is one of the above-described ultrasonic generating devices. The material wave beauty device of the above structure can generate ultrasonic waves with a target drive. Because, 匕, the ultrasonic beauty device can effectively give a beauty effect to: In order to introduce the invention of the present application, the foregoing description has been appropriately and fully described with reference to the accompanying drawings. As a peer, it should be recognized that changes and/or improvements can be made to the embodiments. Therefore, by the peers, the second is also 2; or; as long as the program does not exceed the scope of the patent application, the modification plan or improvement plan is included in the scope of the rights of the corresponding patent target book. BRIEF DESCRIPTION OF THE DRAWINGS: (A) to (c) are schematic views for explaining the basic contents of the present invention. Fig. 2 is a flow chart showing the operation of the target drive driving process of the ultrasonic generating device according to the embodiment of the ultrasonic generating device according to the embodiment. 4 is a schematic diagram illustrating a target driving frequency. Figure 5 shows the frequency of calculating the intersection point based on the vibration points and the anti-spectral vibration points.

2014-8318-PF 37 1317304 率, 再計算目標驅動頻率的流程圖。 點的阻抗 圖6是表示基於諧振點及反諧振點,計算交 的流種圖。 圖7是表示基於阻抗頻率特性的傾斜,先計算交 率 、再计算目標驅動頻率的流程圖。 巷圖8(A) 、(B)是表示基於阻抗偏 目榡驅動頻率運算處理的流程圖。 圖9是表示超音波產生裝置用於超音 的局部剖視圖。 點的 移判斷是否運行 波美容裝置例子 圖1 〇 ( A )、( β )是表示背景技術所有關的超音波彦 裝置結構的示意圖。 圖11 ( A) 、( Β )是表示背景技術所有關的超音 生裝置結構的示意圖。 圖 圖 示意 圖1 2 ( A )、( B )是表示超音波振盪塊的特性的示意 圖13 ( A )、( B)是表示超音波振盪塊的特性的示音 圖14(A) 、(B)是表示超音波振動塊的振動模式的 【主要元件符號說明】 1、 500A、500B〜超音波產生裝置; 2、 23〜超音波振盪塊; 11、511A、511B~驅動部; 2014-8318-PF 38 -1317304 12、512A、512B〜超音波振子; 1 3、51 3 A、51 3 B 〜'^刺 0八; 14〜測定部; 1 5 ~控制部; 1 6〜存儲部; • 20~超音波美容裝置; . 21〜機殼(收容容器); 2 2〜電路塊; Φ 112~放大電路; 113〜振盪電路; 141〜電流檢測電路; ' 142〜阻抗運算部; - 143〜頻率控制部; 151〜頻率運算部; 152〜電壓控制部; 153〜驅動頻率控制部; ® 513-1A、513-1B〜接合面; 513-2A、513-2B〜放射面; 514A〜粘接劑; 514 B〜螺栓。 392014-8318-PF 37 1317304 Rate, a flow chart for calculating the target drive frequency. Point impedance Figure 6 is a flow diagram for calculating the intersection based on the resonance point and the anti-resonance point. Fig. 7 is a flow chart showing the calculation of the intersection rate based on the impedance frequency characteristic and the calculation of the target drive frequency. Lanes 8(A) and (B) are flowcharts showing the calculation process based on the impedance bias 榡 drive frequency. Fig. 9 is a partial cross-sectional view showing the ultrasonic generating device for supersonic. The point shift is judged whether or not the wave cosmetic device is operated. Fig. 1 〇 (A), (β) are schematic diagrams showing the structure of the ultrasonic wave device related to the background art. Figures 11(A) and (() are schematic diagrams showing the structure of a supersonic device related to the background art. Schematic diagrams 1 2 (A) and (B) are diagrams showing the characteristics of the ultrasonic oscillation block. 13 (A) and (B) are diagrams 14(A) and (B) showing the characteristics of the ultrasonic oscillation block. It is a description of the main component symbols indicating the vibration mode of the ultrasonic vibration block. 1. 500A, 500B to ultrasonic generation devices; 2. 23 to ultrasonic oscillation blocks; 11, 511A, 511B to drive units; 2014-8318-PF 38 - 1317304 12, 512A, 512B ~ ultrasonic vibrator; 1 3, 51 3 A, 51 3 B ~ '^ thorn 0 eight; 14 ~ measurement unit; 1 5 ~ control unit; 1 6 ~ storage unit; Ultrasonic beauty device; . 21 ~ casing (housing container); 2 2 ~ circuit block; Φ 112 ~ amplification circuit; 113 ~ oscillation circuit; 141 ~ current detection circuit; ' 142 ~ impedance calculation unit; - 143 ~ frequency control 151 to frequency calculation unit; 152 to voltage control unit; 153 to drive frequency control unit; ® 513-1A, 513-1B to joint surface; 513-2A, 513-2B to radiation surface; 514A to adhesive; 514 B ~ bolts. 39

2014-8318-PF2014-8318-PF

Claims (1)

,1317304 十、申請專利範圍: 1-種超音波產生裝置,其特徵在於包括: 驅動部,生成電振盪; ,音波振子’將上述驅動部生成的上述電振盈轉換成 超曰波的機械振盪; 立,輪構件’一個面上接合上述超音波振子,將上述超 , 振子轉換的上述超音波的機械《傳輸到另-個面上 的放射面上; wI _ 敎部,敎上述超音波振子的阻抗; 接觸?:部’基於應傳輸上述超音波的機械振盪的對象物 -特心輸構件的有負载時上述超音波振子的阻抗頻率 傳幹構件2上述超音波的機械振盈的物件物不接觸上述 2件的無負載時上述超音波振子的阻抗頻率特性的交 的阻抗以及上述測定部測定的阻抗,計算岸驅動上述 超音波振子的目標驅動頻率…動上述 趙立、、古尨工斤 貝手控制上述驅動部’使得上述 S/振子Μ异出的該目標驅動頻率振盪。 2.如切專利範圍第Μ所述的 中上述測定部基於上述驅動部在上述超音波其 ,電壓時流入上述超音波振子㈣流,測 盪的對象物接觸上述傳輸構件的有負載機械振 羊们生及應傳輸上述超音波的機械振蘯的物件物 2014-8318-PF 40 •1317304 率料W:豸傳輪構件的無負載時上述超音波振子的阻抗頻 辜特性,根據該測定結果預先計算出的值。 中上2申請專利範圍第1項所述的超音波產生裝置,其 頻㈣Γ部還由上述測定部測定上述超音波振子的阻抗 的諸振頻率及反譜振頻率,基於該測定到的譜 1率及反諧振頻率計算上述交點的阻抗。 φ μ,t月專利範圍第1項所述的超音波產生裝置,A 函數返目標驅動頻率表述為與上述交點的頻率相關的線性 率 上述控制部使用上述線性函數計算上述目標驅動頻 中上請專利範圍第1項所述的超音波產生裝置,其 到外部因素對阻。 振點或諧振點幅度為考慮 ’、,^ V員率特性變化影響的頻率。 中上專利範圍第1項所述的超音波產生裝置,宜 動二=述测定部測定以多個頻率的電_驅 勒上这超曰波振子的情況時的多, 率和上述多個頻率計算阻抗頻率的傾斜 J多個頻 抗頻率特性的傾斜 叙、於計算出的阻 处s彳示驅動頻率。 中還專利範圍第1項所述的超音波產生裳置,直 二,存儲以上述目標驅動頻率驅動 波: =時的阻抗或上述有負載時的阻抗的存::子時 上述控制部由上述測定部對上述 H 载時在上述超音波、夺或上述有負 皮振子的驅動狀態下的阻抗進行測定,對 2014-8318-PF 41 1317304 測定的該阻抗和存儲名μ、+. +以 开碎在上述存儲部中的阻抗 據比較的結果判斷〇計算上述目標 ^ ^ 斷結果計算上述目標㈣㈣。 +根心 二:!超音波美容裝置,其特徵在於:使用申請專 軌圍第1至8項中任一項所述的超音波產生裝置。 裉 匈 利, 1317304 X. Patent application scope: 1-type ultrasonic generating device, characterized in that: the driving portion generates an electric oscillation; and the acoustic vibrator converts the electric vibration generated by the driving portion into a super-chopping mechanical oscillation The vertical member of the wheel member is joined to the ultrasonic vibrator on one surface, and the supersonic wave-converted mechanical device "transferred to the other surface"; wI _ 敎 portion, 敎 the above-mentioned ultrasonic vibrator Impedance; contact? : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : When the load is not applied, the impedance of the impedance frequency characteristic of the ultrasonic transducer and the impedance measured by the measuring unit calculate the target driving frequency of the ultrasonic transducer. The above-mentioned Zhao Li, the ancient 斤 斤 贝 控制 control The drive unit oscillates the target drive frequency in which the S/vibrator is different. 2. The measurement unit according to the third aspect of the invention, wherein the driving unit flows into the ultrasonic vibrator (four) in a voltage at the time of the ultrasonic wave, and the object to be oscillated contacts the load-bearing mechanical vibration of the transmission member. We generate and transmit the mechanically vibrated object of the above-mentioned ultrasonic wave 2014-8318-PF 40 •1317304 Rate material W: The impedance frequency characteristic of the above-mentioned ultrasonic vibrator when there is no load on the transmission wheel member, based on the measurement result The calculated value. In the ultrasonic generating device according to the first aspect of the invention, wherein the frequency (four) crotch portion is further configured by the measuring unit, the vibration frequency and the inverse spectral frequency of the impedance of the ultrasonic vibrator are measured, and based on the measured spectrum 1 The rate and the anti-resonant frequency are used to calculate the impedance of the above intersection. φ μ, the ultrasonic generating device according to the first aspect of the patent range, the A function return target driving frequency is expressed as a linear rate related to the frequency of the intersection point, and the control unit calculates the target driving frequency using the linear function. The ultrasonic generating device according to the first aspect of the patent, which is resistant to external factors. The amplitude of the vibration point or resonance point is the frequency that takes into account the influence of the change in the characteristics of the '', '' In the ultrasonic generating device according to the first aspect of the invention, the measuring unit measures the electric power at a plurality of frequencies, and the rate and the plurality of frequencies. Calculate the slope of the impedance frequency and the slope of the multiple frequency-response frequency characteristics. The calculated resistance s indicates the driving frequency. The ultrasonic wave generated in the first aspect of the patent range is generated, and the second drive is used to store the drive wave at the target drive frequency: the impedance at the time of the load or the impedance at the time of the load: The measuring unit measures the impedance in the driving state of the ultrasonic wave or the negative skin vibrator at the time of the H load, and the impedance and the memory name μ, +. + measured in 2014-8318-PF 41 1317304 are opened. The impedance in the storage unit is judged based on the result of the comparison, and the target (4) (4) is calculated by calculating the target result. + Roots 2:! The ultrasonic wave-splitting device is characterized in that the ultrasonic wave generating device according to any one of the items 1 to 8 is applied.匈 Hungary 2014-8318-PF 422014-8318-PF 42
TW095133830A 2005-09-27 2006-09-13 Supersonic wave cosmetology apparatus with supersonic wave generator TW200714376A (en)

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