JP2751156B2 - Control device for electromagnetic vibrator - Google Patents

Control device for electromagnetic vibrator

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Publication number
JP2751156B2
JP2751156B2 JP62099420A JP9942087A JP2751156B2 JP 2751156 B2 JP2751156 B2 JP 2751156B2 JP 62099420 A JP62099420 A JP 62099420A JP 9942087 A JP9942087 A JP 9942087A JP 2751156 B2 JP2751156 B2 JP 2751156B2
Authority
JP
Japan
Prior art keywords
electromagnetic vibrator
power supply
circuit
excitation coil
current
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Expired - Fee Related
Application number
JP62099420A
Other languages
Japanese (ja)
Other versions
JPS63267608A (en
Inventor
丈義 野中
敏郎 関根
嘉昭 大倉
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Shinko Electric Co Ltd
Original Assignee
Shinko Electric Co Ltd
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Shinko Electric Co Ltd filed Critical Shinko Electric Co Ltd
Priority to JP62099420A priority Critical patent/JP2751156B2/en
Publication of JPS63267608A publication Critical patent/JPS63267608A/en
Application granted granted Critical
Publication of JP2751156B2 publication Critical patent/JP2751156B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

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Description

【発明の詳細な説明】 [産業上の利用分野] 本発明は、励磁コイルと、これに断続電流を供給する
制御回路を備えた電磁フィーダ、パーツフィーダ、バイ
ブレータなどの電磁振動機の制御装置に関するものであ
る。 [従来技術] 一般に電磁振動機は、電磁石とばねとの組合わせ機構
において、周期的に励磁コイルに励磁電流を断続的に供
給し、断続的に発生する磁気吸引力とばねの復元力との
相互作用により振動作用を得る。このように電磁振動機
用励磁コイルに周期的に電流を供給する手段は、上記励
磁コイルに商用周波数の全波ないし半波整流電圧を供給
することが行われている。この際、上記ばねは商用周波
数(半波整流時)又は商用周波数の2倍(全波整流時)
にて共振すべく積層枚数の変更ないしばねの変更などに
より共振するように調整されている。このばね調整は、
面倒であるばかりか、かなりの熟練を要することになる
が、このばね調整を省くためには、可変周波数電源とし
て単相インバータ回路を用いて周波数調整にて代換えが
可能である。この単相インバータによる制御手段を備え
た電磁振動機は第3図に示す通りである。同第3図にお
いて、1は直流電源で、商用電源電圧を整流のうえ、平
滑コンデンサでリップルを除去するなどにより構成され
る。2は逆変換回路で、4個のスイッチング素子として
のトランジスタ2T1〜2T4及び4個のダイオード2D1〜2D4
を図示の接続にて構成している。そして、この逆変換回
路2の入力側には上記直流電源1が接続され、出力側に
は電磁振動機用励磁コイル3が接続される。4は上記逆
変換回路2中のトランジスタ2T1〜2T4用ベース駆動回路
である。 上記構成において、各トランジスタ2T1〜2T4はベース
駆動回路4の作用を伴い、例えば周知のPWM方式に基づ
く逆変換作用をなし、電磁振動機用励磁コイル3に所望
の周波数の交流電圧を印加する。このとき、上記励磁コ
イル3には、上記交流電圧に対しほぼ90度遅れの電流が
供給され、励磁コイル3への流入電流の方向は逆変換回
路2の出力周波数に応じて変化する。 この際、励磁コイル3へのいづれの方向に電流が流入
しても磁気吸引力が得られるので、この磁気吸引力と、
電磁振動機の有するばねの復元力との相互作用にて逆変
換回路2の出力周波数の2倍の振動を発生する。 [発明が解決しようとする課題] 上記第3図に示す電磁振動機の制御回路においては、
通常の単相インバータとしてのトランジスタなどの4個
のスイッチング素子を要し、かつこれらのスイッチング
素子の駆動回路及び当該駆動回路用電源を要する。ま
た、とりわけPWM制御を採用する場合、電圧の極性切替
え時においても電圧レベルは減少することなく一定であ
ることに関連して、各スイッチング素子のアーム短絡防
止のために一対のスイッチング素子の導通切替え時点に
おいて十分なデッドタイムを設ける必要が生じ、スイッ
チング素子の制御が複雑化する傾向があった。 [課題を解決するための手段] 本発明は、電磁振動機の有する特有の性質としての
電磁振動機用励磁コイルがほぼ純粋の誘導負荷であるこ
と、当該励磁コイルに流れる電流の方向は動作上何ら
影響を受けないなどに注目してなされたものである。即
ち、本発明は電磁振動機用励磁コイルに一方向に規制さ
れた励磁電流を断続的に供給する制御装置を要旨とし、
その目的は、 (A)電磁振動作用を担う励磁コイル (B)前記励磁コイルの各端子から、それぞれ独立のス
イッチング素子を介して直流電源に、当該直流電源から
上記励磁コイルに電流が供給される極性にて接続される
回路手段 (C)上記各スイッチング素子に直列に、かつ上記直流
電源に対して逆極性に接続され上記直流電源と上記励磁
コイルとで閉回路を構成する2個のダイオード (D)上記励磁コイルに対して、一定方向の電流を一定
周期にて供給するように各スイッチング素子をPWM制御
するための駆動回路。 からなる電磁振動機用制御装置によって達成される。 [作用] 2個のスイッチング素子(トランジスタ)の制御に基
づき、電磁振動機用励磁コイルに対し、PWM方式にて得
られる交流電圧を印加し常に一定方向の電流を上記励磁
コイルに断続的に与えることにより磁気吸引力を断続的
に与え、ばねの復元力との相互作用にて加振力を得る。 [実施例] 以下、第1図に示す実施例について具体的に説明す
る。同第1図において、11は直流電源である。12は逆変
換回路で、トランジスタ12T1、12T2及びダイオード12
D1、12D2を図示の通りにブリッジ接続し、入力側を上記
直流電源に接続している。そして、この逆変換回路12の
出力点P1、P2は電磁振動機用励磁コイル13の各入力端子
に接続される。14はトランジスタ12T1、12T2のベース駆
動回路で、PWM制御を担うための構成要素として三角波
発生器、正弦波発生器、コンパレータ及び極性反転回路
などからなる周知の回路手段によって構成される。 上記構成において、ベース駆動回路がトランジスタ12
T1、12T2に対してPWM制御を行う過程において電磁振動
機用励磁コイル13には第2図(イ)に示す通りの出力を
得る。この出力の発生は、出力端P1において、トラン
ジスタ12T1がオフ時は出力0電位(以下、“L"と称す
る)、オン時は直流電源11の電位(以下、“H"と称す
る)となること、出力端P2において、トランジスタ12
T2オフ時は“H"、オン時は“L"となることの組合わせに
よって達成される。即ち、出力端P1が“H"で、出力端P2
が“L"のときに正方向の電圧が出され、出力端P1が“L"
出力端P2が“H"のときは負方向の電圧が得られる。 一方、出力端P1、P2が共に“L"又は“H"のときは出力
が0になるように規制される。このようなトランジスタ
12T1、2T2のPWM制御に基づき上記第2グラフ(イ)にて
示す出力が励磁コイル13に与えられたとすると、この実
効正弦波は第2グラフ(ロ)に示される通りに得られ
る。これによって励磁コイル13への流入電流は出力端P1
が“H"出力端P2が“L"のときは直流電流11→トランジス
タ12T1→励磁コイル13→トランジスタ12T2→直流電源11
の閉回路に流れ、出力端P1が“L"、出力端P2が“H"のと
きは励磁コイルが電流減となり、励磁コイル13→ダイオ
ード12D1→直流電源11→ダイオード12D2→励磁コイル13
の閉回路に流れる。以上の動作に基づき、電磁振動機用
励磁コイル13に対して一方向に断続的に電流を与え、電
磁振動機に備えられているばねの復元力と電磁石の相互
作用をなし、電磁振動機を駆動する。 [効果] 以上述べたように、本発明に係る電磁振動機用制御装
置は電磁振動機の有する特性(ばねの共振による減衰を
補償するに足るだけのごく僅かのエネルギー供給で動作
する)を巧みに利用して、この電磁振動機用励磁コイル
への電力供給を担い、一方向のみに断続電流を供給する
制御装置の構成を要旨としている。これに伴い、従来用
いられた単相インバータ回路に比スイツチング素子は4
個から2個に半減し、かつ従来の単相全波インバータ回
路であって、PWM制御においては、アーム短絡防止のた
め相応のデッドタイムを設ける考慮が不要で、これらス
イッチング素子の駆動回路の簡素化を図ることができる
実利かある、。 さらに、従来のように電磁振動機用コイルに流れる電
流方向を変える全波整流用単相インバータ回路により電
磁振動機用励磁コイルを駆動する場合と、同一加振力を
与えるに要する実効電流を比較してみると、スイッチン
グ素子を通じて流出する電流の最大値を2Idcとすれば従
来の全波整流形単相インバータ回路では、 となり、これに対して本発明に係わる制御装置では、 となる。 従って、電磁振動機に同一加振力を与えるに要する実
効電流は約86%に減少する。
Description: BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a control device for an electromagnetic vibrator such as an electromagnetic feeder, a parts feeder, and a vibrator provided with an exciting coil and a control circuit for supplying an intermittent current thereto. Things. [Prior Art] In general, an electromagnetic vibrator uses a combination mechanism of an electromagnet and a spring to intermittently supply an exciting current to an exciting coil intermittently to generate an intermittent magnetic attraction force and a spring restoring force. Vibration is obtained by the interaction. As described above, the means for periodically supplying a current to the excitation coil for the electromagnetic vibrator supplies a full-wave or half-wave rectified voltage of a commercial frequency to the excitation coil. At this time, the spring is used at the commercial frequency (at half-wave rectification) or twice the commercial frequency (at full-wave rectification).
In order to resonate, it is adjusted to resonate by changing the number of layers or changing the spring. This spring adjustment
Not only is it troublesome, but also requires considerable skill, but in order to omit this spring adjustment, a single-phase inverter circuit can be used as a variable frequency power supply, which can be replaced by frequency adjustment. The electromagnetic vibrator provided with the control means by this single-phase inverter is as shown in FIG. In FIG. 3, reference numeral 1 denotes a DC power supply, which is configured by rectifying a commercial power supply voltage and removing a ripple with a smoothing capacitor. 2 is the inverse transform circuit, the transistor 2T 1 ~2T 4 and four diodes 2D 1 ~2D 4 as four switching elements
Are configured with the connections shown. The DC power supply 1 is connected to the input side of the inverse conversion circuit 2, and the excitation coil 3 for the electromagnetic vibrator is connected to the output side. 4 is a base driving circuit transistor 2T 1 ~2T 4 in the inverse transform circuit 2. Applying the above configuration, each transistor 2T 1 ~2T 4 involves the operation of the base drive circuit 4, for example, an inverted transformation action based on the well-known PWM method, an AC voltage of desired frequency electromagnetic vibration machine excitation coil 3 I do. At this time, a current delayed by approximately 90 degrees with respect to the AC voltage is supplied to the exciting coil 3, and the direction of the current flowing into the exciting coil 3 changes according to the output frequency of the inverse conversion circuit 2. At this time, even if a current flows in either direction to the excitation coil 3, a magnetic attraction force can be obtained.
Interaction with the restoring force of the spring of the electromagnetic vibrator generates a vibration twice the output frequency of the inverse conversion circuit 2. [Problem to be Solved by the Invention] In the control circuit of the electromagnetic vibrator shown in FIG.
It requires four switching elements such as transistors as ordinary single-phase inverters, and requires a drive circuit for these switching elements and a power supply for the drive circuit. In particular, when PWM control is employed, the voltage level is not reduced and remains constant even when the polarity of the voltage is switched, so that the conduction switching of a pair of switching elements is performed to prevent an arm short circuit of each switching element. It is necessary to provide a sufficient dead time at the time, and control of the switching element tends to be complicated. [Means for Solving the Problems] According to the present invention, the exciting coil for the electromagnetic vibrator as a unique property of the electromagnetic vibrator is an almost pure inductive load, and the direction of the current flowing through the exciting coil is different from the operation. It was made with a focus on being unaffected. That is, the gist of the present invention is a control device that intermittently supplies an excitation current regulated in one direction to an excitation coil for an electromagnetic vibrator,
The objectives are as follows: (A) an excitation coil that performs an electromagnetic vibration action; (B) a current is supplied from each terminal of the excitation coil to a DC power supply via an independent switching element, and from the DC power supply to the excitation coil. Circuit means (C) two diodes connected in series with each of the switching elements and having opposite polarities to the DC power supply and forming a closed circuit with the DC power supply and the exciting coil ( D) A drive circuit for performing PWM control of each switching element so as to supply a current in a constant direction to the excitation coil at a constant cycle. This is achieved by an electromagnetic vibrator control device comprising: [Operation] Based on the control of two switching elements (transistors), an alternating voltage obtained by a PWM method is applied to the excitation coil for the electromagnetic vibrator, and a current in a constant direction is intermittently applied to the excitation coil. Thereby, a magnetic attraction force is intermittently applied, and an exciting force is obtained by interaction with the restoring force of the spring. [Example] Hereinafter, the example shown in Fig. 1 will be specifically described. In FIG. 1, reference numeral 11 denotes a DC power supply. Reference numeral 12 denotes an inverse conversion circuit, which includes transistors 12T 1 and 12T 2 and a diode 12
D 1 and 12D 2 are bridge-connected as shown, and the input side is connected to the DC power supply. Then, output points P 1 and P 2 of the inverse conversion circuit 12 are connected to respective input terminals of the excitation coil 13 for the electromagnetic vibrator. Reference numeral 14 denotes a base drive circuit of the transistors 12T 1 and 12T 2 , which is constituted by well-known circuit means including a triangular wave generator, a sine wave generator, a comparator, a polarity inversion circuit, and the like as components for performing PWM control. In the above configuration, the base drive circuit is
In the process of performing the PWM control on T 1 and 12T 2 , an output as shown in FIG. Generation of the output, at the output P 1, when transistor 12T 1 is turned off the output zero potential (hereinafter, referred to as "L"), during the on the potential of the DC power supply 11 (hereinafter, referred to as "H") and It becomes possible, at the output end P 2, transistor 12
T 2 off at the time of "H", on-time is achieved by a combination of that becomes "L". That is, the output terminal P 1 is “H” and the output terminal P 2
There "L" voltage of the positive direction is issued when the output terminal P 1 is "L"
When the output P 2 is "H" voltage in the negative direction is obtained. On the other hand, when the output terminals P 1 and P 2 are both “L” or “H”, the output is regulated to be 0. Such a transistor
Assuming that the output shown in the second graph (a) is given to the excitation coil 13 based on the PWM control of 12T 1 and 2T 2 , this effective sine wave is obtained as shown in the second graph (b). As a result, the current flowing into the exciting coil 13 is reduced to the output terminal P 1
When the but "H" output P 2 is "L" DC current 11 → transistor 12T 1 → exciting coil 13 → transistor 12T 2 → DC power source 11
Flows in the closed circuit, the output end P 1 is "L", the exciting coil when the output terminal P 2 is "H" becomes current decrease, the exciting coil 13 → diode 12D 1 → DC power source 11 → diode 12D 2 → excitation Coil 13
Flows into a closed circuit. Based on the above operation, a current is intermittently applied in one direction to the excitation coil 13 for the electromagnetic vibrator, and the interaction between the electromagnet and the restoring force of the spring provided in the electromagnetic vibrator is performed. Drive. [Effects] As described above, the control device for an electromagnetic vibrator according to the present invention skillfully utilizes the characteristics of the electromagnetic vibrator (operates with a very small energy supply sufficient to compensate for the damping due to the resonance of the spring). The gist of the present invention is to supply power to the exciting coil for the electromagnetic vibrator and supply a discontinuous current in only one direction. Accordingly, the number of switching elements is four compared to the conventional single-phase inverter circuit.
It is a conventional single-phase full-wave inverter circuit that halves the number from two to two. In PWM control, there is no need to consider providing an appropriate dead time to prevent arm short-circuiting, and the drive circuit for these switching elements is simplified. Practical that can be achieved. Furthermore, the effective current required to apply the same excitation force is compared with the case where the excitation coil for the electromagnetic vibrator is driven by a single-phase inverter circuit for full-wave rectification that changes the direction of the current flowing through the coil for the electromagnetic vibrator as before. Assuming that the maximum value of the current flowing through the switching element is 2Idc, in the conventional full-wave rectification type single-phase inverter circuit, On the other hand, in the control device according to the present invention, Becomes Therefore, the effective current required to apply the same exciting force to the electromagnetic vibrator is reduced to about 86%.

【図面の簡単な説明】 第1図は本発明の実施例を示す回路図、第2図は動作を
説明するためのグラフ、第3図は従来の回路図である。 11……直流電源 12……逆変換回路 12T1、12T2……トランジスタ 12D1、12D2……ダイオード 13……電磁振動機用励磁コイル 14……ベース駆動回路
BRIEF DESCRIPTION OF THE DRAWINGS FIG. 1 is a circuit diagram showing an embodiment of the present invention, FIG. 2 is a graph for explaining the operation, and FIG. 3 is a conventional circuit diagram. 11 DC power supply 12 Inverting circuits 12T 1 and 12T 2 Transistors 12D 1 and 12D 2 Diode 13 Excitation coil for electromagnetic vibrator 14 Base drive circuit

Claims (1)

(57)【特許請求の範囲】 1.次の各項(A〜D)の構成要素を備えた電磁振動機
の制御装置 (A)電磁振動作用を担う励磁コイル (B)前記励磁コイルの各端子から、それぞれ独立のス
イッチング素子を介して直流電源に、当該直流電源から
上記励磁コイルに電流が供給される極性にて接続される
回路手段 (C)上記各スイッチング素子に直列に、かつ上記直流
電源に対して逆極性に接続され上記直流電源と上記励磁
コイルとで閉回路を構成する2個のダイオード (D)上記励磁コイルに対して、一定方向の電流を一定
周期にて供給するように各スイッチング素子をPWM制御
するための駆動回路。
(57) [Claims] A control device for an electromagnetic vibrator having the following components (A to D): (A) an exciting coil that performs an electromagnetic vibration action; and (B) an excitation coil that performs an electromagnetic vibration action. Circuit means (C) connected to the DC power supply in a polarity in which a current is supplied from the DC power supply to the exciting coil. (C) The DC means connected in series to the switching elements and in the opposite polarity to the DC power supply. Two diodes (D) forming a closed circuit with a power supply and the excitation coil (D) A drive circuit for performing PWM control of each switching element so as to supply a current in a constant direction to the excitation coil at a constant cycle. .
JP62099420A 1987-04-21 1987-04-21 Control device for electromagnetic vibrator Expired - Fee Related JP2751156B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP62099420A JP2751156B2 (en) 1987-04-21 1987-04-21 Control device for electromagnetic vibrator

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP62099420A JP2751156B2 (en) 1987-04-21 1987-04-21 Control device for electromagnetic vibrator

Publications (2)

Publication Number Publication Date
JPS63267608A JPS63267608A (en) 1988-11-04
JP2751156B2 true JP2751156B2 (en) 1998-05-18

Family

ID=14246978

Family Applications (1)

Application Number Title Priority Date Filing Date
JP62099420A Expired - Fee Related JP2751156B2 (en) 1987-04-21 1987-04-21 Control device for electromagnetic vibrator

Country Status (1)

Country Link
JP (1) JP2751156B2 (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH02205488A (en) * 1989-02-03 1990-08-15 Fujitsu Ltd Searching method for original point

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
AT374631B (en) * 1981-09-15 1984-05-10 Elin Union Ag FLOW CONVERTER

Also Published As

Publication number Publication date
JPS63267608A (en) 1988-11-04

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