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JPS5949478B2 - Thermal expansion absorption device for liquid metal piping - Google Patents
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JPS5949478B2 - Thermal expansion absorption device for liquid metal piping - Google Patents

Thermal expansion absorption device for liquid metal piping

Info

Publication number
JPS5949478B2
JPS5949478B2 JP56087666A JP8766681A JPS5949478B2 JP S5949478 B2 JPS5949478 B2 JP S5949478B2 JP 56087666 A JP56087666 A JP 56087666A JP 8766681 A JP8766681 A JP 8766681A JP S5949478 B2 JPS5949478 B2 JP S5949478B2
Authority
JP
Japan
Prior art keywords
liquid metal
piping
thermal expansion
bellows
pipe
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
JP56087666A
Other languages
Japanese (ja)
Other versions
JPS57204395A (en
Inventor
「こう」介 坂野
茂男 林
実 赤津
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.)
Kawasaki Heavy Industries Ltd
Original Assignee
Kawasaki Heavy 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 Kawasaki Heavy Industries Ltd filed Critical Kawasaki Heavy Industries Ltd
Priority to JP56087666A priority Critical patent/JPS5949478B2/en
Publication of JPS57204395A publication Critical patent/JPS57204395A/en
Publication of JPS5949478B2 publication Critical patent/JPS5949478B2/en
Expired legal-status Critical Current

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Description

【発明の詳細な説明】 本発明は、液体金属用配管の熱膨脹吸収装置に関する。[Detailed description of the invention] The present invention relates to a thermal expansion absorption device for liquid metal piping.

液体金属冷却高速増殖炉では、1次冷却系および2次冷
却系の熱媒体としてナトリウム等の液体金属を用いるが
、1次及び2次冷却系の通常運転の温度は、約500℃
と高温である。
In a liquid metal cooled fast breeder reactor, liquid metal such as sodium is used as a heat medium in the primary and secondary cooling systems, and the normal operating temperature of the primary and secondary cooling systems is approximately 500°C.
and high temperature.

従来、このような高温の熱媒体を流す配管は、配管の熱
膨脹による応力を緩和するため、複雑な配管引廻しとす
るのが通例である。
Conventionally, piping through which such a high-temperature heat medium flows has generally been designed to have a complicated piping layout in order to relieve stress caused by thermal expansion of the piping.

この場合配管長が長大になるため、ハンガ・スナツバ数
の増大、保温材の増大のみならず配管内圧力損失の増大
に循環ポンプ揚程の増大ひいては建物物量の増大をoも
たらし、プラント建設費の増大を招く要因となつている
。近年このようなプラント建設費の増大を改善する手段
として、配管系にベローズ継手を用いて熱膨脹を吸収し
、配管系をコンパクト化する試みが5なされているが、
前述のような高温条件下で使用するベローズ継手を設計
することは、次のような困難性を有している。
In this case, the length of the piping becomes long, which not only increases the number of hangers and snares, increases the need for heat insulating material, but also increases the pressure loss within the piping, increases the circulation pump lift, and increases the amount of building material, resulting in an increase in plant construction costs. This is a factor that leads to In recent years, attempts have been made to reduce the size of the piping system by using bellows joints in the piping system to absorb thermal expansion as a means of resolving the increase in plant construction costs.
Designing a bellows joint for use under high temperature conditions as described above has the following difficulties.

すなわち、このような条件下でベローズ継手に作用する
荷重条件を分類すると、プラント起動・0停止時の大き
な湿度変動に対応する繰り返し変位荷重(2次荷重)お
よびプラントが通常出力に達してからの高温状態下にお
ける圧力等の1次荷重とに大別できる。
In other words, if we classify the load conditions that act on bellows joints under these conditions, we can classify them into cyclic displacement loads (secondary loads) that correspond to large humidity fluctuations when the plant starts and stops, and loads that apply after the plant reaches normal output. It can be broadly classified into primary loads such as pressure under high temperature conditions.

ベローズの高温構造設計上、疲労及びクリープ5損傷制
限ならびに歪制限を満足しなければならないが、疲労損
傷に対しては、2次荷重が支配因子となり、クリープ損
傷および歪制限に対しては圧力荷重によつて発生するベ
ローズ要素の曲げ応力が支配的な因子となる。
In the high-temperature structural design of bellows, fatigue and creep5 damage limits and strain limits must be satisfied, but secondary loads are the governing factor for fatigue damage, and pressure loads are the dominant factor for creep damage and strain limits. The bending stress of the bellows element caused by the bending stress is the dominant factor.

’0−般に1次荷重に対しては、ベローズ肉厚を厚くす
る方が発生応力の低減が可能であり、逆に2次荷重に対
しては、ベローズ肉厚を薄くする方が発生応力が低減で
きる。
'0 - In general, for primary loads, it is possible to reduce the generated stress by increasing the bellows wall thickness, and conversely, for secondary loads, it is better to reduce the bellows wall thickness to reduce the generated stress. can be reduced.

このように相反する性質の荷重に耐え、しかも、ノ5所
期の目的に沿うよラコンパクトなベローズ継手の設計を
成立させることには、相当な困難がともなう。
It is extremely difficult to design a bellows joint that is compact enough to withstand these contradictory loads and still meet the intended purpose.

本発明は、このように困難なベローズ継手ハ1一の設計
に対し相反する2種の荷重の発生状況が、プラント起動
・停止時と通常運転時とで、異なることに着目し、例え
ば、ベローズによつて吸収すべき荷重をプラント起動・
停止時のみに限定することにより、その設計成立性を得
やすくする方法を提供せんとするものである。
The present invention focuses on the fact that two types of loads that are contradictory to the design of bellows joints, which are difficult to design, differ between plant start-up/stop and normal operation. The load to be absorbed by
The purpose of the present invention is to provide a method that makes it easier to obtain the feasibility of the design by limiting it to only when the system is stopped.

第1図は高速増殖炉発電プラント熱輸送系の構成を簡単
に示すものであり、第2図は、高速増殖炉発電プラント
の実施例を基にして出力運転範囲における1次系ナトリ
ウムと2次系ナトリウムの電気出力に対する温度を示し
たものである。
Figure 1 simply shows the configuration of the heat transport system of a fast breeder reactor power plant, and Figure 2 shows the primary sodium and secondary sodium systems in the output operating range based on an example of a fast breeder reactor power plant. It shows the temperature versus the electrical output of the sodium system.

図において、1次冷却系2の中間熱交換器3の入口温度
変化を示す曲線イについてみると、電気出力30%〜1
00%の間に変化する温度範囲は、530℃−490℃
=40℃、同様に2次冷却系4の中間熱交換器3の出口
温度を示す曲線口についてみると505℃−490℃=
15℃、同様に1次冷却系2の中間交換器3の出口温度
を示す曲線ハについてみると、395℃−375℃=2
0℃、同様に2次冷却系4の中間熱交換器3の入口温度
を示す曲線二についてみると、325℃−280℃=4
5℃となり、電気出力30%〜100%の間での温度変
化は、15℃〜45℃である。つまり常温を30℃とし
た場合、常温30℃〜電気出力100q6の温度までの
総熱膨脹量に対し、出力運転範囲である電気出力30q
6〜100%の間の熱膨脹量の割合はごくわずかである
。試算すると、曲線口の場合、電気出力30%−100
%の熱膨脹量ΔI! 1−(505℃−4900C)・
α・11これに対し常温30℃〜電気出力100%まで
の熱膨脹量Δ2,=(505℃−30℃)α・lであり
、全体の熱膨脹量に対する出力運転範囲のそれの比率は
、15:475でわずか3.2%である。そこで例えば
電気出力30(F6〜100f)までの高温域でのわず
かな熱膨脹吸収を配管自体で、常温30℃〜電気出力3
0%までの低温域での大きな熱膨脹吸収をベローズで吸
収するものとすれば、配管の吸収すべき熱膨脹量はわず
かであり、ペローズに対しては高温域における1次応力
を低減することができる。(この電気出力30%の設定
は、プラントの条件によつて変るもので、これに限定さ
れるものではない。)具体的には先ず配管内部の液体金
属とベローズとを隔絶する為に、配管の外周にベローズ
を遊嵌して配管と配管を接続し、更に該ベローズと配管
内部との間に液体金属の凝固部分を設け、該凝固部分に
おいて液体金属を凝固又は溶融できるようにし、配管内
部を流れている液体金属の温度が低い間は、凝固部分の
液体金属を溶融して、ベローズで配管の熱膨脹を吸収す
るようにし、配管内を流れている液体金属の温度がある
一定温度以上になつた時、凝固部分にある液体金属を凝
固させて、実質上この凝固した液体金属で配管を一体化
し、高温域での配管の熱膨脹を配管自体で吸収するよう
にすると共に、液体金属の圧力をも保持して、ベローズ
にはその荷重と温度の影響を与えないようにし、配管の
熱膨脹吸収形態を低温域と高温域の二つに分けた事を特
徴とするものである。
In the figure, when looking at curve A showing the change in inlet temperature of the intermediate heat exchanger 3 of the primary cooling system 2, the electrical output is 30% to 1
The temperature range that changes between 00% is 530℃-490℃
= 40°C, similarly looking at the curved opening indicating the outlet temperature of the intermediate heat exchanger 3 of the secondary cooling system 4, it is 505°C - 490°C =
Similarly, if we look at the curve C showing the outlet temperature of the intermediate exchanger 3 of the primary cooling system 2, 395°C - 375°C = 2.
Similarly, when looking at curve 2 showing the inlet temperature of the intermediate heat exchanger 3 of the secondary cooling system 4, 325°C - 280°C = 4
5°C, and the temperature change between 30% and 100% of electrical output is 15°C to 45°C. In other words, if the normal temperature is 30℃, the total thermal expansion from the normal temperature of 30℃ to the temperature of 100q6 of electrical output is the output operating range of 30q of electrical output.
The percentage of thermal expansion between 6 and 100% is negligible. According to a trial calculation, in the case of a curved opening, the electrical output is 30% - 100
Thermal expansion amount ΔI in %! 1-(505℃-4900C)・
α・11 On the other hand, the amount of thermal expansion from room temperature 30°C to 100% electrical output is Δ2, = (505°C - 30°C) α・l, and the ratio of that in the output operating range to the overall amount of thermal expansion is 15: 475, which is only 3.2%. Therefore, for example, the piping itself can absorb the slight thermal expansion in the high temperature range up to 30 degrees Fahrenheit (F6 to 100F), which is an electrical output of 30 degrees Fahrenheit to an electrical output of 3.
If the bellows absorbs the large thermal expansion in the low temperature range down to 0%, the amount of thermal expansion that should be absorbed by the piping is small, and the primary stress on the bellows in the high temperature range can be reduced. . (This setting of 30% electrical output varies depending on the plant conditions and is not limited to this.) Specifically, first, in order to isolate the liquid metal inside the pipe from the bellows, A bellows is fitted loosely around the outer periphery of the pipe to connect the pipes, and a liquid metal solidification part is provided between the bellows and the inside of the pipe, so that the liquid metal can be solidified or melted in the solidification part, and the inside of the pipe is While the temperature of the liquid metal flowing in the pipe is low, the liquid metal in the solidified part is melted and the bellows absorbs the thermal expansion of the pipe, and the temperature of the liquid metal flowing in the pipe rises above a certain temperature. When the liquid metal is frozen, the liquid metal in the solidified portion is solidified, and the solidified liquid metal essentially integrates the pipe, allowing the pipe itself to absorb the thermal expansion of the pipe in the high temperature range, and reducing the pressure of the liquid metal. It is also characterized by the fact that the bellows is not affected by the load and temperature, and the thermal expansion absorption mode of the piping is divided into two regions: a low temperature region and a high temperature region.

以下、本発明の詳細を添付図面に示す一実施例と共に説
明する。第3図は本実施例である。図において、配管1
2の外周に外筒18を一体的に設け、この外筒18と配
管12との間の環状隙問に断熱材20を充填させている
。一方配管13は、その一方端に拡管部17を設け、前
記外筒18の外周に一定隙間をもたせて被装している。
配管13及び拡管部17の1部分には保温材14がまか
れている。外管18に設けたフランジ15と、配管13
の拡管部17に設けたフランジ16にベローズ9を溶接
によつて接続し、実質上配管12と13をベローズ9で
接続している。尚、図中21はヒータ、22は冷却管、
23は冷却フイン、19は金属の凝固部分、24は配管
12と13の摺接部分である。
Hereinafter, details of the present invention will be explained in conjunction with an embodiment shown in the accompanying drawings. FIG. 3 shows this embodiment. In the figure, piping 1
An outer cylinder 18 is integrally provided on the outer periphery of the pipe 2, and an annular gap between the outer cylinder 18 and the pipe 12 is filled with a heat insulating material 20. On the other hand, the pipe 13 is provided with an enlarged pipe part 17 at one end thereof, and is covered with the outer periphery of the outer cylinder 18 with a certain gap therebetween.
A heat insulating material 14 is spread over a portion of the pipe 13 and the expanded tube portion 17. The flange 15 provided on the outer tube 18 and the piping 13
A bellows 9 is connected by welding to a flange 16 provided on an expanded pipe portion 17 of the pipe 1, and the bellows 9 substantially connects the pipes 12 and 13. In addition, in the figure, 21 is a heater, 22 is a cooling pipe,
23 is a cooling fin, 19 is a solidified metal portion, and 24 is a sliding contact portion between the pipes 12 and 13.

次に本実施例の作用を説明する。Next, the operation of this embodiment will be explained.

本実施例では、例えば電気出力30q6〜100(:!
Iまでの高温域での熱膨脹吸収を配管自体で、常温30
℃〜電気出力30f1までの低温域の熱膨脹吸収をベロ
ーズで吸収するものとして説明する。先ず、常温の30
℃〜電気出力30%までの間は、ヒータ21によつて凝
固部19にある液体金属を溶融する。
In this embodiment, for example, the electrical output is 30q6 to 100 (:!
The piping itself absorbs thermal expansion in the high temperature range up to 30℃ at room temperature.
The following description assumes that the bellows absorbs thermal expansion in the low temperature range from .degree. C. to 30 f1 of electrical output. First, at room temperature 30
℃ to 30% electric output, the liquid metal in the solidification section 19 is melted by the heater 21.

なお液体金属たとえば、ナトリウムは約98℃で溶融す
る。従つて、この間の配管の熱膨脹は、凝固部分の液体
金属の溶融と配管12と13との摺接部で摺動し、ベロ
ーズ9で吸収する。この低温域では、液体金属の温度は
さほど高くなく、ベローズ9は高温状態にさらされない
。又断熱材20と凝固部19にある液体金属によつて熱
は遮られる。次に電気出力30q6〜100q1)の間
は、ヒータ21を遮断し、内部に冷却材を流す冷却管2
2と冷却フイン23の相乗効果で凝固部にある液体金属
を冷却し凝固させる。
Note that liquid metals such as sodium melt at about 98°C. Therefore, the thermal expansion of the piping during this period is absorbed by the bellows 9 due to the melting of the liquid metal in the solidified portion and the sliding contact between the piping 12 and 13. In this low temperature range, the temperature of the liquid metal is not very high, and the bellows 9 is not exposed to high temperature conditions. Heat is also blocked by the heat insulating material 20 and the liquid metal in the solidified portion 19. Next, between the electrical outputs 30q6 and 100q1), the heater 21 is shut off and the cooling pipe 2, which flows the coolant inside, is turned off.
2 and the cooling fins 23, the liquid metal in the solidification section is cooled and solidified.

冷却管には、冷熱源より冷却材が供給される。この液体
金属の凝固により、配管12と13の摺動は抑制され、
実質上1本の配管となる。従つてベローズ9にはさらに
追加される伸縮力は作用しない。この時の配管の熱膨脹
量は、ごくわずかであるので、配管のベンド部等で吸収
するものとするが、配管の引廻しはわずかで済む。
Coolant is supplied to the cooling pipe from a cold source. Due to the solidification of this liquid metal, sliding between the pipes 12 and 13 is suppressed,
It becomes essentially one pipe. Therefore, no additional stretching force acts on the bellows 9. Since the amount of thermal expansion of the piping at this time is very small, it will be absorbed by the bends of the piping, but only a small amount of piping will be required.

又液体金属の熱は、断熱材20と凝固した液体金属によ
つて完全に遮られる。以上詳述した通り本発明によれば
、常温からある温度までの低温域の熱膨脹をベローズで
吸収するようにし、ある温度以上の高温域での熱膨脹の
吸収を、凝固部分の液体金属を凝固させることによつて
配管自体で吸収するようにしたので、ベローズは常に低
温域でのみ使用されることになり、高温でのクリープ強
度を考慮する必要はなく、又高温域での伸縮作用を除く
ことにより、ベローズの疲労寿命の増大がはかれ、設計
を容易ならしめると共に配管自体の吸収すべぎ熱膨脹量
を微小にできるので、その引廻しを従来のものから大幅
に短縮できる等、その効果は顕著なものがある。
Further, the heat of the liquid metal is completely blocked by the heat insulating material 20 and the solidified liquid metal. As detailed above, according to the present invention, thermal expansion in a low temperature range from room temperature to a certain temperature is absorbed by the bellows, and thermal expansion in a high temperature range above a certain temperature is absorbed by solidifying the liquid metal in the solidified part. As a result, the pipe itself absorbs the water, so bellows are always used only in low temperature ranges, and there is no need to consider creep strength at high temperatures, and the expansion and contraction effect in high temperature ranges can be eliminated. This increases the fatigue life of the bellows, simplifies the design process, and minimizes the amount of thermal expansion that must be absorbed by the piping itself, making it possible to significantly shorten the length of the piping compared to conventional systems. There is something.

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

第1図は高速増殖炉発電プラントの一例を示した説明用
図、第2図は高速増殖炉発電プラントの一実施例として
の電気出力と熱媒体の温度との関係を示した説明用図、
第3図は本実施例である。 1・・・原子炉、 2・・・1次冷却系、 3・・・中
間熱、交換器、 3ζ・・蒸気発生器、 4・・・2次
冷却系、1・・・水蒸気系、 5・・・タービン、 6
ζ・始水ポンプ、 6・・・2次循環ポンプ、 7・・
・主循環ポンプ、9・・・ベローズ、 12、13・・
・配管、 19・・・凝固部分、 20・・・断熱材
、 21・・・ヒータ、22・・・冷却管、 23・・
・冷却フイン。
FIG. 1 is an explanatory diagram showing an example of a fast breeder reactor power plant; FIG. 2 is an explanatory diagram showing the relationship between electric output and heat medium temperature as an example of a fast breeder reactor power plant;
FIG. 3 shows this embodiment. 1... Nuclear reactor, 2... Primary cooling system, 3... Intermediate heat, exchanger, 3ζ... Steam generator, 4... Secondary cooling system, 1... Steam system, 5 ...Turbine, 6
ζ・Start water pump, 6...Secondary circulation pump, 7...
・Main circulation pump, 9... bellows, 12, 13...
・Piping, 19... Solidifying part, 20... Insulating material, 21... Heater, 22... Cooling pipe, 23...
・Cooling fins.

Claims (1)

【特許請求の範囲】[Claims] 1 液体金属用配管の接続部において、配管の外周部に
ベローズを遊嵌し、該ベローズを介して配管と配管を接
続し、該ベローズと配管内部との間に液体金属の凝間部
分を設け、該凝固部分に液体金属を凝固又は溶融するた
めの加熱器と冷却器を設け、該液体金属が溶溶融状態の
時はベローズで、凝固状態の時は配管自体で熱膨脹を吸
収するようにしたことを特徴とする液体金属用配管の熱
膨脹吸収装置。
1. At the connection part of liquid metal piping, a bellows is loosely fitted to the outer periphery of the piping, the piping is connected via the bellows, and a liquid metal condensation part is provided between the bellows and the inside of the piping. A heater and a cooler for solidifying or melting the liquid metal are installed in the solidification section, and thermal expansion is absorbed by the bellows when the liquid metal is in a molten state, and by the pipe itself when it is in a solidified state. A thermal expansion absorption device for liquid metal piping, characterized by:
JP56087666A 1981-06-08 1981-06-08 Thermal expansion absorption device for liquid metal piping Expired JPS5949478B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP56087666A JPS5949478B2 (en) 1981-06-08 1981-06-08 Thermal expansion absorption device for liquid metal piping

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP56087666A JPS5949478B2 (en) 1981-06-08 1981-06-08 Thermal expansion absorption device for liquid metal piping

Publications (2)

Publication Number Publication Date
JPS57204395A JPS57204395A (en) 1982-12-15
JPS5949478B2 true JPS5949478B2 (en) 1984-12-03

Family

ID=13921261

Family Applications (1)

Application Number Title Priority Date Filing Date
JP56087666A Expired JPS5949478B2 (en) 1981-06-08 1981-06-08 Thermal expansion absorption device for liquid metal piping

Country Status (1)

Country Link
JP (1) JPS5949478B2 (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS60181274U (en) * 1984-05-15 1985-12-02 谷端 義雄 welding torch tip
JPS62202978U (en) * 1986-06-13 1987-12-24
JPH0576668U (en) * 1992-03-11 1993-10-19 石川島播磨重工業株式会社 Welding wire support electrode structure

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS60181274U (en) * 1984-05-15 1985-12-02 谷端 義雄 welding torch tip
JPS62202978U (en) * 1986-06-13 1987-12-24
JPH0576668U (en) * 1992-03-11 1993-10-19 石川島播磨重工業株式会社 Welding wire support electrode structure

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JPS57204395A (en) 1982-12-15

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