JPS60220840A - Precise balancing method of rotating body - Google Patents
Precise balancing method of rotating bodyInfo
- Publication number
- JPS60220840A JPS60220840A JP7805184A JP7805184A JPS60220840A JP S60220840 A JPS60220840 A JP S60220840A JP 7805184 A JP7805184 A JP 7805184A JP 7805184 A JP7805184 A JP 7805184A JP S60220840 A JPS60220840 A JP S60220840A
- Authority
- JP
- Japan
- Prior art keywords
- unbalance
- rotating body
- centrifugal force
- rotating shaft
- weight
- 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.)
- Granted
Links
- 238000000034 method Methods 0.000 title description 3
- 238000012937 correction Methods 0.000 claims description 34
- 230000010355 oscillation Effects 0.000 abstract 5
- 238000010586 diagram Methods 0.000 description 5
- 238000009434 installation Methods 0.000 description 2
- 238000012546 transfer Methods 0.000 description 2
- RYGMFSIKBFXOCR-UHFFFAOYSA-N Copper Chemical compound [Cu] RYGMFSIKBFXOCR-UHFFFAOYSA-N 0.000 description 1
- 230000001133 acceleration Effects 0.000 description 1
- 230000002411 adverse Effects 0.000 description 1
- 238000005119 centrifugation Methods 0.000 description 1
- 238000007796 conventional method Methods 0.000 description 1
- 229910052802 copper Inorganic materials 0.000 description 1
- 239000010949 copper Substances 0.000 description 1
- 238000006073 displacement reaction Methods 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 238000005516 engineering process Methods 0.000 description 1
- 230000005484 gravity Effects 0.000 description 1
- 238000003754 machining Methods 0.000 description 1
- 238000005259 measurement Methods 0.000 description 1
- 238000000691 measurement method Methods 0.000 description 1
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01M—TESTING STATIC OR DYNAMIC BALANCE OF MACHINES OR STRUCTURES; TESTING OF STRUCTURES OR APPARATUS, NOT OTHERWISE PROVIDED FOR
- G01M1/00—Testing static or dynamic balance of machines or structures
- G01M1/30—Compensating imbalance
- G01M1/32—Compensating imbalance by adding material to the body to be tested, e.g. by correcting-weights
- G01M1/326—Compensating imbalance by adding material to the body to be tested, e.g. by correcting-weights the body being a vehicle wheel
Landscapes
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Testing Of Balance (AREA)
- Constituent Portions Of Griding Lathes, Driving, Sensing And Control (AREA)
Abstract
Description
【発明の詳細な説明】
一般に回転体においてはアンバランスを補正する作業が
必要である。例えば、研削盤の砥石や車輌の中軸のアン
バランスは、前者の場合では工作精度に悪影響を与え、
後者の場合では走行性、特に高速時の走行性に悪影響を
与えるからである。DETAILED DESCRIPTION OF THE INVENTION In general, it is necessary to correct unbalance in a rotating body. For example, in the former case, unbalance of the grinding wheel of a grinding machine or the center axis of a vehicle has a negative effect on machining accuracy;
This is because in the latter case, the running performance, especially at high speeds, is adversely affected.
回転体バランシング方法として、従来採られているもの
としては機械から回転体を取り外して重力の釣合を静的
にとる方法や、オートバランサーを用いるものなどがあ
るが、前者は機械を止めていちいち回転体を取り外さな
ければならず、手間が煩雑で、かつ粗いバランスとりし
かできず、また、後者は大型で機械コストが高いものに
なる等の問題点があり、このようなことから精密なバラ
ンシングを安価に行うことかぐさ、かつ、機械を止める
必要のないバランシング技術の開発が望まれでいる。Conventional methods for balancing rotating bodies include removing the rotating body from the machine and balancing the gravity statically, and using an auto balancer. The rotating body has to be removed, which is time consuming and only rough balancing can be done.Also, the latter requires large size and high machine cost.For these reasons, precise balancing is not possible. It is desired to develop a balancing technology that can do this at low cost and that does not require stopping the machine.
本発明は、上記の如き事情に艦みてなされたものであっ
て、回転体のアンバランス補正作業において、その補正
作業の基礎的な資料となるアンバランス量と回転角を、
簡単な作@’r−、正確かつ迅速に、試行錯誤する事な
しに測定することができ、ひいては、補正作業を簡単、
正確、かつ迅速に行える回転体の精密バランシング方法
を提供り−ることを目的とするものである。The present invention was made in consideration of the above-mentioned circumstances, and in the unbalance correction work of a rotating body, the unbalance amount and rotation angle, which are the basic data for the correction work, are
Simple operation@'r- allows measurement to be carried out accurately and quickly without trial and error, which in turn makes correction work easy.
It is an object of the present invention to provide a precision balancing method for a rotating body that can be performed accurately and quickly.
この目的に対応し゛(、この発明の回転体の精密バラン
シング方法は、回転体の一定回転半径上の任意の位置に
質量が等しい2個のアンバランス補正用重りを取り付は
可能に構成し、かつ前記回転体の回転軸の振動を検出す
る振動計を備え、a、:前記アンバランス補正用重りを
成句けない状態での前記回転軸のアンバランス量による
振動振幅
φ:a+が生じる位置
B:アンバランス補正用重りを1個取り付けた状態での
前記回転体の遠心力による前記回転軸の振動振幅
C:アンバランス補正用mりをπだけ移動させて取り付
けた状態での前記回転体の遠心力による前記回転軸の振
動振幅
としたとき、
前記2個のアンバランス補正用重りをそれぞれ下記の角
度α、βの位置、
α;π+φ
+ (008” (al / 2 + a+丁7丁)β
=π+φ
−(cos’(a、/2r −ト − a、 )に取り
付けることを特徴とするものである。In order to achieve this purpose, the precision balancing method for a rotating body of the present invention is configured such that two unbalance correction weights having the same mass can be attached to any position on a constant rotation radius of the rotating body, and a vibration meter for detecting vibrations of the rotating shaft of the rotating body, a: position B where vibration amplitude φ due to the unbalance amount of the rotating shaft in a state where the unbalance correction weight cannot be corrected: a+ occurs; : Vibration amplitude C of the rotating shaft due to the centrifugal force of the rotating body with one unbalance correction weight attached: C of the vibration of the rotating body with the unbalance correction weight moved and attached by π When the vibration amplitude of the rotating shaft due to centrifugal force is taken as, the two unbalance correction weights are at the following angles α and β, respectively, α; π + φ + (008” (al / 2 + a + 7 teeth) β
=π+φ−(cos'(a,/2r−t−a,).
以下、この発明の詳細を一実施例を示1図面について説
明する。Hereinafter, details of the present invention will be explained with reference to one drawing showing one embodiment.
第1図(A)、(B)は本発明の測定方法を実施するた
めに使用する装置全体についての説明図であり、1は回
転体で、ここでは、研削盤用の砥石を例示している。こ
の回転体は取り付は用フランジ2を介して回転軸3に固
定されている。この取り付は用フランジ2には、一定半
径rの環状の溝4が配設されており、この溝4には質量
の等しい2個のアンバランス補正用重り5.6が移動か
つ取り外し自在に装置されている。例えば回転軸の軸受
部13の振動を検出するための振動it (非接触変位
計、または加速度ピックアップ等)7より発した信号は
、増幅器8と、回転軸3の回転数と一致しない信号をカ
ットするためのフィルター9を介して、AD変換器等1
0を通してマイコン11に入力し、表示器12を介して
、作業者と対話式にバランシング作業を行なうことがで
きる。FIGS. 1(A) and 1(B) are explanatory diagrams of the entire apparatus used to carry out the measurement method of the present invention, in which 1 is a rotating body, and here a grinding wheel for a grinding machine is shown as an example. There is. This rotating body is fixed to a rotating shaft 3 via a mounting flange 2. For this installation, the flange 2 is provided with an annular groove 4 having a constant radius r, and two unbalance correction weights 5.6 of equal mass are movable and removable in this groove 4. Equipment has been installed. For example, the signal emitted from the vibration it (non-contact displacement meter or acceleration pickup, etc.) 7 for detecting the vibration of the bearing part 13 of the rotating shaft is sent to the amplifier 8, which cuts off signals that do not match the rotational speed of the rotating shaft 3. AD converter etc. 1 through a filter 9 for
0 to the microcomputer 11 and the operator can perform the balancing work interactively via the display 12.
このような装置を用いて、アンバランス量、すなわち、
遠心力としてのアンバランス量及びその回転角を測定す
るためには、まず補正用重り5゜6を溝4から取り外し
て、回転体1を回転させ、回転体1の遠心力による電圧
値a、のデータをマイコンに転送する。Using such a device, the amount of unbalance, i.e.
In order to measure the amount of unbalance as centrifugal force and its rotation angle, first remove the correction weight 5.6 from the groove 4, rotate the rotating body 1, and measure the voltage value a due to the centrifugal force of the rotating body 1. transfer the data to the microcontroller.
次に質量が同一の補正用重り5ないし6を試し用の重り
とし、任意の基準位置に取り(=Iけて、回転体1を回
転させ、その時の回転体1の遠心力による電圧値Bをマ
イコンに転送する。Next, use the correction weights 5 and 6 of the same mass as trial weights, set them at an arbitrary reference position (=I, rotate the rotating body 1, and set the voltage value B due to the centrifugal force of the rotating body 1 at that time. transfer to the microcontroller.
さらに、任意の基準位置に取り付けた試し用の重りを、
基準位置と180度反対銅に取り付けて、回転体1を回
転させ、その時の回転体1の遠心力による電圧値Cをマ
イコンに転送する。そのあと、マイコンには、以下の計
算をさせる。Furthermore, a trial weight attached to an arbitrary reference position,
It is attached to a copper plate 180 degrees opposite the reference position, rotates the rotating body 1, and transmits the voltage value C due to the centrifugal force of the rotating body 1 at that time to the microcomputer. After that, the microcontroller performs the following calculations.
アンバランス補正用重り5または6単体の遠心力をaと
覆ると、
a=+−a、/2 ・・・(1)式
14型位−と補正用重りなしの状態のアンバランスの位
置のなす角度をφとすると、
第2図(A>の場合
φ−cos”((a’−C”+a+) / (2・a
−a+) )・・・(2)式
第2図(B)の場合
φz= 006−’ ((a” −C’十aこ)/(2
−a−a、))・・・(3)式
以上の情報では、補正用重り取り付は位置の解が2種類
出てくるので、その正誤を判定する必要がある。そこで
、試し用重りを、基準位置より90度の位置に取り付け
、回転体を回転させて、その時の回転体1の遠心力によ
る電圧値Eをマイコンに転送する。第3図から、予め計
算できるel及びelとEを比較し、2種類の解のうち
、どちらが正しいかを、ここで判定し、補正用重り2個
を、それぞれどの位置に取り付けたら良いかは、表示器
に表示される。Substituting the centrifugal force of the unbalance correction weight 5 or 6 alone as a, a = + - a, /2 ... (1) Equation 14 - and the unbalance position without the correction weight If the angle formed by
-a+))...For formula (2) in Figure 2 (B), φz= 006-'((a''-C'10ako)/(2
-a-a,))...With the information in equation (3) and above, two types of positional solutions come out for the correction weight attachment, so it is necessary to determine whether they are correct or incorrect. Therefore, a trial weight is attached at a position 90 degrees from the reference position, the rotating body is rotated, and the voltage value E due to the centrifugal force of the rotating body 1 at that time is transferred to the microcomputer. From Figure 3, compare el and el and E, which can be calculated in advance, and determine which of the two solutions is correct, and determine where the two correction weights should be attached. , will be displayed on the display.
基準位置から901i[の位置に補止用重りを取り付け
て回転させたときのアンバランス量eは第3図(A)の
場合
el =8” +8+ + 2 ” a −8+ ・f
iinφ、・(4)式第3図(B)の場合
e、=a’+aご+2−a−a+−5inφ、・(5)
式%式%
図の方が、正しい状態であることがわかる。The unbalance amount e when the supplementary weight is attached to the position 901i from the reference position and rotated is el = 8" +8+ + 2" a -8+ ・f in the case of Fig. 3 (A).
iinφ, ・(4) In the case of Figure 3 (B), e, = a'+a+2-a-a+-5inφ, ・(5)
It can be seen that the formula % formula % figure is more correct.
このときのアンバランス位置φは、(2)式よりめられ
る。The unbalance position φ at this time can be determined from equation (2).
補正用重りのない場合の振幅a1は遠心力アンバランス
量に比例するから、この遠心力アンバランス量をF、と
すると
a、=C−F、 ・・・(6)式
%式%)
同様に、補正用重り1個の遠心力アンバランス!laは
、霧を重りの質量、ωを回転体の角速度とすると、
a=Q−−・r・ω2 ・・・(7)式%式%
(6)式(7)式より
F1= (al/a ) −m −r −ω” ・=
(8)式このアンバランスを補正するためには2個のア
ンバランス補正用重り5.6をその合力りが、FIと同
じ大きさで、方向が反対になるように、取り付は角を決
めれば良い。The amplitude a1 when there is no correction weight is proportional to the amount of centrifugal force unbalance, so if this amount of centrifugal force unbalance is F, then a, = C - F, ... (6) formula % formula %) Similarly Then, the centrifugal force unbalance of one correction weight! When la is the mass of the fog and ω is the angular velocity of the rotating body, then a=Q−・r・ω2 ... (7) formula% formula% (6) From formula (7), F1= (al /a) −m −r −ω” ・=
Equation (8) To correct this unbalance, attach the two unbalance correction weights 5.6 at the corners so that the resultant force is the same magnitude as FI and in the opposite direction. All you have to do is decide.
補正用重り5.6の遠心力は、それぞれm・「・♂であ
るから、第4図より
cosθ=al/2a ・(9’)式
%式%
はアンバランスの方向に対して、補正用重り2個を振り
分けた時の、2個の重りのな1角麿を示す。Since the centrifugal force of the correction weight 5.6 is m and "・♂, respectively, cosθ=al/2a from Fig. 4. Equation (9') % Formula % is the correction weight for the direction of unbalance. When two weights are distributed, it shows two weightless one-kakumaro.
ゆえに、取り付けるべきアンバランス補正用重りは、基
準位向に対して、
α−π+φ十〇O8−’(at/ 2a ) −(10
)式β−π+φ−cos” (a、/ 2a > ・・
−(11)式である。Therefore, the unbalance correction weight to be attached is α-π+φ10O8-'(at/2a)-(10
) formula β-π+φ-cos” (a, / 2a > ・・
−(11).
表示器に表示された角度α及びβに基づいて、アンバラ
ンス補正用重りを取り付けることにより、バランシング
作業は完了する。The balancing work is completed by attaching the unbalance correction weight based on the angles α and β displayed on the display.
以上の説明から明らかな通り、この発明ではアンバラン
ス補正用重りを取り付けない状態ぐの前記回転軸のアン
バランス量による振動振幅、アンバランス補正用重りを
1個取り付けた状態での回転体の遠心力による回転軸の
振動振幅、及びアンバランス補正用重りを反対側に取り
付けた場合の遠心力による回転軸の振動振幅を検出する
だけで、アンバランス補正用重りの取り付は位置を決定
することができ、回転体を機械から取り外寸必要なしに
^精度のバランシングを容易に行なうことができる。As is clear from the above explanation, in this invention, the vibration amplitude due to the unbalance amount of the rotating shaft without the unbalance correcting weight attached, and the centrifugation of the rotating body with one unbalance correcting weight attached. The installation position of the unbalance correction weight can be determined by simply detecting the vibration amplitude of the rotating shaft due to force and the vibration amplitude of the rotation shaft due to centrifugal force when the unbalance correction weight is installed on the opposite side. This makes it possible to easily perform accurate balancing without having to remove the rotating body from the machine.
第1図(A)は回転体にアンバランス補正用重りを取り
付けた状態を示す正面説明図、第1図(B)は第1図(
A>に承り回転体の側面説明図、第2図は基準位置とア
ンバランス補正用重りなしのアンバランスの位置のなす
角度を示すベクトル線図、第3図は基準位置から90麿
の位置に重りをつけて(2)式と(3)式で計算したφ
の値の判定をづるベクトル線図、及び第4図はアンバラ
ンスによる遠心力と大きさが等しく方向が反対のベクト
ルを発生させた場合の、補正用重りのベクトルとの関係
を示すベクトル線図である。
1・・・回転体 2・・・取り付は用フランジ 3・・
・回転軸 4・・・アンバランス補正用重り固定溝5.
6・・・アンバランス補正用重り
復代理人弁理士 川 井 治 男
第1図
(A) (B)
第2図
(Al (B)
」
υ 0
(A)(B)Fig. 1 (A) is a front explanatory view showing the state in which the unbalance correction weight is attached to the rotating body, and Fig. 1 (B) is the illustration shown in Fig. 1 (
A> A side explanatory diagram of the rotating body, Figure 2 is a vector diagram showing the angle between the reference position and the unbalanced position without the unbalance correction weight, Figure 3 is the position 90 m from the reference position. φ calculated using equations (2) and (3) with weight added
A vector diagram showing the determination of the value of , and Figure 4 is a vector diagram showing the relationship with the correction weight vector when a vector is generated that is equal in magnitude and opposite in direction to the centrifugal force due to unbalance. It is. 1...Rotating body 2...Flange for mounting 3...
・Rotating axis 4... Weight fixing groove for unbalance correction 5.
6... Weight for unbalance correction Patent attorney Osamu Kawai Figure 1 (A) (B) Figure 2 (Al (B) ' υ 0 (A) (B)
Claims (1)
個のアンバランス補正用重りを取り付は可能に構成し、
かつ前記回転体の回転軸の振動を検出する振動計を備え
、 al:前記アンバランス補正用重りを取付けない状態で
の前記回転軸のアンバランス量による振動振幅 φ:a1が生じる位置 B:アンバランス補正用重りを1個取り付・ノだ状態で
の前記回転体の遠心力による前記回転軸の振動振幅 C:アンバランス補正用重りをπだ番ノ移動させて取り
付番ノた状態での前記回転体の遠心力による前記回転軸
の振動振幅 としたとき、 前記2個のアンバランス補正用重りをそれぞれ下記の角
度α、βの位置、 α;π+φ +(cos’(at/2 +C−2a+)/2)β=π
+φ −(cos’(a+/2 十G−2a1/2)に取り付
けることを特徴とする回転体の精密バランシング方法。[Claims] 2 whose mass is equal to any position on a constant radius of rotation of a rotating body
It is configured so that it is possible to install several unbalance correction weights,
and a vibration meter for detecting vibrations of the rotation shaft of the rotating body, al: position B: where vibration amplitude φ due to the unbalance amount of the rotation shaft in a state where the unbalance correction weight is not attached: a1 occurs; Vibration amplitude C of the rotating shaft due to the centrifugal force of the rotating body when one balance correction weight is attached and left open: When the unbalance correction weight is moved by π and installed When the vibration amplitude of the rotating shaft is caused by the centrifugal force of the rotating body, the two unbalance correction weights are positioned at the following angles α and β, α;π+φ +(cos'(at/2 +C −2a+)/2)β=π
+φ −(cos′(a+/2 10G−2a1/2)).
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP59078051A JPH0663898B2 (en) | 1984-04-18 | 1984-04-18 | Precision balancing method for rotating body |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP59078051A JPH0663898B2 (en) | 1984-04-18 | 1984-04-18 | Precision balancing method for rotating body |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS60220840A true JPS60220840A (en) | 1985-11-05 |
JPH0663898B2 JPH0663898B2 (en) | 1994-08-22 |
Family
ID=13651047
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP59078051A Expired - Lifetime JPH0663898B2 (en) | 1984-04-18 | 1984-04-18 | Precision balancing method for rotating body |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH0663898B2 (en) |
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN111024312A (en) * | 2019-12-13 | 2020-04-17 | 鲁西化工集团股份有限公司动力分公司 | Impeller fan on-site dynamic balance method |
WO2024043236A1 (en) * | 2022-08-23 | 2024-02-29 | 株式会社かいわ | Balancer |
Citations (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS5837530A (en) * | 1981-08-31 | 1983-03-04 | Agency Of Ind Science & Technol | Measuring method for unbalance of disc-like rotary body |
-
1984
- 1984-04-18 JP JP59078051A patent/JPH0663898B2/en not_active Expired - Lifetime
Patent Citations (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS5837530A (en) * | 1981-08-31 | 1983-03-04 | Agency Of Ind Science & Technol | Measuring method for unbalance of disc-like rotary body |
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN111024312A (en) * | 2019-12-13 | 2020-04-17 | 鲁西化工集团股份有限公司动力分公司 | Impeller fan on-site dynamic balance method |
WO2024043236A1 (en) * | 2022-08-23 | 2024-02-29 | 株式会社かいわ | Balancer |
Also Published As
Publication number | Publication date |
---|---|
JPH0663898B2 (en) | 1994-08-22 |
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