JPH0243118A - Electromagnetic oscillation feeder - Google Patents

Electromagnetic oscillation feeder

Info

Publication number
JPH0243118A
JPH0243118A JP18988788A JP18988788A JPH0243118A JP H0243118 A JPH0243118 A JP H0243118A JP 18988788 A JP18988788 A JP 18988788A JP 18988788 A JP18988788 A JP 18988788A JP H0243118 A JPH0243118 A JP H0243118A
Authority
JP
Japan
Prior art keywords
trough
mass
base
electromagnet
reaction force
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.)
Pending
Application number
JP18988788A
Other languages
Japanese (ja)
Inventor
Takeyoshi Nonaka
野中 丈義
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 JP18988788A priority Critical patent/JPH0243118A/en
Publication of JPH0243118A publication Critical patent/JPH0243118A/en
Pending legal-status Critical Current

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Abstract

PURPOSE:To make close to zero (0) the reaction force of an electromagnetic oscillation feeder to the installation ground by fixing a drive electromagnet to one of a trough and an opposed mass arranged below the trough, while fixing a contact electrode element to the other, and arranging slant plate springs between the trough and a base and between the opposed mass and the base. CONSTITUTION:An electromagnet 22 is monolithically mounted on a balance weight 19 extending laterally in a line below a trough part 2. This weight 19 is coupled to a basic block 17 through a pair of right and left flat springs. In an L-shaped movable core 14, its horizontal part 14c is arranged in opposition to the magnetic pole face of the magnet 22 and is mounted on a flat spring mounting blocks 12a, 12b of the trough part 2 through arm parts 14a, 14b formed at a vertical part 14d. With this arrangement, both the trough and the opposed mass oscillated, respectively, with a mutual phase difference of 180 degrees so that thereaction force to the base can be made zero (0) substantially. It is thus possible to make the reaction force to the installation ground zero (0).

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は電磁振動フィーダに関する。[Detailed description of the invention] [Industrial application field] The present invention relates to an electromagnetic vibration feeder.

〔従来技術及びその問題点〕[Prior art and its problems]

第5図は電磁振動フィーダの従来例を示すものであるが
、トラ76υは駆動側ウェイ) C37Jと前後−対の
傾斜板はね關割により結合されている。そして駆動側ウ
ェイトr33は防振はね(至)(ロ)により地上に支持
されている。駆動側ウェイ) C321には支持部材(
ト)を介してコイル(至)を巻装させた電磁石Cηが取
付けられておシ、これと空隙をおいて接極子−がトラフ
3υ側に固定されている。公知のようにコイル国に交流
を通電すると交番吸引力が電磁石Cηと接極子關との間
に発生し、これによってトラフGυははゾ板ばね口割に
長手方向に対しはゾ垂直方向に振動を行う。
FIG. 5 shows a conventional example of an electromagnetic vibration feeder, in which a tiger 76υ is connected to a driving side way C37J and a pair of front and rear inclined plates by a spring joint. The drive side weight r33 is supported on the ground by anti-vibration springs (to) (b). drive side way) C321 has a support member (
An electromagnet Cη having a coil (to) wound thereon is attached via the armature Cη, and an armature Cη is fixed to the trough 3υ side with a gap between the electromagnet Cη and the electromagnet Cη. As is well known, when an alternating current is applied to the coil, an alternating attractive force is generated between the electromagnet Cη and the armature, which causes the trough Gυ to vibrate in the direction perpendicular to the longitudinal direction of the leaf spring. I do.

然るに地上にはトラフ(Illの振動によシ板はね曽を
介して反力が伝達され、これによシ防振ばね曳(至)に
よ)防振を行っているとはいえ駆動側ウェイトr33の
振巾に応じて反力が地上に伝達される。今、トラフ例の
質量をm、及び駆動側ウェイ) I33の質量をm、及
びトラフ(IIIの振巾をxl及び駆動側ウェイト田の
振巾をX、とした場合、Tnt / mt = X! 
/xt  という関係が成立する。即ち、X! = m
、 7m2 X xl  である。従って地上に伝わる
反力は防振ばね(ロ)のばね定数をに、とすると、kt
 xxl  となる。この式から解るように反力を小さ
くするためには、防振ばね(ロ)のばね定数に、を小さ
くして、質量町 を大きくすればよいのであるが、ばね
定数に、を小さくするということは防振による支持が非
常に不安定となシ、この振動フィーダ全体がふらふらし
て不安定となる。従ってトラフ3υ内で移送される部品
又は材料の状態を不安定とする。又、駆動側ウェイ)・
3zの質量町を大きくすることも考えられるが、これで
は振動フィーダの全体の質量は大きくな夛、つまシ取扱
いが不便となる。又、材料コストの上昇と\もに装置コ
ストを上昇させ、又、駆動側ウェイトC33の質量を大
きくするといっても限界がある。
However, even though vibration isolation is carried out on the ground by the trough (the reaction force is transmitted through the vibration isolation plate and the vibration isolation spring tension), the drive side The reaction force is transmitted to the ground according to the swing width of the weight r33. Now, if the mass of the trough example is m, the mass of the drive side weight field is m, the width of the trough (III) is xl, and the width of the drive side weight field is X, then Tnt / mt = X!
/xt holds true. That is, X! = m
, 7m2 X xl. Therefore, the reaction force transmitted to the ground is kt, assuming that the spring constant of the anti-vibration spring (b) is
xxl becomes. As can be seen from this equation, in order to reduce the reaction force, the spring constant of the anti-vibration spring (b) should be made smaller, and the mass should be made larger. This means that the support provided by vibration isolation is extremely unstable, and the entire vibrating feeder becomes unstable. This makes the state of the parts or materials transported within the trough 3υ unstable. Also, drive side way)・
It may be possible to increase the mass of 3z, but this would increase the overall mass of the vibrating feeder and make handling the pick inconvenient. Moreover, the increase in material cost also increases the device cost, and there is a limit to increasing the mass of the drive side weight C33.

〔発明が解決しようとする問題点〕[Problem that the invention seeks to solve]

本発明は上記問題に鑑みてなされ、コストをそれほど上
昇させることなく、これが設置される地上への反力をほ
とんど零とすることができる電磁振動フィーダを提供す
ることを目的とする。
The present invention has been made in view of the above problems, and an object of the present invention is to provide an electromagnetic vibration feeder that can reduce the reaction force to the ground where it is installed to almost zero without significantly increasing the cost.

〔課題を解決するための手段〕[Means to solve the problem]

上記目的は、トラフと、該トラフを基台に結合する前後
一対の第1傾斜板ばねと、前記トラフの下方に配設され
る対向質量と、該対向質量を前記基台に結合する前後一
対の第2傾斜板ばねと、前記トラフと前記対向質量との
うち一方に固定される駆動電磁石と、他方に固定され、
前記駆動電磁石に吸引される接極子とから成る電磁振動
フ4−ダによシ達成される。
The above object includes a trough, a pair of front and rear first inclined leaf springs that connect the trough to the base, a facing mass disposed below the trough, and a front and rear pair of first inclined leaf springs that connect the facing mass to the base. a second inclined leaf spring; a drive electromagnet fixed to one of the trough and the opposing mass; and a drive electromagnet fixed to the other;
This is achieved by an electromagnetic vibration folder consisting of an armature attracted to the drive electromagnet.

〔作 用〕[For production]

前後一対の第1傾斜板ばねによシ基台に結合されるトラ
フと、前後一対の第2傾斜板ばねによシ基台に結合され
る対向質量とを構成要素とする電磁振動フィーダにおい
て、前記トラフと前記対向質量とのうち一方に固定され
る駆動電磁石と他方に固定される接極子との間に交番吸
引力が発生し、互いに引きよせられ、離されながら前記
トラフと前記対向質量の両方が相互に180@の位相差
をもって振動する。よって基台に伝達される。反力を殆
んど零とすることができる。
An electromagnetic vibration feeder comprising a trough coupled to a base by a pair of front and rear first inclined leaf springs, and an opposing mass coupled to the base by a pair of front and rear second inclined leaf springs, An alternating attractive force is generated between the drive electromagnet fixed to one of the trough and the opposing mass and the armature fixed to the other, and the trough and the opposing mass are drawn toward and away from each other. Both vibrate with a phase difference of 180@. Therefore, it is transmitted to the base. The reaction force can be reduced to almost zero.

〔実施例〕〔Example〕

以下、本発明の実施例による電磁振動フィーダについて
第1図乃至第4図を参照して説明する。
EMBODIMENT OF THE INVENTION Hereinafter, an electromagnetic vibration feeder according to an embodiment of the present invention will be described with reference to FIGS. 1 to 4.

図において電磁振動フィーダは全体として(1)で示さ
れ、そのトラフ部(2)は第1図において左右に直線的
に延びており、トラフ本体(5)は第3図に示すように
樋状では″iU字状の断面を有し、その一端に材料投入
口(4)及び他端に材料排出口(3)を備えている。又
、トラフ本体(5)の両縁部には帯状の耳部(7)が一
体的に形成され、これに本実施例によれば蓋(6)が当
てられてボルト(8)により閉塞されている。
In the figure, the electromagnetic vibration feeder is indicated as (1) as a whole, its trough part (2) extends linearly from side to side in Figure 1, and the trough body (5) is shaped like a gutter as shown in Figure 3. The trough body (5) has an iU-shaped cross section, and has a material input port (4) at one end and a material discharge port (3) at the other end. A lug (7) is integrally formed, and according to this embodiment, a lid (6) is applied to this and closed by a bolt (8).

即ちトラフは密閉構造とされる。後述のようにトラフ部
(2)が振動すると投入口(4)から投入された材−科
は第1図において左方へと移送され、排出口(3)の下
端に形成される排出口(9)を介して次工程に供給され
る。
That is, the trough has a closed structure. As described later, when the trough part (2) vibrates, the material input from the input port (4) is transferred to the left in FIG. 9) to the next process.

第3図に明示されるようにトラフ(5)の耳部(7)に
はコ字形状の一対の角材(10a)(10b)が上述の
ボルト(8)によシ共締めされ、又、下滝部においては
、角柱状の一対の板ばね取付はブロック(12a)(x
2b)がボルトσυによシ固定されている。これは第1
図に示されるように前後左右一対の傾斜板ばね(16a
)(16a)(16b)(16b)によシペースプaツ
ク(ロ)にボルトにより固定されている。更に第3図に
明示されるように、板ばね取付ブロック(12a)(1
2b)にはスペーサ(13a)(13b)を介してはゾ
丁字形状の接極子としての可動コア(ロ)がゲル) (
15a)(15b)によシそのアーム部(14a)(1
4b)において固定されている。
As clearly shown in FIG. 3, a pair of U-shaped square members (10a, 10b) are fastened together with the bolts (8) on the ears (7) of the trough (5), and At the lower waterfall part, a pair of prismatic leaf springs are mounted on blocks (12a) (x
2b) is fixed by a bolt συ. This is the first
As shown in the figure, a pair of inclined leaf springs (16a
) (16a) (16b) (16b) is fixed to the spacer spout (b) with bolts. Further, as clearly shown in FIG. 3, the leaf spring mounting block (12a) (1
2b), the movable core (b) as a T-shaped armature is connected to the gel via the spacers (13a) and (13b).
15a) (15b) and its arm portion (14a) (1
4b).

即ち、本実施例によれば可動コアα4はトラフ部(2)
と一体的に構成され、トラフ側可動部の質量を構成する
ものである。又、この可動コア(ロ)は側方からみると
第1図に示されるようにL字形状、他側方からみると逆
り字形状であシ、コイルQυを巻装したE型電磁石のの
磁極面と空隙を置いてその水平部分(14C)が対向し
ている。そしてこの垂直部(14d)から上述のアーム
部(14a)(14b)が延びておシ、これが上述した
ようにポル) (15a)(t5b)によシ板ばね取付
ブayり(12m)(12b)に固定されている。
That is, according to this embodiment, the movable core α4 is located at the trough portion (2).
It is configured integrally with the trough side movable part and constitutes the mass of the trough side movable part. Also, this movable core (B) has an L-shape when viewed from the side as shown in Figure 1, and an inverted-shape when viewed from the other side. Its horizontal portion (14C) faces the magnetic pole surface of the magnetic pole with an air gap in between. The above-mentioned arm parts (14a) and (14b) extend from this vertical part (14d), and as described above, these arm parts (15a) and (t5b) are attached to the leaf spring mounting bracket (12m) ( 12b).

電磁石のは第3図に明示されるようにトラフ部(2)の
下方に配設され、左右に直線的に延びるバランスウェイ
) (111に一体的に固定されている。、尚、このバ
ランスウェイトCl51は第2図に示されるように前後
左右一対の板ばね(201)(20a)(20b)(2
0b)  によシ上述のペースブロックαηに結合され
ている。
As clearly shown in Figure 3, the electromagnet is disposed below the trough part (2) and is integrally fixed to the balance way (111) extending linearly from side to side. As shown in FIG.
0b) is coupled to the above-mentioned pace block αη.

又、本実施例によればトラフ側の板はね(tea)(t
ea)(16b)(16b)とバランスウェイト側の板
ばね(20a)(20a)(20b)(20b)の傾斜
角は同一である。そして電磁振動フィーダ(1)全体は
床上に防振ゴム(至)により支持されるが、本発明によ
ればこれは必ずしも必要ではなく、地上に伝わる反力を
更に減少させるために用いられている。又、上述のよう
に構成される板はね(161)(16a)等を含む振動
駆動部全体は筒状のカバー翻によシ閉塞されている。更
に本実施例によればトラフ部(2)や板ばね取付はブロ
ック(12a)(12b)、可動コアα線などからなる
トラフ側可動部の質量とこれをベースブayりαηに結
合する駆動用の板ばね(16a)(16a)(16b)
(16b)の全ばね定数とによって定まる共振周波数は
バランスウェイトα9及びこれに固定される電磁石■な
どからなるバランスウェイト側可動部の質量と、バラン
スウェイトα窃とペースブロック(ロ)とを結合する板
ばね(20a)(20a)(20b)(20b)の全ば
ね定数とで定まる共振周波数とははシ一致するように定
められている。
Furthermore, according to this embodiment, the trough side plate tea (t
ea) (16b) (16b) and the balance weight side leaf springs (20a) (20a) (20b) (20b) have the same inclination angle. The entire electromagnetic vibration feeder (1) is supported on the floor by a vibration isolating rubber, but according to the present invention, this is not necessarily necessary and is used to further reduce the reaction force transmitted to the ground. . Further, the entire vibration driving section including the plate springs (161), (16a), etc. configured as described above is closed by a cylindrical cover cover. Furthermore, according to this embodiment, the trough part (2) and the plate springs are attached to the blocks (12a) (12b), the mass of the trough side movable part consisting of the movable core α line, etc., and the drive unit that connects this to the base air αη. Leaf springs (16a) (16a) (16b)
The resonant frequency determined by the total spring constant of (16b) combines the mass of the balance weight side movable part consisting of the balance weight α9 and the electromagnet ■ fixed to it, the balance weight α and the pace block (b). The resonant frequency determined by the total spring constant of the leaf springs (20a) (20a) (20b) (20b) is determined to match.

更に本実施例によれば上述のトラフ側可動部全体の重心
とバランスウェイト側可動部全体の重心とがほゞ一致す
るように各部分の寸法、質量分布が定められている。或
いはこれら重心を結ぶ直線が板ばね(16a)(16b
)(20a)(20b)の傾斜角によって決まるトラフ
部(2)の振動方向にはゾ平行となるように定められて
いる。
Further, according to this embodiment, the dimensions and mass distribution of each part are determined so that the center of gravity of the entire trough-side movable section and the center of gravity of the entire balance weight-side movable section described above substantially coincide. Or, the straight line connecting these centers of gravity is the leaf spring (16a) (16b
) (20a) (20b) The vibration direction of the trough portion (2) determined by the inclination angle of (20b) is set to be parallel to the vibration direction.

本発明の実施例による振動フィーダは以上のように構成
されるが次にこの作用について説明する。
The vibratory feeder according to the embodiment of the present invention is constructed as described above, and its operation will be explained next.

コイル(211に交流を通電すると電磁石のと可動コア
(ロ)の水平部(14c)との間に交番吸引力が発生し
、トラフ(2)及びバランスウェイト叫は1800の位
相差をもって相互に相反する方向に振動する。又、振動
方向は板ばね(16a)(16a)(16b)(16b
)及び(20a)(20a)(20b)(20b)の傾
斜方向によって規制されこれらの長手方向に対しはゾ垂
直方向にトラフ部(2)及びバランスウェイト四は振動
する。又、トラフ側可動部の重心とバランスウェイト側
可動部の重心とがほゞ一致するように構成されているの
でトラフ(2)は左右全体にわたって均一な振動を行う
When alternating current is applied to the coil (211), an alternating attractive force is generated between the electromagnet and the horizontal part (14c) of the movable core (b), and the trough (2) and the balance weight force are opposed to each other with a phase difference of 1800. It vibrates in the direction of the leaf springs (16a) (16a) (16b) (16b
) and (20a), (20a), (20b), and (20b), and the trough portion (2) and the balance weight 4 vibrate in a direction perpendicular to these longitudinal directions. Furthermore, since the center of gravity of the trough-side movable section and the center of gravity of the balance weight-side movable section are substantially aligned, the trough (2) vibrates uniformly over the entire left and right sides.

本実施例の構成を振動学的にみると、第4図に示される
ような振動系を構成する。即ち、トラフ側可動部の質量
をmlとし、ペースプayり(17)の質量を−及びバ
ランスウェイト側の質量をmHとし、又、これら質量と
ペースブロックαηと結合するばねのはね定数を第4図
に示すようにに、 、k、及びksとすれば上述の電磁
石にと可動コアα尋との間の交番吸引力をFs inω
tとすれば第4図に示すように矢印で示すように180
°位相を変えた加振力となシ、従りてこれら質量m、 
、mHは、はゾ共振周波数に近い振動を行うので相互に
180°位相を変えた振動を行う。即ち、質量雇い町が
もつとも近接するときがペースブロック−に対しもつと
も近接するときであシ、又、これから最も遠ざかったと
きが相互に最も遠ざかった時である。又、これら質量町
、m、は180’位相を変えた振動を行うのでペースブ
ロックαη、即ち質量−に伝達される反力は相反する方
向となシ、相殺することになる。即ち、トラフ側可動部
の質量m1の振巾はXl、ばね定数はk。
When the configuration of this embodiment is viewed from a vibrational perspective, a vibration system as shown in FIG. 4 is constructed. That is, the mass of the movable part on the trough side is ml, the mass of the pace support (17) is - and the mass of the balance weight side is mH, and the spring constant of the spring that connects these masses and the pace block αη is expressed as ml. As shown in Figure 4, if , k, and ks, the alternating attractive force between the electromagnet and the movable core α is Fs inω
If t is 180 as shown by the arrow in Figure 4.
° The excitation force with a different phase, therefore, these masses m,
, mH vibrate close to the resonant frequency, so they vibrate with a phase difference of 180° from each other. That is, the time when the mass hire town is the closest to the pace block is the time when it is the closest to the pace block, and the time when it is furthest from this is the time when it is the furthest from each other. Moreover, since these masses m and oscillate with a phase difference of 180', the reaction forces transmitted to the pace block αη, that is, the mass −, are in opposite directions and cancel each other out. That is, the amplitude of the mass m1 of the trough side movable part is Xl, and the spring constant is k.

であるので、”l×に1の反力が質量m、に加わ)、又
、逆位相の反力としてm3の振巾X3 xばね定数に、
が質量m、に伝達される。従ってxIXk、=x3Xk
3  であればペースブロック(ロ)の質量に加わる反
力は完全に相殺されて地上に伝わる反力は零となる。こ
の場合には防振ばね(ト)は不要となるのであるが、実
際には少しのアンバランスがあるので、この分を防振ば
ね(至)によシ地上に伝えられる反力は非常に小さいも
のとすることができる。
Therefore, a reaction force of 1 is applied to the mass m), and as a reaction force with the opposite phase, the amplitude of m3 x the spring constant,
is transmitted to mass m. Therefore xIXk, =x3Xk
3, the reaction force applied to the mass of the pace block (b) is completely canceled out, and the reaction force transmitted to the ground becomes zero. In this case, the anti-vibration spring (T) is not needed, but since there is actually a slight imbalance, the reaction force that can be transmitted to the ground by the anti-vibration spring (T) is extremely large. It can be made small.

以上、本発明の実施例について述べたが、勿論、本発明
はこれに限定されることなく、本発明の技術的思想に基
づいて種々の変形が可能である。
The embodiments of the present invention have been described above, but of course the present invention is not limited thereto, and various modifications can be made based on the technical idea of the present invention.

例えば、以上の実施例ではトラフ部(2)側に可動コア
(X4を固定し、バランスウェイトCIQに電磁石のを
固定するようにしたが、これを逆にしてもよい。
For example, in the above embodiment, the movable core (X4) is fixed to the trough portion (2) side, and the electromagnet is fixed to the balance weight CIQ, but this may be reversed.

即ち電磁石のをトラフ部(2)側に固定させ、可動コア
(ロ)をバランスウェイトσI側に固定させるようにし
てもよい。
That is, the electromagnet may be fixed to the trough portion (2) side, and the movable core (b) may be fixed to the balance weight σI side.

又、以上の実施例では可動コアα◆の形状を一側方から
みてL字形状としたが、これに代えて下方に垂下するだ
けの形状であってもよい。この場合には例えばE型の電
磁石は実施例では下向きとされたが、横方向に向けて取
付ければよい。尚、実施例のように可動コアα尋を一側
方からみてL字形状にした方がバランスウェイト側可動
部の重心とトラフ側可動部の重心とを一致させるための
構成を容易に得ることができる。或いはこれら重心を結
ぶ直線がこれら振動方向にt1″i平行とする構成を容
易に得ることができる。又、以上の実施例ではトラフ側
可動部の共振周波数とバランスウェイト側可動部の共振
周波数がほり等しいものとしたがこれらが異なっていて
もかまわない。要するにベースブロックanに加えられ
る反力を殆んど零とすべく、(トラフ側可動部の振巾)
×(これをベースブロックα力側に結合する板ばねのば
ね定数)が(バランスウェイト側可動部の振巾)×(コ
レをベースブロックα力側に結合する板ばねのばね定数
)にはゾ等しくなるようにすればよい。
Further, in the above embodiment, the shape of the movable core α♦ is L-shaped when viewed from one side, but instead of this, it may be shaped so that it simply hangs downward. In this case, for example, the E-type electromagnet is directed downward in the embodiment, but may be installed horizontally. In addition, if the movable core α fathom is L-shaped when viewed from one side as in the embodiment, it is easier to obtain a structure for aligning the center of gravity of the balance weight side movable part with the center of gravity of the trough side movable part. Can be done. Alternatively, it is possible to easily obtain a configuration in which the straight line connecting these centers of gravity is parallel to these vibration directions t1''i.Also, in the above embodiment, the resonant frequency of the trough side movable part and the resonant frequency of the balance weight side movable part are Although they are assumed to be equal, it does not matter if they are different.In short, in order to make the reaction force applied to the base block an almost zero, (the swing width of the movable part on the trough side)
× (spring constant of the leaf spring that connects this to the α force side of the base block) is (swing width of the movable part on the balance weight side) × (spring constant of the leaf spring that connects this to the α force side of the base block) Just make sure they are equal.

〔発明の効果〕〔Effect of the invention〕

以上述べたように本発明の電磁振動フィーダによれば、
この振動フィーダを設置する地上又は床上への反力をは
ゾ零とすることができ、又、これを低コスト及び小重量
で行うことができる。
As described above, according to the electromagnetic vibration feeder of the present invention,
The reaction force on the ground or floor where the vibratory feeder is installed can be reduced to zero, and this can be done at low cost and with small weight.

【図面の簡単な説明】[Brief explanation of the drawing]

第1図は本発明の実施例による電磁振動フィーダの部分
破断側面図、第2図は同背面図、第3図は第1図におけ
る]I[−I線方向断面図、第4図は本実施例の作用原
理をするための振動系を示す模式図及び第5図は従来例
の電磁振動フィーダの側面図である。 なお図において、
FIG. 1 is a partially cutaway side view of an electromagnetic vibration feeder according to an embodiment of the present invention, FIG. 2 is a rear view of the same, FIG. 3 is a sectional view taken along the ]I[-I line in FIG. A schematic diagram showing a vibration system for explaining the working principle of the embodiment and FIG. 5 are side views of a conventional electromagnetic vibration feeder. In the figure,

Claims (3)

【特許請求の範囲】[Claims] (1)トラフと、該トラフを基台に結合する前後一対の
第1傾斜板ばねと、前記トラフの下方に配設される対向
質量と、該対向質量を前記基台に結合する前後一対の第
2傾斜板ばねと、前記トラフと前記対向質量とのうち一
方に固定される駆動電磁石と、他方に固定され、前記駆
動電磁石に吸引される接極子とから成る電磁振動フィー
ダ。
(1) A trough, a pair of front and rear first inclined plate springs that connect the trough to the base, a facing mass disposed below the trough, and a pair of front and rear inclined leaf springs that connect the facing mass to the base. An electromagnetic vibration feeder comprising a second inclined plate spring, a drive electromagnet fixed to one of the trough and the opposing mass, and an armature fixed to the other and attracted to the drive electromagnet.
(2)前記接極子は側方から見て略L字形状であり、そ
の水平部分が前記駆動電磁石の磁極面に空隙をおいて対
向している請求項(1)に記載の電磁振動フィーダ。
(2) The electromagnetic vibration feeder according to claim 1, wherein the armature has a substantially L-shape when viewed from the side, and a horizontal portion thereof faces the magnetic pole surface of the drive electromagnet with a gap therebetween.
(3)前記トラフ側可動部の重心と前記対向質量側可動
部の重心とがほゞ一致しているが、これら重心を結ぶ直
線が前記トラフ及び対向質量の振動方向とほゞ平行であ
る請求項(1)又は(2)に記載の電磁振動フィーダ。
(3) The center of gravity of the trough-side movable part and the center of gravity of the opposing mass-side movable part substantially coincide, but a straight line connecting these centers of gravity is substantially parallel to the vibration direction of the trough and the opposing mass. The electromagnetic vibration feeder according to item (1) or (2).
JP18988788A 1988-07-29 1988-07-29 Electromagnetic oscillation feeder Pending JPH0243118A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP18988788A JPH0243118A (en) 1988-07-29 1988-07-29 Electromagnetic oscillation feeder

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP18988788A JPH0243118A (en) 1988-07-29 1988-07-29 Electromagnetic oscillation feeder

Publications (1)

Publication Number Publication Date
JPH0243118A true JPH0243118A (en) 1990-02-13

Family

ID=16248843

Family Applications (1)

Application Number Title Priority Date Filing Date
JP18988788A Pending JPH0243118A (en) 1988-07-29 1988-07-29 Electromagnetic oscillation feeder

Country Status (1)

Country Link
JP (1) JPH0243118A (en)

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WO2012147838A1 (en) * 2011-04-27 2012-11-01 シンフォニアテクノロジー株式会社 Article separation and conveyance device
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WO2013008553A1 (en) * 2011-07-08 2013-01-17 シンフォニアテクノロジー株式会社 Oscillation device, goods conveyance device, and goods classification device
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US9315330B2 (en) 2011-07-08 2016-04-19 Sinfonia Technology Co., Ltd. Vibration device, article conveyance device, and article sorting device
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JP2013095564A (en) * 2011-11-02 2013-05-20 Daishin:Kk Vibration type conveyance device
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JP2013133219A (en) * 2011-12-27 2013-07-08 Sinfonia Technology Co Ltd Article separation and conveyance device

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