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JPS6260571B2 - - Google Patents
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JPS6260571B2 - - Google Patents

Info

Publication number
JPS6260571B2
JPS6260571B2 JP21208983A JP21208983A JPS6260571B2 JP S6260571 B2 JPS6260571 B2 JP S6260571B2 JP 21208983 A JP21208983 A JP 21208983A JP 21208983 A JP21208983 A JP 21208983A JP S6260571 B2 JPS6260571 B2 JP S6260571B2
Authority
JP
Japan
Prior art keywords
belt
belts
power transmission
tensile elasticity
elasticity
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
Application number
JP21208983A
Other languages
Japanese (ja)
Other versions
JPS60104832A (en
Inventor
Shinobu Sagisawa
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Fuji Electric Co Ltd
Original Assignee
Fuji Electric Corporate Research and Development Ltd
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Fuji Electric Corporate Research and Development Ltd filed Critical Fuji Electric Corporate Research and Development Ltd
Priority to JP21208983A priority Critical patent/JPS60104832A/en
Publication of JPS60104832A publication Critical patent/JPS60104832A/en
Publication of JPS6260571B2 publication Critical patent/JPS6260571B2/ja
Granted legal-status Critical Current

Links

Classifications

    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F16ENGINEERING ELEMENTS AND UNITS; GENERAL MEASURES FOR PRODUCING AND MAINTAINING EFFECTIVE FUNCTIONING OF MACHINES OR INSTALLATIONS; THERMAL INSULATION IN GENERAL
    • F16GBELTS, CABLES, OR ROPES, PREDOMINANTLY USED FOR DRIVING PURPOSES; CHAINS; FITTINGS PREDOMINANTLY USED THEREFOR
    • F16G1/00Driving-belts

Landscapes

  • Engineering & Computer Science (AREA)
  • General Engineering & Computer Science (AREA)
  • Mechanical Engineering (AREA)
  • Devices For Conveying Motion By Means Of Endless Flexible Members (AREA)

Description

【発明の詳細な説明】[Detailed description of the invention] 【発明の属する技術分野】[Technical field to which the invention pertains]

この発明は一般産業用の原動機と被動機側のプ
ーリ間に架け渡して動力伝達を行う多連結合形伝
動ベルトに関する。
The present invention relates to a multi-coupled power transmission belt for general industrial use that spans between a prime mover and a pulley on a driven machine side to transmit power.

【従来技術とその問題点】[Prior art and its problems]

まず、第1図に基本的なベルト伝動機構を示
す。図において1は駆動側プーリ、2は被動側プ
ーリ、3がプーリ1と2の間に巻掛けたベルトで
あり、運転時にはベルトの上側が張り側、下側が
弛み側となつてベルトとプーリ表面との間の摩擦
力で動力の伝達の行われることは周知の通りであ
る。また伝達動力が比較的大きい一般産業機械で
は通常複数本のベルトを巻掛けて使用し、かつこ
の場合にはすべりが少なく伝動効率のよいVベル
トが広く採用されている。 ところで、上記ベルト伝動機構の運転時には、
ベルト伝動機構に振動発生が見られ、特に動力伝
達系内に歯車装置などが一緒に組込まれていると
振動騒音が強くなることがある。またこの振動騒
音は、ある時はうなり音的に変化して運転保守要
員に不安感を与えることがある。 かかる騒音の発生メカニズムについて発明者の
考察したところによれば、その原因は次記に詳記
するように、個々のベルトについてその引張り弾
性がベルトの全長に亙つて一様でないことに起因
していることが判明した。すなわち、一般に市販
されているベルトを試料として、その全長に亙る
引張り弾性分布を調べるために次記の検査を行つ
た。まず1本のベルト3に第2図のようにベルト
3を16等分して各位置に〜番号をつけて標点
とする。さらに標点からプーリ1,2の軸間距
離lに相当する距離だけ離れた地点から等間隔に
′〜′の標点をつけ、そしてこのベルト3を第
1図のようにプーリ1と2の間に架け渡し、プー
リ1,2に力Pを与えてベルト3に張力を加えな
がら駆動側からプーリを回転させる。ここでベル
トの標点が第1図に示す×点に来た時の標点
と′間のベルト長さを測つてベルトの伸び分△
lを求め、この測定値から標点〜′間の平均
引張り弾性C=△l/Pを算出する。同様な操作
を各標点〜の各点について行うことにより、
第3図に示す引張り弾性分布が得られる。第3図
から明らかなようにベルトはその全長に亙る引張
り弾性が均一でなく、弾性の大きい領域と小さな
領域が存在する。このような傾向は程度の違いこ
そあれ、市販のベルトには1本1本についてそれ
ぞれ固有の弾性分布を示すことが発明者の行つた
検査結果から確認されている。その原因は次の点
にあると推定される。すなわち、頭記したVベル
トの製法は、第4図ないし第6図に示すようにま
ずドラム4の上に幅の広いベース用の未加硫ゴム
5を巻付け、さらにこのベース層の上に曲げ剛性
強化用のゴム6を巻付ける。次に芯線コード7を
狭いピツチ間隔でスパイラル状に連続巻したもの
を加硫する。次いで第5図に示した破線に沿つて
定寸法幅で輪切りし、最後にその周面に布8を巻
付けてVベルト3を完成する。このように幅の広
いものから輪切りして作られた芯線コード入りベ
ルト3の製品は、その周方向に沿つた場所により
スパイラル巻されたコード7の本数が多いところ
もあれば逆に少ないところもあり、かつこのコー
ドは全長のいずれかの地点で途切れている。また
製造工程で帯状のゴムを巻付けるために当然その
継ぎ目も存在する。しかも芯線コード7はベルト
に作用する張力のかなりの割合を分担しているこ
とから、この結果としてベルト3は周方向に沿つ
て引張り弾性の大きい領域と、小さい領域が形成
されることになる。 ところで第1図に示したベルト伝動機構におい
て、ベルト3によりプーリ1と2の間に伝達され
るトルクT1,T2は次式で表されることは周知
の通りである。 T1=R1(F1−F2) T2=R2(F1−F2) なお、F1、F2はそれぞれ張り側、弛み側のベ
ルト張力、R1、R2はプーリ1,2の半径であ
る。一方、第1図、第2図に示したベルト3の全
長について長さlの領域の平均的な弾性が小さい
領域をA、弾性が大きい領域をBとして、それぞ
れA、B領域の弾性をC1、C2とする。なおベル
トに張力を与えない状態では前記のA、B領域の
長さはいずれもlであり、また第3図の測定結果
に見られるように、1本のベルトについて一般に
A領域とB領域は互いにベルトの反対側位置にあ
る。ここでベルト3をプーリ1,2に架け渡し、
先記と同時に力Pを加えてベルト3に張力を与え
ながら回転した場合に、それぞれA領域とB領域
がベルトの張り側に来た時のベルトの各伸び分△
lはベルト長さlに対してF1C1、F1C2となり、
この状態を図示すると第7図、第8図のごとくで
ある。一方、それぞれA領域と、B領域がベルト
の弛み側に来た時のベルトの各伸び分△lはベル
ト長さlに対してF1C1、F2C2となる。このこと
から、ベルト3の張り側に弾性が小さいA領域、
弛み側に弾性の大きいB領域が来た状態と、逆に
ベルトの張り側にB領域、弛み側にA領域が来た
状態とでベルトの伸び分△lが変わり、かつその
ベルトの伸び分の差、すなわち第9図における角
度△θ(ラジアン)は次式で表される。 △θ={(F1C1−F2C2)−(F1C2−F2C1)}/R2 =(C1−C2)(F1+F2)/R2 すなわちA、B領域の弾性C1、C2の差が大き
いと△θは大きくなり、かつこの伸び分の変化が
公転周期で繰り返し発生することになる。なおベ
ルトの公転周期はベルトの周速をv、ベルトの全
長をLとすればL/vで表される。この結果、ベ
ルト伝動機構の運転時には、被動側の軸に第10
図に示すような振幅△θ、周波数v/Lの捩り振
動が生じることになる。この場合の振動周波数
は、一例としてベルト長さ1.5m、プーリの直径
150mmのベルト伝動機構をモデルとして算出する
と回転速度が2000r.p.mでは10.5Hz、4000r.p.mで
は21Hzとなる。 上記のように運転時におけるベルトの伸びの差
が基因して振動が発生した場合に、伝動機構を構
成している回転軸、歯車等の固有振動数が先記し
たベルトから生じる励振振動数と一致すると、共
振作用により大きな捩り振動となり、特に歯車装
置があると大きな騒音が発生する。またプーリの
回転軸の曲げ固有振動数と励振振動数が一致して
共振すると振動の増大や軸の破損を引き起こすお
それもある。さて、上記はベルトが1本の場合に
ついて述べたが、実際の伝導装置のように複数本
のベルトを並列に巻掛けた多連ベルトの場合に
は、振動の様子がさらに複雑になる。すなわち、
今同じプーリに2本のベルトを平行して架け渡し
た場合には、2本のベルト相互の相対的な位置の
如何によつて、各ベルトの周上の弾性分布が第1
1図あるいは第12図における(イ)、(ロ)のようにな
る。このうち、第11図の場合は各ベルトの弾性
(イ)と(ロ)が位相的に重畳し合つて2本のベルトの合
成弾性は(ハ)のようになり、弾性の最大値と最小値
との差Dが大きくなる。一方、第12図の場合は
弾性分布(イ)と(ロ)が位相的に互いに相殺し合うので
合成弾性は(ハ)のようになり、弾性の最大値と最小
値の差Dは小さくなり、全長に亙つて平均化す
る。一方、周知のようにベルトは運転時に生じる
クリープにより、プーリとの間で局部的にスリツ
プしながら移動するが、この場合にこのスリツプ
量は個々のベルトによつて異なることから、実際
の運転時には時間とともに各ベルトの周方向の相
対位置が変化し、第11図と第12図の状態が交
互に繰り返して生じることになる。この結果、被
動側のプーリ軸には第13図のように時間ととも
に振幅が変化する捩り振動が生じる。さらに使用
ベルトの本数が多くなれば益々複雑な不規則な捩
り振動が生じ、この結果として発生する振動騒音
はうなり音となり、機械の保守員に不安感を与え
る。
First, FIG. 1 shows a basic belt transmission mechanism. In the figure, 1 is the driving pulley, 2 is the driven pulley, and 3 is the belt wrapped between pulleys 1 and 2. During operation, the upper side of the belt is the tension side and the lower side is the slack side, and the belt and pulley surface are It is well known that power is transmitted by the frictional force between the two. Furthermore, in general industrial machines that transmit relatively large amounts of power, a plurality of belts are usually used, and in this case, V-belts with less slippage and high transmission efficiency are widely used. By the way, when the belt transmission mechanism is operated,
Vibration is observed in the belt transmission mechanism, and vibration noise may be particularly strong if a gear device or the like is also incorporated into the power transmission system. In addition, this vibration noise sometimes changes to a humming sound and gives a feeling of anxiety to operation and maintenance personnel. According to the inventor's study of the mechanism by which such noise is generated, the cause is that the tensile elasticity of each belt is not uniform over the entire length of the belt, as detailed below. It turned out that there was. That is, using a commercially available belt as a sample, the following tests were conducted to examine the tensile elasticity distribution over its entire length. First, as shown in Fig. 2, one belt 3 is divided into 16 equal parts and each position is numbered to serve as a gauge point. Furthermore, gauge points '~' are placed at equal intervals from a point away from the gauge point by a distance corresponding to the distance l between the axes of pulleys 1 and 2, and this belt 3 is connected between pulleys 1 and 2 as shown in Fig. The pulleys are rotated from the drive side while applying tension to the belt 3 by applying a force P to the pulleys 1 and 2. When the belt gauge point reaches point x shown in Figure 1, measure the length of the belt between the gauge point and
l is determined, and from this measured value, the average tensile elasticity C=Δl/P between the gauge point and '' is calculated. By performing similar operations for each point of each gauge point,
The tensile elasticity distribution shown in FIG. 3 is obtained. As is clear from FIG. 3, the tensile elasticity of the belt is not uniform over its entire length, and there are regions of high elasticity and regions of low elasticity. Although the degree of this tendency varies, it has been confirmed from the test results conducted by the inventor that each commercially available belt exhibits its own unique elasticity distribution. The reason for this is presumed to be the following. That is, the manufacturing method of the above-mentioned V-belt is as shown in FIGS. 4 to 6. First, a wide unvulcanized rubber 5 for the base is wrapped around the drum 4, and then a wide base layer of unvulcanized rubber 5 is wrapped around the drum 4. Rubber 6 for reinforcement of bending rigidity is wrapped around it. Next, the core wire cord 7 is continuously wound spirally at narrow pitch intervals and then vulcanized. Next, the V-belt 3 is completed by cutting it into rounds with a fixed width along the broken line shown in FIG. 5, and finally wrapping the cloth 8 around the circumferential surface. In this way, a belt 3 with a core wire cord made by cutting a wide material into rings has a large number of spirally wound cords 7 in some places and a small number in other places depending on the location along the circumferential direction. Yes, and this cord is interrupted at some point along its length. Naturally, seams also exist because the rubber band is wrapped in the manufacturing process. Moreover, since the core cord 7 shares a considerable proportion of the tension acting on the belt, as a result, the belt 3 has regions of high tensile elasticity and regions of low tensile elasticity along the circumferential direction. By the way, in the belt transmission mechanism shown in FIG. 1, it is well known that the torques T1 and T2 transmitted between the pulleys 1 and 2 by the belt 3 are expressed by the following equation. T1 = R1 (F1 - F2) T2 = R2 (F1 - F2) Note that F1 and F2 are the belt tensions on the tight side and slack side, respectively, and R1 and R2 are the radii of pulleys 1 and 2. On the other hand, regarding the entire length of the belt 3 shown in FIGS. 1 and 2, let A be the region where the average elasticity is small in the region of length l, and B be the region where the average elasticity is large, and the elasticity in the A and B regions, respectively, is C1. , C2. Note that when no tension is applied to the belt, the lengths of the A and B regions are both l, and as seen in the measurement results in Figure 3, the A and B regions of one belt are generally They are located on opposite sides of the belt. Here, belt 3 is stretched over pulleys 1 and 2,
When belt 3 is rotated while applying tension at the same time as described above, each elongation of the belt △ when area A and area B come to the tension side of the belt, respectively.
l is F1C1, F1C2 for belt length l,
This state is illustrated in FIGS. 7 and 8. On the other hand, when the A region and the B region come to the slack side of the belt, the elongation Δl of the belt becomes F1C1 and F2C2 with respect to the belt length l. From this, it can be seen that the A region where elasticity is small on the tension side of the belt 3,
The amount of elongation △l of the belt changes depending on the state where the B region with high elasticity is on the slack side and the state where the B region is on the tension side of the belt and the A region on the slack side, and the amount of elongation of the belt is The difference, that is, the angle Δθ (radians) in FIG. 9, is expressed by the following equation. △θ={(F1C1−F2C2)−(F1C2−F2C1)}/R2 = (C1−C2)(F1+F2)/R2 In other words, if the difference between the elasticities C1 and C2 in areas A and B is large, △θ becomes large, Moreover, this change in elongation occurs repeatedly during the revolution period. Note that the revolution period of the belt is expressed as L/v, where v is the circumferential speed of the belt and L is the total length of the belt. As a result, when the belt transmission mechanism is in operation, the 10th
A torsional vibration with an amplitude Δθ and a frequency v/L as shown in the figure is generated. In this case, the vibration frequency is, for example, belt length 1.5 m, pulley diameter
When calculating using a 150mm belt transmission mechanism as a model, the rotation speed is 10.5Hz at 2000r.pm and 21Hz at 4000r.pm. As mentioned above, when vibration occurs due to the difference in elongation of the belt during operation, the natural frequency of the rotating shaft, gears, etc. that make up the transmission mechanism is equal to the excitation frequency generated by the belt mentioned above. If they match, the resonance effect will result in large torsional vibrations, which will generate large noises, especially if there is a gear system. Furthermore, if the natural bending frequency of the rotary shaft of the pulley and the excitation frequency match and resonate, there is a risk of increased vibration and damage to the shaft. Now, the above description has been made regarding the case where there is only one belt, but in the case of a multi-belt in which multiple belts are wound in parallel as in an actual transmission device, the state of vibration becomes even more complicated. That is,
If two belts are placed in parallel on the same pulley, the elastic distribution on the circumference of each belt will be the first depending on the relative position of the two belts.
It will look like (a) and (b) in Figure 1 or Figure 12. In the case of Fig. 11, the elasticity of each belt is
When (a) and (b) are superimposed topologically, the composite elasticity of the two belts becomes as shown in (c), and the difference D between the maximum and minimum elasticity values becomes large. On the other hand, in the case of Figure 12, the elasticity distributions (a) and (b) cancel each other out topologically, so the composite elasticity is as shown in (c), and the difference D between the maximum and minimum elasticity values becomes small. , averaged over the entire length. On the other hand, as is well known, the belt moves while slipping locally between it and the pulley due to creep that occurs during operation.In this case, the amount of slip varies depending on the individual belt, so in actual operation The relative position of each belt in the circumferential direction changes with time, and the states shown in FIGS. 11 and 12 occur alternately and repeatedly. As a result, torsional vibration whose amplitude changes with time occurs on the driven pulley shaft as shown in FIG. 13. Furthermore, as the number of belts used increases, more and more complex and irregular torsional vibrations occur, and the resulting vibration noise becomes a whirring noise, which gives a sense of anxiety to machine maintenance personnel.

【発明の目的】[Purpose of the invention]

この発明は上記の点にかんがみなされたもので
あり、多連ベルトにおいて上述のようにベルトの
製法上避け得ない各ベルト固有の不均一な引張り
弾性分布が原因となつて発生する励振力を巧みに
抑制できるようにした多連結合形伝動ベルトを提
供することを目的とする。
This invention has been developed in view of the above points, and is a method to skillfully reduce the excitation force generated in multiple belts due to the uneven tensile elasticity distribution unique to each belt, which is unavoidable due to the belt manufacturing method as described above. It is an object of the present invention to provide a multi-coupled power transmission belt that can suppress the above.

【発明の要点】[Key points of the invention]

上記目的を達成するために、この発明は第1図
ないし第3図で述べた手法により、個々のベルト
についてその全長に亙る引張り弾性分布を実測に
より求め、この弾性分布を基に多連ベルトを構成
する各ベルトにおける弾性の大きな領域と小さな
領域の位置をベルト相互間で相殺するように周方
向へ偏位させることによつて、多連ベルト全体で
の合成弾性分布を全長に亙つてほぼ均等化させる
ように各ベルト相互の相対位置を設定し、かつこ
の相対位置を保持したまま連結手段を介して各ベ
ルトを相互一体に結合するようにし、運転時に発
生する軸の捩り振動、および2次的に生じる振動
騒音を低減させるようにしたものである。
In order to achieve the above object, the present invention measures the tensile elasticity distribution over the entire length of each belt using the method described in FIGS. By deviating the positions of the large and small elastic regions of each belt in the circumferential direction so as to cancel each other out, the composite elastic distribution of the entire multi-belt can be made almost uniform over the entire length. The relative positions of the respective belts are set so that the belts are aligned with each other, and the belts are integrally connected to each other through the connecting means while maintaining this relative position, thereby reducing torsional vibration of the shaft that occurs during operation, and secondary vibrations. This is designed to reduce the vibration noise generated by the engine.

【発明の実施例】[Embodiments of the invention]

以下図示実施例に基づき、この発明の構成並び
に組立手順について述べる。 この発明による多連結合形伝動ベルトを組立る
には、まず多連ベルトを構成する各ベルトについ
て、個々にその全長に亙る引張り弾性分布を実測
して求める。この手法の原理については先に第1
図ないし第3図で述べたが、実際には一例として
第14図に示すようなストロボスコープ方式の測
定装置で実測される。図において9は駆動モー
タ、10は被動負荷としてのフライホイール、1
1は回転速度またはトルクを検出するピツクアツ
プ、12は測定器、13はその指示計、14はス
トロボである。プーリ1と2の間にはあらかじめ
その弾性分布がわかつている基準ベルト15が架
け渡してあり、そのベルト上には所定の位置にス
トロボ基準マーク15aが付してある。ここで被
検査ベルト3の周上の複数箇所にチヨーク等でマ
ーク3aを付けておき、1本ずつ基準ベルト15
と並べてプーリ1,2に架け渡し、モータ9を運
転する。この場合に、基準ベルト15と被検査ベ
ルト3の弾性分布が第11図のように位相的に一
致しているときは、ベルトの公転周波数の周期で
変化する速度変動あるいはトルク変動が大きく指
示計13に現れる。逆に弾性分布が第12図のよ
うに位相的に相殺するようにずれているときは、
指示計13の指示は最小になる。この際にストロ
ボスコープの光源をベルトの公転速度に同期させ
て明滅させ、ベルト15の基準マーク15aと被
検査ベルト3のマーク3aの相対位置を検出する
ことにより、基準ベルト15の弾性分布を基準に
これと対比して被検査ベルト3の弾性分布が求め
られる。また、ここで後記のベルト組立作業のた
めに弾性の最大、最小箇所の位置を表す指示マー
クをベルト上に標記しておく。なお上記のストロ
ボスコープ方式の他に、ロータリーエンコーダ方
式によつて被検査ベルトの引張り弾性分布を求め
る方法もある。 次に上記測定法によつてその弾性分布を求めた
個々のベルトを用いて多連結合形伝動ベルトを組
立構成する手順について述べる。まず所定本数の
ベルトを並べ、各ベルトごとに前記工程で標記さ
れた弾性の大きい領域と小さい領域を表す指示マ
ークを頼りに、各領域が多連ベルト相互間で位相
的に一致しないように周方向に偏位させ、多連ベ
ルトとして各ベルトの合成弾性分布がベルトの全
周に亙つてほぼ均等となるようにベルト相互間の
相対位置を決める。この場合に多連ベルトが2本
のベルトで構成される場合には、第15図のよう
に各ベルト固有の弾性分布との相互間で弾性
最大箇所と最小箇所とが位相的に一致して並ぶよ
うにベルト相互の相対位置を決める。これにより
2本のベルトの合成弾性分布はTで示すように全
長Lに亙つて均一となる。同様に多連ベルトが3
本ベルトからなる場合には、第16図のごとく各
ベルトについて固有の弾性分布、、の合成
分布Tがベルト全長Lに亙つて均一となるように
ベルトを並べ替えてベルト相互の相対位置を設定
する。すなわち前記手法によるベルト相互の相対
位置は丁度ベクトル合成の作図法と同様にして決
められる。したがつて3本のベルトの個々の弾性
分布およびその弾性値がまちまちであつても、上
記した方法で適正な相対位置決めを行うことによ
り、多連ベルトとしての合成弾性分布を全長域に
亙つてほぼ均一化できることになる。 上記のようにして全長に亙る弾性分布が均一に
なるように多連ベルトの各ベルト相対位置が決ま
つたところで、次にこの相対位置を保持したま
ま、連結手段を介して多連ベルトを構成する各ベ
ルトの相互間を機械的に一体結合し、これにより
多連結合形伝動ベルトが組立構成されることにな
る。 次に複数本のベルトをベルト相互の相対位置を
保持したまま一体結合する連結手段のいくつかの
実施例を第17図ないし第20図に示す。各図に
おいて3〜3は先記した弾性分布の均等化工
程を経て周方向の相対位置が決められた多連ベル
トを構成する3本のベルトである。かかるベルト
3〜3の相対位置を保持して各ベルトの相互
を一体結合するために、第17図の実施例では、
連結手段としてベルト3〜3にまたがり、そ
の全長に亙つて背面側に幅の広いバツクバンド1
6を貼着し、このバツクバンド16を介して3本
のベルトを一体結合している。なおこのバツクバ
ンド16は未加硫のものを各ベルトに重ねて加硫
し、一体化することも可能である。 第18図の実施例は、連結手段としてあらかじ
め各ベルト3〜3の背面に長手方向に沿つて
突出する歯列17を形成しておき、ベルト間の相
対位置を決めた状態で歯列付きの幅の広いバツク
バンド18を各ベルト3〜3の歯列17にま
たがつて係合被着し、これによりベルト3〜3
を相互一体に結合したものである。この実施例
ではベルトを1本単位で交換ないしは組替えるこ
とができ、先述のようにあらかじめ弾性分布測定
結果を基にベルトの周上に最大の弾性箇所と最小
の弾性箇所を表す指示マークを施しておくことに
より、このマークを頼りに使用先で多連結合形伝
動ベルトの組立あるいは交換を実施することも可
能である。 第19図の実施例は、連結手段としてあらかじ
め個々のベルト3〜3にそれぞれ左右両側に
突出する歯列17を形成しておき、ベルト間の相
対位置を設定した上で歯列17同士を噛み合わせ
て一体結合したものであり、この実施例でも第1
8図の実施例と同様に使用先で多連結合形伝動ベ
ルトの組立、あるいは交換が行える。 第20図の実施例は、各ベルト3〜3の背
面に長手方向に沿つて多数のねじ穴19をあけて
おき、ベルト相互の相対位置決めがなされた後に
各ベルト3〜3にまたがり、周上の複数箇所
に連結片20をねじ止め締結して一体結合したも
のである。 以上の各実施例のように、複数本のベルトを組
合わせた多連ベルトの弾性分布の均等化操作を行
つた後に、ベルト相互間の相対位置を保持したま
ま各ベルトの相互を連結手段で一体結合したこと
により、運転使用中に各ベルト3〜3がプー
リとの間で別々にスリツプすることがなく、した
がつて常に多連ベルトとして合成弾性の均等分布
状態が維持されることになる。
The configuration and assembly procedure of the present invention will be described below based on the illustrated embodiments. To assemble the multi-coupled power transmission belt according to the present invention, first, the tensile elasticity distribution over the entire length of each belt constituting the multi-coupled belt is actually measured and determined. The principle of this method will be explained in the first part.
Although described with reference to FIGS. 3 to 3, actual measurement is actually performed using a stroboscope-type measuring device as shown in FIG. 14 as an example. In the figure, 9 is a drive motor, 10 is a flywheel as a driven load, 1
1 is a pickup for detecting rotational speed or torque, 12 is a measuring device, 13 is an indicator thereof, and 14 is a strobe. A reference belt 15 whose elastic distribution is known in advance is stretched between pulleys 1 and 2, and strobe reference marks 15a are attached at predetermined positions on the belt. Here, marks 3a are attached to multiple locations on the circumference of the belt to be inspected 3 using a chiyoke or the like, and one by one the reference belt 15 is
The motor 9 is operated by connecting the pulleys 1 and 2 side by side. In this case, when the elastic distributions of the reference belt 15 and the belt to be inspected 3 match in phase as shown in FIG. Appears on the 13th. On the other hand, when the elastic distribution shifts so as to offset each other topologically as shown in Figure 12,
The indicator 13 indicates the minimum value. At this time, the light source of the stroboscope is made to flicker in synchronization with the revolution speed of the belt, and the relative position of the reference mark 15a of the belt 15 and the mark 3a of the belt to be inspected 3 is detected, thereby making the elastic distribution of the reference belt 15 a reference. In contrast to this, the elasticity distribution of the belt 3 to be inspected is determined. In addition, for the purpose of belt assembly work to be described later, indication marks indicating the positions of the maximum and minimum elasticity points are marked on the belt. In addition to the stroboscope method described above, there is also a method of determining the tensile elasticity distribution of the belt to be inspected using a rotary encoder method. Next, a procedure for assembling a multiple coupled power transmission belt using individual belts whose elastic distributions have been determined by the above measurement method will be described. First, a predetermined number of belts are lined up, and, relying on the indication marks indicating the areas of high elasticity and areas of low elasticity marked in the above process for each belt, the circumference is adjusted so that each area does not match topologically among the multiple belts. The relative positions of the belts are determined so that the composite elasticity distribution of each belt is substantially uniform over the entire circumference of the belt as a multiple belt. In this case, when the multi-belt is composed of two belts, the maximum elasticity point and the minimum elasticity point match topologically with respect to the elasticity distribution unique to each belt, as shown in Fig. 15. Determine the relative positions of the belts so that they line up. As a result, the composite elasticity distribution of the two belts becomes uniform over the entire length L as shown by T. Similarly, the multiple belt is 3
In the case of this belt, as shown in Fig. 16, the belts are rearranged and the relative positions of the belts are set so that the composite distribution T of the unique elasticity distribution of each belt is uniform over the entire length L of the belt. do. That is, the relative positions of the belts using the method described above are determined in the same way as the drawing method of vector composition. Therefore, even if the individual elasticity distributions and elasticity values of the three belts vary, by performing appropriate relative positioning using the method described above, the composite elasticity distribution as a multi-belt can be maintained over the entire length range. This means that it can be made almost uniform. Once the relative position of each belt in the multiple belt is determined as described above so that the elasticity distribution over the entire length is uniform, next, while maintaining this relative position, the multiple belt is configured via the connecting means. The belts connected to each other are mechanically and integrally connected to each other, thereby assembling a multiple-coupled power transmission belt. Next, several embodiments of connecting means for integrally connecting a plurality of belts while maintaining their relative positions are shown in FIGS. 17 to 20. In each figure, numerals 3 to 3 indicate three belts constituting a multiple belt whose relative positions in the circumferential direction have been determined through the process of equalizing the elasticity distribution described above. In order to maintain the relative positions of the belts 3 to 3 and integrally connect each belt to each other, in the embodiment shown in FIG.
A wide back band 1 on the back side spanning the entire length of the belts 3 to 3 as a connecting means.
6 is attached, and the three belts are integrally connected via this back band 16. Incidentally, this back band 16 can also be made of an unvulcanized material and stacked on each belt and vulcanized to integrate them. In the embodiment shown in FIG. 18, a row of teeth 17 is formed in advance on the back surface of each belt 3 to 3 to protrude along the longitudinal direction as a connecting means, and with the relative positions between the belts determined, A wide back band 18 is fitted over the tooth rows 17 of each belt 3-3, and thereby the belts 3-3
It is a combination of two parts that are integrally connected to each other. In this embodiment, the belt can be replaced or rearranged one by one, and as mentioned earlier, indication marks are placed on the circumference of the belt to indicate the maximum elasticity points and the minimum elasticity points based on the elasticity distribution measurement results. By keeping these marks in mind, it is also possible to assemble or replace the multi-coupled power transmission belt at the site of use, relying on this mark. In the embodiment shown in FIG. 19, rows of teeth 17 protruding from both sides of the belts 3 to 3 are formed in advance on each of the belts 3 to 3 as a connecting means, and the rows of teeth 17 are engaged with each other after setting the relative positions between the belts. In this example, the first
As in the embodiment shown in FIG. 8, the multiple coupling type transmission belt can be assembled or replaced at the site of use. In the embodiment shown in FIG. 20, a large number of screw holes 19 are drilled along the longitudinal direction on the back surface of each belt 3 to 3, and after the belts are positioned relative to each other, the belts straddle each belt 3 to The connecting pieces 20 are integrally connected by screwing and fastening the connecting pieces 20 at a plurality of locations. As in each of the above embodiments, after performing an operation to equalize the elasticity distribution of a multiple belt in which a plurality of belts are combined, each belt is connected to each other by a connecting means while maintaining the relative position between the belts. By being integrally connected, each belt 3 to 3 will not slip separately between the pulleys during operation, and therefore, an even distribution of composite elasticity will always be maintained as a multiple belt. .

【発明の効果】【Effect of the invention】

以上述べたようにこの発明は、多連ベルトを構
成する複数本の各ベルトについて、その全長に亙
る引張り弾性分布を実測し、これを基に多連ベル
トを組立構成する際には各ベルトの弾性の大きな
領域と小さな領域とを相対的に周方向へ偏位させ
ることにより、多連ベルトとしての合成引張り弾
性分布が全長に亙つてほぼ均等化されるように位
置決め設定し、かつこの相対位置を保持したまま
連結手段により各ベルトを相互一体に結合して多
連結合形伝動ベルトを組立構成したものであり、
したがつてベルトの製法上避け得ない各ベルト固
有の不均一な引張り弾性を互いに補償し合つて引
張り弾性分布の均等な多連結合形伝動ベルトを得
ることができ、これによりベルトの不均等な弾性
分布が原因となつてベルト伝動系に生じる捩り振
動および2次的に派生する振動騒音を良好に抑制
できる優れた効果が得られる。
As described above, the present invention measures the tensile elasticity distribution over the entire length of each of the plurality of belts constituting the multiple belt, and based on this, when assembling and configuring the multiple belt, each belt is By relatively displacing the large elasticity region and the small elasticity region in the circumferential direction, positioning is performed so that the synthetic tensile elasticity distribution as a multiple belt is approximately equalized over the entire length, and this relative position Each belt is integrally connected to each other by a connecting means while maintaining the same, thereby assembling a multiple-coupled transmission belt,
Therefore, by mutually compensating for the uneven tensile elasticity inherent to each belt, which is unavoidable due to the belt manufacturing method, it is possible to obtain a multi-coupled power transmission belt with an even tensile elasticity distribution. An excellent effect can be obtained in that torsional vibrations occurring in the belt transmission system due to elastic distribution and secondary vibration noise can be suppressed.

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

第1図はベルト伝動機構の原理構成図、第2図
はベルトの展開図、第3図は第2図のベルトにお
ける引張り弾性分布図、第4図ないし第6図は芯
線コード入Vベルトを製造工程順に示したコード
巻装状態図、中間完成品の部分断面図、および完
成ベルトの斜視断面図、第7図ないし第9図はそ
れぞれ運転時に生じるベルトの伸びの変化を表す
説明図、第10図は1本ベルトによる運転時に被
動軸へ加わる捩り振動の波形図、第11図および
第12図はそれぞれ2連ベルトの異なるベルト相
対位置における引張り弾性分布図、第13図は2
連ベルトによる運転時に被動軸に加わる捩り振動
の波形図、第14図はストロボスコープ方式の引
張り弾性分布測定装置の構成図、第15図および
第16図はそれぞれ2連ベルトおよび3連ベルト
を対象としたこの発明によるベルト間の相対位置
決め手順を示す説明図、第17図ないし第20図
はそれぞれこの発明によるベルト相互の連絡手段
の構成を示す異なる実施例の斜視断面図である。 1,2……プーリ、3,3〜3……ベル
ト、7……芯線コード、16……バツクバンド、
17……歯列、18……歯付きバツクバンド、2
0……連結片。
Fig. 1 is a diagram of the principle configuration of the belt transmission mechanism, Fig. 2 is a developed view of the belt, Fig. 3 is a tensile elasticity distribution diagram of the belt in Fig. 2, and Figs. 4 to 6 are V-belts with core cords. A cord winding state diagram, a partial sectional view of an intermediate finished product, and a perspective sectional view of a completed belt are shown in the order of the manufacturing process. Figure 10 is a waveform diagram of torsional vibration applied to the driven shaft during operation with a single belt, Figures 11 and 12 are tensile elasticity distribution diagrams at different belt relative positions of a double belt, respectively, and Figure 13 is a waveform diagram of torsional vibration applied to the driven shaft during operation with a single belt.
A waveform diagram of torsional vibration applied to the driven shaft during operation with a continuous belt, Fig. 14 is a configuration diagram of a stroboscope-type tensile elasticity distribution measurement device, and Figs. 15 and 16 are for a double belt and a triple belt, respectively. FIGS. 17 to 20 are perspective sectional views of different embodiments showing the structure of communication means between belts according to the present invention. 1, 2... Pulley, 3, 3~3... Belt, 7... Core wire cord, 16... Back band,
17...Tooth row, 18...Toothed back band, 2
0...Connection piece.

Claims (1)

【特許請求の範囲】 1 複数本のベルトを並列して相互一体に結合し
てなる多連結合形伝動ベルトであつて、個々のベ
ルトについて実測により求めたベルトの全長に亙
る引張り弾性分布を基に、各ベルトにおける引張
り弾性の大きな領域と小さな領域の位置をベルト
相互の間で相対的に周方向へ偏位させることによ
り、多連ベルトとしての合成引張り弾性分布が全
長に亘りほぼ均等になるように各ベルト相互間の
相対位置を定め、この相対位置を保持したまま連
結手段を介して各ベルトを相互一体に結合したこ
とを特徴とする多連結合形伝動ベルト。 2 特許請求の範囲第1項記載のベルトにおい
て、各ベルトが芯線コード入りベルトであること
を特徴とする多連結合形伝動ベルト。 3 特許請求の範囲第1項記載のベルトにおい
て、各ベルトの周上には引張り弾性分布の実測で
求めた引張り弾性の最大箇所と最小箇所を表す指
示マークが標記されていることを特徴とする多連
結合形伝動ベルト。 4 特許請求の範囲第1項記載のベルトにおい
て、連結手段として各ベルトの背面にまたがつて
全周に幅広のバツクバンドを貼着し、このバツク
バンドを介して各ベルトを相互一体に結合したこ
とを特徴とする多連結合形伝動ベルト。 5 特許請求の範囲第1項記載のベルトにおい
て、連結手段として各ベルトに背面に突出する歯
列を形成するとともに、これら各ベルトの全周に
またがつて歯列付きのバツクバンドを係合被着
し、このバツクバンドを介して各ベルトを相互一
体に結合したことを特徴とする多連結合形伝動ベ
ルト。 6 特許請求の範囲第1項記載のベルトにおい
て、連結手段として各ベルトの両側面に突出する
歯列を形成し、該歯列と歯列を噛み合わせて各ベ
ルトを相互一体に結合したことを特徴とする多連
結合形伝動ベルト。 7 特許請求の範囲第1項記載のベルトにおい
て、ベルト上の複数箇所で各ベルトの相互にまた
がつて連結片を固定し、この連結片を介して各ベ
ルトを相互一体に結合したことを特徴とする多連
結合形伝動ベルト。
[Scope of Claims] 1. A multi-coupled power transmission belt formed by connecting a plurality of belts in parallel and integrally with each other, which is based on the tensile elasticity distribution over the entire length of the belt determined by actual measurements for each belt. In addition, by shifting the positions of the regions of large and small tensile elasticity in each belt relative to each other in the circumferential direction, the synthetic tensile elasticity distribution as a multiple belt becomes almost uniform over the entire length. 1. A multi-coupled power transmission belt characterized in that the relative positions of the belts are determined as such, and the belts are integrally connected to each other via a connecting means while maintaining this relative position. 2. The belt according to claim 1, wherein each belt is a core cord-containing belt. 3. The belt according to claim 1, characterized in that each belt is marked with indicator marks on its circumference indicating the maximum and minimum points of tensile elasticity determined by actual measurement of the tensile elasticity distribution. Multiple connection type power transmission belt. 4. In the belt according to claim 1, a wide back band is attached all around the back side of each belt as a connecting means, and each belt is integrally connected to each other via this back band. A multi-coupled power transmission belt with special features. 5. In the belt according to claim 1, each belt is provided with a row of teeth protruding from the back side as a connecting means, and a back band with a row of teeth is fitted over the entire circumference of each belt. A multi-coupled power transmission belt characterized in that each belt is integrally coupled to each other via this back band. 6. In the belt according to claim 1, a row of teeth protruding from both sides of each belt is formed as a connecting means, and the rows of teeth are engaged with each other to integrally connect each belt. A multi-coupled power transmission belt with special features. 7. The belt according to claim 1, characterized in that connecting pieces are fixed across the belts at a plurality of locations on the belt, and the belts are integrally connected to each other via the connecting pieces. Multi-coupled power transmission belt.
JP21208983A 1983-11-11 1983-11-11 Multiple coupling type driving belt Granted JPS60104832A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP21208983A JPS60104832A (en) 1983-11-11 1983-11-11 Multiple coupling type driving belt

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP21208983A JPS60104832A (en) 1983-11-11 1983-11-11 Multiple coupling type driving belt

Publications (2)

Publication Number Publication Date
JPS60104832A JPS60104832A (en) 1985-06-10
JPS6260571B2 true JPS6260571B2 (en) 1987-12-17

Family

ID=16616689

Family Applications (1)

Application Number Title Priority Date Filing Date
JP21208983A Granted JPS60104832A (en) 1983-11-11 1983-11-11 Multiple coupling type driving belt

Country Status (1)

Country Link
JP (1) JPS60104832A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0353479U (en) * 1989-09-26 1991-05-23

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
KR100625072B1 (en) * 2002-01-29 2006-09-19 가부시키가이샤 제이텍트 Electric power steering system

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0353479U (en) * 1989-09-26 1991-05-23

Also Published As

Publication number Publication date
JPS60104832A (en) 1985-06-10

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