JP2001200826A - Male screw member - Google Patents

Male screw member

Info

Publication number
JP2001200826A
JP2001200826A JP2000007149A JP2000007149A JP2001200826A JP 2001200826 A JP2001200826 A JP 2001200826A JP 2000007149 A JP2000007149 A JP 2000007149A JP 2000007149 A JP2000007149 A JP 2000007149A JP 2001200826 A JP2001200826 A JP 2001200826A
Authority
JP
Japan
Prior art keywords
screw member
male screw
bolt
face
axis
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Pending
Application number
JP2000007149A
Other languages
Japanese (ja)
Inventor
Tsuyoshi Sugiura
強 杉浦
Hiroshi Kurauchi
浩 倉内
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.)
Sugiura Seisakusho Co Ltd
Original Assignee
Sugiura Seisakusho Co Ltd
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Sugiura Seisakusho Co Ltd filed Critical Sugiura Seisakusho Co Ltd
Priority to JP2000007149A priority Critical patent/JP2001200826A/en
Publication of JP2001200826A publication Critical patent/JP2001200826A/en
Pending legal-status Critical Current

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  • Length Measuring Devices Characterised By Use Of Acoustic Means (AREA)
  • Force Measurement Appropriate To Specific Purposes (AREA)

Abstract

PROBLEM TO BE SOLVED: To provide a male screw member which realizes an appropriate fastening by measuring the axial force of the male screw member such as a bolt by ultrasonic wave. SOLUTION: The squareness of the end surfaces of both the end parts of the male screw member to the shaft straight line of the male screw member is set to 0.0005-0.1 mm. Regarding the actual angle θ of the end surfaces of both the end parts of the male screw member to a virtual plane perpendicular to the axis which is perpendicular to the axis of the male screw member, tan θis set to 0.02 or below. The flatness of the end surfaces of both the end part of the male screw member can be set to 0.0005-0.1 mm, and the ten-point average roughness Rz of the end surfaces of both the end parts can be set to 1-15.

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】この発明は、ボルト等のおね
じ部材に関する。
The present invention relates to a male screw member such as a bolt.

【0002】[0002]

【背景技術】ボルトやナット等の締め付け力が過大・過
小にならないように、締め付けトルクが所定値になった
とき、締め付け完了とするインパクトレンチ等が広く用
いられている。しかし、ボルト・ナットの噛み合わせが
不良であったり、異物を噛み込んだりしたときは、締め
込みが完了していなくても締め付けトルクが設定値まで
上昇し、それで締め込みを止めてしまう場合も生じ得
る。
2. Description of the Related Art An impact wrench or the like that completes tightening when a tightening torque reaches a predetermined value so that a tightening force of a bolt, a nut, or the like does not become excessive or excessive is widely used. However, if the bolts and nuts are not properly engaged or foreign matter is caught, the tightening torque may increase to the set value even if the tightening is not completed, and the tightening may stop. Can occur.

【0003】このような締め付けトルクに代えて又はこ
れに加え、ボルト又はナットを締め付けたときにボルト
軸部に発生する引張り力(ボルト軸力)を参照して、締
め込みを完了する試みもある。そこで、ボルト軸力の増
大に従ってボルトは軸方向にわずかに伸びる(ボルト軸
方向長さが僅かに大きくなる)から、このボルトの伸び
を超音波を利用して測定し、その伸びが所定値になった
とき締め込み完了とすることが考えられる。その場合、
ボルトの軸方向に超音波を発射し、ボルトの軸方向の両
端面で繰り返し反射して往復する超音波の伝搬時間の増
加をみて、ボルトの伸びひいてはボルト軸力を測定する
ことができる。
[0003] Instead of or in addition to such a tightening torque, there is also an attempt to complete the tightening by referring to the tensile force (bolt axial force) generated in the bolt shaft when the bolt or nut is tightened. . Therefore, the bolt slightly expands in the axial direction as the bolt axial force increases (the length in the bolt axial direction slightly increases). The extension of the bolt is measured using ultrasonic waves, and the elongation reaches a predetermined value. It is conceivable that the tightening is completed when it becomes. In that case,
Ultrasonic waves are emitted in the axial direction of the bolt, and the axial propagation force of the bolt and thus the axial force of the bolt can be measured by observing the increase in the propagation time of the ultrasonic wave that is repeatedly reflected and reciprocated at both axial end faces of the bolt.

【0004】[0004]

【発明が解決しようとする課題】しかし、一般にボルト
の軸方向の両端部の端面は、鍛造・鋳造等により形成さ
れた面で規定され、特にボルト軸部の先端面は鍛造等に
よる複雑な3次元形態をしているのが普通である。その
ため超音波をボルト軸方向に往復させても、伝搬される
超音波が端面で軸方向に対し斜めに反射したり乱反射し
たりして、伝搬時間を求めるのが困難であったり、伝搬
時間の誤差が大きくて、実用に供し得ない事情があっ
た。
However, generally, the end faces at both ends in the axial direction of the bolt are defined by surfaces formed by forging, casting, or the like. It usually has a dimensional form. Therefore, even if the ultrasonic wave is reciprocated in the bolt axis direction, the transmitted ultrasonic wave is reflected obliquely or irregularly with respect to the axial direction at the end face, making it difficult to determine the propagation time, or The error was so large that it could not be put to practical use.

【0005】この発明の課題は、超音波でボルト等のお
ねじ部材の軸力を測定することを可能とし、適正な締め
付けを実現するおなじ部材を提供することにある。
[0005] It is an object of the present invention to provide an identical member which enables the axial force of a male screw member such as a bolt to be measured by ultrasonic waves and realizes proper tightening.

【0006】[0006]

【課題を解決するための手段及び発明の効果】この発明
は、おねじ部材の軸直線に対する、おねじ部材の両端部
の各端面の直角度が0.0005〜0.1mmとされ
る。また、おねじ部材の軸線に直角な仮想の軸直角平面
に対する、おねじ部材の両端部の各端面の実際角度θに
ついて、tanθが0.02以下とする。さらに、おね
じ部材の両端部の各端面の平面度が0.0005〜0.
1mm、上記両端部の各端面の十点平均粗さRzを1〜
15とすることができる。
According to the present invention, the perpendicularity of each end face of both ends of the male screw member to the axis straight line of the male screw member is 0.0005 to 0.1 mm. In addition, tan θ is set to 0.02 or less with respect to an actual angle θ of each end surface of both ends of the male screw member with respect to a virtual axis perpendicular to the axis of the male screw member. Furthermore, the flatness of each end face of both ends of the male screw member is 0.0005 to 0.5.
1 mm, the ten-point average roughness Rz of each end face of the both ends is 1 to
15 can be set.

【0007】ここで直角度(直角度公差)は、ボルト等
のおねじ部材の両端部の各端面が、おねじ部材の軸線
(軸直線:データム直線)に対し垂直で、0.0005
〜0.1mmだけ離れた2つの平行な仮想平面の間に画
定されることを意味する(JIS B 0021参照)。
直角度がこの範囲にあることによって、超音波等による
おねじ部材の締め付け軸力を測定する上で超音波等が両
端部の各端面で良好に反射し、その超音波等が軸方向の
両端で繰り返し往復する伝搬時間の、ボルト等の伸びに
よる増加を検出することができ、ボルト等の軸力を参照
しながら適正な軸力に達したときに締め込みを完了する
ことが可能となる。
Here, the perpendicularity (perpendicularity tolerance) is 0.0005, where each end face of both ends of the male screw member such as a bolt is perpendicular to the axis of the male screw member (axial straight line: datum straight line).
It means defined between two parallel virtual planes separated by 〜0.1 mm (see JIS B 0021).
When the squareness is within this range, the ultrasonic waves and the like are reflected well at each end face at both ends in measuring the tightening axial force of the male screw member by the ultrasonic waves, and the ultrasonic waves and the like are reflected at both ends in the axial direction. It is possible to detect the increase in the propagation time of reciprocating reciprocation due to the elongation of the bolt or the like, and it is possible to complete the tightening when the proper axial force is reached while referring to the axial force of the bolt or the like.

【0008】上記直角度が0.1mmを超えると、超音
波の反射角度がおねじ部材の軸線に対し相当傾くので、
超音波の伝搬時間とボルト等の伸びが対応しにくくな
り、直角度が0.0005mmより小さくなると、製造
の際の工程が複雑になり、製造設備のコストの増大する
ので、上記の範囲に直角度を規定する。
If the perpendicularity exceeds 0.1 mm, the reflection angle of the ultrasonic wave is considerably inclined with respect to the axis of the male screw member.
If the propagation time of ultrasonic waves and the elongation of bolts and the like become difficult to correspond to each other, and the squareness is smaller than 0.0005 mm, the manufacturing process becomes complicated, and the cost of manufacturing equipment increases. Specify the angle.

【0009】また、おねじ部材の軸線に直角な仮想の
(幾何学的)軸直角平面に対する、おねじ部材の両端部
の各端面の実際角度θについて、tanθが0.02以
下とすることで、おねじ部材の軸力測定のための超音波
等の反射の繰り返しを精度よく行わせ、ボルト等の軸力
の測定、ひいては締め付けの完了時期をより正確に設定
することができる。上記各端面の実際角度θのtanθ
が0.02を超えるようになると、上記各端面で反射す
る超音波の反射方向と、おねじ部材の軸方向とのずれが
が大きくなり、超音波等の伝搬時間の増加がおねじ部材
の軸方向に作用する引っ張り力(軸力)による伸びに起
因するものか、超音波等の斜め反射に起因するもの判断
が困難になるため、上記tanθの範囲に設定する。
The actual angle θ of each end face of the both ends of the male screw member with respect to an imaginary (geometric) axis perpendicular plane perpendicular to the axis of the male screw member is set so that tan θ is 0.02 or less. This makes it possible to accurately repeat the reflection of ultrasonic waves or the like for measuring the axial force of the male screw member, and to more accurately set the measurement of the axial force of a bolt or the like and, consequently, the completion time of the tightening. Tanθ of the actual angle θ of each end face
Is greater than 0.02, the deviation between the reflection direction of the ultrasonic wave reflected at each of the end faces and the axial direction of the male screw member increases, and the propagation time of ultrasonic waves or the like increases, and Since it is difficult to judge whether it is caused by elongation due to a tensile force (axial force) acting in the axial direction or due to oblique reflection of ultrasonic waves or the like, the value is set to the range of tan θ described above.

【0010】さらに、平面度はおねじ部材の両端部の各
端面を幾何学的平行2平面で挟んだとき、その平行2平
面の間隔が最小となる場合の、当該平行2平面の間隔で
表わされる(JIS B 0621参照)。そして、おね
じ部材の両端部の各端面の平面度が0.0005〜0.
1mmとされることで、おねじ部材の軸力測定のために
超音波等を軸方向で繰り返し伝搬させてその伝搬時間の
増加を見る場合に、両端面での反射波が拡散にくくな
り、伝搬信号の指向性が向上し、軸力測定の信頼性が向
上する。平面度が0.1mmを超えると、おねじ部材の
いわばうねりにより超音波等が分散して伝搬時間をどの
信号波でみるか判定処理が困難又はあいまいなものとな
り、逆に0.0005mmを下回ると、製造工程が複雑
化し、またおねじ部材のコストもあがるので、平面度を
上記範囲に定めることが望ましい。
Further, the flatness is represented by the distance between the two parallel planes when the distance between the two parallel planes is minimized when each end face of both ends of the male screw member is sandwiched between the two parallel geometric planes. (See JIS B 0621). And the flatness of each end face of both ends of the male screw member is 0.0005 to 0.5.
When the length is set to 1 mm, when an ultrasonic wave or the like is repeatedly propagated in the axial direction for measuring the axial force of the male screw member and the propagation time is increased, the reflected waves on both end surfaces are hardly diffused, and the propagation becomes difficult. The directivity of the signal is improved, and the reliability of the axial force measurement is improved. When the flatness exceeds 0.1 mm, the ultrasonic wave is dispersed by the so-called undulation of the male screw member, and it becomes difficult or ambiguous to determine which signal wave the propagation time is to be observed in, and conversely, it is less than 0.0005 mm. Therefore, the manufacturing process becomes complicated, and the cost of the male screw member increases. Therefore, it is desirable to set the flatness within the above range.

【0011】また、おねじ部材の両端部の各端面の十点
平均粗さRzが1〜15されることにより、軸力測定で
超音波等を用いる場合、各端面で超音波等が乱反射しに
くくなり、超音波等の伝搬時間の増加を検出する信号波
の指向性や強度が大きくなって、信頼性の高い軸力測定
が可能となる。上記の表面粗さRzが15以上になる
と、超音波等の信号波が各端面で乱反射して信号の指向
性・強度を減じ、上記Rzが1以下になると、加工工程
が煩雑で高コストなものとなるため、表面粗さRzを上
記の範囲に規定することが望ましい。
In addition, when the ten-point average roughness Rz of each end face of both ends of the male screw member is set to 1 to 15, when the ultrasonic force or the like is used for measuring the axial force, the ultrasonic wave or the like is irregularly reflected at each end face. As a result, the directivity and strength of a signal wave for detecting an increase in propagation time of an ultrasonic wave or the like increase, and a highly reliable axial force measurement becomes possible. When the above-mentioned surface roughness Rz is 15 or more, signal waves such as ultrasonic waves are irregularly reflected at each end face to reduce the directivity and intensity of the signal. When the above-mentioned Rz is 1 or less, processing steps are complicated and costly. Therefore, it is desirable to define the surface roughness Rz in the above range.

【0012】なお、ボルト等のおねじ部材の軸力を測定
しつつ締め込みを実施する場合に、その軸力測定の手段
は、超音波に限らず、おねじ部材の両端面での反射を利
用するものとして、所定の電波、振動波、衝撃波等を利
用することも可能であり、上記のおねじ部材の特徴は、
超音波以外の軸力測定媒体にも有効である。
When tightening while measuring the axial force of a male screw member such as a bolt, the means for measuring the axial force is not limited to ultrasonic waves. As a thing to use, it is also possible to use a predetermined radio wave, vibration wave, shock wave, etc.
It is also effective for axial force measurement media other than ultrasonic waves.

【0013】[0013]

【発明の実施の形態】以下、図面に示す実施例を参照し
つつ本発明の実施の形態を説明する。図1に示すおねじ
部材としてのボルト1は、頭部2と軸部3を有する。ボ
ルト両端部の各端面、言い換えれば頭部2の端面4と軸
部3の端面5は、ボルト軸線Aに対する直角度が0.0
005〜0.1mmの範囲に設定され、なかでも0.0
01〜0.08mm、特に0.01〜0.07mmの範
囲で形成される。つまり、図2に示すようにボルト1の
各端面4及び5は、ボルト軸線Aに垂直(直角)で、上
記範囲(距離t)だけ離れた2つの平行な仮想平面P
1、P2の間に画定されている。
Embodiments of the present invention will be described below with reference to embodiments shown in the drawings. A bolt 1 as a male screw member shown in FIG. 1 has a head 2 and a shaft 3. Each of the end faces of both ends of the bolt, in other words, the end face 4 of the head 2 and the end face 5 of the shaft 3 have a perpendicularity to the bolt axis A of 0.0.
005 to 0.1 mm, especially 0.0
It is formed in the range of 0.01 to 0.08 mm, particularly 0.01 to 0.07 mm. That is, as shown in FIG. 2, each of the end faces 4 and 5 of the bolt 1 is perpendicular (perpendicular to) the bolt axis A and two parallel virtual planes P separated by the range (distance t).
1, defined between P2.

【0014】また、図3に示すように、ボルト軸線Aに
垂直(直角)な幾何学的平面Pに対し、ボルト1の両端
部の各端面4、5のなす角度(交差角度)θは、tan
θ(図のb/a)が0.02以下とされ(下限値として
は0.00003)、なかでも0.00006〜0.0
16、特に0.0006〜0.014程度の範囲とされ
る。これはθに換算すれば(tan−1θとも言える
が)、θ又はtan−1θは1.2度以下(下限値とし
ては0.001度)、なかでも0.003〜0.9度、
特に0.03〜0.8度程度に設定できる。
As shown in FIG. 3, an angle (intersecting angle) θ between the end faces 4 and 5 at both ends of the bolt 1 with respect to a geometric plane P perpendicular (perpendicular) to the bolt axis A is tan
θ (b / a in the figure) is set to 0.02 or less (0.00003 as the lower limit), and especially 0.00006 to 0.0
16, particularly in the range of about 0.0006 to 0.014. If this is converted to θ (it can also be called tan −1 θ), θ or tan −1 θ is 1.2 degrees or less (the lower limit is 0.001 degrees), and especially 0.003 to 0.9 degrees. ,
In particular, it can be set to about 0.03 to 0.8 degrees.

【0015】また、ボルト1の両端部の各端面4、5の
平面度は、0.0005〜0.1mmとされ、なかでも
0.001〜0.08、特に0.002(又は0.0
1)〜0.07程度に設定される。
The flatness of each of the end faces 4 and 5 at both ends of the bolt 1 is 0.0005 to 0.1 mm, particularly 0.001 to 0.08, especially 0.002 (or 0.02 mm).
1) It is set to about 0.07.

【0016】さらに、ボルト1の両端部の各端面4、5
のそれぞれの表面粗さが、十点平均粗さRzで15以下
とされ(下限値として例えば1)、なかでもRzが1.
5〜11とされる。特に、Rzが2〜8(さらには5〜
7)が望ましい。
Further, the end faces 4, 5 at both ends of the bolt 1 are provided.
Has a surface roughness of 15 or less in ten-point average roughness Rz (for example, 1 as a lower limit value).
5 to 11. In particular, Rz is 2 to 8 (further 5 to 5
7) is desirable.

【0017】上記のようにボルトの両端面4、5の直角
度、平面度及び表面粗さを定めることにより、例えば図
4に示すように、ボルト1にナット7を螺合してボルト
1又はナット7を締め込む場合、ボルトの軸力Tf(図
5)を超音波を利用して測定しながら、インパクトレン
チ等の締め込み装置又は工具で締め込み工程又は作業を
実施することができる。ボルト軸力Tfは締め込みによ
ってボルトの軸方向に生じる引張り力であり、この引張
り力(ボルト軸力)が増大すれば、ボルトは軸方向に多
少伸びるため、この伸び量を超音波の伝搬時間の増加に
より検出することにより間接的にボルト軸力を測定し、
予め定められたボルト軸力に達したところで締め込みを
完了する。
By determining the perpendicularity, flatness, and surface roughness of both end surfaces 4 and 5 of the bolt as described above, for example, as shown in FIG. When the nut 7 is tightened, the tightening process or operation can be performed with a tightening device or tool such as an impact wrench while measuring the axial force Tf (FIG. 5) of the bolt using ultrasonic waves. The bolt axial force Tf is a tensile force generated in the axial direction of the bolt by tightening. If the tensile force (bolt axial force) increases, the bolt slightly expands in the axial direction. Bolt axial force is measured indirectly by detecting the increase in
Tightening is completed when a predetermined bolt axial force is reached.

【0018】例えば図4(a)に示すように、ボルト1
の頭部端面4又は軸部端面5のいずれかに(ナット7を
締め込むのであればボルト1の頭部端面4)に超音波式
ボルト軸力計10の検出部(トランデューサ)11を当
て、ボルトの軸方向に超音波を発する。その超音波はボ
ルト1の軸部端面5で反射して、ボルト頭部側に戻り、
頭部端面4で再び反射するというように、両端面4、5
で反射を繰り返して往復(例えば数百〜数千回)する。
この超音波の伝搬時間を測定することにより、締め込み
に伴うボルト1の伸び、ひいてはボルト1の軸力を測定
できる。図4(a)の場合は1つのトランスデューサ1
1で超音波の発信と受信を兼ねるが、同図(b)に示す
ように、ボルトの1の両端面4、5にそれぞれ発信用及
び受信用のトランスデューサ11、12を当ててもよ
く、この場合でも多数回往復した超音波の伝搬時間の変
化をみることになる。
For example, as shown in FIG.
The detecting unit (transducer) 11 of the ultrasonic bolt axial force meter 10 is applied to either the head end surface 4 or the shaft end surface 5 (the head end surface 4 of the bolt 1 if the nut 7 is tightened). Emits ultrasonic waves in the axial direction of the bolt. The ultrasonic wave is reflected by the shaft end surface 5 of the bolt 1 and returns to the bolt head side,
Both end faces 4, 5 are reflected at head end face 4 again.
To reciprocate (for example, several hundred to several thousand times).
By measuring the propagation time of this ultrasonic wave, the elongation of the bolt 1 due to the tightening, and thus the axial force of the bolt 1 can be measured. In the case of FIG. 4A, one transducer 1 is used.
1 transmits and receives an ultrasonic wave, but as shown in FIG. 3B, transmitting and receiving transducers 11 and 12 may be applied to both end surfaces 4 and 5 of the bolt 1, respectively. Even in this case, a change in the propagation time of the ultrasonic wave that has reciprocated many times is observed.

【0019】このように超音波を利用してボルト軸力を
測定しようとする場合、図6(a)に示すようにボルト
の両端面4、5の直角度が前述の範囲を逸脱すると、超
音波がボルト軸方向に傾斜するように反射し、ボルト軸
部の側面でも反射して、伝搬経路が長くなるので、ボル
トの伸びに伴う伝搬時間の増加とを区別できにくくな
る。また、同図(b)のようにボルト1の両端面4、5
の平面度が前述の範囲を逸脱すると、超音波の反射波が
うねりのある端面で分散し、超音波の伝搬時間が把握困
難になる。さらに同図(c)のようにボルト1の両端面
4、5の表面粗さRzが上記範囲から外れると、超音波
が両端面4、5で乱反射し、その強度を減じる(いわば
減衰される)ため、超音波の指向性のある往復波を生じ
にくい。
When the axial force of a bolt is to be measured using ultrasonic waves, if the perpendicularity of both end surfaces 4 and 5 of the bolt deviates from the aforementioned range as shown in FIG. The sound wave is reflected so as to be inclined in the bolt axis direction, and is also reflected on the side surface of the bolt shaft portion, so that the propagation path becomes longer. Therefore, it is difficult to distinguish the increase in the propagation time due to the elongation of the bolt. Also, as shown in FIG.
If the flatness deviates from the above-mentioned range, the reflected wave of the ultrasonic wave is dispersed on the undulating end face, and it becomes difficult to grasp the propagation time of the ultrasonic wave. Further, when the surface roughness Rz of the both end surfaces 4 and 5 of the bolt 1 is out of the above range as shown in FIG. 3C, the ultrasonic wave is irregularly reflected on the both end surfaces 4 and 5 and its intensity is reduced (in other words, attenuated). Therefore, it is difficult to generate a reciprocal wave having directivity of ultrasonic waves.

【0020】上記の実施例では、ボルトの両端面の直角
度、平面度、表面粗さを相乗的に画定したことにより、
超音波の反射ひいては伝搬時間の検出に伴い、超音波が
ボルト軸方向に沿い易く、かつ分散しにくく、しかも乱
反射が抑制されて、ボルト軸力の測定が可能となり、か
つその精度も高いものとなる。
In the above embodiment, the squareness, flatness, and surface roughness of both end faces of the bolt are synergistically defined.
With the detection of the reflection of the ultrasonic wave and, consequently, the propagation time, the ultrasonic wave is easy to follow along the bolt axis direction and is hard to disperse, and the irregular reflection is suppressed, so that the bolt axial force can be measured and its accuracy is high. Become.

【0021】なお、以上の説明では、一般的なボルトを
例に採ったが、頭部のないボルト等、他のおねじ部材に
本発明を適用することもできる。
In the above description, a general bolt is taken as an example, but the present invention can be applied to other screw members such as a bolt without a head.

【0022】図7に示すように、ボルト76の頭部側端
面に凹部56を形成するとともに、軸部側端面にも凹部
48を形成し、凹部56の底面57を頭部側の基準平面
(ボルト軸線にほぼ直角な平面、以下同じ)、凹部48
の底面49を軸部側の基準平面とすることができる。こ
の場合、頭部側の底面57の広さは、ボルト軸線を中心
にして、例えばボルト軸部の断面dを投影した平面とほ
ぼ同等とすること、あるいはそれより大きくすること、
あるいはそれより狭くすることができる。また、軸部側
の凹部48の底面49は、軸部断面dより小さくなる。
そして、頭部側の基準平面57の直径d1(多角形の場
合はその広さを示す対角線等)と軸部側の底面49の直
径d2との関係は、d1>d2、d1<d2あるいは、d1=
d2のいずれも可能である。
As shown in FIG. 7, a concave portion 56 is formed on the head-side end surface of the bolt 76, and a concave portion 48 is also formed on the shaft-side end surface. A plane substantially perpendicular to the bolt axis, the same applies hereinafter), recess 48
Can be used as a reference plane on the shaft portion side. In this case, the width of the bottom surface 57 on the head side is, for example, substantially equal to or larger than the plane on which the cross section d of the bolt shaft is projected, with the bolt axis as the center.
Alternatively, it can be narrower. Further, the bottom surface 49 of the concave portion 48 on the shaft portion side is smaller than the shaft portion cross section d.
The relationship between the diameter d1 of the reference plane 57 on the head side (a diagonal line indicating the size of the polygon in the case of a polygon) and the diameter d2 of the bottom surface 49 on the shaft side is d1> d2, d1 <d2, or d1 =
Any of d2 is possible.

【0023】図7(b)に示すように、ボルト77の頭
部側の基準平面57の広さ(d1)と軸部側の基準平面
49の広さ(d2)とがボルト軸線に関して同軸状の位
置に等しい領域(d1=d2)で存在する場合は、それら
基準平面57及び49を結ぶ筒状(例えば円筒状)の内
側の領域で超音波の反射を繰り返して往復伝搬させるこ
とができる。従って超音波の反射に必要な基準平面を最
小とすることができ、精度の高い基準平面の形成領域が
小さくて済むことにより、加工も容易で製造コストを抑
えることができる。
As shown in FIG. 7B, the width (d1) of the reference plane 57 on the head side of the bolt 77 and the width (d2) of the reference plane 49 on the shaft side are coaxial with the bolt axis. Is present in a region (d1 = d2) equal to the position of (1), ultrasonic waves can be repeatedly reflected and reciprocally propagated in a region inside a cylindrical (for example, cylindrical) connecting these reference planes 57 and 49. Therefore, the reference plane necessary for the reflection of the ultrasonic wave can be minimized, and the formation area of the high-precision reference plane can be small, so that the processing is easy and the manufacturing cost can be suppressed.

【0024】図7(c)のように、ボルト78の軸部側
端面36を凹部の底面として形成することなく、軸部端
面を全体にわたって平面に形成して基準平面36とする
一方で、ボルト頭部側は前述のような凹部56を形成
し、その底面57を基準平面とすることもできる。この
場合、その底面57の広さd1はボルト軸部の断面dと
等しいかそれよりやや大きく形成することができる。こ
の場合、d1とdとの広さの比は、例えばd1=0.7d
〜1.3d、中でも0.9d〜1.1dとすることがで
きる。なお図14(a)のように両端に凹部56及び4
8を形成する場合、各基準平面の大きさの比率はd1=
0.5d2〜2d2、中でも0.7d2〜1.3d2、特に
0.8d2〜1.2d2程度とすることができ、d1=d2
にほぼ相当させたものが(b)に示す例である。
As shown in FIG. 7 (c), the shaft end surface 36 of the bolt 78 is not formed as the bottom surface of the concave portion, but the entire shaft end surface is formed as a flat surface to serve as the reference plane 36. The concave portion 56 as described above is formed on the head side, and the bottom surface 57 can be used as a reference plane. In this case, the width d1 of the bottom surface 57 can be formed equal to or slightly larger than the cross section d of the bolt shaft portion. In this case, the ratio of the width of d1 to d is, for example, d1 = 0.7d
1.3d, especially 0.9d to 1.1d. As shown in FIG. 14A, concave portions 56 and 4 are provided at both ends.
8, the ratio of the size of each reference plane is d1 =
0.5d2 to 2d2, especially 0.7d2 to 1.3d2, especially about 0.8d2 to 1.2d2, and d1 = d2
Is substantially equivalent to the example shown in FIG.

【0025】さらに、図7(d)に示すように、ボルト
頭部側の凹部56の底面57を可及的に大きくし、ボル
ト軸部側の凹部48の底面49も可及的に大きくするこ
とができる。これは言い換えれば凹部56の盛り上がり
部59や、凹部48の盛り上がり部50を可及的に最小
限にすることを意味する。この場合、超音波等の反射に
寄与する基準平面57、49を広くとることができる。
Further, as shown in FIG. 7D, the bottom surface 57 of the concave portion 56 on the bolt head side is made as large as possible, and the bottom surface 49 of the concave portion 48 on the bolt shaft side is made as large as possible. be able to. In other words, it means that the raised portion 59 of the concave portion 56 and the raised portion 50 of the concave portion 48 are minimized. In this case, the reference planes 57 and 49 that contribute to the reflection of ultrasonic waves and the like can be widened.

【0026】なお、凹部56の盛り上がり部59や、凹
部48の盛り上がり部50は、前述のように例えば両頭
研削盤等で除去して、図8(a)に示すように、ボルト
頭部側の端面に凹部をなくし、ほぼ全体にわたり平坦な
基準平面57とし、また軸部側についても凹部をなく
し、ほぼ全体が平坦な基準平面49とすることができ
る。このような後工程における盛り上がり部59、50
の研削等による除去を予定している場合は、図7(d)
のようにそれら盛り上がり部59、50を最小限にする
ことで、研削による切除量を少なくして、後工程での研
削等を簡単に行うことができる。なお、盛り上がり部5
9、50の切除とともに、鍛造加工、例えば冷間鍛造加
工(熱間鍛造、温間鍛造も採用可能)による基準平面5
7、49もわずかな研削代で研削して、最終的に表面粗
さや平面度等を整えることもできる。このようにする場
合でも、予め冷鍛加工により直角度等の精度の高い平面
が成形されているため、研削等によって一層面精度の高
い基準面とすることができる。
The raised portion 59 of the concave portion 56 and the raised portion 50 of the concave portion 48 are removed by, for example, a double-ended grinding machine as described above, and as shown in FIG. It is possible to form a reference plane 57 that is substantially flat throughout the entire surface by eliminating the concave portion on the end face, and eliminates the concave portion on the shaft portion side as well. Such raised portions 59 and 50 in the post-process.
7 (d) when removal by grinding or the like is planned.
By minimizing the raised portions 59 and 50 as described above, the amount of cutting by grinding can be reduced, and grinding and the like in a later step can be easily performed. In addition, the swelling part 5
The reference plane 5 formed by forging, for example, cold forging (hot forging and warm forging can also be adopted), together with the cuts 9 and 50.
7, 49 can also be ground with a slight grinding allowance to finally adjust the surface roughness, flatness and the like. Even in this case, since a plane with high accuracy such as a squareness is formed in advance by cold forging, a reference plane with higher surface accuracy can be obtained by grinding or the like.

【0027】また、図8(b)に示すように、そのよう
に盛り上がり部を除去した状態で、当初の冷鍛加工等に
よる基準平面57、49(あるいはその面に研削等によ
る仕上げを施した面)の、ボルト軸線を中心とする各広
さd1、d2についても、上述の凹部56、48で説明し
たように、それらd1とd2との比率を定めることができ
る。
Further, as shown in FIG. 8 (b), the reference planes 57 and 49 (or the surfaces thereof were finished by grinding or the like) by cold forging or the like in the state where the raised portions were removed as described above. As for the widths d1 and d2 of the surface) about the bolt axis, the ratio between d1 and d2 can be determined as described in the above-described recesses 56 and 48.

【0028】さらに前述のような冷鍛加工等による基準
平面を作る発想ではなく、従来と同様なラフなボルト頭
部端面及び軸部端面から、例えば研削等の仕上げ加工に
よりボルト頭部にd1の基準平面を、ボルト軸部にd2の
基準平面をそれぞれ形成することも可能である。
Further, instead of the idea of forming a reference plane by cold forging as described above, d1 is applied to the bolt head by finishing such as grinding from the rough end face of the bolt head and the end face of the shaft as in the prior art. It is also possible to form a d2 reference plane on the bolt shaft portion, respectively.

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

【図1】本発明の一実施例のボルトを示す正面図。FIG. 1 is a front view showing a bolt according to an embodiment of the present invention.

【図2】ボルトの端面の直角度を説明する図。FIG. 2 is a diagram illustrating a perpendicularity of an end face of a bolt.

【図3】ボルトの端面の幾何学的基準面に対する角度を
示す図。
FIG. 3 is a diagram illustrating an angle of an end face of a bolt with respect to a geometric reference plane.

【図4】ボルトの軸力を測定する例を示す図。FIG. 4 is a diagram illustrating an example of measuring an axial force of a bolt.

【図5】超音波の伝搬(反射)を概念的に示す図。FIG. 5 is a diagram conceptually showing propagation (reflection) of an ultrasonic wave.

【図6】超音波の伝搬(反射)を端面の直角度、平面度
及び表面粗さとの関係で概念的に示す図。
FIG. 6 is a diagram conceptually showing propagation (reflection) of an ultrasonic wave in relation to a squareness of an end face, flatness, and surface roughness.

【図7】この発明のボルトのいくつかの具体例を示す工
程図。
FIG. 7 is a process chart showing some specific examples of the bolt of the present invention.

【図8】図7のさらに別の例を簡略に示す図。FIG. 8 is a view schematically showing still another example of FIG. 7;

【符号の説明】[Explanation of symbols]

1 ボルト(おねじ部材) 4 端面(ボルト頭部の) 5 端面(ボルト軸部の) 1 bolt (male screw member) 4 end face (of bolt head) 5 end face (of bolt shaft)

Claims (8)

【特許請求の範囲】[Claims] 【請求項1】 おねじ部材の軸線に対する、おねじ部材
の両端部の各端面の直角度が0.0005〜0.1mm
とされたことを特徴とするおねじ部材。
1. The perpendicularity of each end face of both ends of the male screw member to the axis of the male screw member is 0.0005 to 0.1 mm.
A male screw member characterized by the above.
【請求項2】 おねじ部材の軸線に対する、おねじ部材
の両端部の各端面の直角度が0.0005〜0.1mm
とされ、かつ前記両端部の各端面の平面度が0.000
5〜0.1mmとされたことを特徴とするおねじ部材。
2. The perpendicularity of each end face of both ends of the male screw member to the axis of the male screw member is 0.0005 to 0.1 mm.
And the flatness of each end face of the both ends is 0.000
A male screw member having a thickness of 5 to 0.1 mm.
【請求項3】 おねじ部材の軸線に対する、おねじ部材
の両端部の各端面の直角度が0.0005〜0.1mm
とされ、かつ前記両端部の各端面の十点平均粗さRzが
1〜15とされたことを特徴とするおねじ部材。
3. The perpendicularity of each end face of both ends of the male screw member to the axis of the male screw member is 0.0005 to 0.1 mm.
And a ten-point average roughness Rz of each end face of the both end portions is set to 1 to 15.
【請求項4】 おねじ部材の軸線に対する、おねじ部
材の両端部の各端面の直角度が0.0005〜0.1m
mとされ、かつ前記両端部の各端面の平面度が0.00
05〜0.1mmとされ、さらに前記両端部の各端面の
十点平均粗さRzが1〜15とされたたことを特徴とす
るおねじ部材。
4. The perpendicularity of each end face of both ends of the male screw member to the axis of the male screw member is 0.0005 to 0.1 m.
m, and the flatness of each end face of the both ends is 0.00
A male screw member characterized in that the ten-point average roughness Rz of each end face of the both end portions is 1 to 15.
【請求項5】 おねじ部材の軸線に直角な仮想の軸直角
平面に対する、おねじ部材の両端部の各端面の実際角度
θについて、tanθが0.02以下とされたことを特
徴とするおねじ部材。
5. The tan θ is set to 0.02 or less with respect to an actual angle θ of each end face of both ends of the male screw member with respect to an imaginary plane perpendicular to an axis of the male screw member. Screw member.
【請求項6】 おねじ部材の軸線に直角な仮想の軸直角
平面に対する、おねじ部材の両端部の各端面の実際角度
θについて、tanθが0.02以下とされ、かつ前記
両端部の各端面の平面度が0.1mm以下とされたこと
を特徴とするおねじ部材。
6. An actual angle θ of each end face of both ends of the male screw member with respect to an imaginary plane perpendicular to the axis of the male screw member, tan θ is set to 0.02 or less, and A male screw member characterized in that the flatness of the end face is 0.1 mm or less.
【請求項7】 おねじ部材の軸線に直角な仮想の軸直角
平面に対する、おねじ部材の両端部の各端面の実際角度
θについて、tanθが0.02以下とされ、かつ前記
両端部の各端面の十点平均粗さRzが15以下とされた
ことを特徴とするおねじ部材。
7. An actual angle θ of each end face of both ends of the male screw member with respect to an imaginary axis perpendicular plane perpendicular to the axis of the male screw member, tan θ is set to 0.02 or less, and A male screw member having a ten-point average roughness Rz of 15 or less on an end face.
【請求項8】 おねじ部材の軸線に直角な仮想の軸直角
平面に対する、おねじ部材の両端部の各端面の実際角度
θについて、tanθが0.02以下とされ、かつ前記
両端部の各端面の平面度が0.1mm以下とされ、さら
に前記両端部の各端面の十点平均粗さRzが15以下と
されたことを特徴とするおねじ部材。
8. An actual angle θ of each end face of both ends of the male screw member with respect to an imaginary axis perpendicular to the axis of the male screw member, tan θ is set to 0.02 or less, and each of the both ends is A male screw member, wherein the flatness of the end face is 0.1 mm or less, and the ten-point average roughness Rz of each end face of the both ends is 15 or less.
JP2000007149A 2000-01-14 2000-01-14 Male screw member Pending JP2001200826A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP2000007149A JP2001200826A (en) 2000-01-14 2000-01-14 Male screw member

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP2000007149A JP2001200826A (en) 2000-01-14 2000-01-14 Male screw member

Publications (1)

Publication Number Publication Date
JP2001200826A true JP2001200826A (en) 2001-07-27

Family

ID=18535572

Family Applications (1)

Application Number Title Priority Date Filing Date
JP2000007149A Pending JP2001200826A (en) 2000-01-14 2000-01-14 Male screw member

Country Status (1)

Country Link
JP (1) JP2001200826A (en)

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2005279920A (en) * 2004-03-02 2005-10-13 Sannohashi Corp Axial force detecting fastening tool, bolt, and method of manufacturing the bolt
JP2010071392A (en) * 2008-09-18 2010-04-02 Sannohashi Corp Method of manufacturing bolt and bolt
JP2011230226A (en) * 2010-04-27 2011-11-17 Hino Motors Ltd Control device of fastening force of hydraulic torque wrench
WO2017082325A1 (en) * 2015-11-12 2017-05-18 日本精工株式会社 Steering device and assembling method for steering device

Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2005279920A (en) * 2004-03-02 2005-10-13 Sannohashi Corp Axial force detecting fastening tool, bolt, and method of manufacturing the bolt
JP4524197B2 (en) * 2004-03-02 2010-08-11 株式会社サンノハシ Axial force detection fastening tool, bolt, bolt manufacturing method
JP2010071392A (en) * 2008-09-18 2010-04-02 Sannohashi Corp Method of manufacturing bolt and bolt
JP2011230226A (en) * 2010-04-27 2011-11-17 Hino Motors Ltd Control device of fastening force of hydraulic torque wrench
WO2017082325A1 (en) * 2015-11-12 2017-05-18 日本精工株式会社 Steering device and assembling method for steering device

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