JPS6166945A - Method and device for measuring young's modulus and internal friction - Google Patents

Method and device for measuring young's modulus and internal friction

Info

Publication number
JPS6166945A
JPS6166945A JP59190129A JP19012984A JPS6166945A JP S6166945 A JPS6166945 A JP S6166945A JP 59190129 A JP59190129 A JP 59190129A JP 19012984 A JP19012984 A JP 19012984A JP S6166945 A JPS6166945 A JP S6166945A
Authority
JP
Japan
Prior art keywords
platinum
sample
electrode
jig
modulus
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
JP59190129A
Other languages
Japanese (ja)
Other versions
JPH0137687B2 (en
Inventor
Kenichi Matsushita
健一 松下
Taira Okamoto
平 岡本
Masahiko Shimada
昌彦 島田
Hisao Takeuchi
久雄 竹内
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.)
Osaka University NUC
Sumitomo Electric Industries Ltd
Original Assignee
Osaka University NUC
Sumitomo Electric Industries 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 Osaka University NUC, Sumitomo Electric Industries Ltd filed Critical Osaka University NUC
Priority to JP59190129A priority Critical patent/JPS6166945A/en
Publication of JPS6166945A publication Critical patent/JPS6166945A/en
Publication of JPH0137687B2 publication Critical patent/JPH0137687B2/ja
Granted legal-status Critical Current

Links

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
    • G01N3/32Investigating strength properties of solid materials by application of mechanical stress by applying repeated or pulsating forces
    • G01N3/38Investigating strength properties of solid materials by application of mechanical stress by applying repeated or pulsating forces generated by electromagnetic means
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01NINVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N33/00Investigating or analysing materials by specific methods not covered by groups G01N1/00 - G01N31/00
    • G01N33/38Concrete; Lime; Mortar; Gypsum; Bricks; Ceramics; Glass
    • G01N33/388Ceramics

Landscapes

  • Physics & Mathematics (AREA)
  • Electromagnetism (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 Or Analyzing Materials By The Use Of Ultrasonic Waves (AREA)
  • Investigating Strength Of Materials By Application Of Mechanical Stress (AREA)
  • Measurement Of Mechanical Vibrations Or Ultrasonic Waves (AREA)

Abstract

PURPOSE:To measure nonconductive ceramics, etc., by providing a platinum electrode on one end surface of a plate type sample to be measured by applying platinum paste. CONSTITUTION:The sample 1 is placed on a jig 2 which has two projection parts with the platinum electrode 11 down. Platinum wires 7 are provided to the projection parts of the jig 2 and the platinum electrode 12 of the sample 1 is placed on the platinum wires 7. Earth-side wires is superposed on a container 3. Then, when the sample 1 is placed on the two platinum wires, the platinum electrode 11 on the sample 1 contacts the earth-side platinum wire between the two platinum wires 7 and is set on a driving electrode 11 on the jig 2. Then, an alternating voltage is applied from an alternating voltage source 5 between the electrode 8 and platinum electrode 11 to oscillate the sample 1. At this time, the electrode is placed in the center of the sample 1 to double the amplitude of the oscillation, thereby obtaining efficient oscillation. For the purpose, a measurement is taken while the ambient temperature is varied.

Description

【発明の詳細な説明】 (イ)技術分野 本発明はセラミックス、金属、木材等のヤング率、内部
摩擦を測定する方法及び’A jlvf“に関するもの
で測定状f1が導電性が無くてもulいN度範囲(−2
50°C〜1300°C)で測定し得るものである。
Detailed Description of the Invention (a) Technical Field The present invention relates to a method for measuring the Young's modulus and internal friction of ceramics, metals, wood, etc. N degree range (-2
50°C to 1300°C).

(0)従来技術の問題点 従来のヤング率測定法として第2図に示すような試14
1を2木の白金線7によって吊下げて」(娠させる方法
がある。1oは加熱用炉体、8がシューカー、9が検出
器である。この方法では吊下用白金線の共振が生じ、測
定状$1の共振周波数が見つけがたく、白金線が太いた
めそこで生ずる振動のロスが大きい。又吊下げている点
が振動の節となっているため試料を振動させる効率が悲
くヤング率内部摩擦の測定値の誤差が大きい。又この方
法では、炉体11部に孔(10’)が開いているため雰
囲気の1凋整かむ・)かしい。
(0) Problems with the conventional technology As a conventional method for measuring Young's modulus, trial 14 as shown in Figure 2
1 is suspended by two platinum wires 7. 1o is a heating furnace body, 8 is a shoer, and 9 is a detector. In this method, resonance of the hanging platinum wires occurs. It is difficult to find the resonant frequency of $1 in the measurement state, and the platinum wire is thick, so there is a large vibration loss.Also, the hanging point is a node of vibration, so the efficiency of vibrating the sample is poor. The error in the measured value of internal friction is large.In addition, this method has a hole (10') in the furnace body 11, which makes it difficult to stabilize the atmosphere.

(ハ)発明の間車 固体6才1のヤング撞く及び内部摩擦を共振性て測定゛
4る場合、いかに試t1を効率よく振動させるかが改質
′Cあり1記従来2人の問題を解決すべく種々検A1シ
た結果本発明に到った。
(C) During the invention, when measuring the Young's vibration and internal friction of a 6-year-old solid vehicle by resonance, how to vibrate the test t1 efficiently is a modification 'C1. As a result of various tests to solve the problem, we have arrived at the present invention.

本発明の特徴は、板状潤定試t1の一端面に白金ペース
)中布等によっ゛C白金電極を付Ijすることにある。
A feature of the present invention is that a platinum electrode (Ij) is attached to one end surface of the plate-shaped moisture test t1 using a platinum paste or the like.

これによってノ1導電P1のセラミックス、木(イブラ
スチック等の測定も可能になった。
This has made it possible to measure ceramics, wood (i-plastic, etc.) with a conductivity of P1.

第3図は本発明の測定に用いる試$11の斜視図であり
、その端面に白金電極11を付I″i−する。この試$
1を白金電極をド面として2つの凸出部を有する冶I!
21・に載仕る。治具の凸出部には各々白金線7が設置
1られ、試料の白金電極12の部分が白金線7の1−に
載るようにする。3はアース側の線が重なる個所である
。第4図は測定試料が治具のLに載った状態の1而図で
あり、これを第1図に示す如り、1°〔空1)l’ I
ll I l又は雰囲気ガス導入1]4を有する容器3
内に設置する。試第1が2本の白金線の1に載った場合
、試料1−の白金電極が2木の白金線のうちアース側の
1本と接触し、史に治具1の駆動電極8のににくるよう
にする。駆動電極8と試$1而1−の白金電極との間に
交番電圧を交番電圧源5によって印加し試ネ1を振動さ
せる。この特、電極を試料の中央に置くことによって娠
動娠中が約21八となり非常に効率よい振動が生じる。
FIG. 3 is a perspective view of a sample 11 used in the measurement of the present invention, and a platinum electrode 11 is attached to the end face of the sample 11.
1 has two protrusions with the platinum electrode as a do-face!
Published on 21. A platinum wire 7 is installed on each of the protrusions of the jig so that the platinum electrode 12 portion of the sample rests on the platinum wire 7 1-. 3 is the location where the ground side wires overlap. Figure 4 shows a state in which the measurement sample is placed on L of the jig.
ll I l or atmospheric gas introduction 1] Container 3 with 4
Installed inside. When test No. 1 is placed on one of the two platinum wires, the platinum electrode of sample No. 1 comes into contact with one of the two platinum wires on the ground side, and the drive electrode 8 of jig No. Make sure to come. An alternating voltage is applied by an alternating voltage source 5 between the drive electrode 8 and the platinum electrode of the sample 1 to vibrate the sample 1. In this particular case, by placing the electrode in the center of the sample, the gestational period is about 218, and very efficient vibration is produced.

容器3内は外部加熱により特定温度に維持することによ
り1300℃まで測定することができる。低温の場合は
油体ヘリウムを使m L 、 −2soでまでiす能で
ある。又測定雰囲気としてはr【空、並びにAr、N2
などの11酸化性雰囲気にすることができる。
By maintaining the inside of the container 3 at a specific temperature by external heating, measurements can be made up to 1300°C. At low temperatures, oil-body helium can be used to reduce the temperature down to m L , -2so. In addition, the measurement atmosphere was r [empty, as well as Ar and N2].
It is possible to create an oxidizing atmosphere such as 11.

治具2は高温に耐えられるようにA(!203やBN製
とする。・試料1の大きさは、IX 5X 211mm
〜3×15XI50mmの範囲内であるが治具の寸法を
変えることによって他の任意の大きさにすることができ
る。
Jig 2 is made of A (!203 or BN) to withstand high temperatures. - The size of sample 1 is IX 5X 211mm.
Although it is within the range of 3 x 15 x I50 mm, it can be made to any other size by changing the dimensions of the jig.

次に実施例によって説明する。Next, an example will be explained.

実施例 AQ203及びSi3N4焼結体テI 、5+n X 
l05m X GOsmの大きさに加1.シ、その一端
面に白金ペーストをゆ石焼付は第1図に示す装置を用い
て常温及び、高l易Cのヤング率、内部摩擦を測定した
。その結果を第5図に示す。白丸(El)、黒丸(E2
)は各々ΔQ203、Si3N4のヤング率、内角(Q
2L黒角(Qllは各々AQ203.5i3Naの内部
摩擦である。
Example AQ203 and Si3N4 sintered body TeI, 5+nX
In addition to the size of l05m x GOsm, 1. After baking a platinum paste on one end surface, Young's modulus and internal friction were measured at room temperature and at a high temperature using the apparatus shown in FIG. The results are shown in FIG. White circle (El), black circle (E2
) are ΔQ203, Young's modulus of Si3N4, and interior angle (Q
2L black angle (Qll is the internal friction of AQ203.5i3Na, respectively.

【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の正面断面図、第2図は従来
の7Illl定法の説明図、第3図は本発明の測定に用
いる試f1の斜視図、第4図は本発明の試!4のセント
状態を示す1而図及び第5図は本発明の測定法及び装置
nによる実施例のヤング率、内部摩擦のi!II+定結
果である。 1:試料、2:治具、3:容器、4:排気[1、又は導
入11.5:交番電圧源、6:熱電対、7:白金線、8
:駆動電極、9:検出器、IO=炉体、10′:空孔、
11:白金電極、 El : AQ203ヤング率、1
号2 : 5iaN4ヤ/グ率、Ql : 5i3tJ
+内部摩擦、Q2 : AQ203内部摩擦。
Fig. 1 is a front sectional view of the measuring device of the present invention, Fig. 2 is an explanatory diagram of the conventional 7Ill standard method, Fig. 3 is a perspective view of sample f1 used in the measurement of the present invention, and Fig. 4 is a test sample of the present invention. ! Figure 1 and Figure 5, which show the cent state of 4, are Young's modulus and internal friction i! II+ constant result. 1: Sample, 2: Jig, 3: Container, 4: Exhaust [1 or introduction 11.5: Alternating voltage source, 6: Thermocouple, 7: Platinum wire, 8
: Drive electrode, 9: Detector, IO=Furnace body, 10': Hole,
11: Platinum electrode, El: AQ203 Young's modulus, 1
No. 2: 5iaN4 Y/G rate, Ql: 5i3tJ
+ Internal friction, Q2: AQ203 internal friction.

Claims (3)

【特許請求の範囲】[Claims] (1)固体試料の板状一端面に白金電極を付し、この試
料を特定間隔をもって白金線が装着された凸出する部分
を有する治具上に載せ、該板状試料の白金電極と駆動用
電極との間に交番電圧を印加して共振動せしめ、周囲温
度を変化せしめて測定することを特徴とするヤング率及
び内部摩擦の測定方法。
(1) A platinum electrode is attached to one end surface of a plate-shaped solid sample, and the sample is placed on a jig having a protruding part to which a platinum wire is attached at a specific interval, and the platinum electrode of the plate-shaped sample and the drive A method for measuring Young's modulus and internal friction, characterized in that measurement is performed by applying an alternating voltage between the measuring electrode and an electrode to cause resonance and changing the ambient temperature.
(2)試料を共振させる際の周波数が50Hz〜200
00Hzの範囲であることを特徴とする特許請求の範囲
第1項記載のヤング率及び内部摩擦の測定方法。
(2) The frequency when making the sample resonate is 50Hz to 200Hz.
2. The method for measuring Young's modulus and internal friction according to claim 1, wherein the Young's modulus and internal friction are measured in a range of 0.00 Hz.
(3)真空排気口又は雰囲気ガス導入口を有する加熱手
段を具備する容器内に板上固体試料を載せる耐熱性治具
が設置され、該治具には白金線が上面に装着された凸出
部があり、該治具中には温度測定のための熱電対が装着
され、上記治具に装着された白金線を通じ交番電圧源が
設けられ、板状固体試料の一端面には白金電極が設けら
れていることを特徴とするヤング率及び内部摩擦の測定
装置。
(3) A heat-resistant jig for placing the solid sample on a plate is installed in a container equipped with a heating means having a vacuum exhaust port or an atmospheric gas inlet, and the jig has a protruding surface with a platinum wire attached to the top surface. A thermocouple for temperature measurement is attached to the jig, an alternating voltage source is provided through a platinum wire attached to the jig, and a platinum electrode is attached to one end surface of the plate-shaped solid sample. A device for measuring Young's modulus and internal friction, characterized in that:
JP59190129A 1984-09-10 1984-09-10 Method and device for measuring young's modulus and internal friction Granted JPS6166945A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP59190129A JPS6166945A (en) 1984-09-10 1984-09-10 Method and device for measuring young's modulus and internal friction

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP59190129A JPS6166945A (en) 1984-09-10 1984-09-10 Method and device for measuring young's modulus and internal friction

Publications (2)

Publication Number Publication Date
JPS6166945A true JPS6166945A (en) 1986-04-05
JPH0137687B2 JPH0137687B2 (en) 1989-08-09

Family

ID=16252873

Family Applications (1)

Application Number Title Priority Date Filing Date
JP59190129A Granted JPS6166945A (en) 1984-09-10 1984-09-10 Method and device for measuring young's modulus and internal friction

Country Status (1)

Country Link
JP (1) JPS6166945A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH03243845A (en) * 1990-02-21 1991-10-30 Masaru Sakata Method and device for measuring elasticity coefficient of solid material with shock sound
JPH0469736U (en) * 1990-10-29 1992-06-19

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH03243845A (en) * 1990-02-21 1991-10-30 Masaru Sakata Method and device for measuring elasticity coefficient of solid material with shock sound
JPH0469736U (en) * 1990-10-29 1992-06-19

Also Published As

Publication number Publication date
JPH0137687B2 (en) 1989-08-09

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