JPH0334640Y2 - - Google Patents

Info

Publication number
JPH0334640Y2
JPH0334640Y2 JP1986169991U JP16999186U JPH0334640Y2 JP H0334640 Y2 JPH0334640 Y2 JP H0334640Y2 JP 1986169991 U JP1986169991 U JP 1986169991U JP 16999186 U JP16999186 U JP 16999186U JP H0334640 Y2 JPH0334640 Y2 JP H0334640Y2
Authority
JP
Japan
Prior art keywords
temperature
furnace chamber
temperature measuring
sensors
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
JP1986169991U
Other languages
Japanese (ja)
Other versions
JPS6375795U (en
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 filed Critical
Priority to JP1986169991U priority Critical patent/JPH0334640Y2/ja
Publication of JPS6375795U publication Critical patent/JPS6375795U/ja
Application granted granted Critical
Publication of JPH0334640Y2 publication Critical patent/JPH0334640Y2/ja
Expired legal-status Critical Current

Links

Classifications

    • B—PERFORMING OPERATIONS; TRANSPORTING
    • B30—PRESSES
    • B30B—PRESSES IN GENERAL
    • B30B11/00—Presses specially adapted for forming shaped articles from material in particulate or plastic state, e.g. briquetting presses, tabletting presses
    • B30B11/001—Presses specially adapted for forming shaped articles from material in particulate or plastic state, e.g. briquetting presses, tabletting presses using a flexible element, e.g. diaphragm, urged by fluid pressure; Isostatic presses
    • B30B11/002—Isostatic press chambers; Press stands therefor

Landscapes

  • Physics & Mathematics (AREA)
  • Fluid Mechanics (AREA)
  • Engineering & Computer Science (AREA)
  • Mechanical Engineering (AREA)
  • Powder Metallurgy (AREA)

Description

【考案の詳細な説明】 (産業上の利用分野) 本考案は、熱間静水圧加圧装置に係り、数百乃
至数千気圧の不活性ガスを圧力媒体とし、さらに
同時に千数百度から2000℃以上の高温を発生し
て、粉末材料を高密度に焼結したり、鋳造品の局
部欠陥を圧潰により改善したり、また、種々の材
料を拡散接合したりするのに用いられる。
[Detailed description of the invention] (Field of industrial application) The present invention relates to a hot isostatic pressurization device, which uses an inert gas of several hundred to several thousand atmospheres as a pressure medium, and simultaneously heats the temperature from several hundred degrees to 2000 degrees. It is used to generate high temperatures of 0.degree. C. or higher to sinter powder materials to high density, to improve local defects in cast products by crushing them, and to diffusion bond various materials.

(従来の技術) 熱間静水圧加圧装置(以下、HIPという)は、
その炉内の温度管理が重要であり、このために、
実公昭58−13277号公報の技術がある。
(Conventional technology) Hot isostatic pressurization equipment (hereinafter referred to as HIP) is
Temperature control inside the furnace is important, and for this reason,
There is a technique disclosed in Japanese Utility Model Publication No. 58-13277.

この従来の技術は熱電対を設置して、炉内の温
度を上げることにより、ゼーベツク効果が生じ、
このとき生じた起電力をリード線によつて外部に
取出し、温度に変換するものであり、熱電対素線
としては、白金−ロジウム、タングステン−レニ
ウム等がある。
This conventional technology installs a thermocouple to increase the temperature inside the furnace, which creates the Seebetzk effect.
The electromotive force generated at this time is taken out to the outside through a lead wire and converted into temperature. Examples of thermocouple wires include platinum-rhodium and tungsten-rhenium.

また、熱電対を黒鉛、セラミツク等の有頂筒状
の保護管に収めたものもある。
There is also a thermocouple housed in a capped cylindrical protective tube made of graphite, ceramic, or the like.

(考案が解決しようとする問題点) 前述の従来技術において、HIP処理を連続運
転、繰返し運転等を行うと、温度誤差が大きくな
る。
(Problems to be Solved by the Invention) In the above-mentioned conventional technology, if the HIP treatment is performed continuously or repeatedly, the temperature error becomes large.

これは、起電力という物理量が環境の影響を受
け易いためである。
This is because the physical quantity called electromotive force is easily influenced by the environment.

従つて、HIPにおける2000℃、1000atm以上の
高温、高圧処理では、熱電対の寿命は、低温、低
圧下に対して著しく短かく、コスト的にも問題と
なる。
Therefore, in the high temperature and high pressure treatment of 2000° C. and 1000 atm or more in HIP, the life of the thermocouple is significantly shorter than that at low temperature and low pressure, which also poses a cost problem.

例えば、2000℃、1000atmの条件下では約1時
間で約1%(20℃)の劣化を起こす。
For example, under conditions of 2000°C and 1000 atm, deterioration of about 1% (20°C) occurs in about 1 hour.

本考案は従来の炉内温度測定が起電力によつて
いたものを改め、物質の熱膨張を利用し、材料の
線膨張係数を測定することによつて温度と線膨張
係数との関係から温度を知るとともに、その際、
HIP装置はその性質上、圧力により炉内の温度分
布に違いを生じ易く、特に、炉室下部の温度勾配
は圧力により大きく異なることから当該部分の温
度勾配の影響を補正し得るようにしたことを目的
とする。
This invention replaces the conventional method of measuring temperature inside a furnace based on electromotive force, and uses the thermal expansion of substances to measure the coefficient of linear expansion of the material, thereby determining the relationship between temperature and coefficient of linear expansion. In addition to knowing the temperature,
Due to the nature of HIP equipment, the temperature distribution inside the furnace tends to vary depending on the pressure, and in particular, the temperature gradient in the lower part of the furnace chamber varies greatly depending on the pressure, so we designed it to be able to compensate for the effect of the temperature gradient in that part. With the goal.

(問題点を解決するための手段) 本考案は高圧シリンダ1と、その上下開口部を
密封する上蓋2および下蓋3とによつて画成され
る高圧室4内に、上部が封止された有頂筒状の断
熱層6およびその内部に同心的に配置された加熱
要素8とにより囲繞された炉室9を有し、その炉
室9の温度を測定する測温計を備えている熱間静
水圧加圧装置において、次のような技術的手段を
講じることによつて前述目的を達成したものであ
る。
(Means for Solving the Problems) The present invention has a high pressure chamber 4 defined by a high pressure cylinder 1 and an upper cover 2 and a lower cover 3 that seal the upper and lower openings thereof. It has a furnace chamber 9 surrounded by a capped cylindrical heat insulating layer 6 and a heating element 8 arranged concentrically therein, and is equipped with a thermometer for measuring the temperature of the furnace chamber 9. The above object has been achieved in the hot isostatic pressurizing device by taking the following technical measures.

すなわち、本考案は炉室9内の径方向対応位置
でかつ加熱要素8と径方向略同位置に、耐熱性を
有し線膨張可能な測温棒12がその棒長手方向を
炉室9の高さ方向に沿わされて備えられており、
測温棒12の線膨張による伸縮を測るセンサー1
8の複数を同じ高さ位置に設け該センサー18の
それぞれに長さの異なる測温棒12を各別に設け
たことを特徴とするものである。
That is, in the present invention, a heat-resistant and linearly expandable temperature measuring rod 12 is placed at a radially corresponding position within the furnace chamber 9 and at approximately the same radial position as the heating element 8. It is provided along the height direction,
Sensor 1 that measures expansion and contraction due to linear expansion of temperature measuring rod 12
8 are provided at the same height position, and each of the sensors 18 is provided with a temperature measuring rod 12 having a different length.

(作用) HIP処理中において、炉室9の温度により、測
温棒12が線膨張によつて伸縮する。
(Function) During the HIP process, the temperature measuring rod 12 expands and contracts due to linear expansion depending on the temperature of the furnace chamber 9.

この伸縮により、電磁誘導によるセンサー18
のときは、磁界が変化し、誘導起電力が生じ、こ
の起電力をリード線等により、炉外に伝送し、温
度に換算する。
Due to this expansion and contraction, the electromagnetic induction sensor 18
At this time, the magnetic field changes and an induced electromotive force is generated. This electromotive force is transmitted to the outside of the furnace via lead wires and converted into temperature.

また、センサー18は歪みゲージ22によると
きは、歪み量を炉外に伝送し、温度に換算する。
Further, when the sensor 18 uses the strain gauge 22, the amount of strain is transmitted to the outside of the furnace and converted into temperature.

炉室9の下部における温度勾配部の影響による
測温誤差の補正は、複数本の測温棒12の個々を
センサー18により測定することにより可能とな
る。
Correction of the temperature measurement error due to the influence of the temperature gradient section in the lower part of the furnace chamber 9 becomes possible by measuring each of the plurality of temperature measurement rods 12 with the sensor 18.

すなわち、第9図で示す如く、X部におけるセ
ンサー18とY部におけるセンサー18の相対的
な長さを測定することによりA部の温度が測定で
き、Y部におけるセンサー18とZ部におけるセ
ンサー18の相対的な長さを測定することにより
B部の温度を測定することが可能となる。
That is, as shown in FIG. 9, the temperature of the A section can be measured by measuring the relative lengths of the sensor 18 at the X section and the sensor 18 at the Y section, and the temperature of the A section can be measured by measuring the relative lengths of the sensor 18 at the Y section and the sensor 18 at the Z section. It becomes possible to measure the temperature of part B by measuring the relative length of.

したがつて、A部より下の温度分布の影響(及
び/又は、B部より下の温度分布の影響)を補正
することができるため、温度測定を正確におこな
うことが可能となる。
Therefore, it is possible to correct the influence of the temperature distribution below section A (and/or the influence of the temperature distribution below section B), making it possible to accurately measure temperature.

更に、常にほゞ同一の圧力で使用する場合、測
温部の温度が同じであれば下部の温度勾配は常に
同じであることから、熱電対等の他の方法で校正
しておくことにより、実用上は十分使用可能とな
る。
Furthermore, when using at almost the same pressure all the time, the temperature gradient at the bottom will always be the same if the temperature of the temperature measuring part is the same, so by calibrating with other methods such as thermocouples, The top is fully usable.

(実施例) 以下、図面を参照して本考案の実施例を詳述す
る。
(Example) Hereinafter, an example of the present invention will be described in detail with reference to the drawings.

第1図において、1は高圧シリンダであり、上
下開口部を有する円筒体である。
In FIG. 1, 1 is a high-pressure cylinder, which is a cylindrical body having upper and lower openings.

2は上蓋、3は下蓋であり、高圧シリンダ1の
上下開口部を密封しており、ここに、高圧シリン
ダ1、上蓋2および下蓋3とによつて画成される
高圧室4を有する。
2 is an upper lid, and 3 is a lower lid, which seals the upper and lower openings of the high-pressure cylinder 1, and has a high-pressure chamber 4 defined by the high-pressure cylinder 1, the upper lid 2, and the lower lid 3. .

なお、上蓋2および下蓋3はそれぞれ挿脱自在
であり、プレスフレーム5が係合されることによ
つてプレス軸力は坦持可能であり、プレスフレー
ム5は走行架台形、旋回形等がある。
Note that the upper lid 2 and the lower lid 3 can be inserted and removed freely, and the press axial force can be supported by engaging the press frame 5. be.

6は断熱層であり、上部が封止された有頂筒状
であり、上蓋2に吊具7によつて支持され、高圧
室4内に同心的に配置されている。
Reference numeral 6 denotes a heat insulating layer, which has a capped cylindrical shape with a sealed upper part, is supported by a hanger 7 on the upper lid 2, and is arranged concentrically within the high pressure chamber 4.

8は加熱要素であり、断熱層6の内部に同心的
に配置され、ここに、加熱要素8、断熱層6で囲
繞された炉室9を有し、この炉室9の下部には炉
床10を有し、この炉床10は試料台であり、被
処理体11を本実施例では下部より挿脱自在とし
ている。
A heating element 8 is arranged concentrically inside the heat insulating layer 6, and has a furnace chamber 9 surrounded by the heating element 8 and the heat insulating layer 6, and a hearth in the lower part of the furnace chamber 9. 10, this hearth 10 is a sample stand, and in this embodiment, the object to be processed 11 can be freely inserted and removed from the lower part.

なお、加熱要素8はこれを多段に設けるもので
あつてもよい。
Note that the heating element 8 may be provided in multiple stages.

12は測温棒であり、第2図に示す如く、炉室
9内における径方向対応位置で、加熱要素8と同
心円上(径方向略同一位置)に配置され、その棒
長手方向は炉室9の高さ方向に沿わせている。
Reference numeral 12 denotes a temperature measuring rod, and as shown in FIG. 2, it is arranged concentrically with the heating element 8 (approximately the same position in the radial direction) at a radially corresponding position in the furnace chamber 9, and the rod's longitudinal direction is radially corresponding to the heating element 8. 9 along the height direction.

この測温棒12はタングステン、セラミツクス
等のように、耐熱性を有し線膨張可能な材料より
なつており、第3図、第4図に示す構造で支持さ
れている。
The temperature measuring rod 12 is made of a heat-resistant and linearly expandable material such as tungsten or ceramics, and is supported by the structure shown in FIGS. 3 and 4.

すなわち、第5図に示す如く試料台10にネジ
13で着脱自在とされた有頂筒状の保護筒14の
上部に、第3図で示す如くメネジ14Aを形成
し、このメネジ14Aに測温棒12の頂部オネジ
15をネジ込むか、又は、第4図に示す如くピン
16によつて取付けられている。
That is, as shown in FIG. 3, a female thread 14A is formed on the top of a crested cylindrical protection tube 14 which is detachably attached to the sample stage 10 with a screw 13 as shown in FIG. It is attached by screwing in the top male thread 15 of the rod 12 or by a pin 16 as shown in FIG.

なお、保護筒14はグラフアイト、黒鉛等によ
りなり、試料台10への取付けは、第6図で示す
如くネジ17によるものであつてもよい。
The protective tube 14 may be made of graphite, graphite, or the like, and may be attached to the sample stage 10 using screws 17 as shown in FIG.

又、ピン16はタングステン、セラミツクス等
によりなる。
Further, the pin 16 is made of tungsten, ceramics, or the like.

18はセンサーであり、第5図、第6図の実施
例では円筒磁石19にコイル20を巻回してお
り、磁石19を試料台10に図外の支持具で取付
け、磁石19内の中心に、第7図でも示すように
測温棒12の下端を挿通することにより構成され
ている。
18 is a sensor, and in the embodiment shown in FIGS. 5 and 6, a coil 20 is wound around a cylindrical magnet 19. The magnet 19 is attached to the sample stage 10 with a support (not shown), and a , as shown in FIG. 7, is constructed by inserting the lower end of the temperature measuring rod 12.

従つて、この第5図、第6図の実施例ではHIP
処理中の炉室9の温度変化により、測温棒12が
線膨張して伸縮し、この伸縮により磁界が変化
し、誘導起電力が生じ、この起電力をリード線等
により炉外へ伝送し、温度に換算することにな
る。
Therefore, in the embodiments shown in FIGS. 5 and 6, HIP
Due to temperature changes in the furnace chamber 9 during processing, the temperature measuring rod 12 expands and contracts linearly, and this expansion and contraction changes the magnetic field, generating an induced electromotive force, which is transmitted to the outside of the furnace through lead wires, etc. , which will be converted into temperature.

更にまた、第8図で示す如く、金属板21にス
トレインゲージ22を取付け、金属板21に測温
棒12が伸縮するのを歪みとして読取るようにし
たセンサー18であつてもよい。
Furthermore, as shown in FIG. 8, the sensor 18 may be such that a strain gauge 22 is attached to a metal plate 21 and the expansion and contraction of the temperature measuring rod 12 on the metal plate 21 is read as strain.

すなわち、センサー18は第5〜7図で示す電
磁誘導を利用したものでも、第8図に示す歪ゲー
ジでもよい。
That is, the sensor 18 may be a sensor using electromagnetic induction as shown in FIGS. 5 to 7, or a strain gauge as shown in FIG.

更に、センサー18の測定はリード線等によつ
て下蓋3より炉外に取出すことができる。
Furthermore, the measurement by the sensor 18 can be taken out of the furnace through the lower lid 3 using a lead wire or the like.

第9図は下部の温度勾配部の影響による測温誤
差を補正できるようにしたもので、センサー18
の位置は同じとし、測温棒12の長さに符号A,
Bの如く差を有するものを用いたものであり、セ
ンサー18のX,Y位置の相対長さAを、センサ
ー18のY,Z位置の相対長さBの温度を測定す
ることにより、誤差を補正できる。
Figure 9 shows a sensor 18 that can correct temperature measurement errors due to the influence of the temperature gradient section at the bottom.
The positions of are the same, and the length of the temperature measuring rod 12 is marked A,
By measuring the relative length A between the X and Y positions of the sensor 18 and the relative length B between the Y and Z positions of the sensor 18, the error can be eliminated. It can be corrected.

すなわち、HIP装置はその性質上、圧力により
炉内の温度分布に違いを生じやすい。特に、炉室
下部の温度分布は圧力により大きく異なる。本考
案の線膨張を利用した温度計の場合、この炉室下
部の温度分布の違いが温度測定の精度の大きな影
響を及ぼす。すなわち、炉室下部の温度勾配によ
つて測温棒12の伸びが異なるのである。この炉
室下部の温度勾配の影響を補正するため第9図に
示す如く、センサー18の位置を同じ高さに設置
し、長さの異なる測温棒12を符号A,Bの如く
差を有するように個別に設置すると、センサX,
Yによつて相対高さ(長さ)Aの部分の温度を測
定することが可能となり、センサY,Zによつて
相対高さ(長さ)Bの部分の温度を測定すること
が可能となる。したがつて、A部より下の温度分
布の影響(及び/又は、B部より下の温度分布の
影響)を補正することができるため、温度測定を
正確に行うことが可能となる。
In other words, due to the nature of HIP equipment, pressure tends to cause differences in temperature distribution within the furnace. In particular, the temperature distribution in the lower part of the furnace chamber varies greatly depending on the pressure. In the case of the thermometer using linear expansion of the present invention, this difference in temperature distribution in the lower part of the furnace chamber has a large effect on the accuracy of temperature measurement. That is, the elongation of the temperature measuring rod 12 differs depending on the temperature gradient in the lower part of the furnace chamber. In order to compensate for the influence of the temperature gradient in the lower part of the furnace chamber, the sensors 18 are installed at the same height as shown in FIG. When installed individually like this, sensors X,
Sensor Y makes it possible to measure the temperature at the relative height (length) A, and sensors Y and Z make it possible to measure the temperature at the relative height (length) B. Become. Therefore, it is possible to correct the influence of the temperature distribution below section A (and/or the influence of the temperature distribution below section B), making it possible to accurately measure temperature.

その他、第1図において、圧媒(アルゴン等の
不活性ガス)の供給、排出手段等を具有してい
る。
In addition, as shown in FIG. 1, it is equipped with means for supplying and discharging a pressure medium (inert gas such as argon), etc.

また、加熱要素の給電回路等、HIPに必要な部
材は当然具備されており、センサー18の検出は
増巾器等により、演算部(測定制御部)等に連絡
される。
Furthermore, necessary components for HIP such as a power supply circuit for the heating element are naturally provided, and the detection by the sensor 18 is communicated to the calculation section (measurement control section) etc. through an amplifier or the like.

(考案の効果) 本考案によれば、炉内(室)の測温にさいし
て、従来例の如く、熱電対による起電力という物
理量が環境の影響を受け易いものを用いず、測温
棒の熱膨張を利用し、材料の線膨張係数を測定す
ることによつて、温度と線膨張係数との関係(比
例関係)を知るものであるから、HIPにおいて連
続運転、繰返し運転等を行つても、安定した測温
が可能で、また、再現性がよいため寿命も長くで
きる。
(Effects of the invention) According to the invention, when measuring the temperature inside the furnace (room), a temperature measuring stick is not used, unlike the conventional example, in which the physical quantity of electromotive force caused by a thermocouple is easily influenced by the environment. The relationship (proportional relationship) between temperature and linear expansion coefficient can be determined by measuring the linear expansion coefficient of the material using the thermal expansion of It also enables stable temperature measurement and has good reproducibility, so it can have a long service life.

また、測温棒は加熱要素と径方向同位置(同心
円上)に配置されているので、測温のために必要
なスペースを低減でき、結果として炉室の容積の
より効率的な使用が可能となる。
In addition, since the temperature measuring rod is placed radially at the same position as the heating element (on a concentric circle), the space required for temperature measurement can be reduced, resulting in more efficient use of the volume of the furnace chamber. becomes.

更に、HIP装置はその性質上、圧力により炉内
の温度分布に違いを生じやすい。特に、炉室下部
の温度分布は圧力により大きく異なる。本考案の
線膨張を利用した温度計の場合、この炉室下部の
温度分布の違いが温度測定の精度に大きな影響を
及ぼす。すなわち、炉室下部の温度勾配によつて
測温棒12の伸びが異なるのである。この炉室下
部の温度勾配の影響を補正するため本考案ではセ
ンサー18の位置を同じ高さに設置し、長さの異
なる測温棒12を符号A,Bの如く差を有するよ
うに各別に設置することによつて、センサX,Y
によつて相対高さ(長さ)Aの部分の温度を測定
することが可能となり、センサY,Zによつて相
対高さ(長さ)Bの部分の温度を測定することが
可能となる。したがつて、A部より下の温度分布
の影響(及び/又は、B部より下の温度分布の影
響)を補正することができないため、温度測定を
正確に行うことが可能となる。
Furthermore, due to the nature of HIP equipment, pressure tends to cause differences in temperature distribution within the furnace. In particular, the temperature distribution in the lower part of the furnace chamber varies greatly depending on the pressure. In the case of the thermometer using linear expansion of the present invention, this difference in temperature distribution in the lower part of the furnace chamber has a large effect on the accuracy of temperature measurement. That is, the elongation of the temperature measuring rod 12 differs depending on the temperature gradient in the lower part of the furnace chamber. In order to compensate for the influence of the temperature gradient in the lower part of the furnace chamber, in the present invention, the sensor 18 is installed at the same height, and the temperature measuring rods 12 of different lengths are placed separately as shown by the symbols A and B. By installing sensors
It becomes possible to measure the temperature at a portion of relative height (length) A, and it becomes possible to measure the temperature at a portion of relative height (length) B using sensors Y and Z. . Therefore, since it is not possible to correct the influence of the temperature distribution below part A (and/or the influence of temperature distribution below part B), it is possible to accurately measure temperature.

従つて、HIP装置に固有の問題点を解決するこ
とができるので、本考案は通常の線膨張を利用し
た温度測定装置と異なり、固有の意義があるもの
である。
Therefore, since the problems specific to HIP devices can be solved, the present invention has unique significance, unlike ordinary temperature measuring devices that utilize linear expansion.

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

図面は本考案の実施例を示し、第1図は縦断立
面図、第2図は第1図−線拡大断面図、第3
図と第4図は測温棒取付け(支持部)の2例を示
す断面図、第5図と第6図はセンサー部分の2例
を示す断面図、第7図はセンサーの斜視図、第8
図はセンサーの他の例を示す立面図、第9図は測
温棒の配置例を示す説明図である。 1……高圧シリンダ、2……上蓋、3……下
蓋、4……高圧室、6……断熱層、8……加熱要
素、9……炉室、12……測温棒、18……セン
サー。
The drawings show an embodiment of the present invention, and FIG. 1 is a vertical sectional elevation view, FIG. 2 is an enlarged cross-sectional view taken along lines from FIG.
Figures 5 and 4 are cross-sectional views showing two examples of temperature measuring rod attachment (support part), Figures 5 and 6 are cross-sectional views showing two examples of the sensor part, Figure 7 is a perspective view of the sensor, 8
The figure is an elevational view showing another example of the sensor, and FIG. 9 is an explanatory diagram showing an example of the arrangement of temperature measuring rods. DESCRIPTION OF SYMBOLS 1... High pressure cylinder, 2... Upper cover, 3... Lower cover, 4... High pressure chamber, 6... Heat insulation layer, 8... Heating element, 9... Furnace chamber, 12... Temperature measuring rod, 18... …sensor.

Claims (1)

【実用新案登録請求の範囲】 高圧シリンダ1と、その上下開口部を密封する
上蓋2および下蓋3とによつて画成される高圧室
4内に、上部が封止された有頂筒状の断熱層6お
よびその内部に同心的に配置された加熱要素8と
により囲繞された炉室9を有し、その炉室9の温
度を測定する測温計を備えている熱間静水圧加圧
装置において、 炉室9内の径方向対応位置でかつ加熱要素8と
径方向略同位置に、耐熱性を有し線膨張可能な測
温棒12がその棒長手方向を炉室9の高さ方向に
沿わされて備えられており、測温棒12の線膨張
による伸縮を測るセンサー18の複数を同じ高さ
位置に設け、該センサー18のそれぞれに長さの
異なる測温棒12を各別に設けたことを特徴とす
る熱間静水圧加圧装置。
[Claims for Utility Model Registration] A high-pressure chamber 4 defined by a high-pressure cylinder 1 and an upper cover 2 and a lower cover 3 that seal the upper and lower openings of the cylinder has a crested cylindrical shape whose upper part is sealed. A hot isostatic press having a furnace chamber 9 surrounded by a heat insulating layer 6 and a heating element 8 arranged concentrically therein, and equipped with a thermometer for measuring the temperature of the furnace chamber 9. In the pressure device, a heat-resistant and linearly expandable temperature measuring rod 12 is installed at a radially corresponding position in the furnace chamber 9 and at approximately the same position in the radial direction as the heating element 8 . A plurality of sensors 18 are provided along the longitudinal direction and measure the expansion and contraction due to linear expansion of the temperature measuring rod 12. A plurality of sensors 18 are provided at the same height position, and temperature measuring rods 12 of different lengths are attached to each of the sensors 18. A hot isostatic pressurizing device characterized in that it is separately provided.
JP1986169991U 1986-11-05 1986-11-05 Expired JPH0334640Y2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP1986169991U JPH0334640Y2 (en) 1986-11-05 1986-11-05

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP1986169991U JPH0334640Y2 (en) 1986-11-05 1986-11-05

Publications (2)

Publication Number Publication Date
JPS6375795U JPS6375795U (en) 1988-05-20
JPH0334640Y2 true JPH0334640Y2 (en) 1991-07-23

Family

ID=31104300

Family Applications (1)

Application Number Title Priority Date Filing Date
JP1986169991U Expired JPH0334640Y2 (en) 1986-11-05 1986-11-05

Country Status (1)

Country Link
JP (1) JPH0334640Y2 (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2008032419A (en) * 2006-07-26 2008-02-14 Denso Corp Temperature detection element

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP6057812B2 (en) 2013-04-02 2017-01-11 株式会社神戸製鋼所 Processing apparatus and workpiece temperature measurement method
JP6433375B2 (en) * 2015-05-21 2018-12-05 株式会社神戸製鋼所 Temperature correction method for hot isostatic pressurizer

Family Cites Families (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5370478A (en) * 1976-12-06 1978-06-22 Fujitsu Ten Ltd High temperature sensor for motorcar
JPS5711129A (en) * 1980-06-24 1982-01-20 Kyokuto Kaihatsu Kogyo Co Ltd Transportation vehicle
JPS59193998U (en) * 1983-05-19 1984-12-22 株式会社神戸製鋼所 Hot isostatic press equipment

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2008032419A (en) * 2006-07-26 2008-02-14 Denso Corp Temperature detection element

Also Published As

Publication number Publication date
JPS6375795U (en) 1988-05-20

Similar Documents

Publication Publication Date Title
US5962791A (en) Pirani+capacitive sensor
CN114364959B (en) Non-invasive thermometer
JP2006119139A (en) Combustion kiln
EP3070444B1 (en) A surface temperature measuring device
KR101503570B1 (en) Heat treatment apparatus and temperature measuring method thereof
JP2022515626A (en) Remote sealing system with improved temperature compensation
JP3608241B2 (en) Thermal deformation measuring device
Masui Development of a magnetic suspension densimeter and measurement of the density of toluene
Merlone et al. Gas-controlled heat pipes for accurate liquid-vapor transition measurements
Sears et al. Pressurized thermobalance apparatus for use in oxidizing atmospheres at high temperatures
Glawe et al. Long term drift of some noble and refractory metal thermocouples at 1600 K in air, argon, and vacuum
JPH0684929B2 (en) Inpile creep test equipment
JP2909922B2 (en) Temperature compensation method for thermomechanical analysis
GB2114293A (en) Equipment for calibration of instruments having a temperature sensing unit
CN114430802B (en) Thermometer
RU171596U1 (en) DEVICE FOR RESEARCH OF RADIATION SURVEILLANCE OF NUCLEAR FUEL OF ENERGY REACTORS
CN104395718A (en) Temperature measuring system and temperature measuring device
JPH0467136B2 (en)
JPH05248961A (en) Displacement amount measuring device
Ulanovskiy et al. An approach to Tungsten-rhenium thermocouple calibration in the temperature range 1200-2500° C
JPH06240302A (en) Measuring method and device in hot isostatic pressing device
KR101715174B1 (en) Apparatus for measuring thermal conductivity using hot-wire
Brost et al. High Temperature Heat Pipe Furnaces for Material Processing
JPH0523573A (en) Control method of pressure in ultra high pressure equipment
Boyd An isothermal calorimeter for solid-state reactions