JPS59170217A - Method for measuring hardening depth - Google Patents

Method for measuring hardening depth

Info

Publication number
JPS59170217A
JPS59170217A JP4506683A JP4506683A JPS59170217A JP S59170217 A JPS59170217 A JP S59170217A JP 4506683 A JP4506683 A JP 4506683A JP 4506683 A JP4506683 A JP 4506683A JP S59170217 A JPS59170217 A JP S59170217A
Authority
JP
Japan
Prior art keywords
diameter
frequency
power
shaft
depth
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
JP4506683A
Other languages
Japanese (ja)
Inventor
Seiichi Fukamachi
深町 成一
Etsuo Ban
伴 悦夫
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.)
Jeol Ltd
Original Assignee
Jeol Ltd
Nihon Denshi KK
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 Jeol Ltd, Nihon Denshi KK filed Critical Jeol Ltd
Priority to JP4506683A priority Critical patent/JPS59170217A/en
Publication of JPS59170217A publication Critical patent/JPS59170217A/en
Pending legal-status Critical Current

Links

Classifications

    • CCHEMISTRY; METALLURGY
    • C21METALLURGY OF IRON
    • C21DMODIFYING THE PHYSICAL STRUCTURE OF FERROUS METALS; GENERAL DEVICES FOR HEAT TREATMENT OF FERROUS OR NON-FERROUS METALS OR ALLOYS; MAKING METAL MALLEABLE, e.g. BY DECARBURISATION OR TEMPERING
    • C21D1/00General methods or devices for heat treatment, e.g. annealing, hardening, quenching or tempering
    • C21D1/55Hardenability tests, e.g. end-quench tests

Landscapes

  • Chemical & Material Sciences (AREA)
  • Engineering & Computer Science (AREA)
  • Physics & Mathematics (AREA)
  • Thermal Sciences (AREA)
  • Crystallography & Structural Chemistry (AREA)
  • Mechanical Engineering (AREA)
  • Materials Engineering (AREA)
  • Metallurgy (AREA)
  • Organic Chemistry (AREA)
  • Investigating Or Analyzing Materials By The Use Of Magnetic Means (AREA)

Abstract

PURPOSE:To measure simply the correct hardening depth of a shaft-shaped hardened article by determining beforehand the frequency of exciting power peculiar to the diameter of the article at which the iron loss and the heardening depth of the article has relation represented by a straight line. CONSTITUTION:A shaft 3 to be measured is put in the center hole 2 in an exciting coil 1, and the diameter D of the shaft 3 is inputted in a controller 6. The frequency of the AC power of an AC power source 4 set by the input is considered to be frequency at which the iron loss and the hardening depth of the shaft 1 of the diameter D has relation represented by a straight line. The value of power W from a wattmeter 5 is sent to the controller 6, and the iron loss is calculated from the power W and a constant K depending on the diameter D and the kind of the shaft 3. The hardening depth of the shaft 3 is then calculated and displayed on a display device 7.

Description

【発明の詳細な説明】 [産業上の利用分野廖 )1\発明はシ’(r)1〜払力乞入物の)充入深1j
LをJiす定づるソフ;入に関づる。
[Detailed Description of the Invention] [Industrial Field of Application] 1\The invention is based on 1~Filling Depth 1j
The software that defines L; relates to entering.

E fM来技術] シi・ノド状焼入物の焼入層の深度(1ス後焼入深度と
称り)は、焼入層の鉄損と焼入深I哀とが焼入物の種類
に因りおよそ比例的関係をもって変化りる事実を使って
測定することが出来る。
EfM New Technology] The depth of the hardened layer of the groove-shaped hardened material (referred to as the hardened depth after 1 step) is determined by the iron loss of the hardened layer and the hardened depth I of the hardened material. It can be measured using the fact that it varies in a roughly proportional manner depending on the type.

この様な測定は、例えば第1図に示す様に行なうことが
出来る。即ち、ドーナツ状に巻いた励磁=1イル1の中
心孔2へ焼入物3を口通さけ、該励磁コイルに交流電源
から、例えば50サイクルの交流電力を印加し、磁束を
前記焼入物・3の焼入層に充分入り込む様にし、該焼入
層の1ス損を検出しC該焼入深度を測定している。図で
は、この焼入層の鉄損に9.4応じた前記励磁コイル1
の電力を電力訓5から求め、深度を測定しCいる。
Such measurements can be performed, for example, as shown in FIG. That is, the hardened material 3 is passed through the center hole 2 of the excitation coil 1 wound in a donut shape, and AC power of, for example, 50 cycles is applied to the excitation coil from an AC power source to direct the magnetic flux to the hardened material.・The quenching depth is measured by making sure that the quenching layer penetrates sufficiently into the quenching layer No. 3, and detecting the 1 loss of the quenching layer. In the figure, the excitation coil 1 corresponds to the iron loss of this hardened layer by 9.4.
Determine the power from the power calculation 5, measure the depth, and calculate the depth.

しかし、前記測定においては、焼入層の1ス損と焼入深
度がおよそ比例的関係にあることを使った測定で、焼入
層の鉄損と焼入層IQが直線関係(比例関係)にあるこ
とを児つけ該直線関係を使った、’i′lj定ではない
。即ち、従来は一般の焼入物の焼入層に充分磁束が入る
交流電力の周波数として、例えば50サイクルを選び、
焼入物の径に関係なく焼入深度の異る複数の焼入物を用
、0し、各々の1人1C″!を検出し、第2図の様なJ
3よそ比例的関係にある焼入ご1τ1妄とQノ冊(1の
特性線を)j(めCJ3さ、直線的部分(△)だり1・
、(つl鉄損から焼入深度を求めるか、又は全部分を使
い、検出した鉄損を該1う性腺に照し合せて焼入深度を
もとめるかしている。これ(゛は、前者の場合では測定
範囲が−1・λしく狭くなり、i多者の場合は茗しく厄
介である。又、何れの場合も、測定の箱(Qは必ずしも
J〜いどは菖えない。
However, in the above measurement, the core loss of the hardened layer and the hardened layer IQ are in a linear relationship (proportional relationship). 'i'lj is not definite using the linear relationship. That is, in the past, for example, 50 cycles were selected as the frequency of AC power that would allow sufficient magnetic flux to enter the hardened layer of general hardened materials.
Using multiple quenched products with different quenching depths regardless of the diameter of the quenched products, 0 is used to detect each individual 1C''!
3 There is a relatively proportional relationship between quenching and Q (the characteristic line of 1), and the linear part (△) and 1.
The quenching depth is determined from the iron loss, or the entire part is used and the detected iron loss is compared to the gonad to determine the quenching depth. In the case of , the measurement range becomes narrow by -1·λ, and in the case of many i, it becomes complicated.Also, in any case, the measurement box (Q does not necessarily fall within J~).

[発明の[1的] 本発明1よこの様な問題点を解決づることをl l I
I’)’としくイ「したちのく−ある。
[Object 1 of the invention] Invention 1 aims to solve such problems.
I')' Toshikui "There is Shichichinoku.

[発明の(1,1成] イ(川明〔よろ用定俳へさシト)1へ:(人焼入物を、
1fil)聚に:Iイルの磁力線中に配眠し、該焼入物
の鉄損を検出しC該焼入物の焼入深度を測定り°る方法
におい(、予め、シX・フト状焼入物の径の逆数を定数
としく鉄((!ど焼入深度が直線関係になる前記焼入物
のCYに’l’、’l右の励磁電力の周波数を種々の大
きざの径のシ【・71へ状焼入物に対し′C求めておさ
、励1j電力の周波数を測定カベきシ17]1〜状焼入
物の径に特有の(aにして該焼入物の焼入深度を測定づ
−るばにした新規な焼入深度測定方法である。
[Invention (1, 1)] I (Kawaaki [Yoryoyo Teihai Hesashito) 1: (Human-quenched products,
1fil) In the method of measuring the quenching depth of the quenched material by placing it in the magnetic field lines of the quenched material and detecting the iron loss of the quenched material. The reciprocal of the diameter of the quenched material is set as a constant, and the quenching depth is in a linear relationship with the CY of the quenched material. [・71 Determine 'C for the wedge-shaped quenched material, measure the frequency of the excitation 1j electric power, and measure the frequency of the excitation 1j power. This is a new method for measuring quench depth.

本発明の原1(J!は次の様な実験に基づく。The basis of the present invention 1 (J!) is based on the following experiment.

直径りがD+  (=20mm)で焼入深j哀が夫々1
+(−’1m l:)  、   t  2   <=
1.  5mm)  、   t  3   (=2m
m)、j4(=2.5mm)、is  (=3mm)、
 t6  (’3.5’n1ln) t?  (−4n
1m) +’ l: s  (=4.5mm) t =
  (= 5mm)である9本のシャツ1〜、直径りが
D2  (= 30mm) テ焼入深度が夫々tl、t
:、tz、’t、+、’js、t6,17.js、t9
である9本のシャツ]〜、直径りがD3  (−400
1n1)Cy、l′c  人 j?je  ji  /
りく 人 ’t  l   1  、   L   2
   、  1 3   、  1.   /、   
、   j   S   。
The diameter is D+ (=20mm) and the quenching depth is 1.
+(-'1ml:), t2<=
1. 5mm), t3 (=2m
m), j4 (=2.5mm), is (=3mm),
t6 ('3.5'n1ln) t? (-4n
1m) +' l: s (=4.5mm) t =
(= 5 mm), the diameter is D2 (= 30 mm), and the quenching depth is tl and t, respectively.
:, tz, 't, +, 'js, t6,17. js, t9
9 shirts] ~, the diameter is D3 (-400
1n1) Cy, l'c person j? je ji /
Riku person't l 1, L 2
, 1 3 , 1. /,
, jS.

し6+’l−/、12.[!!である9本のシx7ノト
、及び、1′1径りがD4(=50111m)で焼入深
度が夫lンt、+ 、 t 2. 、 [3、L /、
 、 t S 、 t 6 、 t、 7 、18.1
りである9本のシV71−を用意し、全Cのシ入・71
〜についで、励磁電力の周波紗[を[!(=511z 
> 、 f 2  (=61−1z ) 、 f 3.
(−711z   >’+   f  4   (=8
1−lz   )  、   f  s   (=9 
 トlz)、f6(−101−1z )、、f7’  
(=11.1−lz >、 f gf=−1211z 
  >r+((−−1311z   >、   f、a
    (=  1/Il+/>、r、+     <
=15  トlz   )   、   f、ユ   
(・ 161−11  >、「1s   (=1711
z  >、  f、、t   (=181−lz  )
r、、(=19  ト1z   )  、  f7t 
   (=201−1z   )  −r、t(=30
11z)に順次Cり変し、その都痘、鉄損Wを測定しく
みた。尚、前記の如き直径及び焼入側+iのシ17ノト
をjハんだのは最も実用的なシャツ1〜lごがらひある
。又、前記の如き周波数を声/υだのは、この杆’(’
L ” t’)I〜に十分県東を−入り込ませる1^]
波数(磁束浜透麿ど周波数の平方(付は反比例する)だ
からである、この結果を第3図〜第6図に承り。第3図
・〜第6図は夫々、励磁電力の周波数[をパラメータど
した直径D+ 、D2.Dg、I)4、のシトフ]〜の
焼入深爪鉄損1h竹を示()−ものてC(りる、1 εf::3図、第4図、第5図、第61:21各lくの
焼入側f!′g、’ 、 g’)、Ir、!17を性i
)1 ラ、直径D + ノ’;/ t / l−”Q 
Li 励磁電力の周波数がf(a  の吟、D′i径D
1どシャ、)1゛のEi’(5:C!(拐買等)に依っ
てぎまる定数をに1として、i′:、1f1(よ焼入側
)すtこ比1シリし、直行1〕2のシI7−ノ1゛・1
000丁7.のIIテ、1り2を定数として以JP に
i焼焼入!良に化則し、直径D3のシ鬼・71〜では[
6の同、1(二を定数として鉄損(ま])z入深爪に比
例し、直径D4のシ1/フI〜(゛はf3のIt寺、I
X4を定数として1人1iは焼入深度に比例しているこ
とが分かる。以上のことから、シャツ1〜状焼入物の釦
、損と焼入側1αとが直線的関係になる励磁電力の周波
数が、該シャット状力゛シ入物の直径に応じて存在づ−
ることが分かる。尚、実験にJ、れば前記直線関係が存
在する励磁電力の周波数は一通冨のシャフトにおいては
、5iiZ−2011zである。さて、そこで、予め、
シ鬼・)[〜状焼入物の径に応じて前記直線関係を発生
Cヒる周波数を求めておき、実際の焼入物の深麿を測定
ぐる場合に、励磁型)jの周波数を該焼入物の直径に特
有の周波数にし、検出された鉄損から焼入側1αを搾出
するJ、うにづれば、正確な焼入側、妄が菖しく簡単に
求められる。
6+'l-/, 12. [! ! 9 pieces x 7 points, 1'1 radius is D4 (=50111 m), and the quenching depth is 1, +, t2. , [3,L/,
, t S , t 6 , t , 7 , 18.1
Prepare 9 C V71-, which is
~ Next, the frequency gauze of excitation power [[!] (=511z
> , f 2 (=61-1z), f 3.
(-711z >'+ f 4 (=8
1-lz), fs (=9
f6(-101-1z), f7'
(=11.1-lz >, f gf=-1211z
>r+((--1311z >, f, a
(= 1/Il+/>, r, + <
=15 trlz), f, yu
(・ 161-11 >, “1s (=1711
z >, f,, t (=181-lz)
r,, (=19 t1z), f7t
(=201-1z) -r, t(=30
11z), and measured the smallpox and iron loss W. It should be noted that the most practical shirts 1 to 1 are made by soldering 17 pieces of diameter and quenched side +i as described above. Also, it is this rod '('
L ” t') Enough of the eastern part of the prefecture enters I~1^]
This is because the wave number (magnetic flux transmission rate is inversely proportional to the square of the frequency). This result is shown in Figures 3 to 6. Figures 3 to 6 show the frequency [of the excitation power], respectively. Parameters of diameter D+, D2.Dg, I) 4, quenched deep claw iron loss 1h bamboo () Fig. 5, No. 61:21 each of the hardened sides f!'g,', g'), Ir,! 17 is gender i
)1 la, diameter D + ノ';/t/l-"Q
Li The frequency of excitation power is f(a, D′i diameter D
1 dosha,) 1゛Ei' (5:C! (reduction, etc.), assuming that the constant that depends on 1 is 1, i':, 1f1 (hardened side) t ratio is 1 series, Straight line 1〕2 no si I7-no1゛・1
000 7. II Te, 1 and 2 are constants and then JP is quenched! It has been improved to a good standard and has a diameter of D3.
Same as 6, 1 (with 2 as a constant, iron loss (ma)) is proportional to the depth of z, and the diameter D4 is 1/F I ~ (゛ is It temple of f3, I
It can be seen that 1i per person is proportional to the quenching depth with X4 as a constant. From the above, it can be seen that the frequency of the excitation power at which the button loss of the shirt-like quenched material and the quenched side 1α is in a linear relationship exists depending on the diameter of the shirt-like quenched material.
I understand that. Incidentally, if J is determined in the experiment, the frequency of the excitation power at which the above linear relationship exists is 5iiZ-2011z for a shaft with a maximum of one pass. Well, then, in advance,
After determining the frequency at which the above linear relationship occurs according to the diameter of the ~-shaped quenched material, and when measuring the depth of the actual quenched material, the frequency of the excitation type)j is determined. By setting the frequency to be specific to the diameter of the quenched material and extracting the quenched side 1α from the detected iron loss, the exact quenched side can be easily obtained.

[実施例] 第7図(ま本発明の方法の一実施例を示した焼入深度測
定装買の(■略を示したもので、図中第1図L、二’(
用いた香舅と同一のちのは同一構成要素である。
[Example] Figure 7 (shows (■ omitted) of a quenching depth measuring device showing an example of the method of the present invention; Figures 1 L and 2' (
The components that are the same as the incense used are the same.

図中6は演f、3 fi能を1iif+えた制御器:i
“7で、外部から入力されるシA・)l−の径りど該シ
トフ1〜の種類(・二依ってさ」、る定数1(、電力品
(5で検出された電]J f+i]W (シ(・フトの
鉄損に対応してる)との演紳を行ない、シトノ1〜の焼
入深度1を算出りると共に、シト71〜の径が入力され
た時に励磁電力の周波数が該直径に111右の値になる
様に交流電源4を二]ン1−ロールする。7は該焼入深
度を表示づ−る表示に置Cある。IIJi <の如ぎ独
習におい−(、’ ili’l定1Jべきシャツ1〜3
を励磁コイルの中心孔2へ挿入し、制御装置6へ該シV
フト3の直径りを入力〕jる。
In the figure, 6 is the function f, and 3 is a controller with fi function 1iif+: i
"At 7, the diameter of the externally input signal A. ] W (corresponds to the iron loss of the shaft), calculates the quenching depth 1 of the shaft 1~, and when the diameter of the seat 71~ is input, the frequency of the excitation power is calculated. Roll the AC power supply 4 two times so that the diameter becomes the value 111.7 is placed on the display that indicates the quenching depth. ,'ili'l fixed 1J shirts 1-3
into the center hole 2 of the excitation coil, and send the cylinder to the control device 6.
Enter the diameter of the foot 3.

該入力にJ、り交流電源4の交流電力の周波数(31該
ii′I径1つのシX・フトに(13いて鉄損と焼入深
度が直線関係をもつ周波数の値foとなる。而して、電
力ii1’ 571” ’うの電力Wが前記イス11伶
11装箇6へ送られると、該制御装置はWどRどの演砦
を行い、シャツ(〜の焼入深度10を算出”づる。
The input is J, and the frequency of the AC power from the AC power supply 4 (31). Then, when the electric power W of the electric power ii1'571''' is sent to the chair 11 and the 11 equipment 6, the control device performs the W do R operation and calculates the quenching depth 10 of the shirt (... “Zuru.

尚、シト71−の直径に特有の周波数10は次の様にし
ても求めることが出来る。
Note that the frequency 10 specific to the diameter of the seat 71- can also be determined as follows.

第8図に示J様に直径りで焼入深、度が11.し2.1
3の三水のシAl]+−10,11,12を用!ユする
。そして各シャツ1−を励磁コイル13,14.15の
中心孔に夫々配置し、可変周波数電源゛1Gから交流電
力を印加し、鉄損検出器(電力計)17.18.19で
夫々鉄損を検出し、それらを制御装置20へ送る様にり
る。この際交流電力の周波数を先りf1にした時、鉄損
検出器17,18.19から人々d 1. (12、d
 gの1ス静値が検出されたとJる。この時、制御装置
20はdl、(13から第9図の直線Cを作成し、焼入
深度(2に対する鉄損値d 2/ と鉄損検出器18の
出力d、どの差を算出し、その差((12’ −+12
 < O)を表示器21へ送る。該表示器は該差を表示
ザる。
The quenching depth and degree are 11. 2.1
3 of the three waters Al] +-10, 11, 12 is used! I'm going to do it. Then, each shirt 1- is placed in the center hole of the excitation coil 13, 14, 15, respectively, AC power is applied from the variable frequency power supply 1G, and the iron loss detector (power meter) 17, 18, 19 detects the iron loss. are detected and sent to the control device 20. At this time, when the frequency of AC power is first set to f1, people d1. (12, d
It is assumed that one static value of g has been detected. At this time, the control device 20 creates a straight line C in FIG. 9 from dl, The difference ((12' - +12
<O) is sent to the display 21. The indicator displays the difference.

Aベレータは該差の正負及び大汚さを考虞して、交流電
力を12にJる。この時、v1損検出器17゜18.1
9.から夫々d 5 、 d 6 、 d 7の鉄損1
1C1が検出され7jと覆る。制御器20は前記と同様
に第9図直線りを作成し、焼入深度t2に対重る鉄1j
)iif+ (16’ と鉄jO検出器18の出力(1
6との差((i 6 ’ −(16>O)を表示器2]
へ送る。Aベレータ1、L該ジfの正f1及び大δざを
者Iノ族して、交流゛電力の周波数をf、、f、、の間
の適宜な値にづる。
The A verator reduces the AC power to 12 J, taking into consideration the positive/negative of the difference and the large contamination. At this time, v1 loss detector 17°18.1
9. The iron loss 1 of d 5 , d 6 , d 7 from
1C1 is detected and changed to 7j. The controller 20 creates the straight line shown in FIG.
) iif+ (16' and the output of the iron jO detector 18 (1
6 ((i 6 ' - (16>O) on display 2)
send to The frequency of the AC power is set to an appropriate value between f, , f, by taking the positive f1 and the large δ difference of A verator 1 and L as a group.

この(、丘な動作を・繰り返し、制御装置i20が作成
りる直線の焼入深度(2に対り−る1ス↑ロ値d 9/
 が鉄損検出器18の出力d9と等しくなる交流電力の
周波′I41[0を求める。この周波数10が直径りの
焼入材(シt171〜)に特有のJi 波数である。
By repeating this hilly motion, the control device i20 creates a linear quenching depth (1 scale ↑ for 2) value d 9/
The frequency 'I41[0 of the AC power at which is equal to the output d9 of the iron loss detector 18 is determined. This frequency 10 is the Ji wave number specific to the diameter-hardened material (sit 171~).

[効果1 本発明l、二依れば、止イ「な)′3に人脈1哀が著し
く f!’J単に求められる3゜
[Effect 1 According to the present invention, there is a significant increase in personal connections in '3.

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

第1図tま従来の焼入深度測定装置の概略図、第2図(
、L焼入深度鉄)t)+ ’lXi性、第3図〜第6図
(,1、直わj:召・一定どし、周波数をパラメータと
した焼入深葭;プ、il’i狛1)1、第7図は本発明
の方法の一実施例としC示したカに人深fα81’i定
装買の概略口、第8図〜第0図1,1.シt・ノ;〜の
1径に1、)イ」の周波数を求める方法を・説明づる為
(こ用いた図て゛ある。 1:励磁コイル 3:シャツ1〜 4:交流電源 5:電力計 6:制御装置 精検出願人 日本電子株式会社 代表者 伊腔 −夫 大灸入潔*−−−−さ 焼入5呆11□ニー÷ 刈先入5采力し−一一ラ 六夾入5ン、バし□
Figure 1 is a schematic diagram of a conventional quenching depth measuring device, Figure 2 (
, L quenching depth iron) t) + 'lXi properties, Figs. Koma1) 1, Figure 7 shows an example of the method of the present invention. This diagram is used to explain how to find the frequency of 1 for each diameter of 1.). 1: Excitation coil 3: Shirts 1 to 4: AC power supply 5: Wattmeter 6: Applicant for the control equipment, representative of JEOL Co., Ltd. Ikuo - Fudai-moxibustion entry Kiyoshi *----Sakening 5 11 □ Knee ÷ Harisaki entry 5 Squeezing - 11 Ra 6 Jyoiri 5 N, Bashi□

Claims (1)

【特許請求の範囲】[Claims] 測定リベさシャフト状焼入物を、励磁]1イルの磁力線
中に配属し、該焼入物の鉄10を検出しで該た2人物の
焼入深度を測定覆る方法において、予め、シト−ノド状
焼入物の径の逆数を定数として鉄損と焼入層1αが直線
関係にf、J−るnζ)記焼入物の径に1!]イjの励
磁電力の周波数を種々の大きさの径のシャフト状焼入物
に対しζ求め−Cお6、励磁電力の周波数を測定(Jべ
さシャフト状焼入物の径に特16゛の値にしC該焼入物
の焼入深度を測定する仔にしたり)z人深度測定方)ム
Measurement In this method, the hardened material in the form of a ribbed shaft is placed in the magnetic field line of 1 field, and the iron 10 of the hardened material is detected to measure the hardened depth of the two persons. The iron loss and the hardened layer 1α have a linear relationship f, J−nζ) with the reciprocal of the diameter of the throat-shaped hardened material as a constant. ] Determine the frequency of the excitation power of Ij for shaft-shaped hardened products of various sizes - C6, measure the frequency of the excitation power (J The value of ゛ is used to measure the quenching depth of the quenched product.
JP4506683A 1983-03-17 1983-03-17 Method for measuring hardening depth Pending JPS59170217A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP4506683A JPS59170217A (en) 1983-03-17 1983-03-17 Method for measuring hardening depth

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP4506683A JPS59170217A (en) 1983-03-17 1983-03-17 Method for measuring hardening depth

Publications (1)

Publication Number Publication Date
JPS59170217A true JPS59170217A (en) 1984-09-26

Family

ID=12708973

Family Applications (1)

Application Number Title Priority Date Filing Date
JP4506683A Pending JPS59170217A (en) 1983-03-17 1983-03-17 Method for measuring hardening depth

Country Status (1)

Country Link
JP (1) JPS59170217A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2008170233A (en) * 2007-01-10 2008-07-24 Toyota Motor Corp Hardening depth measuring instrument and method

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2008170233A (en) * 2007-01-10 2008-07-24 Toyota Motor Corp Hardening depth measuring instrument and method

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