Deprecated: The each() function is deprecated. This message will be suppressed on further calls in /home/zhenxiangba/zhenxiangba.com/public_html/phproxy-improved-master/index.php on line 456
JPS6054615B2 - Bolt axial force measurement method - Google Patents
[go: Go Back, main page]

JPS6054615B2 - Bolt axial force measurement method - Google Patents

Bolt axial force measurement method

Info

Publication number
JPS6054615B2
JPS6054615B2 JP7550880A JP7550880A JPS6054615B2 JP S6054615 B2 JPS6054615 B2 JP S6054615B2 JP 7550880 A JP7550880 A JP 7550880A JP 7550880 A JP7550880 A JP 7550880A JP S6054615 B2 JPS6054615 B2 JP S6054615B2
Authority
JP
Japan
Prior art keywords
bolt
axial force
iron loss
measured
magnetic sensor
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
JP7550880A
Other languages
Japanese (ja)
Other versions
JPS571942A (en
Inventor
忠正 中村
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.)
Shibaura Mechatronics Corp
Original Assignee
Shibaura Engineering Works 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 Shibaura Engineering Works Co Ltd filed Critical Shibaura Engineering Works Co Ltd
Priority to JP7550880A priority Critical patent/JPS6054615B2/en
Publication of JPS571942A publication Critical patent/JPS571942A/en
Publication of JPS6054615B2 publication Critical patent/JPS6054615B2/en
Expired legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01LMEASURING FORCE, STRESS, TORQUE, WORK, MECHANICAL POWER, MECHANICAL EFFICIENCY, OR FLUID PRESSURE
    • G01L5/00Apparatus for, or methods of, measuring force, work, mechanical power, or torque, specially adapted for specific purposes
    • G01L5/24Apparatus for, or methods of, measuring force, work, mechanical power, or torque, specially adapted for specific purposes for determining value of torque or twisting moment for tightening a nut or other member which is similarly stressed

Landscapes

  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Force Measurement Appropriate To Specific Purposes (AREA)

Description

【発明の詳細な説明】 本発明は、磁性材料で作られたボルトの軸力を磁気的
方法によつて測定するボルト軸力測定方法に関するもの
である。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a bolt axial force measuring method for measuring the axial force of a bolt made of a magnetic material by a magnetic method.

一般に、ボルト・ナットで締結された組立構造物にお
いて、特にその組立構造物が動的荷重を受ける場合には
、ボルトの疲労破断を防止するために、適正なボルト軸
力の管理が必要である。
In general, in assembled structures fastened with bolts and nuts, appropriate management of bolt axial force is necessary to prevent bolt fatigue failure, especially when the assembled structure is subjected to dynamic loads. .

通常は、ボルト軸力は、トルク法により、ボルト締付け
時の締付トルクによつて管理されている。しかし、この
トルク法は、ボルト・ナットのねじ面や、ボルト・ナッ
トと被締結物の接触面の摩擦係数のばらつきが大きいた
め、ボルト軸力を所定値に管理することは困難で、ボル
トの軸力に大きなばらつきが生ずるという欠点があつた
。従つて、最近では、磁性材料の鉄損と、極性材料に作
用する引張応力及び圧縮応力の間には、第1図に示すよ
うな密度な関係があることを利用して、磁性材料で作ら
れたボルトの鉄損を測定して、その測定たれた鉄損から
前記ボルトに作用している軸力を測定する磁気的方法が
用いられている。 第1図は、横軸に引張応力及び圧縮
応力を、縦軸に鉄損を取り、磁性材料に作用する応力と
鉄損の関係を示したものである。
Normally, the bolt axial force is controlled by the tightening torque when tightening the bolt using the torque method. However, with this torque method, it is difficult to control the bolt axial force to a predetermined value due to large variations in the coefficient of friction between the threaded surface of the bolt/nut and the contact surface between the bolt/nut and the fastened object. The drawback was that there was a large variation in the axial force. Therefore, in recent years, magnetic materials have been developed by taking advantage of the density relationship shown in Figure 1 between the iron loss of magnetic materials and the tensile stress and compressive stress acting on polar materials. A magnetic method is used in which the iron loss of the bolt is measured and the axial force acting on the bolt is measured from the measured iron loss. FIG. 1 shows the relationship between stress acting on a magnetic material and iron loss, with tensile stress and compressive stress on the horizontal axis and iron loss on the vertical axis.

第1図から明らかなように、磁性材料に圧縮応力が作用
する時は、圧縮応力と鉄損はほぼ直線関係にあるので、
この関係を利用して、鉄損を測定すれば、高い精度で磁
性材料に作用している圧縮応力を求めることができる。
一般に、ボルトを締付けると、ボルト軸部には長手方
向にボルト軸力に対応する引張応力が、ボルト頭部表層
部にはボルト軸力に対応する圧縮応力が作用する。
As is clear from Figure 1, when compressive stress acts on a magnetic material, there is a nearly linear relationship between compressive stress and iron loss, so
By measuring the iron loss using this relationship, the compressive stress acting on the magnetic material can be determined with high accuracy.
Generally, when a bolt is tightened, a tensile stress corresponding to the bolt axial force acts on the bolt shaft in the longitudinal direction, and a compressive stress corresponding to the bolt axial force acts on the surface layer of the bolt head.

従つて、ボルトの頭部表層部の鉄損を測定して、そのボ
ルトに作用する軸力を、高い精度で求めることができる
。 通常、上述の関係を用いて、励磁材料で作られたボ
ルトの鉄損を測定するには、第2図に示すよ’うに、組
立構造物1、1’を締結しているボルト2及びナット3
の内、ボルト2の頭部上面に磁気センサ4を当接させて
鉄損を測定し、その測定した鉄損を軸力変換器(図示せ
す)に入力し、鉄損を軸力に変換して、ボルト2の軸力
を測定する。
Therefore, by measuring the iron loss in the surface layer of the head of the bolt, the axial force acting on the bolt can be determined with high accuracy. Normally, in order to measure the iron loss of a bolt made of an excitation material using the above-mentioned relationship, the bolt 2 and the nut that fasten the assembled structures 1, 1' are used as shown in Figure 2. 3
Among them, the magnetic sensor 4 is brought into contact with the top surface of the head of the bolt 2 to measure the iron loss, and the measured iron loss is input to an axial force converter (shown in the figure) to convert the iron loss to axial force. Then, measure the axial force of bolt 2.

磁気センサ4は、断面コの字形の鉄心5に一次コイル(
励磁コイル)6及び二次コイル(出カニ次電圧コイル)
7を巻いて構成され、一次コイル6の口出線8を外部電
源(図示せず)に、二次コイル7の口出線9を制御装置
(図示せす)に接続し、一次コイル6を交流励磁すると
、鉄心5からの磁束はボルト2の頭部表層部を矢印の方
向に流れ、再び鉄心5に戻る閉磁路を形成する。この場
合、二次コイル7に誘起される出カニ次電圧を、予め設
定された設定電圧に等しくなるように、一次コイル6の
励磁電流を制御し、ボルト2の頭部表層部を流れる磁束
を一定になるようにして、一次コイル6の励磁電流と、
二次コイル7の出カニ次電圧を鉄損測定器(図示せず)
に入力すれば、ボルト2の頭部表層部の鉄損を測定する
ことができる。この測定された鉄損をWilボルト2に
圧縮応力の作用していない時の鉄損をWOとすると、第
1図の関係から、ボルト2に作用する圧縮応力は(W1
−WO)に比例し、これに常数αを乗じた次式から、ボ
ルト2に作用するボルト軸力を求めることができる。こ
こに、定数αは磁束量、ボルトの種類、磁気センサの種
類等により決まるものである。
The magnetic sensor 4 includes a primary coil (
Excitation coil) 6 and secondary coil (output secondary voltage coil)
The lead wire 8 of the primary coil 6 is connected to an external power source (not shown), and the lead wire 9 of the secondary coil 7 is connected to a control device (not shown). When excited with alternating current, the magnetic flux from the iron core 5 flows through the head surface of the bolt 2 in the direction of the arrow, forming a closed magnetic path that returns to the iron core 5 again. In this case, the excitation current of the primary coil 6 is controlled so that the output voltage induced in the secondary coil 7 is equal to a preset voltage, and the magnetic flux flowing through the surface layer of the head of the bolt 2 is controlled. The excitation current of the primary coil 6 is kept constant, and
Measure the output voltage of the secondary coil 7 with an iron loss measuring device (not shown).
By inputting , it is possible to measure the iron loss at the surface layer of the head of the bolt 2. Letting this measured iron loss be Wil and the iron loss when no compressive stress is acting on the bolt 2 as WO, then from the relationship shown in Figure 1, the compressive stress acting on the bolt 2 is (W1
-WO), and the bolt axial force acting on the bolt 2 can be determined from the following equation, which is multiplied by a constant α. Here, the constant α is determined by the amount of magnetic flux, the type of bolt, the type of magnetic sensor, etc.

しかし、この場合、鉄損WOは、ボルトの材質一の成分
、ボルト頭部表層部の加工歪みによる残留応力等の影響
を受けて、ばらつきを生ずるので、(1)式を用いて鉄
損Wiと同一ロツトのボルトの代表のWOから測定した
ボルト軸力には、ばらつきを生ずるという欠点がある。
However, in this case, the iron loss WO varies due to the influence of the component of the bolt material, residual stress due to machining strain on the surface layer of the bolt head, etc., so the iron loss Wi The bolt axial force measured from a representative WO of bolts from the same lot has a drawback of causing variations.

本発明は、上記の欠点を除去するためになされたもので
、異なる2つの励磁周波数で、それぞれ同一ボルトの鉄
損を測定し、その測定された2つの鉄損の差を取り、各
鉄損のばらつきを除去し、前記ボルトに作用する軸力を
求め、ばらつきの小!さいボルト軸力を測定するボルト
軸力測定方法を提供するものである。次に、本発明のボ
ルト軸力測定法について詳細に説明する。
The present invention was made to eliminate the above-mentioned drawbacks.The present invention measures the iron loss of the same bolt at two different excitation frequencies, takes the difference between the two measured iron losses, and calculates each iron loss. , and find the axial force acting on the bolt to find the small variation! The present invention provides a bolt axial force measurement method for measuring small bolt axial force. Next, the bolt axial force measurement method of the present invention will be explained in detail.

一般に、磁気センサをボルトの頭部上面に当接3させ、
磁気センサの一次コイルを、ある励磁周波数で励磁して
、鉄損を測定する場合、ボルトの鉄損は、励磁周波数の
ほぼ1.5乗に比例して増加するので、励磁周波数の高
いほど鉄損の測定精度は良くなり、ボルトの頭部上面の
磁束浸透深さは励1磁周波数の0.5乗に反比例し、励
磁周波数が高いほど、表層効果によつてボルトの頭部表
層部に移行する。
Generally, a magnetic sensor is brought into contact with the top surface of the bolt head,
When measuring iron loss by exciting the primary coil of a magnetic sensor at a certain excitation frequency, the iron loss of the bolt increases approximately in proportion to the 1.5th power of the excitation frequency, so the higher the excitation frequency, the higher the iron loss. The measurement accuracy of loss improves, and the depth of magnetic flux penetration into the upper surface of the bolt head is inversely proportional to the excitation frequency to the 0.5th power. Transition.

また、ボルトの頭部表層部の圧縮応力は、適当な深さの
圧縮応力より大きくなる。以上の関係により、磁束が適
当な深さのボルトの表層部を流れるように2つの励磁周
波数Fl,f2を決定する。例えば、f1=200Hz
,.f2=50Hzとすればよい。第3図は、横軸に軸
力を、縦軸に鉄損を取り、ボルトの頭部上面に磁気セン
サを当接させ、磁気センサの一次コイルを励磁周波数が
f1及びF2(f1〉F2)で励磁した時の、軸力と鉄
損の関係を示したものである。
Further, the compressive stress at the surface layer of the bolt head is greater than the compressive stress at an appropriate depth. Based on the above relationship, the two excitation frequencies Fl and f2 are determined so that the magnetic flux flows through the surface layer of the bolt at an appropriate depth. For example, f1=200Hz
、. It is sufficient to set f2=50Hz. Figure 3 shows the axial force on the horizontal axis and the iron loss on the vertical axis. A magnetic sensor is brought into contact with the upper surface of the bolt head, and the primary coil of the magnetic sensor is excited at frequencies f1 and F2 (f1>F2). This shows the relationship between axial force and iron loss when excited at .

直線10は励磁周波数がf1の時の直線11は励磁周波
数がF2の時の、ボルト軸力と鉄損の関係をそれぞれ示
したものである。なお、直線10,11を挟んで上下に
描かれた点線は、直線10,11上の点のばらつきの範
囲を示すものである。いま、励磁周波数がf1で、ボル
ト軸力が0の時の鉄損をWOlボルト軸力がNの時の鉄
損をWiとし、また励磁周波数がF2で、ボルト軸力が
0の時の鉄損をWO″、ボルト軸力がNの時の鉄損をW
i″とすると、(1)式よりとなる。
Straight line 10 shows the relationship between bolt axial force and iron loss when the excitation frequency is f1, and straight line 11 shows the relationship between bolt axial force and iron loss when the excitation frequency is F2. Note that the dotted lines drawn above and below the straight lines 10 and 11 indicate the range of variations in points on the straight lines 10 and 11. Now, the iron loss when the excitation frequency is f1 and the bolt axial force is 0 is WO, the iron loss when the bolt axial force is N is Wi, and the iron loss when the excitation frequency is F2 and the bolt axial force is 0. The loss is WO'', and the iron loss when the bolt axial force is N is W
When i'', the equation (1) is obtained.

又、WOとWO″の関係を とし、(2),(3),(4)式よりWO,WO″を消
去すると、となる。
Also, if we take the relationship between WO and WO'' and eliminate WO and WO'' from equations (2), (3), and (4), we get the following.

ここに、α″=ータ35−である。また、
α−αβα,α″はそれぞれWO,WO″,Wi
,Wi″の平均値から求め、β,γは(4)式からWO
,WO″の回帰係数として求めればよい。
Here, α″=ta35−. Also,
α−αβα, α″ are WO, WO″, Wi
, Wi'', and β and γ are calculated from equation (4) as WO
, WO''.

(5)式より、WO,WO″に関係なく軸力Nを測定す
ることができる。
From equation (5), the axial force N can be measured regardless of WO and WO''.

即ち、予め締付けるべきボルトと同一材質及び同一形状
の複数個のボルトについて、そのボルトの頭部上面に磁
気センサを当接させて、磁気センサの一次コイルの励磁
周波数Fl,f2の時の鉄損WO,WO″,Wi,Wi
″を測定してその平均値からα,α″を求め、(4)式
からWO,WO″の回帰係数としてβ,γを求めておく
That is, for a plurality of bolts made of the same material and the same shape as the bolts to be tightened in advance, a magnetic sensor is brought into contact with the upper surface of the head of the bolt, and the iron loss at the excitation frequencies Fl and f2 of the primary coil of the magnetic sensor is measured. WO, WO'', Wi, Wi
'' is measured and α and α'' are determined from the average value, and β and γ are determined as regression coefficients of WO and WO'' from equation (4).

次いで、前記ボルトを締付けながら、ボルト頭部上面に
当接させた磁気センサの一次コイルを励磁周波数Fl,
f2で励磁し、鉄損Wi,Wi″をそれぞれ測定し、常
数α,α″,βからα″を求め、これ等の値を軸力換算
器に入力すれは、(5)式から軸力Nを測定することが
できる。
Next, while tightening the bolt, the primary coil of the magnetic sensor that is in contact with the upper surface of the bolt head is set to an excitation frequency Fl,
Excite with f2, measure the iron losses Wi and Wi'', calculate α'' from the constants α, α'', and β, and input these values into the axial force converter. N can be measured.

第3図の直線12はβWl″を、直線13はβWi″+
γを、直線14は(Wi−βWi−γ)を示すものであ
る。直線10,11,12,13を挾んで上下に描かれ
た点線は、直線12上の点のばらつきの範囲を示すもの
である。以上のように、本発明のボルト軸力測定方法に
よれば、異なる2つの励磁周波数を用いて、ボルトの頭
部上面に当接させた磁気センサの一次コイルを励磁して
、各励磁周波数に対する鉄損を求め、それ等の鉄損の差
より前述ボルトに作用している軸力を求めるので、各励
磁周波数に対する鉄損のばらつきを除去でき、ボルト軸
力測定に直接、ボルトの軸力がOの時のばらつきのある
鉄損を用いないので、ばらつきの少ないボルトの軸力を
測定することができる。
The straight line 12 in FIG. 3 represents βWl″, and the straight line 13 represents βWi″+
γ, and the straight line 14 represents (Wi−βWi−γ). Dotted lines drawn above and below the straight lines 10, 11, 12, and 13 indicate the range of dispersion of points on the straight line 12. As described above, according to the bolt axial force measurement method of the present invention, the primary coil of the magnetic sensor that is in contact with the top surface of the bolt head is excited using two different excitation frequencies, and the Since the iron loss is determined and the axial force acting on the bolt is determined from the difference between these iron losses, the variation in iron loss for each excitation frequency can be removed, and the axial force of the bolt can be directly measured when measuring the bolt axial force. Since the iron loss which varies when O is not used, it is possible to measure the axial force of the bolt with little variation.

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

第1図は磁性材料の応力と鉄損の関係を表わす特性曲線
図、第2図は磁気センサをボルトの頭部上面に当接させ
て、鉄損を測定する説明図、第3図は、異なる2つの励
磁周波数により測定した鉄損とボルト軸力の関係を表わ
す特性曲線図である。 1,1″・・・・・・組立構造物、2・・・・・・ボル
ト、3・・・・・・ナット、4・・・・・・磁気センサ
、5・・・・・・鉄心、6・・・・・・一次コイル、7
・・・・・・二次コイル、8,9・・・・・・口出線。
Fig. 1 is a characteristic curve diagram showing the relationship between stress and iron loss of a magnetic material, Fig. 2 is an explanatory diagram of measuring iron loss by bringing a magnetic sensor into contact with the top surface of a bolt head, and Fig. 3 is a diagram showing the relationship between stress and iron loss of magnetic materials. It is a characteristic curve diagram showing the relationship between iron loss and bolt axial force measured at two different excitation frequencies. 1,1″...Assembly structure, 2...Bolt, 3...Nut, 4...Magnetic sensor, 5...Iron core , 6...Primary coil, 7
...Secondary coil, 8,9...Output wire.

Claims (1)

【特許請求の範囲】[Claims] 1 磁性材料で作られたボルトの頭部上面に磁気センサ
を当接させて、前記ボルトの鉄損を測定し、その測定し
た鉄損から前記ボルトに作用している軸力を測定するボ
ルト軸力測定方法において、少なくとも2つの異なる励
磁周波数を用いて前記磁気センサを励磁して、前記各励
磁周波数に対する前記ボルトの鉄損を測定し、この測定
された2つの鉄損値の差から前記ボルトに作用している
軸力を測定することを特徴とするボルト軸力測定方法。
1. A bolt shaft that measures the iron loss of the bolt by placing a magnetic sensor in contact with the top surface of the head of a bolt made of magnetic material, and measures the axial force acting on the bolt from the measured iron loss. In the force measurement method, the magnetic sensor is excited using at least two different excitation frequencies, the iron loss of the bolt is measured for each of the excitation frequencies, and the difference between the two measured iron loss values is used to determine the iron loss of the bolt. A bolt axial force measuring method characterized by measuring the axial force acting on the bolt.
JP7550880A 1980-06-06 1980-06-06 Bolt axial force measurement method Expired JPS6054615B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP7550880A JPS6054615B2 (en) 1980-06-06 1980-06-06 Bolt axial force measurement method

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP7550880A JPS6054615B2 (en) 1980-06-06 1980-06-06 Bolt axial force measurement method

Publications (2)

Publication Number Publication Date
JPS571942A JPS571942A (en) 1982-01-07
JPS6054615B2 true JPS6054615B2 (en) 1985-11-30

Family

ID=13578244

Family Applications (1)

Application Number Title Priority Date Filing Date
JP7550880A Expired JPS6054615B2 (en) 1980-06-06 1980-06-06 Bolt axial force measurement method

Country Status (1)

Country Link
JP (1) JPS6054615B2 (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS63155810U (en) * 1987-04-01 1988-10-13

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5280725A (en) * 1989-09-05 1994-01-25 Wolfgang Stengel Process and device for non-destructive determination of the prestressing condition of ferromagnetic securing elements
JP4948968B2 (en) * 2006-10-27 2012-06-06 Ntn株式会社 Planetary roller type transmission

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS63155810U (en) * 1987-04-01 1988-10-13

Also Published As

Publication number Publication date
JPS571942A (en) 1982-01-07

Similar Documents

Publication Publication Date Title
US2421222A (en) Multirange load measuring apparatus
US2276843A (en) Pressure measuring apparatus
Kleinke et al. A magnetostrictive force sensor
CN108489641B (en) Stress measuring device and method for prestressed steel strand
EP0007963A1 (en) Method and device for measuring or detecting a mechanical change of state or its time derivative
US7146866B2 (en) Magnetostrictive strain sensor and method
JPS6054615B2 (en) Bolt axial force measurement method
GB2210460A (en) Magnetostrictive stress measurement apparatus
JP6352321B2 (en) Non-contact stress measuring method and measuring apparatus by composite resonance method
US3019640A (en) Method of and means for measuring torque of an electric motor drive
JPS6155057B2 (en)
Milnes Magnetic amplifiers
JPS5943323A (en) Torque detecting apparatus
US4474069A (en) Magnetoelastic transducer
JPH0424670B2 (en)
JPH0318137B2 (en)
JPS5839920A (en) Controlling method for bolt axial force utilizing magnetism
JPS5619423A (en) Bolt axial force detector
Kalinin et al. Determining specific power loss in joint area of laminated magnetic core
SU1384972A1 (en) Magnetoelastic torque generator
JP3173365B2 (en) Stress measurement method using magnetostriction effect
JPH0310055B2 (en)
SU1296251A2 (en) Force transducer of rolling
SU938022A1 (en) Device for measuring dynamic parameters of rotating objects
Lloyd et al. The testing of transformer steel