JPS6338109A - Milling surface direction measuring instrument - Google Patents

Milling surface direction measuring instrument

Info

Publication number
JPS6338109A
JPS6338109A JP18150186A JP18150186A JPS6338109A JP S6338109 A JPS6338109 A JP S6338109A JP 18150186 A JP18150186 A JP 18150186A JP 18150186 A JP18150186 A JP 18150186A JP S6338109 A JPS6338109 A JP S6338109A
Authority
JP
Japan
Prior art keywords
angle
measured
shaft
measuring
distance
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
Application number
JP18150186A
Other languages
Japanese (ja)
Other versions
JPH0613967B2 (en
Inventor
Masaji Tamura
田村 正次
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.)
Proterial Ltd
Original Assignee
Hitachi Metals 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 Hitachi Metals Ltd filed Critical Hitachi Metals Ltd
Priority to JP61181501A priority Critical patent/JPH0613967B2/en
Publication of JPS6338109A publication Critical patent/JPS6338109A/en
Publication of JPH0613967B2 publication Critical patent/JPH0613967B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

Links

Abstract

PURPOSE:To enable automatic measuring operation by utilizing a microcomputer and to take a measurement in a short time by rotating a body to be measured and measuring its angle position. CONSTITUTION:This instrument consists of an encoder 1 which measures the angle, a motor 2 which rotates a magnet roll 3, a magnet roll 3 as the body to be measured, a Hall element 4 which measures magnetic force, a distance sensor 5, a slide jig 6 for distance value conversion, a milling surface 7 for the body to be measured, and a shaft 8. Then while the magnetic roll 3 is rotated and the angle position is measured, the position of the milling surface 7 and the distance from one external point to the shaft 8 are measured as well as a magnetic force value and outputted to a one-round X-Y recorder, thereby obtaining the result as shown in graphs. The angle thetaf where the distance is maximum is read in the graphs and the angle thetag where the magnetic force is maximum is read, so that the angle theta of magnetization is found as the difference between thetaf and thetag.

Description

【発明の詳細な説明】 (産業上の利用分野) 本発明は表面に複数個のfd所を有するマグト、・トロ
ールの着磁位置等を測定する装置に関するものである。
DETAILED DESCRIPTION OF THE INVENTION (Field of Industrial Application) The present invention relates to a device for measuring the magnetized position of a magnet or troll having a plurality of fd points on its surface.

(従来の技術) 電子写真装置において磁性現像剤の搬送手段として表面
に複数個の磁極を有するマグネットロールが広く使用さ
れている。このマグネットロールは例えばシャフトに円
筒状磁石を固着し、所定の着磁を施したものであり、そ
のままもしくは円筒状の非磁性スリーブを被せて使用さ
れる。
(Prior Art) Magnet rolls having a plurality of magnetic poles on the surface are widely used as means for conveying magnetic developer in electrophotographic apparatuses. This magnet roll is made by, for example, fixing a cylindrical magnet to a shaft and subjecting it to a predetermined magnetization, and is used as it is or by covering it with a cylindrical non-magnetic sleeve.

従来のマグネットロールの着磁位置を測定する装置とし
ては、第6図に示す様にフライスカット而7を持つシャ
フト8と相似な形状を有する入れ込み弐治具11を使用
していた。
A conventional device for measuring the magnetized position of a magnet roll uses a two-insertion jig 11 having a similar shape to a shaft 8 having a milling cut 7, as shown in FIG.

この装置をフライス面の有る側からシャフト8を治具1
1に挿入すると、針9が磁力によって吸引され、磁極の
方向を指すのでこの方向を治具上の目盛10で読み取り
着磁角度としていた。
Insert the shaft 8 into the jig 1 from the side with the milling surface.
1, the needle 9 is attracted by magnetic force and points in the direction of the magnetic pole, so this direction is read on the scale 10 on the jig and used as the magnetization angle.

(発明が解決しようとする問題点) しかしながら上記従来の測定装置には次の様な問題点が
ある。
(Problems to be Solved by the Invention) However, the conventional measuring device described above has the following problems.

(1)  第7図が入れ込み治具11にシャフト8を挿
入した状態を正面から見た図である。弦ABを持つ半径
r0のシャフトと弦A’B’を待つ半径rやの治具がA
点において接する時2つの弦の角度を求めると、弦A’
B’の垂直二等分線は中心0を通るので、 zB ’ AB=ZM’ OM=θ。−θ8となる。
(1) FIG. 7 is a front view of the shaft 8 inserted into the insertion jig 11. A shaft with radius r0 holding string AB and a jig with radius r waiting for string A'B' are A.
If we find the angle between two strings when they touch at a point, we get string A'
Since the perpendicular bisector of B' passes through the center 0, zB'AB=ZM' OM=θ. -θ8.

ここで、シャフト及びフライス深さとして、例え ば 
r  o  = 2. 5 1璽 、   I  M 
 Ol   =  1. 7  mm 、   1M’
ol= 1.8 tmを代入すると次のようになる。
Here, as the shaft and milling depth, e.g.
r o = 2. 5 1st Seal, I M
Ol=1. 7mm, 1M'
Substituting ol=1.8 tm gives the following.

θ。= CO3−’ (1,7/2.5) =47.1
5゜θ、= CO3−’ (1,8/2.5) =43
.94゜;、ZB’AB=θ。−θつ=3.21゜以上
の結果から直径5顛フライス深さ0.8fiのシャフト
は0.1 mの公差を持つ治具の中で中心を固定したと
しても±3.2度回転出来ることがわかる。
θ. = CO3-' (1,7/2.5) =47.1
5゜θ, = CO3-' (1,8/2.5) =43
.. 94°;, ZB'AB=θ. From the results of -θ = 3.21° or more, a shaft with a diameter of 5 mm and a milling depth of 0.8 fi can be rotated by ±3.2 degrees even if the center is fixed in a jig with a tolerance of 0.1 m. I understand that.

測定対象のマグロールの着磁位置の許容公差は、−aに
±3度であるので平坦部を平行にする機構(止めネジ1
2)がなければこの方法による測定は無意味である。
The permissible tolerance of the magnetized position of the mag roll to be measured is ±3 degrees to -a, so a mechanism to make the flat part parallel (set screw 1
Without 2), measurement using this method is meaningless.

(2)  シャフトと相似な治具である為アイテム毎の
治具を作り、段取り替えを行わなければならない。
(2) Since the jig is similar to the shaft, it is necessary to create a jig for each item and change the setup.

(3)測定の方法が結果を電気出力としていない為自動
化、定量化が難かしい。
(3) Automation and quantification are difficult because the measurement method does not convert the results into electrical output.

したがって本発明の目的は、上記問題点を解消したフラ
イス面方向測定装置を提供することである。
SUMMARY OF THE INVENTION Accordingly, an object of the present invention is to provide a milling face orientation measuring device that eliminates the above-mentioned problems.

(問題点を解決するための手段) 本発明の測定装置は、円筒状シャフトの一部を平坦にカ
ントした面の方向を基準にして別の測定可能な物理量の
角度位置を測定する装置であって、被測定物を回転させ
る手段と角度位置を測定する手段と角度位置を測定する
物理量を測定する手段とシャフトの平坦部の有る位置を
外部の一点からシャフト表面までの距離を測定する手段
と、シャフト表面までの距離を基準位置からの角度の関
数変換をおこなう手段と、測定値を記憶する手段からな
ることを特徴とする。
(Means for Solving the Problems) The measuring device of the present invention is a device that measures the angular position of another measurable physical quantity with reference to the direction of a flat canted surface of a part of a cylindrical shaft. a means for rotating the object to be measured; a means for measuring the angular position; a means for measuring a physical quantity for measuring the angular position; and a means for measuring the distance from a point on the outside of the shaft to the surface of the shaft. , comprising means for converting the distance to the shaft surface into a function of the angle from the reference position, and means for storing the measured value.

(実施例) 以下本発明の詳細を図面により説明する。(Example) The details of the present invention will be explained below with reference to the drawings.

第1図は本発明の一実施例を示す斜視図である。FIG. 1 is a perspective view showing an embodiment of the present invention.

マグネットロール3は、エンコーダー側でチャックされ
、Aの方向からセンターで押されて、一定の中心を保持
して回転する機構となっている。
The magnet roll 3 is chucked on the encoder side, is pushed at the center from the direction of A, and has a mechanism to rotate while holding a constant center.

装置の構成は角度を測定するエンコーダー1とマクネッ
トロール3を回転させるモーター2と被測定物であるマ
グネットロール3と磁力を測定するホール素子4と距離
センサー5と距離値変換用のスライド治具6及び被測定
物のフライス面7とシャフト8からなっている。
The device consists of an encoder 1 that measures angles, a motor 2 that rotates a magnetic roll 3, a magnet roll 3 that is an object to be measured, a Hall element 4 that measures magnetic force, a distance sensor 5, and a slide jig for distance value conversion. 6, a milled surface 7 of the object to be measured, and a shaft 8.

この装置によれば次のようにして測定が行なわれる。マ
グネットロール3を回転し角度位置を測定しながらフラ
イス面の有る位置を外部の一点からシャフト表面までの
距離を測定し、同時に磁力値を測定して一周分X−Yレ
コーダに出力すると第2図の様になる。
According to this device, measurements are performed as follows. While rotating the magnet roll 3 and measuring the angular position, the distance from a point on the outside of the milling surface to the shaft surface is measured, and at the same time the magnetic force value is measured and outputted to the X-Y recorder for one revolution, as shown in Figure 2. It will look like this.

この図より距離の最大値となる角θ、を読み取り、磁力
の最大値となる角θ9を読み取ると着磁角度eはθ、と
θ9の差として求められる。
From this figure, by reading the angle θ, which is the maximum value of the distance, and reading the angle θ9, which is the maximum value of the magnetic force, the magnetization angle e can be determined as the difference between θ and θ9.

上記データ処理は第3図の様にシーケンサ−による動作
制御、マイコンによる測定及び処理によって自動的にパ
ソコンによって、第1表の様に出力する事が可能である
The above data processing can be automatically outputted by a personal computer as shown in Table 1 through operation control by a sequencer and measurement and processing by a microcomputer as shown in FIG.

第1表の内angleと表示されている行が上記の着磁
角である。尚921dとは92.1度の意味である。
In Table 1, the row labeled angle is the above magnetization angle. Note that 921d means 92.1 degrees.

第  1  表 Reading Run 0K (angle)d=degX1/10po1  
909G 920G 899G 876Gpeak  
 910G 921G 899G B76Gmaxfl
t   OG 935G  OG  OGminflt
   OG 898G  OG  0Grflat  
 OG  37G  OG  0Gdiffer   
OG  13G  OG  OGwidth   Od
  Od  Od  Odangle   921d 
1004d 1918d 2718dinterv  
1o04d 914d 799d 882dhalf 
         Od     Od     Od
     OdReading  Run NG  *is  NG  mark pol         926G    930G 
   8970   882Gpeak       
 926G    930G    900G    
882Gmaxflt        OG    9
36G     OG     OGminflt  
      OG    890G     OG  
   0Grflat        OG    4
6G     OG     0Gdiffer   
     OG    16G     OG    
 OGwidth         Od     O
d     Od     Odangle     
     932本   1004d    1926
cl    2725dinterv      10
04d    921d    799d    87
4dhalf          Od     Od
     Od     OdReading  Ru
n 0K  (angle)d=degX1/10po1 
       909G    941G    92
0G    876Gpeak        909
G    941G    920G    877G
max目t        OG    973G  
   OG     0cm1nflt       
 OG    896G     OG     0G
rflat        OG    77G   
  OG     0Gdiffer      OG
    19G    OG    OGwidth 
      Od    Od    Od    O
dangle      910d  1000d  
1915d  2710dinterv     10
00cl   914d   795d   889d
half       Od    Od    Od
    Od本発明では、第1図におけるスライド治具
6は無くとも着磁角度は測定可能である。
Table 1 Reading Run 0K (angle) d=degX1/10po1
909G 920G 899G 876Gpeak
910G 921G 899G B76Gmaxfl
t OG 935G OG OG minflt
OG 898G OG 0Grflat
OG 37G OG 0G differ
OG 13G OG OGwidth Od
Od Od Odangle 921d
1004d 1918d 2718dinterv
1o04d 914d 799d 882dhalf
Od Od Od
OdReading Run NG *is NG mark pol 926G 930G
8970 882Gpeak
926G 930G 900G
882Gmaxflt OG 9
36G OG OG minflt
OG 890G OG
0Grflat OG 4
6G OG 0G different
OG 16G OG
OG width Od O
d Od Odangle
932 pieces 1004d 1926
cl 2725dinterv 10
04d 921d 799d 87
4dhalf Od Od
Od OdReading Ru
n 0K (angle) d=degX1/10po1
909G 941G 92
0G 876Gpeak 909
G 941G 920G 877G
max t OG 973G
OG 0cm1nflt
OG 896G OG 0G
rflat OG 77G
OG 0Gdiffer OG
19G OG OGwidth
Od Od Od O
dangle 910d 1000d
1915d 2710dinterv 10
00cl 914d 795d 889d
half Od Od Od
According to the present invention, the magnetization angle can be measured even without the slide jig 6 shown in FIG. 1.

しかし第4図(a)の様に直接測定した場合理想的条件
の下では距離値R□はθに関して第5図の(a)の様な
グラフとなりその関数は Ra 6 =T −r ocos CX / CO5θ
(0≦θ≦α)となる。
However, when directly measured as shown in Figure 4 (a), under ideal conditions, the distance value R□ becomes a graph with respect to θ as shown in Figure 5 (a), and the function is Ra 6 = T - r ocos CX / CO5θ
(0≦θ≦α).

第4図中)の様にフライス面よりも広い平面を持ち、シ
ャフトの回転に追求して平行に移動するスライド治具6
が有ると治具までの距離値Rb、は第5図(b)の様な
グラフとなりその関数はRb、 = T −r oco
s(α−θ)(0≦θ≦α)となる。
As shown in Fig. 4), the slide jig 6 has a plane wider than the milling surface and moves parallel to the rotation of the shaft.
If there is, the distance value Rb to the jig will be a graph as shown in Fig. 5(b), and its function will be Rb, = T −r oco
s(α−θ) (0≦θ≦α).

さて2つの関数R,,,R,,において、シャフト8の
直径5n、フライス深さ0.81mの場合角度が0度か
ら0.3度に変化した時の変化量ΔR0゜ΔRb、は Δ R,、=0.000023 鳳1 Δ Rb、y  =0.0097 貫層となり、測定し
たい0度近傍の変化量が大となり、通常のセンサーによ
って0.3度の変化を十分測定可能となる。
Now, in the two functions R,,,R,, when the diameter of the shaft 8 is 5n and the milling depth is 0.81m, the amount of change ΔR0°ΔRb when the angle changes from 0 degrees to 0.3 degrees is ΔR ,, = 0.000023 Otori 1 Δ Rb,y = 0.0097 It becomes a translayer, and the amount of change near 0 degrees that is desired to be measured becomes large, and a change of 0.3 degrees can be sufficiently measured with a normal sensor.

通常のセンサーとは0.OQ1龍以上の測定精度が有り
、電気信号として出力する物であれば光学式でもうず電
流式でもダイヤルゲージでも良い、特に先端が十分法(
平らなダイヤルゲージであればスライド治具が無くとも
同様な効果を持つ。
A normal sensor is 0. As long as it has a measurement accuracy higher than OQ1 Dragon and outputs as an electrical signal, an optical type, spiral current type, or dial gauge may be used, especially if the tip has a sufficient measurement accuracy (
A flat dial gauge will have the same effect even without a slide jig.

(効 果) 本発明によれば次の様な効果が得られる。(effect) According to the present invention, the following effects can be obtained.

!11 0.3度の測定精度を1μの精度の有る距離セ
ンサーで可能となる。
! 11 Measurement accuracy of 0.3 degrees is possible with a distance sensor with an accuracy of 1 μ.

(2)磁力の測定値及び角度の測定値とも電圧出力とな
った為マイコンを利用した自動測定が可能となり従来3
〜4本の測定に約30分要していたが1本当り14秒で
測定することができる。
(2) Since both the measured value of magnetic force and the measured value of angle are now voltage output, automatic measurement using a microcomputer is possible, making it possible to perform automatic measurement using a microcomputer.
It used to take about 30 minutes to measure 4 pieces, but now it takes 14 seconds for each piece.

(3)  上記マイコン自動測定装置の測定再実性の公
差を0.36度(使用エンコーダーの分解能)に収める
ことができる。
(3) The measurement reproducibility tolerance of the microcomputer automatic measuring device can be kept within 0.36 degrees (resolution of the encoder used).

(4)  スライド治具6をフライス面の有る位置にセ
ットし自由に上下可能とすれば、シャフト径もフライス
深さも距離センサーの測定可能範囲では任意であるので
フライス面の有る位置に移動可能な構造であれば、段取
り替えの必要がない。
(4) If the slide jig 6 is set at a position where there is a milling surface and can be moved up and down freely, the shaft diameter and milling depth are arbitrary within the measurable range of the distance sensor, so it can be moved to a position where there is a milling surface. With this structure, there is no need for setup changes.

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

第1図は本発明の測定装置を示す図、第2図は出力デー
タープロソト図、第3図は装置の機能を示す図、第4図
(a)は直接測定方法を説明するための図、第4図(b
)は治具測定方法を説明するための図、第5図(a)は
直接測定関数を示す図、第5図(blは治具測定関数を
示す図、第6図は従来装置を示す図、第7図は従来方法
の最大誤差を説明するための図である。 1:エンコーダー、3:マクネノトロール、4:ホール
素子、5:距離センサー、6:スライド治具7:フライ
ス面、8:シャフト、9:針、10:目盛、11:非磁
性体治具、12:止めネジ。 第3図 第4図 (Q)      (b) 第5図
Fig. 1 is a diagram showing the measuring device of the present invention, Fig. 2 is an output data protograph, Fig. 3 is a diagram showing the functions of the device, and Fig. 4 (a) is a diagram for explaining the direct measurement method. , Figure 4 (b
) is a diagram for explaining the jig measurement method, Figure 5 (a) is a diagram showing the direct measurement function, Figure 5 (bl is a diagram showing the jig measurement function, and Figure 6 is a diagram showing the conventional device , Fig. 7 is a diagram for explaining the maximum error of the conventional method. 1: Encoder, 3: Macnenotrol, 4: Hall element, 5: Distance sensor, 6: Slide jig 7: Milling surface, 8: Shaft , 9: Needle, 10: Scale, 11: Non-magnetic jig, 12: Set screw. Figure 3 Figure 4 (Q) (b) Figure 5

Claims (1)

【特許請求の範囲】 2、特許請求の範囲 (1)円筒状シャフトの一部を平坦にカットした面の方
向を基準にして別の測定可能な物理量の角度位置を測定
する装置において、被測定物を回転させる手段と、角度
位置を測定する手段と、角度位置を測定する物理量を測
定する手段と、シャフトの平坦部の有る位置を外部の一
点からシャフト表面までの距離を測定する手段及び測定
値を記憶する手段とからなることを特徴とするフライス
面方向測定装置。 (2)特許請求の範囲前1項記載の装置において、シャ
フト表面までの距離を基準位置からの角度の関数の変換
をおこなう手段を有することを特徴とするフライス面方
向測定装置。
[Scope of Claims] 2. Scope of Claims (1) In an apparatus for measuring the angular position of another measurable physical quantity with reference to the direction of a plane cut flatly from a part of a cylindrical shaft, A means for rotating an object, a means for measuring an angular position, a means for measuring a physical quantity for measuring an angular position, a means for measuring the distance from a point on the outside to the surface of a shaft, and a means for measuring the position of a flat part of a shaft. 1. A milling face direction measuring device, characterized in that it comprises means for storing values. (2) A milling face direction measuring device according to claim 1, further comprising means for converting the distance to the shaft surface into a function of an angle from a reference position.
JP61181501A 1986-08-01 1986-08-01 Milling plane direction measuring device Expired - Lifetime JPH0613967B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP61181501A JPH0613967B2 (en) 1986-08-01 1986-08-01 Milling plane direction measuring device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP61181501A JPH0613967B2 (en) 1986-08-01 1986-08-01 Milling plane direction measuring device

Publications (2)

Publication Number Publication Date
JPS6338109A true JPS6338109A (en) 1988-02-18
JPH0613967B2 JPH0613967B2 (en) 1994-02-23

Family

ID=16101860

Family Applications (1)

Application Number Title Priority Date Filing Date
JP61181501A Expired - Lifetime JPH0613967B2 (en) 1986-08-01 1986-08-01 Milling plane direction measuring device

Country Status (1)

Country Link
JP (1) JPH0613967B2 (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0331708A (en) * 1989-06-29 1991-02-12 Hitachi Metals Ltd Instrument for measuring reference position
JP2011070149A (en) * 2009-08-25 2011-04-07 Ricoh Co Ltd Method and tool for adjusting magnetic pole position of developer carrier
CN103149820A (en) * 2013-03-15 2013-06-12 柯尼卡美能达商用科技(无锡)有限公司 Magnetic angle adjusting device of developer

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5818713A (en) * 1981-07-25 1983-02-03 Nippon Kogaku Kk <Nikon> Positioning device for discoid object
JPS60135712A (en) * 1983-12-23 1985-07-19 Hitachi Zosen Corp Detecting method of angle of rotation of turntable

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5818713A (en) * 1981-07-25 1983-02-03 Nippon Kogaku Kk <Nikon> Positioning device for discoid object
JPS60135712A (en) * 1983-12-23 1985-07-19 Hitachi Zosen Corp Detecting method of angle of rotation of turntable

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0331708A (en) * 1989-06-29 1991-02-12 Hitachi Metals Ltd Instrument for measuring reference position
JP2011070149A (en) * 2009-08-25 2011-04-07 Ricoh Co Ltd Method and tool for adjusting magnetic pole position of developer carrier
CN103149820A (en) * 2013-03-15 2013-06-12 柯尼卡美能达商用科技(无锡)有限公司 Magnetic angle adjusting device of developer

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