JPH0221740B2 - - Google Patents

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Publication number
JPH0221740B2
JPH0221740B2 JP17014682A JP17014682A JPH0221740B2 JP H0221740 B2 JPH0221740 B2 JP H0221740B2 JP 17014682 A JP17014682 A JP 17014682A JP 17014682 A JP17014682 A JP 17014682A JP H0221740 B2 JPH0221740 B2 JP H0221740B2
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JP
Japan
Prior art keywords
strain
modulus
stress
young
plastic
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
JP17014682A
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Japanese (ja)
Other versions
JPS5960242A (en
Inventor
Hironari Mita
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.)
Shimadzu Corp
Original Assignee
Shimadzu Corp
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Filing date
Publication date
Application filed by Shimadzu Corp filed Critical Shimadzu Corp
Priority to JP17014682A priority Critical patent/JPS5960242A/en
Publication of JPS5960242A publication Critical patent/JPS5960242A/en
Publication of JPH0221740B2 publication Critical patent/JPH0221740B2/ja
Granted legal-status Critical Current

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Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N3/00Investigating strength properties of solid materials by application of mechanical stress
    • G01N3/08Investigating strength properties of solid materials by application of mechanical stress by applying steady tensile or compressive forces

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  • Physics & Mathematics (AREA)
  • Health & Medical Sciences (AREA)
  • Life Sciences & Earth Sciences (AREA)
  • Chemical & Material Sciences (AREA)
  • Analytical Chemistry (AREA)
  • Biochemistry (AREA)
  • General Health & Medical Sciences (AREA)
  • General Physics & Mathematics (AREA)
  • Immunology (AREA)
  • Pathology (AREA)
  • Investigating Strength Of Materials By Application Of Mechanical Stress (AREA)

Description

【発明の詳細な説明】 <産業上の利用分野> 本発明は、材料に引張圧縮の繰り返し荷重を加
える引張圧縮繰返試験装置に係り、特には、塑性
領域において材料に加える弾性歪速度が一定にな
るように制御する装置に関する。
[Detailed Description of the Invention] <Industrial Application Field> The present invention relates to a tension/compression cyclic testing device that applies repeated tensile/compressive loads to a material. This invention relates to a device for controlling

<従来の技術> 一般に、材料に弾性歪領域を越えた引張圧縮の
繰り返し荷重が加わるような場合には、その破断
寿命等の特性を把握することが必要となる。この
ような材料特性を調べる試験方法として、特に、
塑性歪速度が一定となるように制御しながら弾塑
性領域にわたる引張圧縮の繰り返し荷重を加える
方法が採用される場合がある。
<Prior Art> Generally, when a material is subjected to repeated tensile/compressive loads that exceed the elastic strain range, it is necessary to understand its characteristics such as its rupture life. In particular, as a test method to investigate such material properties,
A method of repeatedly applying tensile and compressive loads over an elastoplastic region while controlling the plastic strain rate to be constant may be adopted.

<発明が解決しようとする課題> ところで、材料の弾塑性領域にわたつて引張圧
縮荷重を加える場合、その全歪εtには弾性歪εeと
塑性歪εpとが含まれる。すなわち、εt=εe+εpと
なる。しかし、従来、上記の弾塑性領域において
引張圧縮の繰り返し荷重を加える場合の歪み制御
は、弾性歪εeと塑性歪εpとにそれぞれ区別して
個別に制御することは行われておらず、あくまで
も全歪εtで制御している。
<Problems to be Solved by the Invention> By the way, when a tensile and compressive load is applied across the elastic-plastic region of a material, the total strain εt includes an elastic strain εe and a plastic strain εp. That is, εt=εe+εp. However, conventionally, strain control when applying repeated tensile and compressive loads in the above-mentioned elastic-plastic region has not been carried out by separately controlling the elastic strain εe and plastic strain εp, but only the total strain. It is controlled by εt.

一方、材料は塑性変形に伴つて加工硬化等を起
すので、材料のヤング率Eは繰り返し荷重が加わ
るたびに刻々変化する。したがつて、εe=σ/E
(σは材料に加わる応力)の関係式において、ヤ
ング率Eが刻々変化するので、これに応じて弾性
歪εeも一定しなくなる。したがつて、従来は、全
歪εt制御の下で、塑性歪εpを一定速度で変化させ
る試験を行うことは非常に困難であつた。
On the other hand, since the material undergoes work hardening as it undergoes plastic deformation, the Young's modulus E of the material changes every time a repeated load is applied. Therefore, εe=σ/E
In the relational expression (σ is the stress applied to the material), since the Young's modulus E changes from moment to moment, the elastic strain εe also becomes inconsistent. Therefore, conventionally, it has been very difficult to conduct a test in which the plastic strain εp is varied at a constant rate under total strain εt control.

<課題を解決するための手段> 本発明は、このような事情に鑑みてなされたも
のであつて、引張圧縮の繰り返し荷重が加わるこ
とにより、ヤング率が上記のように加工硬化等に
起因して刻々変化しても、弾性歪速度が常に一定
値になるように制御することを目的とする。その
ため、本発明の引張圧縮繰返試験装置では、 弾塑性領域にわたつて材料に引張圧縮の繰り返
し荷重を加えて、その引張圧縮の繰り返しサイク
ル中に材料に加わる応力を測定する応力測定手段
と、 前記繰り返しサイクル中に材料の応力に対応す
る歪みを測定する歪測定手段と、 前記両測定手段からの各測定結果に基づいて見
掛けのヤング率を計算するヤング率計算手段と、 このヤング率計算手段で計算された見掛けのヤ
ング率と前記応力測定手段で測定された応力とに
基づいて見掛けの弾性歪を計算する弾性歪計算手
段と、 予め設定された一定の時間勾配をもつ塑性歪の
波形を与える信号を出力する塑性歪波形出力手段
と、 前記弾性歪計算手段と塑性歪波形出力手段とか
らの両出力により全歪を決定し、この全歪に対応
する信号を出力する全歪波形決定手段と、 この全歪波形決定手段によつて決定された全歪
に対応した荷重を材料に加える試験片荷重制御手
段と、 を備えた構成としている。
<Means for Solving the Problems> The present invention has been made in view of the above circumstances, and it is possible to reduce the Young's modulus due to work hardening etc. as described above by applying repeated loads of tension and compression. The purpose of this invention is to control the elastic strain rate so that it always remains at a constant value even if it changes moment by moment. Therefore, the tensile compression cyclic testing device of the present invention includes a stress measuring means that applies repeated tensile and compressive loads to a material over an elastoplastic region and measures the stress applied to the material during the repeated tensile and compressive cycles; Strain measuring means for measuring strain corresponding to stress in the material during the repeated cycles; Young's modulus calculating means for calculating an apparent Young's modulus based on each measurement result from both measuring means; an elastic strain calculating means for calculating an apparent elastic strain based on the apparent Young's modulus calculated by the stress measuring means and the stress measured by the stress measuring means; and a waveform of plastic strain having a preset constant time gradient. plastic strain waveform output means for outputting a signal to be given, and total strain waveform determination means for determining total strain based on both outputs from the elastic strain calculation means and the plastic strain waveform output means and outputting a signal corresponding to the total strain. and test piece load control means for applying a load to the material corresponding to the total strain determined by the total strain waveform determining means.

<作用> 上記構成において、弾塑性領域にわたつて材料
に引張圧縮の繰り返し荷重を加えるサイクル中に
材料に加わる応力と歪みとを応力測定手段と歪測
定手段によつてそれぞれ測定し、これらの測定結
果に基づいてヤング率計算手段によつて見掛けの
ヤング率を求め、この見掛けのヤング率と応力測
定手段で測定された応力に基づいて弾性歪計算手
段によつて見掛けの弾性歪を計算する。そして、
塑性歪波形出力手段から与えられる一定の時間勾
配をもつ塑性歪の波形信号と、弾性歪計算手段で
計算された見掛けの弾性歪の各種とから全歪波形
決定手段によつて全歪を決定し、この全歪に対応
した荷重を材料に加える。
<Operation> In the above configuration, the stress and strain applied to the material during a cycle in which repeated tensile and compressive loads are applied to the material over the elastic-plastic region are measured by the stress measuring means and the strain measuring means, respectively, and these measurements are performed. Based on the results, the Young's modulus calculation means calculates the apparent Young's modulus, and the elastic strain calculation means calculates the apparent elastic strain based on this apparent Young's modulus and the stress measured by the stress measurement means. and,
The total strain is determined by the total strain waveform determining means from the plastic strain waveform signal having a constant time gradient given by the plastic strain waveform output means and various kinds of apparent elastic strains calculated by the elastic strain calculating means. , a load corresponding to this total strain is applied to the material.

これにより、全歪制御の下で材料に所定の引張
圧縮の繰り返し荷重を加えるとともに、その引張
圧縮の繰り返しサイクル中の塑性領域において、
弾性歪速度が一定となるように制御される。
As a result, a predetermined repeated tension-compression load is applied to the material under total strain control, and in the plastic region during the repeated cycles of tension-compression,
The elastic strain rate is controlled to be constant.

<実施例> 第1図は引張圧縮繰返試験装置の機能ブロツク
図である。同図において、符号1は弾塑性領域に
わたつて材料に引張圧縮の繰り返し荷重を加え
て、その引張圧縮の繰り返しサイクル中に材料に
加わる応力を測定する応力測定手段で、たとえば
ロードセルが適用される。また、2は上記の引張
圧縮の繰り返しサイクル中に材料の応力に対応す
る歪みを測定する歪測定手段で、たとえば歪ゲー
ジが適用される。3は予め設定された一定の時間
勾配(=±k)をもつ塑性歪の波形を与える信号
を出力する塑性歪波形出力手段であつて、本例で
は、第3図の塑性歪−時間線図に示すように、材
料が塑性領域にあるときには弾性歪速度が一定
(=±k)の三角波形の信号を出力する。4は塑
性歪波形出力手段4の出力が最大(=±εp0)と
なつた場合の引張圧縮あるいは圧縮応力の値を測
定する最大引張圧縮測定手段、5は前記の応力測
定手段1、歪測定手段2ならびに最大引張圧縮測
定手段4でのその結果に基づいて見掛けのヤング
率を計算するヤング率計算手段である。また、6
はヤング率計算手段5で計算された見掛けのヤン
グ率と応力測定手段1で測定された応力とに基づ
いて見掛けの弾性歪を計算する弾性歪計算手段、
7は弾性歪計算手段6と塑性歪波形出力手段3と
からの両出力により全歪を決定し、この全歪に対
応する信号を出力する全歪波形決定手段である。
8は全歪波形決定手段7によつて決定された全歪
に対応した荷重を材料に加える試験片荷重制御手
段で、たとえばサーボバルブが適用される。
<Example> FIG. 1 is a functional block diagram of a tension/compression cyclic testing device. In the same figure, reference numeral 1 denotes a stress measurement means that applies repeated tension-compression loads to the material over the elastic-plastic region and measures the stress applied to the material during the repeated cycles of tension-compression. For example, a load cell is applied. . Further, reference numeral 2 denotes a strain measuring means for measuring the strain corresponding to the stress of the material during the above-described repeated cycles of tension and compression, and a strain gauge is applied, for example. 3 is a plastic strain waveform output means for outputting a signal giving a plastic strain waveform with a preset constant time gradient (=±k); in this example, the plastic strain-time diagram in FIG. As shown in the figure, when the material is in the plastic region, a triangular waveform signal with a constant elastic strain rate (=±k) is output. 4 is a maximum tensile compression measuring means for measuring the value of tensile compression or compressive stress when the output of the plastic strain waveform output means 4 reaches the maximum (=±εp 0 ); 5 is the stress measuring means 1 described above and strain measuring means; This is a Young's modulus calculating means for calculating an apparent Young's modulus based on the results of the means 2 and the maximum tension/compression measuring means 4. Also, 6
is an elastic strain calculation means for calculating an apparent elastic strain based on the apparent Young's modulus calculated by the Young's modulus calculation means 5 and the stress measured by the stress measurement means 1;
Reference numeral 7 denotes a total strain waveform determining means that determines the total strain based on both outputs from the elastic strain calculation means 6 and the plastic strain waveform output means 3, and outputs a signal corresponding to this total strain.
Reference numeral 8 denotes test piece load control means for applying a load to the material corresponding to the total strain determined by the total strain waveform determination means 7, and a servo valve is applied, for example.

次に、上記構成の引張圧縮繰返試験装置の制御
動作について、第2図に示す応力−歪み線図を参
照して説明する。
Next, the control operation of the tension/compression cyclic testing apparatus having the above configuration will be explained with reference to the stress-strain diagram shown in FIG.

引張圧縮の繰り返し荷重試験を開始するに先立
つて、予め全歪制御によつて第2図の符号
OPQRSTQまでの1サイクル分だけ材料に引張
圧縮荷重を加え、TQ間およびRS間の各除荷領域
における応力σ1,σ2と歪みε1,ε2とを応力測定手
段1と歪み測定手段2によつてそれぞれ測定し、
これらの測定結果に基づいてヤング率計算手段5
によつてそれぞれの見掛けのヤング率E1(=σ1
ε1)、E2(=σ2/ε2)を求める。引き続いて、これ
らの各見掛けのヤング率E1,E2の平均E0=(E1
E2)/2を算出する。そして、この平均された
見掛けのヤング率E0の値が弾性歪計算手段6に
送出される。
Prior to starting the repeated tension/compression load test, the symbols shown in Figure 2 are adjusted in advance by total strain control.
A tensile and compressive load is applied to the material for one cycle up to OPQRSTQ, and the stresses σ 1 , σ 2 and strains ε 1 , ε 2 in each unloading region between TQ and between RS are measured by stress measuring means 1 and strain measuring means 2. Measured respectively by
Based on these measurement results, Young's modulus calculation means 5
The respective apparent Young's modulus E 1 (=σ 1 /
ε 1 ) and E 2 (=σ 22 ). Subsequently, the average E 0 = ( E 1 +
Calculate E 2 )/2. Then, this average value of the apparent Young's modulus E 0 is sent to the elastic strain calculation means 6.

次に、引張圧縮の繰り返し荷重試験が開始され
て、たとえば、第2図において、材料にQ点から
R点に向かうような圧縮荷重を加える場合には、
弾性歪計算手段6は、ヤング率計算手段5で既に
算出された上記の平均化された見掛けのヤング率
E0と応力測定手段1で測定されされた応力σと
に基づいて見掛けの弾性歪εe(=σ/E0)を計算
する。そして、この弾性歪εeの値を次段の全歪波
形決定手段7に送出する。全歪波形決定手段7
は、塑性歪波形出力手段3から与えられる一定の
時間勾配(±k)をもつ塑性歪εpの波形信号と、
弾性歪計算手段6で計算された見掛けの弾性歪εe
とから全歪εt=εe+εpを決定する。具体的には、
第2図において、たとえば圧縮荷重下における応
力−歪み線上の任意の点をW1とし、このW1点を
通るε軸に平行な直線が、原点Oを通り勾配が見
掛けのヤング率E0の値をもつ直線と交差する点
をW2としたとき、W1点の塑性歪εpは、W点での
全歪εtからW2点での弾性歪εeを差し引いた値、
すなわちεp=εt−εeとなる。したがつて、歪測定
手段2で測定される歪みε(=εt)が弾性歪εeの
値よりも大きい場合(ε≧εe)には、全歪波形決
定手段7からは、応力測定手段1で測定される応
力σと見掛けのヤング率E0から決定される弾性
歪εe(σ/E0)の信号に、塑性歪波形出力手段3
から与えられる一定の時間勾配(圧縮荷重の場合
は−k)をもつ塑性歪εpの信号を加算してこれ
が全歪信号として出力される。このため、歪測定
手段2で測定される歪みε(=εt)が弾性歪εeの
値を越えた後は、材料は弾性歪速度が一定(=−
k)の条件で圧縮されることになる。なお、歪測
定手段2で測定される歪みε(=εt)が弾性歪εe
の値よりも小さい場合(ε<εe)には、全歪波形
決定手段7からは、弾性歪εe(=σ/E0)の信号
のみが全歪信号として出力される。その結果、全
歪εtの波形は、第4図の実線に示すようになる。
そして、試験片荷重制御手段8は、この全歪波形
決定手段7からの全歪εtに対応した荷重を材料に
加える。
Next, when a tensile compression cyclic load test is started and, for example, a compressive load is applied to the material from point Q to point R in Fig. 2,
The elastic strain calculation means 6 calculates the averaged apparent Young's modulus already calculated by the Young's modulus calculation means 5.
The apparent elastic strain εe (=σ/E 0 ) is calculated based on E 0 and the stress σ measured by the stress measuring means 1. Then, the value of this elastic strain εe is sent to the total strain waveform determining means 7 at the next stage. Total distortion waveform determining means 7
is a waveform signal of plastic strain εp with a constant time gradient (±k) given from the plastic strain waveform output means 3,
Apparent elastic strain εe calculated by elastic strain calculation means 6
Determine the total strain εt=εe+εp from in particular,
In Fig. 2, for example, an arbitrary point on the stress-strain line under compressive load is W 1 , and a straight line parallel to the ε axis passing through this W 1 point passes through the origin O and has a gradient of the apparent Young's modulus E 0 . When the point that intersects the straight line with the value is W 2 , the plastic strain εp at the W 1 point is the value obtained by subtracting the elastic strain εe at the W 2 point from the total strain εt at the W point,
That is, εp=εt−εe. Therefore, when the strain ε (=εt) measured by the strain measuring means 2 is larger than the value of the elastic strain εe (ε≧εe), the total strain waveform determining means 7 determines that the stress measuring means 1 The plastic strain waveform output means 3 is applied to the signal of the elastic strain εe (σ/E 0 ) determined from the measured stress σ and the apparent Young's modulus E 0 .
A signal of plastic strain εp having a constant time gradient (-k in the case of compressive load) given by is added and this is output as a total strain signal. Therefore, after the strain ε (= εt) measured by the strain measuring means 2 exceeds the value of the elastic strain εe, the elastic strain rate of the material is constant (=-
It will be compressed under the condition k). Note that the strain ε (=εt) measured by the strain measuring means 2 is the elastic strain εe.
(ε<εe), the total strain waveform determining means 7 outputs only the signal of the elastic strain εe (=σ/E 0 ) as the total strain signal. As a result, the waveform of the total strain εt becomes as shown by the solid line in FIG.
Then, the test piece load control means 8 applies a load corresponding to the total strain εt from the total strain waveform determining means 7 to the material.

塑性歪波形出力手段4の出力が最大(=−εp0
になると(第2図のR点)、圧縮荷重から引張荷
重に代わる。このときの、圧縮応力σ2の値が最大
引張圧縮測定手段4で測定される。そして、R点
からS点に至る除荷領域での歪みε2が歪測定手段
2で測定され、これらの測定値σ2,ε2に基づいて
ヤング率計算手段5によつて見掛けのヤング率
E2=σ2/ε2が計算される。
The output of plastic strain waveform output means 4 is maximum (=-εp 0 )
(Point R in Figure 2), the compressive load is replaced by a tensile load. At this time, the value of the compressive stress σ 2 is measured by the maximum tensile compression measuring means 4. Then, the strain ε 2 in the unloading region from point R to point S is measured by the strain measuring means 2, and based on these measured values σ 2 and ε 2 , the Young's modulus calculation means 5 calculates the apparent Young's modulus.
E 222 is calculated.

次に、第2図において、S点からT点に向かう
ような引張荷重を加える場合の制御動作は、Q点
からR点に圧縮荷重を加える場合と正負の符号が
逆になることを除けば基本的に同じである。そし
て、塑性歪波形出力手段4の出力が最大(=+
εp0)になると(第2図のT点)、引重荷重から圧
縮荷重に代わる。このときの、引張応力σ1の値が
最大引張圧縮測定手段4で測定される。そして、
T点からQ点に至る除荷領域での歪みε1が歪測定
手段2で測定され、これらの測定値σ1,ε1に基づ
いてヤング率計算手段5によつて見掛けのヤング
率E1=σ1/ε1が計算される。ヤング率計算手段5
は、これらの各見掛けのヤング率E1,E2の平均
E0=(E1+E2)/2を算出し、この値を弾性歪計
算手段6に送出する。
Next, in Fig. 2, the control operation when applying a tensile load from point S to point T is different from when applying a compressive load from point Q to point R, except that the positive and negative signs are reversed. Basically the same. Then, the output of the plastic strain waveform output means 4 is maximum (=+
εp 0 ) (point T in Figure 2), the tensile load is replaced by a compressive load. At this time, the value of the tensile stress σ 1 is measured by the maximum tensile compression measuring means 4. and,
The strain ε 1 in the unloading region from point T to point Q is measured by the strain measuring means 2, and based on these measured values σ 1 and ε 1 , the Young's modulus calculation means 5 calculates the apparent Young's modulus E 111 is calculated. Young's modulus calculation means 5
is the average of these apparent Young's moduli E 1 and E 2
E 0 =(E 1 +E 2 )/2 is calculated and this value is sent to the elastic strain calculation means 6.

このようにして、引張圧縮の1サイクルごとに
見掛けのヤング率E0が計算され、この計算結果
が次の1サイクルの引張圧縮の繰り返し荷重を加
える際の見掛けの弾性歪εe(=σ/E0)の計算に
利用される。
In this way, the apparent Young's modulus E 0 is calculated for each cycle of tension compression, and this calculation result is used as the apparent elastic strain εe (=σ/E 0 ) is used for calculation.

なお、第1図の装置は、マイクロコンピユータ
で構成することができるのは勿論である。
It goes without saying that the apparatus shown in FIG. 1 can be constructed from a microcomputer.

<発明の効果> 本発明によれば、塑性領域に至るまで材料に引
張圧縮の繰り返し荷重を加え、その引張圧縮の繰
り返しサイクル中に材料の歪みと応力から見掛け
のヤング率を求め、この見掛けのヤング率に基づ
いて見掛けの弾性歪を計算する一方、この計算し
た見掛けの弾性歪を越えた時点で一定速度で塑性
歪が変化するように全歪を決定し、この全歪に対
応する荷重を材料に加えるようにしたので、全歪
制御の下で材料に所定の引張圧縮の繰り返し荷重
を加えることができるとともに、この引張圧縮の
繰り返しサイクル中の塑性領域において、弾性歪
速度が一定となるように制御することが可能とな
る。その結果、塑性歪に依存した材料の特性、た
とえば疲労強度や残留応力の影響等を調べること
ができるようになる等の優れた効果が発揮され
る。
<Effects of the Invention> According to the present invention, repeated tension and compression loads are applied to a material until it reaches the plastic region, and the apparent Young's modulus is determined from the strain and stress of the material during the repeated cycles of tension and compression. While calculating the apparent elastic strain based on the Young's modulus, the total strain is determined so that the plastic strain changes at a constant speed when the calculated apparent elastic strain is exceeded, and the load corresponding to this total strain is calculated. By applying this to the material, it is possible to apply a predetermined repeated tension-compression load to the material under total strain control, and to keep the elastic strain rate constant in the plastic region during the repeated cycles of tension-compression. It becomes possible to control the As a result, excellent effects such as the ability to investigate material properties dependent on plastic strain, such as fatigue strength and the influence of residual stress, are achieved.

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

図面は本発明の実施例を示すもので、第1図は
引張圧縮繰返試験装置の機能ブロツク図、第2図
は応力−歪み線図、第3図は塑性歪−時間線図、
第4図は全歪−時間線図である。 1……応力測定手段、2……歪測定手段、3…
…塑性歪波形出力手段、5……ヤング率計算手
段、6……弾性歪計算手段、7……全歪波形決定
手段、8……試験片荷重制御手段。
The drawings show an embodiment of the present invention, and FIG. 1 is a functional block diagram of a tensile compression cyclic testing device, FIG. 2 is a stress-strain diagram, and FIG. 3 is a plastic strain-time diagram.
FIG. 4 is a total strain-time diagram. 1... Stress measuring means, 2... Strain measuring means, 3...
... plastic strain waveform output means, 5 ... Young's modulus calculation means, 6 ... elastic strain calculation means, 7 ... total strain waveform determination means, 8 ... test piece load control means.

Claims (1)

【特許請求の範囲】 1 弾塑性領域にわたつて材料に引張圧縮の繰り
返し荷重を加えて、その引張圧縮の繰り返しサイ
クル中に材料に加わる応力を測定する応力測定手
段と、 前記繰り返しサイクル中に材料の応力に対応す
る歪みを測定する歪測定手段と、 前記両測定手段からの各測定結果に基づいて見
掛けのヤング率を計算するヤング率計算手段と、 このヤング率計算手段で計算された見掛けのヤ
ング率と前記応力測定手段で測定された応力とに
基づいて見掛けの弾性歪を計算する弾性歪計算手
段と、 予め設定された一定の時間勾配をもつ塑性歪の
波形を与える信号を出力する塑性歪波形出力手段
と、 前記弾性歪計算手段と塑性歪波形出力手段とか
らの両出力により全歪を決定し、この全歪に対応
する信号を出力する全歪波形決定手段と、 この全歪波形決定手段によつて決定された全歪
に対応した荷重を材料に加える試験片荷重制御手
段と、 を備えることを特徴とする引張圧縮繰返試験装
置。
[Scope of Claims] 1. Stress measuring means for applying repeated tension-compression loads to a material over an elasto-plastic region and measuring the stress applied to the material during the repeated cycles of tension-compression; and strain measuring means for measuring the strain corresponding to the stress; a Young's modulus calculating means for calculating the apparent Young's modulus based on the measurement results from both measuring means; and the apparent Young's modulus calculated by the Young's modulus calculating means. an elastic strain calculation means for calculating an apparent elastic strain based on Young's modulus and the stress measured by the stress measurement means; and a plastic strain calculation means for outputting a signal giving a waveform of plastic strain having a preset constant time gradient. strain waveform output means; total strain waveform determining means for determining total strain from both outputs from the elastic strain calculation means and plastic strain waveform output means and outputting a signal corresponding to the total strain; and this total strain waveform. A tensile compression cyclic testing device comprising: test piece load control means for applying a load to the material corresponding to the total strain determined by the determining means;
JP17014682A 1982-09-29 1982-09-29 Plastic strain control apparatus Granted JPS5960242A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP17014682A JPS5960242A (en) 1982-09-29 1982-09-29 Plastic strain control apparatus

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP17014682A JPS5960242A (en) 1982-09-29 1982-09-29 Plastic strain control apparatus

Publications (2)

Publication Number Publication Date
JPS5960242A JPS5960242A (en) 1984-04-06
JPH0221740B2 true JPH0221740B2 (en) 1990-05-16

Family

ID=15899520

Family Applications (1)

Application Number Title Priority Date Filing Date
JP17014682A Granted JPS5960242A (en) 1982-09-29 1982-09-29 Plastic strain control apparatus

Country Status (1)

Country Link
JP (1) JPS5960242A (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS617442A (en) * 1984-06-21 1986-01-14 Saginomiya Seisakusho Inc Plastic strain controlling apparatus

Also Published As

Publication number Publication date
JPS5960242A (en) 1984-04-06

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