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JP3022333B2 - Manufacturing method of fuel supply electromagnetic pump for oil combustor - Google Patents
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JP3022333B2 - Manufacturing method of fuel supply electromagnetic pump for oil combustor - Google Patents

Manufacturing method of fuel supply electromagnetic pump for oil combustor

Info

Publication number
JP3022333B2
JP3022333B2 JP8194283A JP19428396A JP3022333B2 JP 3022333 B2 JP3022333 B2 JP 3022333B2 JP 8194283 A JP8194283 A JP 8194283A JP 19428396 A JP19428396 A JP 19428396A JP 3022333 B2 JP3022333 B2 JP 3022333B2
Authority
JP
Japan
Prior art keywords
flow rate
terminal
resistance value
pump
predetermined
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 - Lifetime
Application number
JP8194283A
Other languages
Japanese (ja)
Other versions
JPH1037852A (en
Inventor
正剛 木村
晃 豊田
勝広 菅谷
輝雄 御苑
泰常 千葉
健二 五十嵐
Original Assignee
太産工業株式会社
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Publication date
Application filed by 太産工業株式会社 filed Critical 太産工業株式会社
Priority to JP8194283A priority Critical patent/JP3022333B2/en
Publication of JPH1037852A publication Critical patent/JPH1037852A/en
Application granted granted Critical
Publication of JP3022333B2 publication Critical patent/JP3022333B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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Description

【発明の詳細な説明】DETAILED DESCRIPTION OF THE INVENTION

【0001】[0001]

【発明の属する技術分野】本発明は、暖房機などの民生
用の主として小型石油燃焼器へ、例えば白灯油などの液
体燃料を所定量供給するためにこれに組付けられる用途
に用いられる電磁ポンプの特に大量生産時の吐出流量を
所定値に調整する工程を含む製造方法に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to an electromagnetic pump which is used for supplying a predetermined amount of liquid fuel such as white kerosene to a small-sized petroleum combustor for consumer use such as a heater. Particularly, the present invention relates to a manufacturing method including a step of adjusting a discharge flow rate during mass production to a predetermined value.

【0002】[0002]

【従来の技術】上記主として小形石油燃焼器への液体燃
料を定量供給して燃焼させるための送油ポンプとして電
磁ポンプが利用されるようになって久しい。否むしろ電
磁ポンプの開発によって、これら民生用の小形石油燃焼
機器を備えた暖房器、ボイラー或いは乾燥機が爆発的に
市場に提供されるようになった。
2. Description of the Related Art Electromagnetic pumps have been used for a long time as oil feed pumps for supplying a fixed amount of liquid fuel to mainly small oil combustors for combustion. Rather, the development of electromagnetic pumps has exploded the market for heaters, boilers or driers equipped with these small commercial oil fired appliances.

【0003】即ち1960年代には、ガンタイプ油バー
ナ用電磁ポンプとして比較的吐出圧力流量共に大きく、
圧力調整機構等を備え複雑な構成の電磁ポンプが、本願
出願人によって初めて市場に提供された。引続き、米,
麥等の穀類、煙草、食品等の乾燥用として含水率制御回
路などを備えた電磁ポンプが、さらに1970年代の初
頭において、強制給排気形暖房器、さらに石油ストーブ
(所謂石油ファンヒータ)の燃焼器への燃料ポンプとし
て本願出願人によって初めて市場に提供された。
That is, in the 1960s, the discharge pressure and flow rate were relatively large as electromagnetic pumps for gun type oil burners.
An electromagnetic pump having a complicated configuration including a pressure adjusting mechanism and the like was first introduced to the market by the present applicant. Then rice,
Electromagnetic pumps equipped with a moisture content control circuit for drying cereals such as wheat, tobacco, foods, etc., and in the early 1970's, forced supply / exhaust heaters, and combustion of oil stoves (so-called oil fan heaters) For the first time as a fuel pump to a vessel.

【0004】そして該ファンヒータは、価格の低廉であ
ることから大いに市場において歓迎され、現在まで需要
は甚だしく増大した。しかるに現下の経済情勢から販売
価格競争も激しく販売価格は低減の一方で、これに組込
まれる電磁ポンプも甚だしい値下げを余儀なくされる趨
勢にある。しかもその吐出流量特性に対する要求も後述
するように甚だ厳しく、しかもその耐久性、信頼性に対
する保証の要求もまたきびしいものがある。
[0004] The fan heater has been greatly welcomed in the market because of its low price, and the demand has increased greatly up to now. However, due to the current economic situation, there is intense competition in sales prices, and sales prices are decreasing. On the other hand, there is a tendency that the price of electromagnetic pumps incorporated therein is also drastically reduced. In addition, the requirements for the discharge flow rate characteristics are extremely strict as described later, and there are also severe demands for guarantees for its durability and reliability.

【0005】よって本願の狙いとするところは、電磁ポ
ンプ及びその燃焼器への組付け、燃料油の吐出流量を所
定値範囲に維持するための調整工程の合理化、省力化に
よる生産コストダウンと、その品質保証とである。そこ
で先ず前記小形燃焼器、即ち燃料油を霧化、加熱して気
化燃焼させるところのロータリ、又はエアジェット方式
或いは燃料油をヒータで加熱して気化噴射着火燃焼させ
るブンゼン方式等の燃焼器への燃料供給用の電磁ポンプ
は、最も小形構造簡単なものが従来から知られている。
[0005] Accordingly, the present invention aims at assembling the electromagnetic pump and its combustor, streamlining an adjustment process for maintaining the discharge flow rate of fuel oil within a predetermined value range, reducing production costs by saving labor, and Its quality assurance. Therefore, first, the small-sized combustor, that is, a rotary, in which fuel oil is atomized, heated and vaporized and burned, or a combustor such as an air-jet system or a Bunsen system in which fuel oil is heated by a heater and vaporized and ignited and burned, is used. The most compact electromagnetic pump for supplying fuel has been known in the art.

【0006】その構成については殊更説明するまでもな
いが、本発明に利用される電磁ポンプの一例として、そ
の一部断面を表した説明図の図2によって簡単に説明す
る。図2において、電磁ポンプ1の電磁コイル20の軸
心縦貫孔に挿嵌された管柱シリンダ21内をその吐出接
手40側に備えた戻しバネ座34との間に戻しバネ23
と、他端の吸入接手37側との間に補助バネ24とをそ
れぞれ設けて、この両バネの間に圧支されていて、弁バ
ネ25、吸入弁26及び吸入弁座27とをもって成る吸
入弁機構を内蔵したフリーピストン状の電磁プランジャ
22は、前記管柱シリンダ21などを囲繞している電磁
コイル20へのパルス状断続電流の付勢によって発生す
る磁気吸引力と前記戻しバネ23の反発力とを交互に利
用して該管柱シリンダ21内を摺動往復し、前記吸入弁
機構と管柱シリンダ端部位に接続させる吐出オリフィス
41を備えた吐出接手40内に弁バネ28、吐出弁体2
9及び吐出弁座30をもって構成された吐出弁機構との
交互開閉作用と相まってポンプ作用を行ない、図におい
て吸入接手37の吸入口38を覆うフィルタ39から、
濾過された燃料油は該吸入口38、管柱シリンダ21内
を通過し、吐出接手40の吐出オリフィス41から吐出
され、図示しない燃焼器への接続配管を経て該接続配管
が臨む燃焼器の気化器又は火炉の気化室へ放出され、気
化燃焼する構成となる。
Although the structure is not particularly explained, as an example of the electromagnetic pump used in the present invention, it will be briefly described with reference to FIG. In FIG. 2, a return spring 23 is provided between the inside of a tube cylinder 21 inserted in the axial through hole of the electromagnetic coil 20 of the electromagnetic pump 1 and a return spring seat 34 provided on the discharge joint 40 side.
And an auxiliary spring 24 between the other end and the suction joint 37 side. The auxiliary spring 24 is supported by the two springs and has a valve spring 25, a suction valve 26, and a suction valve seat 27. A free-piston electromagnetic plunger 22 having a built-in valve mechanism is provided with a magnetic attraction force generated by the application of a pulsed intermittent current to the electromagnetic coil 20 surrounding the tube cylinder 21 and the like, and a repulsion of the return spring 23. A valve spring 28 and a discharge valve are provided in a discharge joint 40 provided with a discharge orifice 41 for slidingly reciprocating in the tube cylinder 21 by using force alternately and connecting the suction valve mechanism and a tube cylinder end portion. Body 2
9 and a discharge valve mechanism constituted by a discharge valve seat 30 to perform a pumping operation in combination with an opening / closing operation, and a filter 39 covering a suction port 38 of a suction joint 37 in FIG.
The filtered fuel oil passes through the suction port 38 and the inside of the tube cylinder 21, is discharged from the discharge orifice 41 of the discharge joint 40, and is vaporized by the combustor facing the connection pipe via a connection pipe to a combustor (not shown). It is discharged to the vaporization chamber of the vessel or the furnace, and is configured to vaporize and burn.

【0007】前記電磁コイル20へのパルス状断続電流
は、一般的に民生用小形石油燃焼器の燃料油供給電磁ポ
ンプの場合には、商用交流電源を整流しかつツェナダイ
オードを含む電圧安定化回路を経てパルス発振周期およ
び周期中の導通期間すなわちデューテイ比を加減調整す
る回路および該回路に抵抗器を介入させて電流波高値を
調整する等の電磁ポンプの駆動回路によってその吐出流
量を所定値に維持するように制御される。
In general, in the case of a fuel oil supply electromagnetic pump for a small-sized commercial petroleum combustor, the pulsed intermittent current to the electromagnetic coil 20 rectifies a commercial AC power supply and includes a voltage stabilizing circuit including a zener diode. Through a pulse oscillation cycle and a circuit for adjusting the conduction period during the cycle, that is, the duty ratio, and a drive circuit of the electromagnetic pump for adjusting the current peak value by interposing a resistor in the circuit to adjust the discharge flow rate to a predetermined value. It is controlled to maintain.

【0008】前記電磁コイル20へ付勢するパルス状断
続電流は、その周波数が一定範囲の帯域内において、周
波数及びデューテイ比にほぼ比例し、かつ電流の波高値
に応じて電磁ポンプの単位時間あたりの吐出流量を増加
させることは既に従来技術の各文献に開示されて周知で
ある。即ち古くは、特公昭41−17264号の公報、
実公昭41−18863号の公報、特公昭56−387
96号の公報、特公昭57−12865号の公報、更に
は実公昭59−41377号の公報、実公昭63−39
430号の公報等に枚挙に暇がない程の電磁ポンプの吐
出流量制御回路が開示されている。
The pulse-shaped intermittent current applied to the electromagnetic coil 20 has a frequency substantially in proportion to the frequency and the duty ratio within a certain range of the frequency, and varies per unit time of the electromagnetic pump according to the peak value of the current. Increasing the discharge flow rate is already disclosed and well known in prior art documents. That is, in the old days, Japanese Patent Publication No. 41-17264,
JP-B-41-18883, JP-B-56-387
No. 96, Japanese Patent Publication No. 57-12865, Japanese Utility Model Publication No. 59-41377, Japanese Utility Model Publication No. 63-39
No. 430 discloses a discharge flow control circuit for an electromagnetic pump that has no spare time.

【0009】しかしてこれらの吐出流量制御回路は、少
なくとも10余年前迄は電磁ポンプに個々に組付け、要
求される吐出流量に調整し、さらにこれを石油燃焼器に
組込んだ後に更に燃焼状態に則して再調整することが一
般的であった。その直後、前記電磁ポンプも含む石油燃
焼器の製販コストダウンかつ省スペース、及び燃焼器を
ユーザに販売後に生じた不具合、故障などに対するメン
テナンスサービスにおけるポンプの吐出流量を燃焼器に
合わせて調整する作業を必要とせず、部品交換も最小限
度となる互換性と経済性とを求めて前記吐出流量制御回
路を該燃焼器全般の制御回路とを合わせて一体に組込む
方式が採用され始め、これが主流になった。この方式の
回路を以下単に燃焼制御回路と称する。
However, these discharge flow control circuits are individually assembled to the electromagnetic pump until at least 10 years ago, adjusted to the required discharge flow, and further assembled into an oil combustor, and then further burned. It was common to re-adjust according to. Immediately thereafter, work to reduce the production cost and space of the oil combustor including the electromagnetic pump and to save space, and to adjust the discharge flow rate of the pump in the maintenance service for troubles and failures after selling the combustor to the user according to the combustor. In order to achieve compatibility and economics that minimize component replacement and minimize the need for parts replacement, a system in which the discharge flow rate control circuit is integrated with the control circuit of the combustor as a whole has been adopted, and this has become the mainstream. became. This type of circuit is hereinafter simply referred to as a combustion control circuit.

【0010】ところで前記燃焼制御回路と燃焼器と電磁
ポンプとはそれぞれの生産者が相違することが多い。そ
こで後で詳述するが、この燃焼制御回路における吐出流
量制御のためのパルス電流の電圧、周期及びデューテイ
比等は最もきびしい規制ができるが、それでも一定範囲
の許容差があり、電磁ポンプは、電磁コイルの所謂エナ
メル銅線の線径、絶縁被膜の厚さ、固有抵抗値、捲数及
び電磁ポンプの磁気回路の透磁率によって磁化力、磁束
密度の変化で磁力が左右され、ポンプ構成部品の寸法精
度、仕上げ面の表面粗さ、真円度、真直度による電磁プ
ランジャ作動時の摩擦抵抗やこれに加わる温度変化に伴
って燃料油の粘度と関連してのレイノルズ数の変動、バ
ネ定数の許容範囲内の微差などによっても、これらのバ
ラツキの集合によってポンプの吐出性能に甚だしく影響
し、さらに燃焼器に接続する配管とノズルの内径、内面
の粗さ及びそれぞれの長さの許容差内の微差及び燃焼器
自体の火炉内の圧力変化気流の状態によって、電磁ポン
プの吐出流量制御、即ち燃焼器の燃焼量の設定は微妙に
相違するものがある。
By the way, the producer of the combustion control circuit, the combustor and the electromagnetic pump are often different from each other. Therefore, as will be described in detail later, the voltage, cycle, duty ratio, and the like of the pulse current for controlling the discharge flow rate in this combustion control circuit can be regulated most strictly, but there is still a certain range of tolerance, and the electromagnetic pump is The magnetic force is affected by the change in magnetizing force and magnetic flux density depending on the wire diameter of the so-called enameled copper wire of the electromagnetic coil, the thickness of the insulating coating, the specific resistance, the number of turns, and the magnetic permeability of the magnetic circuit of the electromagnetic pump. Dimensional accuracy, surface roughness of finished surface, roundness, frictional resistance during electromagnetic plunger operation due to straightness, fluctuation of Reynolds number related to fuel oil viscosity with temperature change added to it, and spring constant Even if there is a slight difference within the allowable range, the collection of these variations will significantly affect the discharge performance of the pump, and furthermore, the inner diameter of the pipes and nozzles connected to the combustor, the roughness of the inner surface, The differential refinement and conditions of pressure changes air flow in the furnace of the combustor itself in length tolerance Les, the discharge flow rate control of the electromagnetic pump, i.e. a combustor of the combustion amount of settings are those different slightly.

【0011】民生用の石油燃焼器、例えば日本工業規格
に定められた強制通気形開放式石油ストーブ、即ち石油
ファンヒータは、外気温の上下に対応して室温を所望の
温度に保持するため及び容量によって燃焼させる燃料油
を凡そ1〜10ミリリットル毎分の範囲を無段階若しく
は数段の段階的に比例燃焼可能なように吐出制御し、し
かも所定燃焼量の公差は±10%以内に規定されてい
る。
[0011] Consumer petroleum combustors, for example, forced-ventilated open petroleum stoves specified in Japanese Industrial Standards, that is, petroleum fan heaters, maintain the room temperature at a desired temperature in response to an increase or decrease in outside air temperature. The discharge of fuel oil to be burned is controlled so that it can be burned proportionally in a stepless or several steps in a range of about 1 to 10 milliliters per minute, and the tolerance of the predetermined combustion amount is specified within ± 10%. ing.

【0012】しかして、電磁ポンプ自体は吐出流量制御
回路による調整前の個々のポンプの自然最大流量の幅は
凡そ20〜30%程度の上下のバラツキがある。前記制
御回路で吐出流量を調整する場合に、所定(基準)燃焼
量±10%にするには、ポンプ自体ははるかにきびしい
規制がされるのである。例えば燃焼器生産者は、電磁ポ
ンプ受入れの際の吐出流量を所定燃焼量の±6〜7%を
要求しており、電磁ポンプ生産者は、製造工程における
吐出流量調整は所定吐出流量の±2〜2.5%、出荷時
の検査は同じく±4〜5%に規制を必要とするものが多
い現状である。
However, the range of the natural maximum flow rate of the individual pumps before adjustment by the discharge flow rate control circuit in the electromagnetic pump itself varies up and down by about 20 to 30%. When the discharge flow rate is adjusted by the control circuit, the pump itself is much more severely regulated to achieve a predetermined (reference) combustion amount ± 10%. For example, the combustor producer requires the discharge flow rate at the time of receiving the electromagnetic pump to be ± 6 to 7% of a predetermined combustion quantity, and the electromagnetic pump producer requires that the discharge flow rate adjustment in the manufacturing process be ± 2 of the predetermined discharge flow rate. At present, inspections at the time of shipment often require regulations of ± 4 to 5%.

【0013】前記電磁ポンプの電磁コイル及び各部品の
仕上げ寸法精度等は、相当にきびしい許容誤差をもって
管理生産される。例えば電磁プランジャ1つをとっても
その外径寸法は、機械工作及び減摩剤のコーティング処
理を施した上で、その許容差は数ミクロンであり、真円
度、真直度も同様である。この外径寸法等をミクロン以
下に規制するとすれば恐らく、この電磁プランジャのみ
の生産原価で電磁ポンプ1台の価格の10倍前後となる
であろう。それ故、電磁ポンプを構成する各部品の前記
した許容差を現在よりも更にきびしく規制することは、
前記した要求されているコストダウンに逆行するもので
あり、現時点では到底実施できるものではない。
The finished dimensions of the electromagnetic coil and the components of the electromagnetic pump are controlled and produced with considerably tight tolerances. For example, even if a single electromagnetic plunger is used, its outside diameter is several microns after machining and coating with an anti-friction agent, and the same applies to the roundness and straightness. If the outer diameter and the like are restricted to a micron or less, the production cost of this electromagnetic plunger alone will probably be about 10 times the price of one electromagnetic pump. Therefore, to regulate the above-mentioned tolerance of each component constituting the electromagnetic pump more severely than at present,
This is contrary to the required cost reduction and cannot be implemented at present.

【0014】電磁ポンプとこれを組込む燃焼器のそれぞ
れの所定の機種で大量生産されたものが、それらの何れ
を組合わせても所定燃焼量の許容範囲に収まるように、
予め電磁ポンプの吐出流量のバラツキを規制する調整作
業の能率を高めて生産効率の向上、コストの低減をはか
り、しかも石油燃焼器を一般使用者が燃焼量を勝手に調
整したことによって発生するおそれのある事故を未然に
回避するために電磁ポンプ外部に可変抵抗器などの吐出
流量調整機構を取付けない傾向が一般的になった。
An electromagnetic pump and a combustor incorporating the same are mass-produced in respective predetermined models, and any combination thereof is within the allowable range of the predetermined combustion amount.
The efficiency of adjustment work to regulate the variation of the discharge flow rate of the electromagnetic pump in advance is improved to improve production efficiency and reduce costs. In order to avoid accidents with problems, it has become common to not install a discharge flow rate adjusting mechanism such as a variable resistor outside the electromagnetic pump.

【0015】このような従来技術に例えば、特公平7−
101033号の公報に開示されたものが知られてい
る。この従来技術は、その特許請求の範囲に記載されて
いる如く、「フリーピストン状のプランジャを納めたシ
リンダの外周に設けられた電磁コイルと、該電磁コイル
から2本のコイル端末を固定する第1、第2の端子、更
に前記第1の端子との間で固定抵抗器が接続される第3
の端子とを有し、石油燃焼器に組込まれた状態で該石油
燃焼器内の駆動回路から供給される駆動パルスが上記第
2、第3の端子間に供給されて燃料を所定の吐出量で吐
出する石油燃料器の燃料供給用電磁ポンプにおいて、上
記固定抵抗器のない状態で、上記石油燃焼器の駆動回路
から供給される駆動パルスに対して上記所定の吐出量以
上となるように、予め電磁ポンプを製造し、吐出量検査
用駆動回路からの駆動パルスを上記第1、第2の端子に
供給して上記電磁ポンプの吐出量を測定し、このときの
吐出量と基準流量とその偏差に応じて、上記電磁ポンプ
の吐出量に対する上記石油燃焼器に組込んだ状態で上記
所定の吐出量に対する許容範囲内に収まる抵抗値を有す
る固定抵抗値を選定し、該選定した固定抵抗器を上記第
1、第3の端子間に接続することを特徴とする石油燃焼
器の燃料供給用電磁ポンプ」である。
For example, Japanese Patent Publication No.
The one disclosed in the publication of No. 1001033 is known. This prior art, as described in the claims, discloses an electromagnetic coil provided on the outer periphery of a cylinder containing a free-piston plunger and a second coil terminal fixed from the electromagnetic coil. A third terminal in which a fixed resistor is connected between the first terminal, the second terminal, and the first terminal;
And a drive pulse supplied from a drive circuit in the oil combustor in a state of being incorporated in the oil combustor, is supplied between the second and third terminals to discharge fuel at a predetermined discharge rate. In the fuel supply electromagnetic pump of a petroleum fuel device that discharges, in a state where the fixed resistor is not provided, the drive pulse supplied from the drive circuit of the petroleum combustor has a predetermined discharge amount or more. An electromagnetic pump is manufactured in advance, and a drive pulse from a drive circuit for discharge amount inspection is supplied to the first and second terminals to measure a discharge amount of the electromagnetic pump. According to the deviation, a fixed resistance value having a resistance value falling within an allowable range for the predetermined discharge amount in a state of being incorporated in the oil combustor with respect to the discharge amount of the electromagnetic pump is selected, and the selected fixed resistor is selected. Between the first and third terminals. Petroleum combustor fuel supplying solenoid pumps ", characterized in that to connect.

【0016】[0016]

【発明が解決しようとする課題】上記特公平7−101
033号の公報に開示の従来技術において、フリーピス
トン状のプランジャを収めたシリンダの外周に設けた電
磁コイルへ、発振する周期中のデューテイ比を有する所
定断続パルス電流を付勢してポンプ作用を営み、このパ
ルス電流に直列の抵抗を付加して電流値を低減してポン
プの吐出量を減少方向に調整して所定吐出量を得る方法
は従来公知である。
Problems to be Solved by the Invention
In the prior art disclosed in Japanese Patent Publication No. 033, a predetermined intermittent pulse current having a duty ratio during an oscillating cycle is applied to an electromagnetic coil provided on the outer periphery of a cylinder containing a free-piston plunger to perform a pump action. Conventionally, a method of obtaining a predetermined discharge amount by adding a series resistor to the pulse current to reduce the current value and adjust the discharge amount of the pump in a decreasing direction is known.

【0017】即ち、このように電磁コイルへ付勢する電
流に直列の抵抗を与えて電流値を低減したり、或いはリ
リーフ弁、減圧弁などをポンプに備えて、その吐出圧力
や流量を低減することを可能にするためにポンプの吐出
能力を所定の吐出力以上になるように電磁ポンプを予め
製造することは、従来周知で実施されてきたものであ
る。
That is, a current value is reduced by applying a series resistance to the current energized to the electromagnetic coil as described above, or a relief valve, a pressure reducing valve, etc. are provided in the pump to reduce the discharge pressure and flow rate thereof. It is well known and practiced to manufacture an electromagnetic pump in advance so that the discharge capacity of the pump is equal to or higher than a predetermined discharge force in order to enable the above.

【0018】この点通常すべての機器は、その最大出力
以下で所定値に調整された出力で使用されることが当然
であるからである。次に、この従来例では、その特許請
求の範囲の欄で、「吐出量検査用駆動回路から駆動パル
スを上記第1、第2の端子に供給して上記電磁ポンプの
吐出量を測定し、」とあるが、第1の端子との間で固定
抵抗器が接続される第3の端子があっても、「上記固定
抵抗器のない状態で」との特定の有無にかかわらず、第
1、第2の端子間に通電するときは該固定抵抗器は短絡
されていて用をなさない。
In this regard, it is natural that all devices are used with an output adjusted to a predetermined value below its maximum output. Next, in this conventional example, in the column of the claims, "a drive pulse is supplied from the discharge amount inspection drive circuit to the first and second terminals to measure the discharge amount of the electromagnetic pump, However, even if there is a third terminal to which a fixed resistor is connected between the first terminal and the third terminal, regardless of the presence or absence of “without the fixed resistor”, the first terminal When the current flows between the second terminals, the fixed resistor is short-circuited and useless.

【0019】しかるに、この従来例の公報明細書第7欄
第32〜35行に、「若しくは、ある特定の抵抗値の抵
抗器を介在させた状態でポンプの吐出量を測定し、この
測定流量から上述のようにして所定の固定抵抗器を選定
する」と記載されている。この記載では、ある所定の抵
抗値の抵抗器は一体何処に介在させるのかその記載は一
切無いので不明である。
On the other hand, in the publication of the prior art, column 7, lines 32 to 35, "Or, the discharge rate of the pump is measured with a resistor having a specific resistance value interposed, and the measured flow rate is measured. From above, a predetermined fixed resistor is selected as described above. " In this description, it is unknown because there is no description of where a resistor having a predetermined resistance value is interposed.

【0020】またこの従来例の特許請求の範囲の記載
に、「上記電磁ポンプの吐出量を測定し、このときの吐
出量と基準流量とその偏差に応じて」とあるが、基準流
量とその偏差についての説明がなされていないし、これ
らの定義が明確でない。そして、「上記電磁ポンプの吐
出量に対する上記石油燃焼器に組込んだ状態で上記所定
の吐出量に対する許容範囲内に収まる抵抗値を有する固
定抵抗値を選定し、」とあるのは、この従来例の特許公
報の明細書第6欄第4〜7行及び第7欄第24〜35行
にそれぞれ記載された所定の固定抵抗器の選定方法によ
るものであろうが、上記状態でポンプの吐出量を測定
し、この測定流量の基準流量からの偏差に応じて予め実
験データから求めている流量と抵抗値の関係から定まる
固定抵抗器を選定するとあるのみで、該固定抵抗器の選
定に係る手段についての記載が無いので具体性を欠く。
Further, the description in the claims of this conventional example states that "the discharge amount of the electromagnetic pump is measured, and the discharge amount at this time, the reference flow rate, and the deviation thereof". No explanation is given for deviations, and their definitions are not clear. Then, "a fixed resistance value having a resistance value falling within an allowable range for the predetermined discharge amount in a state of being incorporated in the petroleum combustor for the discharge amount of the electromagnetic pump is selected." The method may be based on the method of selecting a predetermined fixed resistor described in column 6 lines 4 to 7 and column 7 lines 24 to 35 of the specification of the Japanese Patent Publication, however, the pump discharge in the above state It is only necessary to measure the amount and to select a fixed resistor determined from the relationship between the flow rate and the resistance value obtained in advance from experimental data according to the deviation of the measured flow rate from the reference flow rate. Since there is no description about the means, it lacks specificity.

【0021】また、前記従来例の特許公報の明細書に従
来技術として記載されているところの実開昭53−31
303号の公報に開示されたコイルに直列に可変抵抗器
を接続し、この可変抵抗器の抵抗値を調整することによ
り電磁ポンプの流量を所定流量に調整すること及び可変
抵抗器を用いて前記固定抵抗器を選定する所謂カットア
ンドトライ法は、その従来例の特許公報の明細書第7欄
第36〜39行で否定されているので採らざるところで
あろう。
Further, Japanese Utility Model Application Laid-Open No. 53-31, which is described in the specification of the above-mentioned prior art patent publication as a prior art.
No. 303, a variable resistor is connected in series to the coil, and the flow rate of the electromagnetic pump is adjusted to a predetermined flow rate by adjusting the resistance value of the variable resistor. The so-called cut-and-try method for selecting a fixed resistor will not be adopted because it is denied in the specification of the patent publication of the prior art at column 7, lines 36 to 39.

【0022】また、抵抗値の異なる固定抵抗器をそれぞ
れ接点の端子に接続して、これをそれぞれ電磁コイルに
ロータリスイッチの回動により切換接続してポンプの吐
出流量を選定することもカットアンドトライ方法である
から、これも前記従来例の従来技術範囲から除外される
(特公平7−66294号の公報を参照)。さらに同一
の生産ロットであって、予め電磁コイルへ直列に付加す
る抵抗値によってその吐出量が凡そ定まる見込みのある
場合には、吐出流量の所定値に調整するために固定抵抗
器の選定は多小の熟練度が必要であり、吐出流量調整者
の所謂勘によっても可能であるが、これも前記従来例の
技術範囲には属さないのみならずポンプ一台毎の人手に
よる抵抗器の選定及び調整はコストアップとなる。
It is also possible to connect the fixed resistors having different resistance values to the terminals of the respective contacts and switch them to the respective electromagnetic coils by turning a rotary switch to select the discharge flow rate of the pump. This method is also excluded from the prior art range of the conventional example (see Japanese Patent Publication No. 7-66294). Further, when the discharge amount is expected to be approximately determined by the resistance value added in series to the electromagnetic coil in advance in the same production lot, the selection of the fixed resistor is often performed in order to adjust the discharge flow rate to a predetermined value. A small degree of skill is required, and it is possible by the so-called intuition of the discharge flow rate adjuster. However, this is not limited to the technical range of the conventional example as well as manual selection of the resistor for each pump and Adjustment increases costs.

【0023】このように特公平7−101033号の公
報に記載の従来例は、前記所定の吐出量に対する許容範
囲内におさまる抵抗値を有する固定抵抗器を選定する手
段が明らかではないので具体性がない。実施不可能とも
考えられる。しかし前記従来例の技術は、その特許公報
の明細書の第6欄第40〜42行、同第7欄第36〜3
9行及び同第9欄第9〜10行に、「固定抵抗器の選定
及び固定抵抗器の接続固定作業が各電磁ポンプ毎に1回
の吐出量測定によって行われる。」との三度にわたる記
載がある。
As described above, in the conventional example described in Japanese Patent Publication No. Hei 7-110103, the means for selecting a fixed resistor having a resistance value falling within an allowable range with respect to the predetermined discharge amount is not clear. There is no. It is considered impossible. However, the technique of the conventional example is described in the specification of the patent publication at column 6, lines 40-42, and at column 7, lines 36-3.
In line 9 and in column 9 lines 9 to 10 of the same statement, "selection of a fixed resistor and connection and fixing of the fixed resistor are performed by one discharge amount measurement for each electromagnetic pump." There is a description.

【0024】これは同一機種の電磁ポンプが、その電磁
コイルに直列に介在させる付加抵抗値と吐出流量との関
係を、横軸に前記付加抵抗値を縦軸に吐出流量をとる
と、その関係線図はほぼ直線的で横軸に対する傾きもほ
ぼ一定の角度であることを前提としているものとみなさ
れる。これを図6に示すと、Q0 を通り横軸とθの傾斜
を有する直線がこれである。図において横X軸に前記付
加抵抗値RΩをとり、縦Y軸に吐出流量値ミリリットル
毎分をとる。X軸R0 は電磁コイルの固定抵抗値、o点
は電磁コイルへの付加抵抗値を増す毎の流量実測値であ
り、Q0 は電磁コイルへの付加抵抗の無いときの流量値
で、試料nの平均値から回帰分析によりY軸方向距離の
二乗和が最小となるようにして求めた最小自乗法による
回帰直線が前記Q0 を通りX軸とθの角度をなすR−Q
直線である。
This is because, when the same type of electromagnetic pump takes the relationship between the additional resistance value and the discharge flow rate which are interposed in series in the electromagnetic coil, and the horizontal axis represents the additional resistance value and the vertical axis represents the discharge flow rate, the relationship is obtained. The diagram is assumed to be premised on the assumption that the diagram is substantially linear and the inclination with respect to the horizontal axis is also substantially constant. When shown in figure 6, is a straight line which has a slope of Q 0 and the street abscissa theta. In the figure, the additional resistance value RΩ is plotted on the horizontal X axis, and the discharge flow rate value milliliters per minute is plotted on the vertical Y axis. The X axis R 0 is the fixed resistance value of the electromagnetic coil, the point o is the actual flow rate measurement value when the additional resistance value to the electromagnetic coil is increased, and Q 0 is the flow rate value when there is no additional resistance to the electromagnetic coil. R-Q regression by the method of least squares the sum of the squares of the Y-axis direction distance is determined as a minimum by regression analysis from the average value of n straight line at an angle of the Q 0 street X-axis and θ
It is a straight line.

【0025】そして所定流量QX に対応するための選定
された付加抵抗値がR′X でこれが求められる値であ
る。 今、付加抵抗値 R1 〜RN ; 説明変数 x これに対する流量値 Q1 〜QN ; 目的変数 yとすると
The selected additional resistance value corresponding to the predetermined flow rate Q X is R ′ X , which is the value to be obtained. Now, assuming that the additional resistance values R 1 to R N ; explanatory variables x, and the corresponding flow rate values Q 1 to Q N ;

【0026】[0026]

【外1】 [Outside 1]

【0027】の各式からy,a,bはそれぞれ求められ
る。しかしながら、前述しさらに詳細に後述するところ
の磁力の変化をもたらす諸要因や電磁ポンプ構成部品の
許容差範囲の寸法精度、表面粗さ、摩擦抵抗、レイノル
ズ数の変化、バネ定数などの微差によるバラツキの集積
が互いに強め合ったり弱め合ったりしてポンプの吐出量
に影響し、前記R−Q直線の「一回の測定」による所謂
一点測定値Q0 ′、若しくはQ0 ″は変動し、しかもこ
のQ0 ′,Q0 ″を通り、所定流量QX に対応する付加
抵抗値を求めるために結んだ直線は一点鎖線、点線で示
すようにX軸との傾斜角θ′,θ″もそれぞれ相違し、
前記回帰直線に必ずしも平行しない。
From the above equations, y, a, and b are respectively obtained. However, due to various factors that cause a change in magnetic force and dimensional accuracy of the tolerance range of the components of the electromagnetic pump, surface roughness, frictional resistance, changes in the Reynolds number, changes in the spring constant, etc. The accumulation of the variation strengthens or weakens each other and affects the discharge amount of the pump, and the so-called one-point measurement value Q 0 ′ or Q 0 ″ by “one measurement” of the RQ straight line fluctuates, In addition, the straight lines passing through these Q 0 ′ and Q 0 ″ and connected to obtain the additional resistance value corresponding to the predetermined flow rate Q X also have the inclination angles θ ′ and θ ″ with respect to the X axis as shown by the dashed line and the dotted line. Each one is different,
It is not necessarily parallel to the regression line.

【0028】このことは、前記した回帰分析の三式にお
けるa,b,yの値がそれぞれ相違するものとなり、一
回の流量測定で「所定の吐出量に対する許容範囲内に収
まる抵抗値を有する固定抵抗器を選定する」ことは不可
能となり、確率が低いものとなる。そこで先ず、電磁ポ
ンプの吐出性能を左右する磁力について考えると、磁化
力は電磁コイルの捲数と、そこに流れる電流値の相乗
積、即ちアンペアターンに基づき、このアンペアターン
により発生する磁束密度を磁化力で除した商が透磁率で
ある。従って磁力の強さはこれらによって設定され、こ
れに前述したポンプの部品の寸法精度、摩擦係数、流体
のレイノルズ数の変動、その他の要因が加味されて吐出
性能のバラツキをポンプ毎に生ずるのである。
This means that the values of a, b, and y in the above three equations of the regression analysis are different from each other, and that a single flow rate measurement has a resistance value within a permissible range for a predetermined discharge amount. It is not possible to "select a fixed resistor" and the probability is low. Therefore, first, when considering the magnetic force that affects the discharge performance of the electromagnetic pump, the magnetizing force is based on the product of the number of turns of the electromagnetic coil and the current value flowing therethrough, that is, based on the ampere turn, the magnetic flux density generated by this ampere turn is calculated. The quotient divided by the magnetizing force is the magnetic permeability. Therefore, the strength of the magnetic force is set by these factors, and the dimensional accuracy of the components of the pump, the coefficient of friction, the fluctuation of the Reynolds number of the fluid, and other factors are taken into consideration, and variations in the discharge performance are generated for each pump. .

【0029】今、電磁コイル固有抵抗値をR0 、付加抵
抗値をR1 〜RN 、印加電圧をE、付勢される電流値を
Aとし、コイルの捲数をTとすると、 E=(R0 +R1 〜RN )A 磁化力Fは、
Now, assuming that the specific resistance value of the electromagnetic coil is R 0 , the additional resistance values are R 1 to R N , the applied voltage is E, the current value to be energized is A, and the number of turns of the coil is T, E = (R 0 + R 1 to R N ) A The magnetizing force F is

【0030】[0030]

【外2】 [Outside 2]

【0031】となる。ここにおいて、電磁コイルの固有
抵抗値R0 に、付加抵抗値を順次増加させた場合の磁化
力A×Tの値を、本発明を適用する電磁ポンプの一例を
用いて求めたものの線図を図4に掲示し説明する。図4
は、横軸に付加抵抗値R1 〜RN をとり、縦軸に磁化力
アンペアターンをとったものである。この電磁コイルへ
の駆動電源からの電圧はDC23.5ボルト±0.05
ボルト、コイル線径0.25±0.005ミリメート
ル、捲数1600+0%〜−1%、コイルの固有抵抗値
31オーム±3% at 20°Cである。図4の場合
は上記電圧、抵抗値、捲数を基準値によって計算したも
ので、図示の通り付加抵抗値−アンペアターンの関係は
曲線となる。
## EQU1 ## Here, a diagram of a value obtained by using the example of the electromagnetic pump to which the present invention is applied to determine the value of the magnetizing force A × T when the additional resistance value is sequentially increased to the specific resistance value R 0 of the electromagnetic coil. This will be described with reference to FIG. FIG.
Takes the additional resistance R 1 to R N in the horizontal axis, is obtained taking the magnetizing force ampere turns on the vertical axis. The voltage from the drive power supply to this electromagnetic coil is DC 23.5 volts ± 0.05
The bolt and coil wire diameter are 0.25 ± 0.005 mm, the number of turns is 1600 + 0% to −1%, and the specific resistance of the coil is 31 ohm ± 3% at 20 ° C. In the case of FIG. 4, the voltage, the resistance value, and the number of windings are calculated based on the reference value. As shown in the drawing, the relationship between the additional resistance value and the ampere turn is a curve.

【0032】電磁ポンプの同一機種ではこのような線図
となる筈であるが、生産ロット及びその中の個々のポン
プでは必ずしも相似の線図になるとは限らない。なぜな
らば、先ず駆動電源電圧、周期、デューテイ比にも極め
て微小の許容差があり、電磁コイルのエナメル被覆電線
及び捲線時のテンションの伸びによる断面積の縮小、被
覆の厚さによる許容差内の外径の増減による捲込み全長
の変動などによるコイルの固有抵抗値の変化、さらに雰
囲気温や燃焼器からの輻射熱による温度変化により、こ
の抵抗値は例えば20°Cから32°Cに上昇すれば本
例の場合、抵抗値は約5%上昇する。このようにしてコ
イルを付勢する電流値は変動し、その捲数にも許容差が
あるので、アンペアターンは、図4の場合に比してX軸
に対する傾斜角及び曲線も変化する。
The same type of electromagnetic pump should have such a diagram, but the production lot and the individual pumps therein do not always have a similar diagram. The reason is that the drive power supply voltage, cycle, and duty ratio also have extremely small tolerances, and the enamel-covered electric wire of the electromagnetic coil and the reduction in cross-sectional area due to the extension of the tension during winding, and the tolerance within the tolerance due to the thickness of the coating. Due to a change in the specific resistance of the coil due to a change in the total winding length due to an increase or decrease in the outer diameter, and a change in the temperature due to the ambient temperature or the radiant heat from the combustor, if the resistance increases from 20 ° C to 32 ° C, for example. In the case of this example, the resistance increases by about 5%. In this manner, the current value for energizing the coil fluctuates, and the number of turns thereof has a tolerance. Therefore, in the ampere turn, the inclination angle and the curve with respect to the X axis also change as compared with the case of FIG.

【0033】そして前記した電磁プランジャ等の磁路を
構成する磁性材料は、予め磁気焼鈍してあっても切削、
研削、研磨、弁座圧入等の塑性加工によって組織が変化
して透磁率が実例として数十パーセント低下することが
あり、真空環境下などで、光輝磁気焼鈍することは、部
品寸法や真円度及び真直度を許容差内に保持することが
熱変形などのために不可能となるおそれがあって、これ
が実施できない等の理由と、これに加うるに前記したポ
ンプを構成する部品の寸法精度の経済性をもって定めら
れた許容差内のバラツキの集積と、さらに特にその縦寸
法の許容差の重合が、図2、図3に示す管柱シリンダ2
1と電磁コイル20との間でその両端部位にそれぞれ嵌
設され、かつ吐出接手40に外嵌するクリップ止輪35
を介して外枠継鉄31と取付けねじ42を螺締着するこ
とで電磁コイル20と共に挟設されている環状磁極32
と環状磁路座板33とによって構成された磁気回路のう
ち就中、前記環状磁極32の下端面と、電磁プランジャ
22の上端部間の磁気空隙gのバラツキ及び電磁コイル
20の縦軸方向の磁気中性点と電磁プランジャ22の磁
気中心点との距離fのバラツキを生じ、ポンプの吐出性
能に大きな影響を与える。
The magnetic material constituting the magnetic path such as the electromagnetic plunger described above can be cut even if it has been magnetically annealed in advance.
The structure may change due to plastic working such as grinding, polishing, or press fitting of the valve seat, and the magnetic permeability may decrease by several tens of percent as an example. There is a risk that it is impossible to maintain the straightness within the tolerance due to thermal deformation and the like, and this cannot be performed, and in addition to this, the dimensional accuracy of the parts constituting the pump described above The accumulation of the variation within the tolerance set with the economical efficiency, and more particularly, the overlap of the tolerance of the vertical dimension, is caused by the cylinder 2 shown in FIGS.
1 and the electromagnetic coil 20, each of which is fitted at both ends thereof, and which is externally fitted to the discharge joint 40.
An annular magnetic pole 32 sandwiched together with the electromagnetic coil 20 by screwing the outer frame yoke 31 and the mounting screw 42 through
And the annular magnetic path seat plate 33, the variation of the magnetic gap g between the lower end surface of the annular magnetic pole 32 and the upper end portion of the electromagnetic plunger 22 and the longitudinal direction of the electromagnetic coil 20. Variations occur in the distance f between the magnetic neutral point and the magnetic center point of the electromagnetic plunger 22, which greatly affects the discharge performance of the pump.

【0034】即ち、前記ポンプ構成部品の縦寸法の許容
差の重合集積と電磁プランジャ22を圧支する戻しバネ
23と補助バネ24のそれぞれの自由高さとバネ定数の
許容差内の異なる値によって前記磁気空隙gと距離fは
変化してくる。電磁プランジャ22に対する磁気吸引力
は磁気空隙の自乗に反比例するから、この磁気空隙gに
ついてのポンプの出力と重大な関係がある。
That is, the above-mentioned accumulation of the vertical dimension tolerances of the pump components and the respective free heights of the return spring 23 and the auxiliary spring 24 for supporting the electromagnetic plunger 22 and different values within the tolerances of the spring constants. The magnetic gap g and the distance f change. Since the magnetic attraction to the electromagnetic plunger 22 is inversely proportional to the square of the magnetic gap, it has a significant relationship with the output of the pump for this magnetic gap g.

【0035】尚、この磁気空隙gや電磁プランジャを圧
支する2つのバネの力関係については、本発明者がかつ
て提案した特公昭57−12863号の公報に詳細に開
示されているので、その説明は省略する。以上説明した
ようにポンプを構成する部品が、個々のポンプの吐出性
能に影響を与える要因を多分に含んでいるので、前掲の
図4に示した線図は個々に大なり小なりの変化を生じ決
して一様ではない。
The relationship between the magnetic gap g and the force of the two springs pressing the electromagnetic plunger is disclosed in detail in Japanese Patent Publication No. 57-12863 proposed by the present inventor. Description is omitted. As described above, since the components that make up the pump include many factors that affect the discharge performance of the individual pumps, the diagram shown in FIG. The consequences are never uniform.

【0036】したがって一回の流量測定、即ち付加抵抗
値−流量測定を該抵抗値の1つに対する流量の所謂一点
測定によって所定流量を調整制御しようとするときは、
そこに不正確で所定流量の許容範囲に設定して合格する
確率が低く、再度やり直す必要等の不経済性を招く。本
発明は、上記詳述したように、従来技術の欠陥を是正
し、電磁ポンプを大量生産する工程において、その吐出
流量を測定値に調整して製造する方法で、ポンプの構成
部品の上記した寸法精度等その他可能な限り極めてきび
しく許容差を規制することを避けて、ポンプの製造及び
メンテナンスのコストを上昇させることなく、そして更
にこの吐出流量を調整する方法の手数と、その増加によ
るコストアップを避けて、省力化により前記二律背反の
問題を解決して吐出性能その他のポンプの品質特性の安
定化により、その信頼性を高めて品質保証をなし、しか
も生産コストダウンを共に成し遂げることを目的とし、
その課題とするものである。
Therefore, when one flow rate measurement, that is, the additional resistance value-flow rate measurement is to be adjusted and controlled by a so-called one-point measurement of the flow rate for one of the resistance values,
There is an inaccuracy, the probability of setting the flow rate within the allowable range of the predetermined flow rate is low, and the cost is low. As described in detail above, the present invention corrects the deficiencies of the prior art, and in a process of mass-producing an electromagnetic pump, in a method of manufacturing by adjusting the discharge flow rate to a measured value, the above-mentioned components of the pump are described above. Avoid strict tolerances such as dimensional accuracy, etc. as much as possible, without increasing the cost of pump production and maintenance, and further increase the number of methods of adjusting the discharge flow rate and increase the cost due to the increase The aim is to solve the above trade-off problem by saving labor, stabilize the discharge performance and other quality characteristics of the pump, improve the reliability and make quality assurance, and achieve the production cost reduction together. ,
That is the subject.

【0037】[0037]

【課題を解決するための手段】上記課題は本発明によ
り、特に、石油燃焼器用燃料供給電磁ポンプの製造方法
であって、摺動往復自在のフリーピストンを嵌着した管
柱シリンダの外周でこれを囲繞する電磁コイルと、該電
磁コイルの捲線の両端末をそれぞれ接続固定する端子A
並びにB、及び更に前記一方の端子Aから固定抵抗器を
介在して接続する端子Cとを備え、石油燃焼器に組込ま
れかつ該燃焼器に備えた駆動回路から供給される駆動パ
ルス状電流が上記端子Cと接続されない残余の端子Bと
端子C間に接続付勢されて、所定の燃料吐出量を維持す
る電磁ポンプであって、前記固定抵抗器を介さず端子
A,B間に前記駆動パルスを付勢時には、前記所定の燃
料吐出量を超えるように予め設計製造されている石油燃
焼器用燃料供給電磁ポンプにおいて、前記石油燃焼器に
備えるべき駆動回路と同等若しくは予め相関関係を測っ
て調整した吐出流量検査用駆動回路からの駆動パルスを
前記端子A,B間に供給するに際して該端子Aに、ポン
プの吐出流量を調整するために選定して付加固定抵抗器
を付加すべく、それぞれ異なる抵抗値を有する固定抵抗
器群のうちの抵抗値が前記付加固定抵抗器として予想さ
れる抵抗値より大及び小の、すなわち下限寄りと上限寄
りの2つの付設固定抵抗器を切換自在に介在させた抵抗
回路により、該切換られた付設固定抵抗器のそれぞれに
応じた電磁ポンプの吐出流量の二測定点を測定して付加
抵抗−流量線図上に二測定点を設定し、前記二測定点を
任意の直線による結合線により結んで、前記付加抵抗−
流量線図上にある所定の燃料吐出量を示す線と前記結合
線との交点から所定の抵抗値を求め、前記所定の燃料吐
出量の許容範囲内に収まるように前記固定抵抗器群のう
ちから上記所定の抵抗値に近似の抵抗値を有するものを
選定し、この選定抵抗器を端子Aと端子C間に仮接続し
て、前記吐出流量検査用駆動回路により前記抵抗回路か
ら切り換えて、残余の端子Bと端子C間に駆動パルスを
供給して、前記所定の燃料吐出量の許容範囲に収まるこ
とを確認したときにのみ前記仮接続した選定抵抗器を付
加固定抵抗器として本接続することができる。
According to the present invention, there is provided, in particular, a method for manufacturing a fuel supply electromagnetic pump for an oil combustor, wherein the method includes the steps of: And a terminal A for connecting and fixing both ends of the winding of the electromagnetic coil, respectively.
B, and a terminal C connected from the one terminal A via a fixed resistor, and a drive pulse-shaped current incorporated in the oil combustor and supplied from a drive circuit provided in the combustor. An electromagnetic pump that is connected and urged between the terminal C and the remaining terminal B that is not connected to the terminal C to maintain a predetermined fuel discharge amount, wherein the drive is performed between the terminals A and B without passing through the fixed resistor. At the time of energizing the pulse, in a fuel supply electromagnetic pump for an oil combustor designed and manufactured in advance to exceed the predetermined fuel discharge amount, adjustment is performed by measuring a correlation equivalent to or a correlation in advance with a drive circuit to be provided in the oil combustor. When supplying a drive pulse from the drive circuit for discharge flow rate inspection between the terminals A and B, it is necessary to add an additional fixed resistor to the terminal A in order to adjust the discharge flow rate of the pump. The resistance value of the fixed resistor group having a different resistance value is larger and smaller than the resistance value expected as the additional fixed resistor, that is, the two attached fixed resistors closer to the lower limit and the upper limit can be switched. Two measurement points of the discharge flow rate of the electromagnetic pump corresponding to each of the switched attached fixed resistors are measured by the interposed resistance circuit, and two measurement points are set on the additional resistance-flow rate diagram. The measurement points are connected by an arbitrary straight-line connecting line, and the additional resistance
A predetermined resistance value is obtained from an intersection of a line indicating a predetermined fuel discharge amount on the flow rate diagram and the connection line, and the fixed resistor group is selected from the fixed resistor group so as to fall within an allowable range of the predetermined fuel discharge amount. From the above, a resistor having a resistance value approximate to the predetermined resistance value is selected, the selected resistor is temporarily connected between the terminal A and the terminal C, and the discharge flow rate inspection drive circuit is switched from the resistance circuit, A drive pulse is supplied between the remaining terminals B and C, and the temporarily connected selected resistor is permanently connected as an additional fixed resistor only when it is confirmed that the predetermined fuel discharge amount falls within the allowable range. be able to.

【0038】[0038]

【発明の実施の形態】以下に添付した図面を用いて本発
明の実施の形態について説明する。図1は、本発明の実
施システム図で、即ち吐出流量を所定値に調整し設定す
る方法の基本的な1つの実施の形態であり、図2,図3
は、上記本発明実施の対象となるところの石油燃焼器用
燃料供給電磁ポンプの一例の一部断面を示す縦断説明図
と、その端子部分を表している平面図である。
Embodiments of the present invention will be described below with reference to the accompanying drawings. FIG. 1 is a diagram showing an implementation system of the present invention, that is, one basic embodiment of a method of adjusting and setting a discharge flow rate to a predetermined value.
FIG. 1 is a vertical sectional view showing a partial cross section of an example of a fuel supply electromagnetic pump for petroleum combustors which is an object of the present invention, and a plan view showing a terminal portion thereof.

【0039】図2の電磁ポンプについては、既にその構
成と作用が説明済であるが、図3において電磁コイル2
0の巻枠と一体の端子盤17には、端子A11,同B1
2,同C13が設けられ、電磁コイルの捲線の一方の端
末14は端子A11に、他方の端末15は端子B12に
それぞれ接続固定され、端子A11と端子C13との間
には、固定抵抗器16を接続可能としてある。
The structure and operation of the electromagnetic pump of FIG. 2 have already been described.
0 terminal B11 and terminal B11
2. The same terminal C13 is provided, one terminal 14 of the winding of the electromagnetic coil is connected and fixed to the terminal A11, and the other terminal 15 is connected and fixed to the terminal B12. A fixed resistor 16 is connected between the terminal A11 and the terminal C13. Can be connected.

【0040】そこで前記図1について説明する。図にお
いて図示しない商用交流などの電源回路から入力され、
石油燃焼器に組み込まれる燃焼制御回路に含まれるもの
と同様の電磁ポンプの吐出量検査用駆動回路2から、所
定電圧、周波数、周期中の導通期間、即ちデューテイ比
が設定されたパルス電流が出力されるようになってい
る。
FIG. 1 will be described. Input from a power supply circuit such as a commercial AC not shown in the figure,
A pulse current in which a predetermined voltage, a frequency, a conduction period during a cycle, that is, a duty ratio is set, is output from a drive circuit 2 for discharge amount inspection of an electromagnetic pump similar to that included in a combustion control circuit incorporated in an oil combustor. It is supposed to be.

【0041】電磁ポンプ1から吐出燃料油は、図示しな
い接続配管ノズルを経て燃焼器の気化器や火炉に導かれ
るのであるが、この配管やノズルの内径寸法長さ、内径
の表面粗さ、燃料間の温度等によるレイノルズ数の変動
や、火炉内の気流、火焔の圧力変動等の要因の変化で、
吐出量が変動することがあるので、燃焼器のこれらの特
性に対して相関関係を予め測って調整した吐出流量検査
用駆動回路2でも、その都度前記パルスを再調整してこ
れを設定することがある。即ち、同一仕様、同機種の電
磁ポンプ及びこれを組込む石油燃焼器であってもそれぞ
れの生産ロット毎に若干の相違があるので、その都度該
相関関係の調整を必要とする現状である。
The fuel oil discharged from the electromagnetic pump 1 is guided to a carburetor or a furnace of a combustor through a connection pipe nozzle (not shown). The length of the inner diameter of the pipe and the nozzle, the surface roughness of the inner diameter, and the fuel Changes in factors such as fluctuations in the Reynolds number due to the temperature between them, airflow in the furnace, and pressure fluctuations in the flame,
Since the discharge amount may fluctuate, the pulse may be readjusted and set every time even in the discharge flow rate inspection drive circuit 2 in which the correlation between these characteristics of the combustor is measured in advance and adjusted. There is. In other words, even with electromagnetic pumps of the same specification, the same model, and an oil combustor incorporating the same, there is a slight difference for each production lot, so that it is necessary to adjust the correlation each time.

【0042】上述の通りこの種の電磁ポンプは、その吐
出性能に影響を与える要因が甚だ多く、最も廉価で圧
力、流量の調整機構を有せず、構造簡単、小形なフリー
ピストンポンプであるために、起磁力を発生するアンペ
アターン、燃料油のレイノルズ数の変動、電磁プランジ
ャの摺動抵抗、弁開閉時の流量損失などが、直ちに吐出
流量の変動となる電磁プランジャの行程長や油圧の変化
をもたらし、電磁プランジャや駆動する力の伝達は剛体
をもってなる構成ではなく、磁力とこれに対するバネの
反発力のみであり、吐出量の調整は、所望の吐出流量以
上に設計製造した電磁ポンプの電源に直列の抵抗値を付
加して電圧を逓降させることによって電流を減じて吐出
流量を所定値まで下降させてこれを保持する方法がポン
プ製造上の部品の前記許容差等の集積により生じる吐出
流量のバラツキを規制するのに構成上最も廉価な方法な
のである。
As described above, this type of electromagnetic pump has a great number of factors affecting its discharge performance, is the least expensive, does not have a pressure and flow rate adjusting mechanism, is simple in structure, and is a small free piston pump. In addition, changes in the stroke length and hydraulic pressure of the electromagnetic plunger, which immediately change the discharge flow rate, due to ampere turns that generate a magnetomotive force, fluctuations in the Reynolds number of fuel oil, sliding resistance of the electromagnetic plunger, and flow loss when the valve is opened and closed. The transmission of the electromagnetic plunger and the driving force is not a rigid structure, but only the magnetic force and the repulsive force of the spring. The discharge amount is adjusted by adjusting the power of the electromagnetic pump designed and manufactured to a desired discharge flow rate or more. The method of reducing the current by adding a series resistance value to the voltage and decreasing the voltage to reduce the discharge flow rate to a predetermined value and hold the same is a method in front of the pump manufacturing parts. Is What the most inexpensive way configured to restrict the variations in the discharge flow rate caused by the accumulation of tolerances and the like.

【0043】しかし、これに対して前述した付加抵抗値
の選定とこれに対するポンプの所定流量の確認作業の省
人省力化と能率向上によるコストダウンとを同時に計ら
なければならない課題となるのである。そこで、再び図
1の説明に戻る。吐出量検査用駆動回路2の一方の出力
端子6と、電磁コイル20の巻線の端末15を接続固定
する端子B12とを結ぶ一方の母線と、同じく他方の出
力端子5からリレー4を経て1つは端子dと前記端子C
13とを結ぶ母線と、リレー4により切替られる端子c
から後述する抵抗器群のうちの抵抗値が下限寄りの小さ
い第1の付設固定抵抗器R1 と、同じく抵抗値が上限寄
りの大きい第2の付設固定抵抗器R2 とをリレー3の端
子aとbとを切換自在に介在させた抵抗回路7を介して
電磁コイル20の他方の端末14が接続固定される端子
A11と結ぶ母線とがあり、前記端子C13と端子A1
1との間には、これも後述する付加固定抵抗器R16が
接続可能である。
However, on the other hand, it is necessary to simultaneously measure the above-mentioned additional resistance value selection and the work of confirming the predetermined flow rate of the pump in order to save labor and labor and to reduce the cost by improving the efficiency. Therefore, the description returns to FIG. One bus connecting the output terminal 6 of the ejection amount inspection drive circuit 2 to the terminal B12 for connecting and fixing the terminal 15 of the winding of the electromagnetic coil 20; One is terminal d and the other is terminal C
13 and a terminal c switched by the relay 4
The first fixed resistor R 1 having a small resistance value near the lower limit and the second fixed resistor R 2 having a large resistance value near the upper limit in a group of resistors described later are connected to terminals of the relay 3. There is a bus connected to a terminal A11 to which the other terminal 14 of the electromagnetic coil 20 is connected and fixed via a resistor circuit 7 in which a and b are switchably interposed. The terminal C13 and the terminal A1 are connected to each other.
1, an additional fixed resistor R16, which will also be described later, can be connected.

【0044】今、吐出圧力検査用駆動回路(以下単に駆
動回路と称する)2から駆動パルスを供給するに当た
り、先ずリレー4の端子cを閉じ、抵抗回路7のリレー
3の端子a,bを切換えて、第1の固定抵抗器R1 と第
2の固定抵抗器R2 とを交互に切換え介して電磁コイル
20を付勢したときの電磁ポンプの第1及び第2の吐出
流量Q1 ,Q2 をそれぞれ測定し、この測定した第1と
第2の吐出流量Q1 ,Q2 と前記第1及び第2固定抵抗
器R1 ,R2 のそれぞれの抵抗値とで図5に示す付加抵
抗値−流量線図上に、この二測定点P1 ,P2 を設定
し、この二測定点P1 ,P2 間を後述説明する結合線に
より結び、この付加抵抗値−流量値線間上にある前記所
定の吐出流量QX を示す線と前記結合線との交点Px
より付加すべき抵抗値RX を求め、前記所定吐出流量に
対して、例えば±2〜2.5%の許容範囲に収まるよう
にするために日本工業規格に定められたものを主体とす
る前記固定抵抗器群の中から前記抵抗値RX と近似の近
似値を有するものを一個の固定抵抗器として選定し、こ
の選定された固定抵抗器Rを前記端子A11と同C13
との間で仮接続すると共に、リレー4の端子cを開き、
端子dを閉じるように切換えて、電磁コイル20が所定
の吐出流量の許容範囲を満足したときのみ前記選定抵抗
器Rを付加固定抵抗器として本接続するものである。
When a drive pulse is supplied from a drive circuit for discharge pressure inspection (hereinafter simply referred to as drive circuit) 2, first, terminal c of relay 4 is closed, and terminals a and b of relay 3 of resistance circuit 7 are switched. When the electromagnetic coil 20 is energized by alternately switching the first fixed resistor R 1 and the second fixed resistor R 2 , the first and second discharge flow rates Q 1 , Q 2 is measured, and the first and second discharge flow rates Q 1 and Q 2 and the resistance values of the first and second fixed resistors R 1 and R 2 are used as additional resistances shown in FIG. value - the diagram flow line, the secondary set the measurement points P 1, P 2, tie the bond line to be described later explained between the second measurement points P 1, P 2, this additional resistance - flow value line between the the resistance value R X to be added by the intersection P x of the a predetermined line indicating a discharge flow rate Q X and the bond line in In order to keep the predetermined discharge flow rate within the allowable range of, for example, ± 2 to 2.5%, the resistance is selected from among the fixed resistor group mainly composed of those defined in Japanese Industrial Standards. A resistor having an approximate value of the value R X is selected as one fixed resistor, and the selected fixed resistor R is connected to the terminals A11 and C13.
And the terminal c of the relay 4 is opened.
The terminal d is switched to be closed, and the selected resistor R is permanently connected as an additional fixed resistor only when the electromagnetic coil 20 satisfies a predetermined allowable range of the discharge flow rate.

【0045】この吐出流量調整及び付加固定抵抗器選定
方法の一実施の形態をフローチャートにより示したもの
が図7である。前記仮接続した固定抵抗器Rによって調
整されたポンプの吐出流量が所定の燃料吐出量の許容範
囲を外れたときは、再度ポンプについての付加抵抗値−
吐出流量特性を見直し、図8に示すフローチャートの通
りの手順によって処理する。また、上記した吐出流量検
査用の駆動回路2から駆動パルスを供給する際に、切換
えリレー4および抵抗回路7を省いて、端子A、11と
端子B、12に直接接続してその一方の母線に前記した
抵抗値の異なるR1 もしくはR2 の抵抗器を介設させ
て、これらの二つの付設固定抵抗器のそれぞれに応じた
電磁ポンプの吐出量の二測定点を測定し、付加抵抗−流
量線図上に二測定点を設定し、以下前記同様の手順手法
によって所定の燃料吐出量に対応した付加固定抵抗器を
選定して上記課題を解決する手段とすることができるも
のである。なお、図5は、前記所定の燃料吐出量に対す
る電磁コイル20の付加抵抗値を求めるために、横軸に
付加抵抗値オームを取り、縦軸に流量値ミリリットル/
分をとって求めた前記結合線の一例であって、これら結
合線については添付の表1〜12についての説明に際し
て後に詳述する。
FIG. 7 is a flowchart showing one embodiment of the method of adjusting the discharge flow rate and selecting the additional fixed resistor. When the discharge flow rate of the pump adjusted by the temporarily connected fixed resistor R is out of the predetermined allowable range of the fuel discharge amount, the additional resistance value of the pump is re-determined.
The discharge flow characteristics are reviewed, and processing is performed according to the procedure shown in the flowchart of FIG. Further, when the drive pulse is supplied from the drive circuit 2 for discharging flow rate inspection, the switching relay 4 and the resistor circuit 7 are omitted, and the terminals A, 11 and the terminals B, 12 are directly connected to one bus. wherein the different R 1 or by interposed resistor to R 2 resistance value, measured two measurement points of the discharge amount of the electromagnetic pump according to each of these two attached fixed resistor, the additional resistance - Two measurement points are set on the flow rate diagram, and an additional fixed resistor corresponding to a predetermined fuel discharge amount is selected by the same procedure as described above, and can be used as means for solving the above problem. FIG. 5 shows an additional resistance value ohm on the horizontal axis and a flow rate value milliliter / liter on the vertical axis in order to determine the additional resistance value of the electromagnetic coil 20 with respect to the predetermined fuel discharge amount.
This is an example of the connection lines obtained by taking a part, and these connection lines will be described later in detail when describing the attached Tables 1 to 12.

【0046】そこで、図4において説明した電磁コイル
20を備えた図2に示した構成の電磁ポンプ1によっ
て、以下その電磁コイル20に付加抵抗値を加えて流量
を所定値に調整する方法を表1〜表12によって比較説
明する。この場合には、電磁ポンプ1を構成する電磁コ
イル20をはじめすべての部品の寸法精度ほか規定され
た基準値になるべく近いものを選定して組み立てた母集
団Nのうちからランダムに抜き取ったn20台の電磁ポ
ンプによってそれぞれの流量調整を行なった。これは流
量特性を揃えたいねらいによる。n20としたのは、品
質管理、抜取検査における前記Nを大きさにかかわら
ず、抜取数nを20、合否判定個数Cを最小限の一定
値、例えばOとしたときに横軸にそのロットの不良率を
とり、縦軸にこのロットが合格するときの確立をとった
O−C曲線がほぼ類似であり、ロットの大きさNはなる
べく大きくした方が相対的な試料nの大きさは小さくて
すむ点を参考として、nの値を20としたものである。
Therefore, a method for adjusting the flow rate to a predetermined value by adding an additional resistance value to the electromagnetic coil 20 by the electromagnetic pump 1 having the configuration shown in FIG. Comparative description will be made with reference to Tables 1 to 12. In this case, n20 units randomly selected from the population N assembled and selected as close as possible to dimensional accuracy of all parts including the electromagnetic coil 20 constituting the electromagnetic pump 1 and other specified reference values. The respective flow rates were adjusted by the electromagnetic pumps described above. This depends on the purpose of making the flow characteristics uniform. The reason why n20 is set is that the number of samples n in the quality control and the sampling inspection, regardless of the size, is 20, and the number of acceptance / rejection determinations C is a minimum constant value, for example, O, and the horizontal axis represents the lot number of the lot. The defect rate is taken, and the OC axis curve established on the vertical axis when this lot passes is almost similar. The larger the lot size N is, the smaller the relative sample n size is. The value of n is set to 20 with reference to the point of success.

【0047】この20台の電磁ポンプを以下述べる流量
調整方法の実験のすべてに供したものである。ただし、
この電磁ポンプが燃料油中に含まれる繊維状その他のフ
ィルタ39を通過するような極めて微細なゴミやポンプ
内の金属の切粉やプラスチックなどの極微小片等の夾雑
物によって、吐出オリフィス41、配管、ノズル内部な
どに付着滞留して燃料油の流動を阻害したり、弁体に付
着してその機能を損ねたり、電磁プランジャ22の摺動
往復作動を妨げて、流動変動することを防止するために
ポンプ内部の清掃等十分留意して実験を行った。
The twenty electromagnetic pumps were used in all experiments of the flow rate adjusting method described below. However,
The discharge orifice 41 and the pipe are formed by extremely fine dust such as the electromagnetic pump passing through a fibrous or other filter 39 included in the fuel oil, or foreign matter such as metal chips or ultra-fine pieces such as plastic in the pump. In order to prevent the fuel oil from adhering to the inside of the nozzle and obstructing the flow of the fuel oil, adhering to the valve body and impairing its function, and obstructing the sliding reciprocating operation of the electromagnetic plunger 22 to prevent the flow from fluctuating. The experiment was conducted with careful attention to cleaning the inside of the pump.

【0048】尚、この外に吸入接手37を含むポンプ内
部が、ポンプ始動時に空である所謂初期吸引時及び燃料
油中の溶存ガスの分離によって発生する電磁プランジャ
22の乱調などの吐出脈動のための流動変動のなるべく
発生しないようにすることを含み、予めポンプ作動時に
は、所謂馴らし運転を実施後、前記流量測定及び所定流
量調整時の流量測定等の実験を行ったものである。 (1)そこで試料n20台の電磁ポンプについて、流量
調整用付加抵抗器の抵抗値がそれぞれ0.0, 2.0,4.3,
6.2, 8.0, 10.0 Ωのときを各計測点としてそれぞれの
計測点のそれぞれの流量を測定したときの付加抵抗値−
吐出流量とそのバラツキを示したものが表1に掲示して
ある。O オームとは、付加抵抗値を付けない電磁コイル
20の固有抵抗値のみの場合である。
In addition, the inside of the pump including the suction joint 37 is discharged due to discharge pulsation such as so-called initial suction which is empty when the pump is started and turbulence of the electromagnetic plunger 22 generated by separation of dissolved gas in fuel oil. In this experiment, the so-called running-in operation was performed in advance when the pump was operated, and experiments were performed on the flow rate measurement and the flow rate measurement at the time of adjusting the predetermined flow rate. (1) Then, with respect to the electromagnetic pumps of 20 samples n, the resistance values of the flow rate adjusting additional resistors are 0.0, 2.0, 4.3,
Additional resistance value when each flow rate at each measurement point is measured with 6.2, 8.0, 10.0 Ω as each measurement point-
Table 1 shows the discharge flow rates and their variations. O ohm is a case where only the specific resistance value of the electromagnetic coil 20 without an additional resistance value is given.

【0049】表中、xm は平均値、HENSAは標準偏
差、MAXは最大値、MINは最小値、Rはネハバをそ
れぞれ示し、以下各表とも共通である。回帰係数は、前
述した最小自乗法により回帰分析をしたときの値であ
り、aは横軸に付加抵抗値R1 〜Rn をとり、縦軸には
これに対応する流量Q1 〜Qn をとった付加抵抗値−吐
出流量線図の傾きであり、bはこの線図の切片を表すも
ので数値の負号の付されているのは、該線図が右肩下が
りであるためである。γは相関係数である。即ち、前記
Rをx、Qをyで表すときは、
In the table, x m is the average value, HENSA is the standard deviation, MAX is the maximum value, MIN is the minimum value, and R is Nehaba, which are common to the following tables. The regression coefficient is a value obtained by performing a regression analysis by the least square method described above, and a represents the additional resistance values R 1 to R n on the horizontal axis, and the corresponding flow rates Q 1 to Q n on the vertical axis. Where b is the slope of the added resistance value-discharge flow rate diagram, and b represents the intercept of the diagram, and the reason why a negative sign is attached to the numerical value is that the diagram is falling to the right. is there. γ is a correlation coefficient. That is, when R is represented by x and Q is represented by y,

【0050】[0050]

【外3】 [Outside 3]

【0051】となる。表2は、回帰式換算流量で平均値
が示される。このように、前記した通り電磁ポンプの構
成部品の寸法精度その他の許容差をその標準値になるべ
く近いものを選択して組込んでも、個々のポンプには、
このような吐出流量のバラツキがあり、その3σ(標準
偏差)/xm の100分率は±12%程度である。
Is as follows. Table 2 shows the average value in the regression equation converted flow rate. In this way, as described above, even if the dimensional accuracy and other tolerances of the components of the electromagnetic pump are selected and incorporated as close as possible to their standard values, each pump has
There are variations of this delivery rate, 100 minutes rate of the 3 [sigma] (standard deviation) / x m is about ± 12%.

【0052】これらの数値の算出等については後述す
る。表3は、実測流量の回帰分析による換算流量に対す
る変化率で付加抵抗値にそれぞれ対応するものを示す。 (2)次に、前記付加抵抗値−吐出流量線図(以下単に
線図と称する。)を図5によって説明する。
Calculation of these numerical values will be described later. Table 3 shows the rate of change of the measured flow rate with respect to the converted flow rate by regression analysis, which corresponds to the added resistance value. (2) Next, the additional resistance value-discharge flow rate diagram (hereinafter simply referred to as a diagram) will be described with reference to FIG.

【0053】図5において、付加抵抗値として予想され
る予想値より大きいものと小さいものとの二つを測定点
として選び、そのときの第一および第二の固定抵抗器R
1 ,R 2を付加したときのポンプの吐出流量を図5上に
1 およびQ2 としてとり、R1 −Q1 、R2 −Q2
結合点P1 ,P 2(計測点P1 (2.0Ω)、P
2 (8.0Ω)が選ばれる)を得、これらを二つの測定
点とする。これらの測定点P1 ,P2 を通る直線の換算
式は、 そして付加抵抗値がR1 とR2 に対する流量値Q1 ,Q
2 よりaとbの値を求めると、
In FIG. 5, two measurement points, one larger than the expected value and the other smaller than the expected value, are selected as measurement points, and the first and second fixed resistors R at that time are selected.
1, the discharge flow rate of the pump when adding R 2 taken as Q 1 and Q 2 on Figure 5, R 1 -Q 1, the point of attachment of R 2 -Q 2 P 1, P 2 (measurement points P 1 (2.0Ω), P
2 (8.0Ω is selected), and these are taken as two measurement points. The conversion formula of a straight line passing through these measurement points P 1 and P 2 is The flow rate values Q 1 and Q for the additional resistance values R 1 and R 2
When the values of a and b are obtained from 2 ,

【0054】[0054]

【外4】 [Outside 4]

【0055】[0055]

【外5】 [Outside 5]

【0056】この二式により求められた流量変数a,b
の値を上記換算式に代入して、付加抵抗値R1 〜RN
対する流量Q1 〜Qn を求め、描いた線図により所定流
量Qx を得べき付加抵抗値Rx を得ることができる。
The flow variables a and b obtained from these two equations
The values are substituted into the conversion equation to obtain the flow rate Q 1 to Q n for additional resistance R 1 to R N, to obtain a predetermined flow rate Q x additional resistance R x to obtain a by diagram depicting it can.

【0057】しかし、これらの換算式の適用は二つの測
定点に固有のものであって、計測点が同じとみなされて
も、同じ結果は得られない。すなわち、二つの測定点を
得た場合は、n=20台の平均的回帰直線は利用でき
ず、個別に二つの測定点を任意の直線による結合線によ
り結んで、この結合線を付加抵抗−流量線図上の付加抵
抗−流量線の仮想線とするしかない。表4のn=20台
の実測値を二つの測定点P1 (2.0Ω)、P2 (8.
0Ω)として、それぞれ二つの測定点を任意の直線によ
る結合線により結び、この結合線による各計測点の流量
を仮想したのが表5である。表4の実測値と表5の仮想
値との比較が表6に示してある。表6において、表4の
各計測点のうちの2.0Ωと8.0Ωとは表5の測定点
として用いられるので、その差は0.00として示して
ある。各電磁ポンプにおいて、各二つの測定点を結ぶ任
意の直線による結合線と、求める所定流量Qx との交点
x に対応する抵抗値となる。このような測定方法は、
二つの測定点を用いるので、いわゆる二点測定法と呼ば
れ、電磁ポンプを大量生産する際に有効である。 (3)次に、前記測定点P1 とP2 とを結ぶ結合線を曲
線として、さらに実測値に近似する付加抵抗−流量線図
を仮想し、所定吐出流量に調整する付加抵抗−流量線図
を仮想し、所定吐出流量に調整する付加抵抗器の選定方
法を図4、図5および表7、表8、表9によって以下説
明する。
However, the application of these conversion equations is specific to two measurement points, and the same result cannot be obtained even if the measurement points are regarded as the same. That is, when two measurement points are obtained, the average regression line of n = 20 units cannot be used, and the two measurement points are individually connected by a connection line of an arbitrary straight line, and this connection line is connected to the additional resistance − There is no choice but to use a virtual line of the additional resistance-flow rate line on the flow rate diagram. The actual measurement values of n = 20 units in Table 4 were measured at two measurement points P 1 (2.0Ω) and P 2 (8.
0 Ω), each of the two measurement points is connected by a connection line formed by an arbitrary straight line, and the flow rate of each measurement point by the connection line is imagined in Table 5. Table 6 shows a comparison between the measured values in Table 4 and the virtual values in Table 5. In Table 6, since 2.0Ω and 8.0Ω among the measurement points in Table 4 are used as the measurement points in Table 5, the difference is shown as 0.00. In the electromagnetic pump, comprising a coupling line by any of a straight line connecting the two measurement points, and the resistance value corresponding to the intersection P x and a predetermined flow rate Q x to be obtained. Such a measurement method is
Since two measurement points are used, this method is called a so-called two-point measurement method and is effective when mass-producing an electromagnetic pump. (3) Next, Examples curve connecting line connecting the measuring points P 1 and P 2, additional resistor approximates the further measured values - virtually the flow chart, the additional resistance is adjusted to a predetermined discharge flow rate - flow line A method of selecting an additional resistor for adjusting the discharge flow rate to a predetermined discharge flow rate will be described with reference to FIGS. 4 and 5 and Tables 7, 8, and 9 below.

【0058】ところで、前述した図4の説明の際に述べ
た電磁コイルの固定抵抗値RO は、単なる直流抵抗値の
みでなく、断続パルス電流が付勢されるときにはインピ
ーダンスとなり、総合的な抵抗値は増大する。この値を
cとし、付加抵抗値r1 〜rn ,R1 〜Rn ,Rx 等を
Xとし、前記したアンペアターンA×Tに電動機として
の電気的および機械的なポンプの効率を乗じた値をaと
し、そして補正係数をbとしたときに、前記付加抵抗値
に対する流量Qは次の換算式から求められる。
Incidentally, the fixed resistance value R O of the electromagnetic coil described in the description of FIG. 4 is not only a mere DC resistance value, but also becomes an impedance when an intermittent pulse current is energized. The value increases. This value is is c, the additional resistance value r 1 ~r n, R 1 ~R n, the R x such as X, multiplied by the electrical and efficiency of the mechanical pump as a motor in ampere-turns A × T described above When the calculated value is a and the correction coefficient is b, the flow rate Q with respect to the additional resistance value is obtained from the following conversion formula.

【0059】[0059]

【外6】 [Outside 6]

【0060】この式から、反対に所定流量を得べき付加
抵抗値xを選定することもでき、上記二点測定法におけ
る換算流量を算出する換算式となるのである。図5に示
す付加抵抗値対吐出流量の実測値の線図から前記c,
a,bも求められる。すなわち、
On the contrary, the additional resistance value x for obtaining the predetermined flow rate can also be selected from this equation, and this is a conversion equation for calculating the converted flow rate in the two-point measurement method. From the diagram of the additional resistance value versus the actually measured value of the discharge flow rate shown in FIG.
a and b are also required. That is,

【0061】[0061]

【外7】 [Outside 7]

【0062】そこで電磁ポンプのそれぞれ個々に相違す
る前記実測流量のデータにより次の各式からそれぞれの
係数は求められる。
Therefore, the respective coefficients are obtained from the following equations based on the data of the actually measured flow rates which are different from each other in the electromagnetic pump.

【0063】[0063]

【外8】 [Outside 8]

【0064】[0064]

【外9】 [Outside 9]

【0065】次に、(1)式に前記(2)、(3)
(4)により得られたc,a,bの値を代入すれば、個
々のポンプにおける付加抵抗値に対する吐出流量の関係
が換算流量となる。
Next, the above equations (2) and (3)
By substituting the values of c, a, and b obtained in (4), the relationship between the discharge flow rate and the additional resistance value of each pump becomes the reduced flow rate.

【0066】表7は、電磁ポンプの生産ロッドごとの母
集団Nからランダムに抜き取った試料n=20における
付加抵抗値に対する吐出流量のバラツキを実測記録した
もので、その各計測点0.0,2.0,4.3,6.
2,8.0,10.0Ωにおける実測値は表1,表4と
同じである。表7のa,b,cの平均値xを(1)式に
代入して得た曲線が図5に示されている。この曲線の離
れた三つの計測点p1(0.0Ω),p2 (6.2Ω),
3 (10.0Ω)を選ぶと、図5に示すように、横軸
に附加抵抗値r1,r2, r3 を、電磁コイル固定抵抗値R
o (図6の説明において前述した)に加えたときの、そ
れぞれの流量の平均値q1 ,q2 ,q3 を縦軸にとっ
て、この両軸の各点を通る線の結合線が前記計測点p1,
2,p3 となる。これらの三つの計測点のうち、p1
2 およびp2 とp3 をそれぞれ結ぶ辺の各中点から立
ち上げた垂線の交点が曲率中心となり、この曲率中心と
前記三つの計測点を結ぶ線が曲率半径ρで、その曲率半
径ρの円弧で前記三つの計測点を結ぶと、その結合線は
前記(1)式に代入して得た曲線と近似する。
Table 7 shows the measured and recorded variation of the discharge flow rate with respect to the additional resistance value for the sample n = 20 randomly extracted from the population N for each production rod of the electromagnetic pump. 2.0, 4.3, 6.
The measured values at 2, 8.0 and 10.0 Ω are the same as Tables 1 and 4. FIG. 5 shows a curve obtained by substituting the average value x of a, b, and c in Table 7 into the equation (1). The three measurement points p 1 (0.0Ω), p 2 (6.2Ω),
When p 3 (10.0Ω) is selected, as shown in FIG. 5, the added resistance values r 1, r 2 , and r 3 are plotted on the horizontal axis, and the fixed resistance value R of the electromagnetic coil is plotted on the horizontal axis.
o (average values q 1 , q 2 , q 3 ) of the respective flow rates when added to (described above in the description of FIG. 6), the combined line of the lines passing through the points on both axes is the measurement value The point p 1 ,
p 2 and p 3 . Of these three measurement points, the intersection of the perpendiculars rising from the respective midpoints of the sides connecting p 1 and p 2 and p 2 and p 3 respectively becomes the center of curvature, and this curvature center and the three measurement points When the connecting line has a radius of curvature ρ and the three measurement points are connected by an arc having the radius of curvature ρ, the connecting line approximates to a curve obtained by substituting the equation (1).

【0067】この生産ロット母集団Nの電磁ポンプのそ
れぞれに対して、前述した図1に示す駆動回路(2)か
ら駆動パルスを供給するにあたり、第一および第二の固
定抵抗器R1 ,R2 を付加したときのポンプの吐出流量
を図5上にQ1 およびQ2 をとり、R1 −Q1 ,R2
2 の結合点P1 ,P2 を得る。この結合点P1 ,P2
は計測点のうちの2.0Ωと8.0Ωの二点が選ばれ、
これらが二つの測定点となる。その選び方は求める付加
抵抗器として予想される抵抗値より大きいものと小さい
ものとの二つがよい。この二つの測定点P1 ,P2 を前
記曲率半径ρをもつ円弧の結合線で結ぶと、この結合線
は付加抵抗−流量線図上の付加抵抗−流量線の仮想線と
することができる。この仮想線を用いて、試料n=20
に適用した計測点の各々の流量が表8に示されている。
表7の実測値と表8の仮想値との比較が表9に示してあ
る。表9において、表7の各計測点のうち2.0Ωと
8.0Ωとは表8の測定点として用いられているので、
その差は0.00として示してある。この結合線と求め
る所定流量QX との交点Px に対応する抵抗値Rx が求
める理論上の付加する付加抵抗値となる。そして、前記
(1)式に表7のa,b,cの平均値を代入して得た曲
線の流量値Qが前記QX に該当し、付加する抵抗値xが
前記Rx に該当することとなる。
When supplying a drive pulse from the drive circuit (2) shown in FIG. 1 to each of the electromagnetic pumps of the production lot population N, the first and second fixed resistors R 1 , R The discharge flow rate of the pump when 2 is added is shown as Q 1 and Q 2 in FIG. 5, and R 1 −Q 1 , R 2
The connection points P 1 and P 2 of Q 2 are obtained. The connection points P 1 and P 2
Is selected from two measurement points, 2.0Ω and 8.0Ω,
These are the two measurement points. There are two ways to select the resistor, one that is larger than the expected resistance value of the additional resistor to be sought and one that is smaller. When these two measurement points P 1 and P 2 are connected by a connecting line of an arc having the radius of curvature ρ, this connecting line can be a virtual line of the additional resistance-flow rate line on the additional resistance-flow rate diagram. . Using this virtual line, the sample n = 20
Table 8 shows the flow rate of each of the measurement points applied to the measurement.
Table 9 shows a comparison between the measured values in Table 7 and the virtual values in Table 8. In Table 9, since 2.0Ω and 8.0Ω among the measurement points in Table 7 are used as the measurement points in Table 8,
The difference is shown as 0.00. The additional resistance to be added the theoretical resistance R x may correspond to the intersection P x and a predetermined flow rate Q X of obtaining this coupling line is determined. Then, the (1) a table 7, b, the flow rate value Q of the curve obtained by substituting the average value of c is corresponding to the Q X in formula, added to the resistance value x corresponds to the R x It will be.

【0068】それから前述の通り、固定抵抗器群の中か
ら、前記抵抗値RX と近似の抵抗値を有するものを一個
の付加すべき固定抵抗器Rとして選定して、これを図1
に示す端子A11、同C13間に仮に接続して、端子C
13、同B12間に駆動回路2からパルス電流を電磁コ
イル20に付勢して、電磁ポンプ1が所定流量( 例えば
毎分6.63ミリリットル±7%受入れ、製造工程間の許容
誤差±2〜2.5 %、DC23.5 ±0.05 V,20℃) の条件を
満足したときのみ、前記固定抵抗器Rを本接続する。こ
の所定流量許容範囲を逸脱した電磁ポンプは、図5、図
8に示すように、新たに付加抵抗値R3 に対応する流量
3 を測り、この両者の線図上の結合点P3 と、前記P
1 、P2 を通る曲率円を求める作業を再度繰り返して、
付加すべき固定抵抗器を選定する。ひるがえって、二つ
の測定点P1 とP2 の外にその中間にある新たに付加抵
抗値R3 に対応する流量Q3 を測り、これら三つの点P
1 、P2 、P3 を用いて円弧を想定し、この円弧を測定
点P1 、P2 の結合線として用いるならば、図5に示す
曲線から円弧を求める必要がなく、単に三点を測定して
その円弧を用いるということで、二点法の変形として簡
単に付加すべき固定抵抗器を選定することができる。 (4)表10〜12は前記したいわゆる一点測定法によ
るデータである。
Then, as described above, from the fixed resistor group, a resistor having a resistance value approximate to the resistance value R X is selected as one fixed resistor R to be added, and this is selected as FIG.
Is temporarily connected between terminals A11 and C13 shown in FIG.
13, a pulse current is energized from the drive circuit 2 to the electromagnetic coil 20 during the period B12, and the electromagnetic pump 1 receives a predetermined flow rate (for example, 6.63 milliliters per minute ± 7%, and a permissible error between manufacturing processes ± 2 to 2.5%). , 23.5 ± 0.05 V DC, 20 ° C.) only when the fixed resistor R is fully connected. Electromagnetic pumps outside this predetermined flow rate tolerance, 5, 8, measure the flow rate Q 3 corresponding to the newly added resistance R 3, a coupling point P 3 on the diagram lines of both , Said P
Repeat the procedure to determine the curvature of a circle passing through the 1, P 2 again,
Select the fixed resistor to be added. In turn, measure the flow rate Q 3 corresponding to the newly added resistance R 3 in the middle out of the two measurement points P 1 and P 2, these three points P
If an arc is assumed using 1 , P 2 and P 3 and this arc is used as a connecting line between the measurement points P 1 and P 2 , there is no need to find the arc from the curve shown in FIG. By measuring and using the arc, it is possible to easily select a fixed resistor to be added as a modification of the two-point method. (4) Tables 10 to 12 show data obtained by the so-called one-point measurement method.

【0069】まず、表10は、一点測定すなわち付加抵
抗値RO で付加抵抗値のないときの流量QO を基準とし
て、これに付加抵抗値Rをそれぞれ加えたときの流量Q
1 の変化率、つまり線図の傾きaは、
First, Table 10 shows that the flow rate Q when adding the additional resistance value R to the flow rate Q O when the one-point measurement, that is, the additional resistance value R O and no additional resistance value is used as a reference.
The rate of change of 1 , ie the slope a of the diagram, is

【0070】[0070]

【外10】 [Outside 10]

【0071】となり、切辺bは付加抵抗値OΩのときの
流量値となる。そして流量値Q−付加抵抗値x(R)と
の関係を示す換算流量は、 Q=b−ax 表10はその実測流量でのバラツキを示している。これ
らを平均化したのが表2であって、これが回帰式換算流
量となる。表11はこの回帰式換算流量から得られる直
線に平行な直線を表10の0Ωの各計測点を通るように
移行させ、その直線により得られた各計測点の流量を換
算流量として示す。したがって、表12では計測点0Ω
が0.00となっている。
Thus, the cut side b is the flow rate value when the additional resistance value is OΩ. The converted flow rate indicating the relationship between the flow rate value Q and the additional resistance value x (R) is as follows: Q = b-ax Table 10 shows the variation in the actually measured flow rate. These are averaged in Table 2, which is the regression equation converted flow rate. In Table 11, a straight line parallel to the straight line obtained from the regression equation converted flow rate is shifted so as to pass through each measurement point of 0Ω in Table 10, and the flow rate at each measurement point obtained by the straight line is shown as a converted flow rate. Therefore, in Table 12, the measurement point 0Ω
Is 0.00.

【0072】表12は前記換算流量に対する実測流量の
変化を示す。すなわち、換算流量値と実測データ値との
誤差を%で示したもので、この誤差が大きいことを証明
している。以上詳述した(1)〜(4)の各流量関係の
表1〜表12に示したデータは、この実験に供した電磁
ポンプが、その構成部品の寸法、精度その他の数値がそ
の許容範囲の基準値に近いものをもって構成したもので
あるにもかかわらず、なお上記した流量のバラツキがあ
る。このような許容範囲の基準値に近い部品を選択して
構成することは、コスト高を伴い、経済上困難であるか
ら、現時点で原価的に許されるコストで収まる前記許容
差内の構成部品をもって組み立てた電磁ポンプでは、そ
の吐出流量特性、すなわ付加抵抗値対流量変化のバラツ
キはさらに大きくなるものである。
Table 12 shows changes in the measured flow rate with respect to the reduced flow rate. That is, the error between the converted flow rate value and the actually measured data value is indicated by%, which proves that this error is large. The data shown in Tables 1 to 12 relating to the respective flow rates of (1) to (4) described in detail above indicate that the electromagnetic pump used in this experiment has the dimensions, accuracy, and other numerical values of its component parts within the allowable range. However, there is still the above-mentioned variation in the flow rate, although it is configured with a value close to the reference value. It is costly and economically difficult to select and configure components that are close to the reference value of such an allowable range. In the assembled electromagnetic pump, the variation in the discharge flow rate characteristic, that is, the variation in the additional resistance value versus the flow rate change is further increased.

【0073】この実験の表1〜表12に示すデータにつ
いてさらに説明する。 (1)の表1〜表3に示したポンプの前記吐出流量特性
のバラツキは前述したように、3σ(シグマ、標準偏
差, HENSA 以下3σという)3σ/xm の100 分率は±
12%程度となる。
The data shown in Tables 1 to 12 of this experiment will be further described. (1) Table 1 as the variation in the discharge flow rate characteristics of the pump shown in Table 3 described above in, 3 [sigma] (sigma standard deviation, 3 [sigma] hereinafter referred Hensa) 100 parts per 3 [sigma] / x m is ±
It is about 12%.

【0074】これは表1〜表3より求めたもので、n=
20台のポンプについて、付加抵抗値0.0, 2.0, 4.3,
6.2, 8.0, 10.0Ωに対するそれぞれの流量を測定し、そ
のバラツキを求めたものである。サンプル(n=20)
の流量の標準偏差の3倍3σを流量の平均値xm で除す
と、99.7%の信頼度で母集団の最大バラツキを求めるこ
とができるのである。
This is obtained from Tables 1 to 3, where n =
For 20 pumps, additional resistance values of 0.0, 2.0, 4.3,
The flow rate was measured for 6.2, 8.0, and 10.0Ω, and the variation was obtained. Sample (n = 20)
By dividing 3 times the standard deviation of the flow rate 3σ by the average value x m of the flow rate, the maximum variation of the population can be obtained with a reliability of 99.7%.

【0075】実際の計算は、各付加抵抗値ごとの流量の
平均値および標準偏差の平均値を求め、上記の3σ/x
m ×100 の式により求めた。すなわち、 xm の平均値=6.960 ml/M, HENSAσの平均値=0.2774 ml/M, 3σ/xm ×100 =11.96 % (2)つぎに、前記いわゆる二点測定法で線図を直線と
みなしたとき、3σ+xm は約±2%程度である。
In the actual calculation, the average value of the flow rate and the average value of the standard deviation for each additional resistance value are obtained, and the above 3σ / x
It was determined by the formula of m × 100. That is, the average value of x m = 6.960 ml / M, the average value of HENSAσ = 0.2774 ml / M, 3σ / x m × 100 = 11.96% (2) Next, a straight line view in the so-called two-point measurement method When considered, 3σ + x m is about ± 2%.

【0076】すなわち、表4のデータより、該二点測定
法による線図を求め、その線図よりそれぞれの抵抗値に
おける流量を概算したものが表5の換算流量で、この換
算流量と表4の実測流量の変化率すなわち誤差率を示し
たものが表6である。つまり、二点測定法により求めた
線図(直線)と実際の実測流量との差がそのポンプの流
量設定精度となる。
That is, from the data in Table 4, a diagram was obtained by the two-point measurement method, and the flow rate at each resistance value was roughly calculated from the diagram, and the converted flow rate in Table 5 was obtained. Table 6 shows the rate of change of the actually measured flow rate, that is, the error rate. That is, the difference between the diagram (straight line) obtained by the two-point measurement method and the actual measured flow rate is the flow rate setting accuracy of the pump.

【0077】実際の計算は、各付加抵抗値ごとの流量の
平均値および標準偏差の平均値を求めて、3σによる母
集団の前記バラツキを推定する。表6には、データが計
算値と誤差率(%)で表されているから、3σ+xm
母集団における推定最大バラツキが求められる。 xm の平均値0.0893 (%) 、δの平均値 0.6256 ( %) 故に、3σ+xm =±1.966 % (3)前記二点測定法において、線図を曲線とした表7
〜表9に示すものは、前記(2)の説明通りの手法によ
り算出して、表9から次のとおり求められる。
In the actual calculation, the average value of the flow rate and the average value of the standard deviation for each additional resistance value are obtained, and the variation of the population due to 3σ is estimated. Table 6, since data is represented by the calculated value and the error rate (%), the estimated maximum variation is obtained in the population at 3 [sigma] + x m. the average value of x m 0.0893 (%), therefore the average value of δ 0.6256 (%), the 3σ + x m = ± 1.966% (3) the two-point measuring method, Table 7 that the diagrams and curves
Table 9 is calculated by the method described in the above (2), and is obtained from Table 9 as follows.

【0078】3σ+xm =±1.69% (4)いわゆる、一点測定法で表10〜表12に示され
るものは、3σ+xm =約±4%程度である。表10の
データの平均値より抵抗−流量特性の線図の傾きを求
め、そのときの傾きはすべて一定であるものとして、そ
れぞれの付加抵抗値における流量を演算して求めた概算
流量表11と表10の実測流量との差が、そのポンプの
設定精度となる。
3σ + x m = ± 1.69% (4) In the so-called one-point measurement method shown in Tables 10 to 12, 3σ + x m = about ± 4%. From the average value of the data in Table 10, the slope of the resistance-flow rate diagram was determined, and the slope at that time was assumed to be constant, and the approximate flow rate table 11 was calculated by calculating the flow rate at each additional resistance value. The difference from the measured flow rate in Table 10 is the setting accuracy of the pump.

【0079】実際の計算はそれぞれの付加抵抗値におけ
る流量の平均値と標準偏差の平均値を求めて、3σによ
る母集団のバラツキを推定する。この場合の抜き取った
試料をnとすると、標準偏差はσn-1 によって求められ
る。なお、本願の明細書で各表に記載されている標準偏
差は、σn であって、これは前記付加抵抗値に対応する
流量測定を試料n=20について実測流量と回帰分析も
しくは他の本願発明の方式による換算流量値と対比し、
解析し説明しているからである。なお、標準偏差σn
対してσn-1 の値はきわめて僅少な増加があることは周
知である。表12は、表11に示される流量の概算値と
表10に示される実測値との誤差(%)を表す。よっ
て、3σ+xm で最大バラツキが推定される。
In the actual calculation, the average value of the flow rate and the average value of the standard deviation at each additional resistance value are obtained, and the variation of the population due to 3σ is estimated. Assuming that the sample taken in this case is n, the standard deviation is obtained by σ n-1 . Note that the standard deviation described in each table in the specification of the present application is σ n , which means that the flow rate measurement corresponding to the additional resistance value was performed by regression analysis with the measured flow rate for the sample n = 20 or other application. In comparison with the converted flow rate value according to the method of the invention,
It is because it is analyzed and explained. It is well known that the value of σ n-1 has a very small increase with respect to the standard deviation σ n . Table 12 shows an error (%) between the approximate value of the flow rate shown in Table 11 and the actually measured value shown in Table 10. Therefore, the maximum variation is estimated at 3σ + x m .

【0080】表12より、xm の平均値−0.688(%) 、
σの平均値 1.5574 ( %) 故に、3σ+xm =±3.98 (%) となるのである。 以上説明したように、(4)の一点測定法では、3σ+
m ≒±4(%)程度であって、本願発明の(2)、
(3)の二点測定法と比較すると、それぞれ2.0倍、2.3
5倍に誤差が拡大される。
From Table 12, it can be seen that the average value of x m -0.688 (%),
The average value of σ is 1.5574 (%). Therefore, 3σ + x m = ± 3.98 (%). As described above, in the one-point measurement method (4), 3σ +
x m ≒ ± 4 (%), and (2) of the present invention,
Compared with the two-point measurement method of (3), it is 2.0 times and 2.3 times, respectively.
The error is magnified 5 times.

【0081】したがって、従来技術であるところの
(4)の一点測定法を利用した場合には、不良率が高く
なり、そのために再調整作業等の手間がかかり、それに
よる不経済性を伴うのみならず、製造工程間における許
容範囲からはみ出す流量のポンプが比較的多いことは、
不合格率が高くなることを意味し、この不合格率が例え
ば100 PPM あったとすれば、この生産ロットの製品が出
荷検査を通過して市場に提供された場合にも、やはり同
率近い不具合品の発生するおそれがあり、品質保証上の
も問題が残り、その信頼性を損なう懸念が大きい。
Therefore, when the one-point measuring method (4), which is the prior art, is used, the defective rate becomes high, which requires time and labor for readjustment and the like, resulting in uneconomical effects. Rather, the fact that there are relatively many pumps with flow rates that exceed the allowable range between manufacturing processes
This means that the rejection rate will be high, and if the rejection rate is, for example, 100 PPM, even if the product of this production lot passes the shipping inspection and is brought to the market, the defective product will still have the same rate May occur, and there remains a problem in quality assurance, and there is a great concern that its reliability will be impaired.

【0082】本願発明による前記(2)、(3)の二点
測定法を使用して所定流量に調整の場合、実測流量に対
する換算流量の誤差は1.69〜1.96%であり、これは流量
の許容範囲内に収まるので、不良率はほとんど皆無とな
るものである。このように、本発明による石油燃焼器用
燃料供給電磁ポンプの製造方法は、上述の説明によるよ
うに吐出流量を所定値に確保するのに信頼性が高く、か
つそれによって再調整や市場クレームの発生を防いで経
済性にも高い利点をもたらすものである。
When the flow rate is adjusted to a predetermined flow rate using the two-point measurement method (2) or (3) according to the present invention, the error of the converted flow rate with respect to the actually measured flow rate is 1.69 to 1.96%, which is the allowable flow rate. Since it falls within the range, there is almost no defect rate. As described above, the method for manufacturing a fuel supply electromagnetic pump for an oil combustor according to the present invention is highly reliable in securing the discharge flow rate to a predetermined value as described above, and thereby, readjustment and the generation of market complaints are caused. And provides a high economical advantage.

【0083】なお、このような電磁ポンプの製造工程間
の流量調整測定は、少なくとも20連以上の流量調整測
定検査装置(以下単に検査装置という)により実施し、
前記した流量測定、これに伴う諸式の演算はじめ、所定
流量の許容範囲に調整する付加固定抵抗器の選択から、
その取付け後の流量の確認およびその記録まですべてコ
ンピュータ処理を伴うもので省人、省力化はもちろん、
その処理時間もきわめて短く、その作業時間も短縮され
る。前記検査装置への電磁ポンプの装脱および電源接続
と切り離しも含めて自動化できる。
The flow rate adjustment measurement during the manufacturing process of such an electromagnetic pump is performed by at least 20 or more flow rate adjustment measurement / inspection devices (hereinafter simply referred to as inspection devices).
From the flow measurement described above, the calculation of various equations accompanying this, from the selection of an additional fixed resistor to be adjusted to an allowable range of a predetermined flow rate,
Everything from the confirmation of the flow rate after installation to the recording of the flow is accompanied by computer processing, saving labor and labor,
The processing time is very short and the working time is also reduced. It can be automated, including loading and unloading of the electromagnetic pump from the inspection device and connection and disconnection of the power supply.

【0084】流量計もしくは流量測定装置は、瞬時読み
取り式の精密流量測定装置もあるが、その取付けスペー
スが大きく、非常に高価であり、しかも本願の場合に
は、電磁ポンプの上記したように少ない流量を図るには
不適なことがあり、本願発明に用いる流量測定装置とし
ては、例えばビューレット(Burette)管を利用する。こ
れにより、所定容量例えば5 〜10ミリリットルを満たす
時間を、電磁弁、光電センサ、時間計等により測定し、
コンピュータで瞬時に流量を計算する方法が採られる。
Although the flow meter or the flow measuring device is a precision flow measuring device of an instantaneous reading type, the mounting space is large, very expensive, and in the case of the present application, the electromagnetic pump is small as described above. In some cases, the flow rate measurement device is not suitable for measuring the flow rate. As the flow rate measurement device used in the present invention, for example, a burette tube is used. Thus, the time required to fill a predetermined volume, for example, 5 to 10 milliliters, is measured by a solenoid valve, a photoelectric sensor, an hour meter, and the like.
A method of calculating the flow rate instantly by a computer is adopted.

【0085】この流量計測の所要時間を、付加抵抗値R
1 ,R2 についてそれぞれの流量Q1 ,Q2 および選定
された固定抵抗器Rを接続したときの流量Qの3回の流
量測定と付帯時間を含めて3分間、180秒としても2
0台でこれを割れば、1台当たり9秒である。順次に流
量の測定、調整、確認を行なえば、マニュアルで電磁ポ
ンプを検査装置に装脱しても充分時間的に余裕がある。
The time required for the flow rate measurement is represented by the additional resistance value R
1 and R 2 are 3 minutes including the flow rates Q 1 and Q 2 and the flow rate Q when the selected fixed resistor R is connected, and three times including the incidental time.
If this is divided by 0 units, it is 9 seconds per unit. If the measurement, adjustment, and confirmation of the flow rate are performed sequentially, there is ample time even if the electromagnetic pump is manually attached to and detached from the inspection device.

【0086】つまり、人手によって1台ごとに処理する
時間の1/20で足りるわけで、したがって本発明の前
記(2)の表4〜表6、(3)の表7表9で述べた二点
測定法は、前記したように確認を含めて3回の流量測定
を行なうにもかかわらず、前記(4)の表10〜表12
で述べたような従来技術の一点測定法における一回測定
および流量の確認を含む2回の流量測定を行なう流量調
整設定方法に比較して、ポンプ1台についてわずか数秒
の時間差があるのみである。しかしながら、この二点測
定法は、前記したように流量調整誤差がきわめて少な
く、実質的にはほとんど所定流量の許容範囲に入り、こ
れを満足させ、品質保証上の信頼性がきわめて高い利点
があり、流量測定、調整、設定、確認の作業所要時間も
前述の通り従来技術のものに比較してほとんど数秒の差
で問題とするに当たらず、かえって再調整設定などの手
間をほとんど必要としないことおよびポンプを構成する
部品お寸法精度その他の標準値に対する許容差をいっそ
うきびしくしてコスト高を招くことがないので経済的で
ある。
That is, 1/20 of the time required to process each unit manually is sufficient, and therefore, the two-times described in Tables 4 to 6 of the above (2) and Table 9 of the above (2) of the present invention are sufficient. In the point measurement method, although the flow rate measurement including the confirmation is performed three times as described above, Table 10 to Table 12 of the above (4) are used.
There is only a time difference of only a few seconds per pump as compared with the flow adjustment setting method of performing two flow measurements including one measurement and flow rate confirmation in the conventional one-point measurement method as described in the above section. . However, this two-point measurement method has the advantage that the flow rate adjustment error is extremely small as described above, and substantially falls within the allowable range of the predetermined flow rate, which is satisfied, and the reliability in quality assurance is extremely high. As described above, the time required for the work of measuring, adjusting, setting, and confirming the flow rate is almost a matter of a few seconds compared to the prior art, and requires little work such as readjustment setting. It is economical because tolerances for parts constituting the pump, dimensional accuracy, and other standard values are not stricter and cost is not increased.

【0087】[0087]

【発明の効果】以上説明したように、本発明によるいわ
ゆる二点測定法を用いた石油燃焼器用燃料供給電磁ポン
プの製造方法は、二測定点を付加抵抗器として予想され
る抵抗値より大および小の、すなわち下限寄りと上限寄
りとの抵抗器を選んで測定して得ると共に、この二測定
点を直線の結合線により結び、この結合線を利用して所
定の抵抗値を求めたことにより、前記したように流量調
整誤差がきわめて少なく、実質的にはほとんど所定流量
の許容範囲に入り、これを満足させ、品質保証上の信頼
性がきわめて高い利点があり、流量測定、調整、設定、
確認の作業所要時間も二測定点を切り換え自在に介在さ
せた二つの抵抗器をもつ抵抗回路により求め、仮接続の
抵抗器の合否の確認もこの抵抗回路からの切り換えで行
なうことにより、前述の通り従来技術のものに比較して
ほとんど数秒の差で問題とするに当たらず、かえって再
調整設定などの手間をほとんど必要としないことおよび
ポンプを構成する部品および寸法精度その他の標準値に
対する許容差をいっそうきびしくしてコスト高を招くこ
とがないので経済的である。
As described above, the method of manufacturing a fuel supply electromagnetic pump for an oil combustor using the so-called two-point measuring method according to the present invention has two measuring points larger than the resistance value expected as an additional resistor. By selecting and measuring a small resistor, that is, a resistor closer to the lower limit and closer to the upper limit, the two measurement points are connected by a straight connection line, and a predetermined resistance value is obtained by using the connection line. As described above, the flow rate adjustment error is extremely small, substantially falls within the allowable range of the predetermined flow rate, and has the advantage of satisfying this, and having extremely high quality assurance reliability, flow rate measurement, adjustment, setting,
The time required for the confirmation work is also determined by a resistance circuit having two resistors with two measurement points switchably interposed, and the confirmation of pass / fail of the temporarily connected resistor is also performed by switching from this resistance circuit. As compared with the prior art, the difference is almost no more than a few seconds, and it requires little trouble such as readjustment setting, and the tolerance of parts and dimensional accuracy and other standard values constituting the pump. It is economical because it does not increase the cost and increase the cost.

【0088】また、本発明の電磁ポンプの製造方法にお
いては、付加抵抗値の選定とこれに対するポンプの所定
流量の確認作業がすべてコンピュータ処理を伴うもの
で、省人、省力化と、能率向上によるコストダウンとを
同時に計ることができる。
In the method of manufacturing the electromagnetic pump according to the present invention, the selection of the additional resistance value and the operation of confirming the predetermined flow rate of the pump in response to the selection all involve computer processing, which saves labor and labor and improves efficiency. Cost reduction can be measured at the same time.

【0089】[0089]

【表1】 [Table 1]

【0090】[0090]

【表2】 [Table 2]

【0091】[0091]

【表3】 [Table 3]

【0092】[0092]

【表4】 [Table 4]

【0093】[0093]

【表5】 [Table 5]

【0094】[0094]

【表6】 [Table 6]

【0095】[0095]

【表7】 [Table 7]

【0096】[0096]

【表8】 [Table 8]

【0097】[0097]

【表9】 [Table 9]

【0098】[0098]

【表10】 [Table 10]

【0099】[0099]

【表11】 [Table 11]

【0100】[0100]

【表12】 [Table 12]

【図面の簡単な説明】[Brief description of the drawings]

【図1】本発明の一実施の形態で、電磁ポンプの吐出流
量を所定値に調整して設定する方法の回路図である。
FIG. 1 is a circuit diagram of a method for adjusting and setting a discharge flow rate of an electromagnetic pump to a predetermined value according to an embodiment of the present invention.

【図2】図1の本発明の実施の対象となる、石油燃焼機
器用燃料供給電磁ポンプの一例の一部断面を表す縦断説
明図である。
FIG. 2 is a longitudinal sectional view showing a partial cross section of an example of a fuel supply electromagnetic pump for petroleum combustion equipment, which is an object of the present invention in FIG.

【図3】図2の電磁ポンプにおけるその端子部分を表し
ている平面図である。
FIG. 3 is a plan view showing a terminal portion of the electromagnetic pump of FIG. 2;

【図4】横軸に付加抵抗値をとり、縦軸にアンペアター
ンをとった電磁ポンプの電磁コイルによる磁力の関係線
図である。
FIG. 4 is a graph showing the relationship between the magnetic force generated by the electromagnetic coil of the electromagnetic pump in which the horizontal axis represents the additional resistance value and the vertical axis represents the ampere-turn.

【図5】横軸に付加抵抗値をとり、縦軸に吐出流量をと
った、電磁ポンプにおけるこの両者の関係を示す線図で
ある。
FIG. 5 is a diagram showing the relationship between the two values in an electromagnetic pump, in which the horizontal axis indicates the additional resistance value and the vertical axis indicates the discharge flow rate.

【図6】横軸に付加抵抗値をとり、縦軸に吐出流量をと
った電磁ポンプにおけるこの両者の関係を回帰分析によ
る回帰直線によって求めた線図である。
FIG. 6 is a graph showing the relationship between the two values in an electromagnetic pump having an additional resistance value on the horizontal axis and a discharge flow rate on the vertical axis, obtained by a regression line by regression analysis.

【図7】本発明による電磁ポンプの吐出量調整および付
加抵抗器を選定する製造方法のフローチャートである。
FIG. 7 is a flowchart of a manufacturing method for adjusting a discharge amount of an electromagnetic pump and selecting an additional resistor according to the present invention.

【図8】本発明による電磁ポンプの吐出量調整および付
加抵抗器を選定する製造方法のフローチャートである。
FIG. 8 is a flowchart of a manufacturing method for adjusting a discharge amount of an electromagnetic pump and selecting an additional resistor according to the present invention.

【符号の説明】[Explanation of symbols]

1 電磁ポンプ 2 吐出量検査用駆動回路 3 リレー 4 リレー 5,6 端子 7 抵抗回路 a,b,c,d 端子 R1,R 2 固定抵抗器 11 端子A 12 端子B 13 端子C 16 固定抵抗器R 20 電磁コイル1 electromagnetic pump 2 discharge quantity inspection driving circuit 3 relays 4 relays 5, 6 terminal 7 resistor circuit a, b, c, d terminal R 1, R 2 fixed resistor 11 terminals A 12 pin B 13 terminal C 16 Resistors R 20 electromagnetic coil

フロントページの続き (72)発明者 御苑 輝雄 東京都大田区池上5丁目23番13号 太産 工業株式会社内 (72)発明者 千葉 泰常 東京都大田区池上5丁目23番13号 太産 工業株式会社内 (72)発明者 五十嵐 健二 東京都大田区池上5丁目23番13号 太産 工業株式会社内 (56)参考文献 特公 平7−101033(JP,B2) (58)調査した分野(Int.Cl.7,DB名) F04B 1/00 - 23/14 F04B 49/00 - 51/00 Continuing on the front page (72) Inventor Teruo Misono 5-23-13 Ikegami, Ota-ku, Tokyo Taisan Industry Co., Ltd. (72) Inventor Yasutane Chiba 5-23-13 Ikegami, Ota-ku, Tokyo Taisan Industry Inside (72) Inventor Kenji Igarashi 5-23-13 Ikegami, Ota-ku, Tokyo Taisan Industry Co., Ltd. (56) References JP-B7-101033 (JP, B2) (58) Fields surveyed (58) Int.Cl. 7 , DB name) F04B 1/00-23/14 F04B 49/00-51/00

Claims (1)

(57)【特許請求の範囲】(57) [Claims] 【請求項1】 摺動往復自在のフリーピストンを嵌着し
た管柱シリンダの外周でこれを囲繞する電磁コイルと、
該電磁コイルの捲線の両端末をそれぞれ接続固定する端
子A並びにB、及び更に前記一方の端子Aから固定抵抗
器を介在して接続する端子Cとを備え、 石油燃焼器に組込まれかつ該燃焼器に備えた駆動回路か
ら供給される駆動パルス状電流が上記端子Cと接続され
ない残余の端子Bと端子C間に接続付勢されて、所定の
燃料吐出量を維持する電磁ポンプであって、 前記固定抵抗器を介さず端子A,B間に前記駆動パルス
を付勢時には、前記所定の燃料吐出量を超えるように予
め設計製造されている石油燃焼器用燃料供給電磁ポンプ
において、 前記石油燃焼器に備えるべき駆動回路と同等若しくは予
め相関関係を測って調整した吐出流量検査用駆動回路か
らの駆動パルスを前記端子A,B間に供給するに際して
該端子Aに、ポンプの吐出流量を調整するために選定し
て付加固定抵抗器を付加すべく、それぞれ異なる抵抗値
を有する固定抵抗器群のうちの抵抗値が前記付加固定抵
抗器として予想される抵抗値より大及び小の、すなわち
下限寄りと上限寄りの2つの付設固定抵抗器を切換自在
に介在させた抵抗回路により、該切換られた付設固定抵
抗器のそれぞれに応じた電磁ポンプの吐出流量の二測定
点を測定して付加抵抗−流量線図上に二測定点を設定
し、 前記二測定点を任意の直線による結合線により結んで、
前記付加抵抗−流量線図上にある所定の燃料吐出量を示
す線と前記結合線との交点から所定の抵抗値を求め、 前記所定の燃料吐出量の許容範囲内に収まるように前記
固定抵抗器群のうちから上記所定の抵抗値に近似の抵抗
値を有するものを選定し、この選定抵抗器を端子Aと端
子C間に仮接続して、前記吐出流量検査用駆動回路によ
り前記抵抗回路から切り換えて、残余の端子Bと端子C
間に駆動パルスを供給して、前記所定の燃料吐出量の許
容範囲に収まることを確認したときにのみ前記仮接続し
た選定抵抗器を付加固定抵抗器として本接続する、 特に大量生産工程において燃焼器に組込む際、所定の燃
料吐出量の許容範囲に保持可能かつ互換性を有すること
を特徴とする石油燃焼器用燃料供給電磁ポンプの製造方
法。
1. An electromagnetic coil which surrounds an outer periphery of a tubular cylinder on which a free reciprocating sliding free piston is fitted;
Terminals A and B for connecting and fixing both ends of the winding of the electromagnetic coil, respectively, and a terminal C for connecting from the one terminal A with a fixed resistor interposed therebetween. A driving pulse-like current supplied from a driving circuit provided in the vessel is connected between the terminal B and the terminal C not connected to the terminal C, and is energized between the terminals C to maintain a predetermined fuel discharge amount; When the drive pulse is energized between the terminals A and B without passing through the fixed resistor, a fuel supply electromagnetic pump for an oil combustor designed and manufactured in advance so as to exceed the predetermined fuel discharge amount. When supplying a drive pulse from the discharge flow rate inspection drive circuit between the terminals A and B, which is equal to or preliminarily adjusted by a drive circuit to be provided in the terminal A, the discharge flow rate of the pump is supplied to the terminal A. In order to select and adjust and add an additional fixed resistor, the resistance value of the fixed resistor group having different resistance values is larger and smaller than the resistance value expected as the additional fixed resistor, that is, Two measurement points of the discharge flow rate of the electromagnetic pump corresponding to each of the switched attached fixed resistors are measured and added by a resistance circuit in which two attached fixed resistors closer to a lower limit and an upper limit are switchably interposed. Two measurement points are set on the resistance-flow rate diagram, and the two measurement points are connected by an arbitrary straight line.
A predetermined resistance value is obtained from an intersection of a line indicating a predetermined fuel discharge amount on the additional resistance-flow rate diagram and the connection line, and the fixed resistance is set so as to fall within an allowable range of the predetermined fuel discharge amount. A resistor having a resistance value approximate to the predetermined resistance value is selected from the group of devices, and the selected resistor is temporarily connected between the terminal A and the terminal C. From the remaining terminals B and C
Only when it is confirmed that the fuel discharge amount falls within the allowable range by supplying a drive pulse during the period, the temporarily connected selected resistor is permanently connected as an additional fixed resistor. A method of manufacturing a fuel supply electromagnetic pump for petroleum combustors, which is capable of maintaining a predetermined fuel discharge amount within an allowable range and being compatible when assembled into a fuel vessel.
JP8194283A 1996-07-24 1996-07-24 Manufacturing method of fuel supply electromagnetic pump for oil combustor Expired - Lifetime JP3022333B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP8194283A JP3022333B2 (en) 1996-07-24 1996-07-24 Manufacturing method of fuel supply electromagnetic pump for oil combustor

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP8194283A JP3022333B2 (en) 1996-07-24 1996-07-24 Manufacturing method of fuel supply electromagnetic pump for oil combustor

Related Child Applications (1)

Application Number Title Priority Date Filing Date
JP34043398A Division JPH11264370A (en) 1998-11-30 1998-11-30 Manufacture of fuel supply electromagnetic pump for oil combustor

Publications (2)

Publication Number Publication Date
JPH1037852A JPH1037852A (en) 1998-02-13
JP3022333B2 true JP3022333B2 (en) 2000-03-21

Family

ID=16322032

Family Applications (1)

Application Number Title Priority Date Filing Date
JP8194283A Expired - Lifetime JP3022333B2 (en) 1996-07-24 1996-07-24 Manufacturing method of fuel supply electromagnetic pump for oil combustor

Country Status (1)

Country Link
JP (1) JP3022333B2 (en)

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP7101033B2 (en) 2018-04-24 2022-07-14 株式会社三共 Pachinko machine

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP7101033B2 (en) 2018-04-24 2022-07-14 株式会社三共 Pachinko machine

Also Published As

Publication number Publication date
JPH1037852A (en) 1998-02-13

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