JPS6345949B2 - - Google Patents
Info
- Publication number
- JPS6345949B2 JPS6345949B2 JP56052775A JP5277581A JPS6345949B2 JP S6345949 B2 JPS6345949 B2 JP S6345949B2 JP 56052775 A JP56052775 A JP 56052775A JP 5277581 A JP5277581 A JP 5277581A JP S6345949 B2 JPS6345949 B2 JP S6345949B2
- Authority
- JP
- Japan
- Prior art keywords
- tire
- circumference
- internal pressure
- layer
- crown
- 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
Links
Classifications
-
- B—PERFORMING OPERATIONS; TRANSPORTING
- B29—WORKING OF PLASTICS; WORKING OF SUBSTANCES IN A PLASTIC STATE IN GENERAL
- B29D—PRODUCING PARTICULAR ARTICLES FROM PLASTICS OR FROM SUBSTANCES IN A PLASTIC STATE
- B29D30/00—Producing pneumatic or solid tyres or parts thereof
- B29D30/06—Pneumatic tyres or parts thereof (e.g. produced by casting, moulding, compression moulding, injection moulding, centrifugal casting)
- B29D30/36—Expansion of tyres in a flat form, i.e. expansion to a toroidal shape independently of their building-up process, e.g. of tyres built by the flat-tyres method or by jointly covering two bead-rings
Landscapes
- Engineering & Computer Science (AREA)
- Mechanical Engineering (AREA)
- Tyre Moulding (AREA)
Description
(産業上の利用分野)
本発明はラジアルタイヤを成形する際、生タイ
ヤのクラウン部の周方向長さを測定し、これを規
定範囲内に制御することにより仕上りタイヤの均
一性を向上するラジアルタイヤの成形方法に関す
る。
(従来の技術及び発明が解決しようとする課題)
ラジアルタイヤの構造はカーカス層上に配置さ
れるブレーカー層のコードが円周方向に近い角度
で配置されている為、その製法は必然的に円筒状
フオーマー上でビード部、カーカス層及び側壁ゴ
ムを張付け成形し、これを膨径してトロイド状に
変形し、そのクラウン部上にブレーカー層とトレ
ツド層を貼設、成形する2段階法によつている。
かかる成形方法においてはカーカス層をトロイド
状に変形する際、カーカスコードに部分的に応力
集中を生ずる場合があり必ずしも均一な膨径が得
られず種々の異なつた外周のタイヤとなる。即ち
トロイド状カーカスの外周を決定するおもな要因
はフオーマー上に配置されるビードワイヤーの間
隔、膨径圧力及び膨径時間があるがこれらを適宜
調整しても特定サイズのものすべて同一の外周に
することは極めて困難である。したがつてこのよ
うに外周の異なつたタイヤに予め一定長さに切断
されたトレツド層を貼設した場合、仕上がりタイ
ヤのクラウン部外面に凹凸が生じ、その結果ラジ
アルフオースバリエーシヨンあるいはラテラルフ
オースバリエーシヨン等の特性を著しく低下させ
る。かかる問題を解決する為、成形タイヤの外周
に応じて各々トレツドの長さを切断する方法があ
るが、この方法では作業能率を低下させるほか、
作業者の目視によつて長さを調整する為成形精度
をあげる為には作業者の熟練を要し、更にその精
度にもおのずと限度がある。本発明はかかる問題
点を解決するもので作業を能率よくかつ精度よく
均一なタイヤを成形するラジアルタイヤの成形方
法を提供することを目的とする。
(課題を解決するための手段)
本発明はカーカス層をその他の構成部材ととも
に成形ドラム上に配置し、これをトロイド状に変
形し、そのクラウン部にブレーカー層又はトレツ
ド層を貼設して生タイヤを形成するラジアルタイ
ヤの成形方法において
(イ) ブレーカー層を貼設する前にタイヤクラウン
部の周長を測定するステツプ及び
(ロ) その周長が規定範囲を外れている場合、その
周長を膨張圧等で規定範囲内に制御するステツ
プ、
とを含むラジアルタイヤの成形方法である。
(実施例)
以下本発明の一実施例を図面にしたがつて説明
する。
第1図は本発明の成形方法のシステムを示す概
略図である。図において生タイヤ1はカーカス層
2をビードワイヤ3及びサイドウオール4ととも
に成形ドラム5上で組合せるとともにこれをトロ
イド状に変形させる。しかる後このトロイド状カ
ーカスの膨径が均一になつているかどうかを検査
する為、生タイヤ1の1周の長さを測定する。生
タイヤ1の外表面の1周分の長さ(L)は下記の式で
算出できる。
L=∫2〓0γ(θ)dθ
ここでγは生タイヤの外表面までの半径で、こ
れは回転角度でラジアンで表わされる。ここで数
値積分を行なう為に微小回転角△θをとると数値
積分は
N△θ=2π、L=N
〓i=1
、γi△θ
で求められる。ここでNは数値積分の為の分割
数、Lは一周分の長さである。又γiはi番目の地
点のタイヤ半径である。ここでγiの求め方は次の
通りである。即ち第1図において生タイヤのクラ
ウン部近傍に変位計7を設置し、該変位計から生
タイヤ外表面までの距離dを測定する。γiはタイ
ヤ回転軸から変位計までの距離Rから前記距離d
を差し引いた値として求められる。尚本発明にお
いて使用される変位計として第3図に示される如
く可動部10に付設された検出ローラ11をタイ
ヤ外週面の回転に追従させてその半径変動を測定
する差動トランス、第4図に示される如くレーザ
ー発振器12からレーザー光を被測定物体13に
照射し、その反射光をイメージセンサー14で検
知する変位計あるいは第5図に示される如く被測
定物体13の側面からレーザーを平行光線にして
照射し、反射側に配置したイメージカメラでこれ
を検知し該被測定物体13の上端の高さ変化を測
定する変位計等を用いることができ、更に接触
型、非接触型いずれでもよい。
これらの変位計により生タイヤ外表面までの距
離dは第6図に示される如くタイヤ1周分の波形
信号として得られる。図において横軸はタイヤ回
転角を縦軸は生タイヤ外表面までの距離dを示
し、Pはタイヤ凹部にTはタイヤ凸部に相当し、
Aは波形の振幅を示す。この波形信号は次にA/
D変換器15に入力され、ここでタイヤ1周のそ
れぞれのタイヤ半径γiがデジタル値に変換されこ
れが計算機16に入力されここで前述の数値積分
によつてタイヤの周長が計算される。以下この計
算値が規定範囲をはずれる場合、電磁弁コントロ
ーラ17により内圧充填用電磁弁18及び内圧放
出用電磁弁19を制御することにより前記生タイ
ヤの内圧を調整し、該生タイヤの周長を規定範囲
内に設定する。この制御方法をフローチヤートと
して第7図に示す。図においてまず生タイヤを膨
径後内圧を所定値に保持し、前記の方法で該生タ
イヤ1周分の周長を測定する。この測定値が規定
上限値より小さく、かつ規定下限値よりも大きい
場合、即ち所定の数値範囲内の場合は修正の必要
なく次のブレーカー層の貼設工程に移す。次に前
記生タイヤの周長の測定値が規定上限値より大き
い場合、その差に応じて生タイヤの内圧をどの程
度減少すべきかを計算し、電磁弁19を断続的に
操作して設定内圧まで減少させる。しかる後生タ
イヤの周長を再度測定する。次に生タイヤの周長
の測定値が規定下限値より小さい場合、その差に
応じて生タイヤの内圧をどの程度増加すべきかを
計算し、電磁弁18を断続的に操作して内圧充填
し設定内圧まで上昇させる。しかる後生タイヤの
周長を再度測定する。このように生タイヤの周長
が所定の範囲内になるまで内圧の調整を繰り返
す。尚この内圧調整は圧力センサー20でモニタ
ーする。
このようにして得られた生タイヤは常に一定範
囲内の周長を有している為、次の工程でブレーカ
ー層、あるいはトレツド層を貼設する場合におい
ても両端部の接合部分がほぼ一定となり高い精度
の成形が可能となり仕上がりタイヤの均一性は向
上する。尚本発明の如く直接生タイヤの周長を測
定する方法の他、光電管方式等でタイヤ半径を測
定する方法、あるいはこれを周長に換算する方法
等があるが、タイヤの半径が周方向に変化してい
る為、精度の高い成形をすることが困難である。
尚本発明ではタイヤの周長を調整するために前
述の如くタイヤ内圧を制御する他、トロイド状に
変形する際ビードの間隔(第1図におけるW)を
調整することも可能である。
以下にタイヤサイズが10.00R20−14PRのスチ
ールラジアルタイヤを各々10本ずつ下記の方法で
成形し仕上がりタイヤのクラウン部中央の周方向
振れを測定した結果を示す。振れ測定はタイヤを
サイズ7.00T×20のリムに装着し、内圧7.25Kg
f/cm2にして差動トランスを用いて測定した。そ
の結果を第1表に示す。
本発明の実施例1は第1図に示す機構を備えた
成形機を用いてトロイド状カーカス層上にブレー
カー層を貼設した後でタイヤ赤道線上の振れ波形
を測定した。数値積分の分割数(N)は60とし規
定上限値及び規定下限値の範囲は1mmである。周
長を内圧調整によつて制御した後、トレツドを貼
設し、通常の加硫工程及び仕上げ工程により製造
した。
一方比較例1は周長を制御する点を除いては実
施例と同じ方法で製造した。
(Industrial Application Field) The present invention is a radial tire that improves the uniformity of finished tires by measuring the circumferential length of the crown portion of a raw tire and controlling it within a specified range when molding a radial tire. It relates to a tire molding method. (Prior art and problems to be solved by the invention) Since the structure of a radial tire is such that the cords of the breaker layer arranged on the carcass layer are arranged at an angle close to the circumferential direction, the manufacturing method is inevitably cylindrical. A two-step method is used in which the bead part, carcass layer, and sidewall rubber are stretched and molded on a shaped former, the diameter of which is expanded to transform it into a toroid shape, and the breaker layer and tread layer are pasted and molded on the crown part. It's on.
In such a forming method, when the carcass layer is deformed into a toroidal shape, stress concentration may occur locally in the carcass cord, and a uniform expansion diameter cannot necessarily be obtained, resulting in tires with various outer circumferences. In other words, the main factors that determine the outer circumference of a toroidal carcass are the spacing between the bead wires placed on the former, the inflation pressure, and the inflation time, but even if these are adjusted appropriately, all of a specific size will have the same outer circumference. It is extremely difficult to do so. Therefore, when a tread layer cut to a certain length is applied to tires with different circumferences, unevenness will occur on the outer surface of the crown of the finished tire, resulting in radial force variation or lateral force variation. Characteristics such as variation are significantly reduced. In order to solve this problem, there is a method of cutting the length of each tread according to the outer circumference of the molded tire, but this method not only reduces work efficiency, but also
Since the length is adjusted by visual inspection by the operator, the operator must be skilled in order to improve the molding accuracy, and furthermore, there is a natural limit to that accuracy. SUMMARY OF THE INVENTION It is an object of the present invention to provide a radial tire molding method that solves these problems and can efficiently mold a uniform tire with high precision. (Means for Solving the Problems) The present invention places a carcass layer together with other constituent members on a forming drum, deforms it into a toroid shape, and attaches a breaker layer or a tread layer to the crown portion of the toroid. In the method of forming a radial tire to form a tire, (a) the step of measuring the circumference of the tire crown before pasting the breaker layer; and (b) the step of measuring the circumference of the tire crown if the circumference is outside the specified range. This is a radial tire molding method that includes the steps of: controlling the pressure within a specified range using inflation pressure, etc. (Example) An example of the present invention will be described below with reference to the drawings. FIG. 1 is a schematic diagram showing a system for the molding method of the present invention. In the figure, a green tire 1 has a carcass layer 2 assembled together with bead wires 3 and sidewalls 4 on a forming drum 5, and is deformed into a toroidal shape. Thereafter, the length of one circumference of the green tire 1 is measured to check whether the expansion diameter of this toroidal carcass is uniform. The length (L) of one circumference of the outer surface of the raw tire 1 can be calculated using the following formula. L=∫ 2 〓 0 γ(θ)dθ Here, γ is the radius to the outer surface of the green tire, which is the rotation angle expressed in radians. Here, if a minute rotation angle △θ is taken to perform numerical integration, the numerical integration can be obtained by N△θ=2π, L= N 〓 i=1 , γi△θ. Here, N is the number of divisions for numerical integration, and L is the length of one round. Also, γi is the tire radius at the i-th point. Here, the method for finding γi is as follows. That is, in FIG. 1, a displacement meter 7 is installed near the crown of the green tire, and the distance d from the displacement meter to the outer surface of the green tire is measured. γi is the distance d from the distance R from the tire rotation axis to the displacement meter.
It is calculated as the value obtained by subtracting the As shown in FIG. 3, the displacement meter used in the present invention includes a fourth differential transformer that causes a detection roller 11 attached to a movable part 10 to follow the rotation of the tire outer surface and measure the radial variation thereof. As shown in the figure, a displacement meter that irradiates a laser beam from a laser oscillator 12 onto an object to be measured 13 and detects the reflected light with an image sensor 14, or as shown in FIG. It is possible to use a displacement meter or the like that emits a light beam, detects it with an image camera placed on the reflection side, and measures the change in height of the upper end of the object to be measured 13, and can also be of either a contact type or a non-contact type. good. Using these displacement meters, the distance d to the outer surface of the raw tire is obtained as a waveform signal for one revolution of the tire, as shown in FIG. In the figure, the horizontal axis shows the tire rotation angle, the vertical axis shows the distance d to the outer surface of the raw tire, P corresponds to the tire concave part, T corresponds to the tire convex part,
A indicates the amplitude of the waveform. This waveform signal is then A/
The data is input to the D converter 15, where each tire radius γi of one tire circumference is converted into a digital value, and this is input to the computer 16, where the circumference of the tire is calculated by the numerical integration described above. If this calculated value is outside the specified range, the internal pressure of the raw tire is adjusted by controlling the internal pressure filling solenoid valve 18 and the internal pressure release solenoid valve 19 by the solenoid valve controller 17, and the circumference of the raw tire is adjusted. Set within the specified range. This control method is shown in FIG. 7 as a flowchart. In the figure, first, after the diameter of a green tire is inflated, the internal pressure is maintained at a predetermined value, and the circumferential length of one round of the green tire is measured using the method described above. If this measured value is smaller than the specified upper limit and larger than the specified lower limit, that is, within the specified numerical range, the process moves to the next breaker layer pasting process without the need for correction. Next, if the measured value of the circumference of the raw tire is larger than the specified upper limit, the amount to reduce the internal pressure of the raw tire is calculated according to the difference, and the solenoid valve 19 is intermittently operated to set the internal pressure. decrease to. After that, the circumference of the raw tire is measured again. Next, if the measured value of the circumference of the raw tire is smaller than the specified lower limit, calculate how much the internal pressure of the raw tire should be increased according to the difference, and intermittently operate the solenoid valve 18 to fill the internal pressure. Raise to the set internal pressure. After that, the circumference of the raw tire is measured again. Adjustment of the internal pressure is repeated in this manner until the circumference of the raw tire falls within a predetermined range. Note that this internal pressure adjustment is monitored by a pressure sensor 20. Since the green tire obtained in this way always has a circumference within a certain range, even when a breaker layer or tread layer is attached in the next step, the joints at both ends will be almost constant. High precision molding becomes possible and the uniformity of the finished tire improves. In addition to the method of directly measuring the circumference of a green tire as in the present invention, there are methods of measuring the tire radius using a phototube method, or converting this into a circumference. Because of these changes, it is difficult to mold with high precision. In the present invention, in addition to controlling the tire internal pressure as described above in order to adjust the circumferential length of the tire, it is also possible to adjust the bead spacing (W in FIG. 1) when deforming into a toroidal shape. Below are the results of measuring the circumferential runout at the center of the crown of the finished tires formed by molding 10 steel radial tires with a tire size of 10.00R20-14PR using the method described below. Runout measurement was carried out with the tire mounted on a rim of size 7.00T x 20, with an internal pressure of 7.25Kg.
Measurements were made using a differential transformer at f/cm 2 . The results are shown in Table 1. In Example 1 of the present invention, a breaker layer was pasted on a toroidal carcass layer using a molding machine equipped with the mechanism shown in FIG. 1, and then the runout waveform on the tire equator was measured. The number of divisions (N) for numerical integration is 60, and the range of the specified upper limit value and specified lower limit value is 1 mm. After controlling the circumferential length by adjusting the internal pressure, a tread was attached, and the product was manufactured through normal vulcanization and finishing steps. On the other hand, Comparative Example 1 was manufactured in the same manner as in the example except that the circumferential length was controlled.
【表】【table】
【表】
表から明らかな如く本発明の実施例1は振幅の
平均値及び標準偏差の値が小さく均一性がかなり
向上していることが明らかである。
(効果)
本発明は上述の通り、ラジアルタイヤの成形工
程において、トロイダル状に膨径したカーカス層
のクラウン部の周長を実測し、実測値と予めの規
定値と比較し、規定範囲を外れている場合に、膨
張力等で規定範囲内に制御するようにしたから、
同一サイズタイヤのカーカス外周をすべて同一に
することができ、仕上りタイヤの均一性を大幅に
向上することが可能となつた。[Table] As is clear from the table, in Example 1 of the present invention, it is clear that the average value and standard deviation of the amplitude are small, and the uniformity is considerably improved. (Effects) As described above, the present invention measures the circumference of the crown portion of the carcass layer expanded in a toroidal shape during the radial tire molding process, compares the measured value with a predefined value, and detects deviations outside the specified range. In this case, it is controlled within the specified range using expansion force, etc.
This makes it possible to make all the carcass circumferences of tires of the same size the same, making it possible to greatly improve the uniformity of finished tires.
第1図は本発明の成形方法のシステムを示す概
略図、第2図は生タイヤの半径変化を示す概略
図、第3図〜第5図は変位計、第6図はタイヤの
振れ波形を示す図、第7図は本発明の成形方法の
フローチヤートを示す。
1……タイヤ、2……カーカス層、5……成形
ドラム、7……変位計、16……計算器、17…
…コントローラー、18,19……電磁弁、20
……内圧センサー。
Fig. 1 is a schematic diagram showing the system of the molding method of the present invention, Fig. 2 is a schematic diagram showing the radius change of a green tire, Figs. 3 to 5 are displacement meters, and Fig. 6 is a diagram showing the tire runout waveform. The figure shown in FIG. 7 shows a flowchart of the molding method of the present invention. DESCRIPTION OF SYMBOLS 1... Tire, 2... Carcass layer, 5... Forming drum, 7... Displacement meter, 16... Calculator, 17...
... Controller, 18, 19 ... Solenoid valve, 20
...Internal pressure sensor.
Claims (1)
ドラム上に配置し、これをトロイド状に変形し、
そのクラウン部にブレーカー層及びトレツド層を
貼設して生タイヤを形成するラジアルタイヤの成
形方法において、 (イ) ブレーカーを貼設する前にタイヤクラウン部
の周長を測定するステツプ及び、 (ロ) その周長が規定範囲を外れている場合、その
周長を膨張圧等で規定範囲内に制御するステツ
プ、 とを含むラジアルタイヤの成形方法。[Claims] 1. Place the carcass layer together with other constituent members on a forming drum, deform it into a toroid shape,
A method for forming a radial tire in which a green tire is formed by pasting a breaker layer and a tread layer on the crown part includes the steps of (a) measuring the circumference of the tire crown before pasting the breaker; ) A method for forming a radial tire, comprising the step of: controlling the circumference within the specified range by using inflation pressure, etc., if the circumference is outside the specified range.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP56052775A JPS57167240A (en) | 1981-04-07 | 1981-04-07 | Molding machine of radial tire |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP56052775A JPS57167240A (en) | 1981-04-07 | 1981-04-07 | Molding machine of radial tire |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS57167240A JPS57167240A (en) | 1982-10-15 |
| JPS6345949B2 true JPS6345949B2 (en) | 1988-09-13 |
Family
ID=12924229
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP56052775A Granted JPS57167240A (en) | 1981-04-07 | 1981-04-07 | Molding machine of radial tire |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS57167240A (en) |
Families Citing this family (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2602863B2 (en) * | 1987-12-25 | 1997-04-23 | 株式会社ブリヂストン | Non-destructive inspection method for pneumatic tires |
| US20100043940A1 (en) * | 2006-11-20 | 2010-02-25 | Bridgestone Corporation | Method for measuring tire, tire measuring device and tire building apparatus |
| JP6620521B2 (en) * | 2015-11-05 | 2019-12-18 | 住友ゴム工業株式会社 | Pneumatic tire manufacturing method |
-
1981
- 1981-04-07 JP JP56052775A patent/JPS57167240A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS57167240A (en) | 1982-10-15 |
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