Deprecated: The each() function is deprecated. This message will be suppressed on further calls in /home/zhenxiangba/zhenxiangba.com/public_html/phproxy-improved-master/index.php on line 456
JPH0333557B2 - - Google Patents
[go: Go Back, main page]

JPH0333557B2 - - Google Patents

Info

Publication number
JPH0333557B2
JPH0333557B2 JP19103783A JP19103783A JPH0333557B2 JP H0333557 B2 JPH0333557 B2 JP H0333557B2 JP 19103783 A JP19103783 A JP 19103783A JP 19103783 A JP19103783 A JP 19103783A JP H0333557 B2 JPH0333557 B2 JP H0333557B2
Authority
JP
Japan
Prior art keywords
stress
toe
stress concentration
joint
weld
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
JP19103783A
Other languages
Japanese (ja)
Other versions
JPS6082495A (en
Inventor
Kazumichi Motozuna
Yasuyoshi Myanari
Keiichi Sakai
Masaki Kitagawa
Kazuyuki Minoda
Toshio Irisawa
Osamu Atokawa
Hidenobu Amano
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.)
IHI Corp
Original Assignee
Ishikawajima Harima Heavy Industries Co 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 Ishikawajima Harima Heavy Industries Co Ltd filed Critical Ishikawajima Harima Heavy Industries Co Ltd
Priority to JP19103783A priority Critical patent/JPS6082495A/en
Publication of JPS6082495A publication Critical patent/JPS6082495A/en
Publication of JPH0333557B2 publication Critical patent/JPH0333557B2/ja
Granted legal-status Critical Current

Links

Landscapes

  • Filling Or Discharging Of Gas Storage Vessels (AREA)

Description

【発明の詳細な説明】 本発明はLNG、LPGなどを積荷する液化ガス
タンカー内に設けられる独立方形タンクの製造方
法に関するものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a method for manufacturing an independent rectangular tank installed in a liquefied gas tanker for loading LNG, LPG, etc.

液化ガスタンカーは、第1図に示すように船殻
1内に独立方形タンク2がローリングチヨツク3
及びサポート4にて殻1内面と隙間をもつて支持
され、独立方形タンク2内にLNG、LPGなどを
積荷した際に低温による収縮移動を許容できるよ
うになつている。低温液体を収容する独立方形タ
ンク2は収縮時の変形応力に対して十分な強度を
有するような構造となつている。
As shown in Figure 1, a liquefied gas tanker has an independent rectangular tank 2 in a hull 1 and a rolling chock 3.
It is supported by a support 4 with a gap between it and the inner surface of the shell 1, so that when LNG, LPG, etc. are loaded into the independent rectangular tank 2, contraction and movement due to low temperatures can be tolerated. The independent rectangular tank 2 containing the low-temperature liquid has a structure that has sufficient strength against deformation stress during contraction.

この独立方形タンク2はアルミニウム合金から
なり例えば第2図に示すように、タンク2内にブ
ラケツトやリブ、型材、スキンプレートなど多数
のタンク部材5を骨組し、各タンク部材5の継目
を溶接して構築している。とろでこの種の液化ガ
スタンカーでIMO CodeにおけるType Bに属す
るタンカーはIMO Codeによつて詳細な疲労強度
解析を行なうことを義務づけられている。このB
タイプタンクの定義はタンクの安全性が正確な解
析と実験で確認され、一時にタンクの大破壊が生
じることのないタンクであり、そのため疲労解
析、破壊解析に重点がおかれている。独立方形タ
ンクはその内部が多数のタンク部材が溶接された
骨付き構造で不静定次数が高いので完全な解析は
困難であつたが、最近コンピユータにより比較的
簡単に解析できるようになつている。しかしなが
ら骨付き構造には必然的に隅肉溶接などが多用さ
れており、溶接形状が不規則なためこの溶接部に
ついては個々に疲労試験を行なう必要がある。従
来この溶接部の疲労強度解析は部材の公称応力を
基礎に行なつており各溶接継手の種類毎に、応力
が繰り返しかかつた場合に、疲労し破壊する回数
とその応力との関係を示したS−N曲線を実験に
より求めそれをもとに公称応力に対する溶接継手
の耐疲労強度を求めている。しかしながら部材の
形状や継手形状、或いは溶接ビードの形状により
耐疲労強度が相違するため各種のS−N曲線を必
要とするので多くの試験が必要である。事実上、
独立方形タンクに表われるすべての継手を各々の
試験で求めたS−N曲線でカバーすることは不可
能である。
This independent rectangular tank 2 is made of an aluminum alloy, and as shown in FIG. 2, for example, a large number of tank members 5 such as brackets, ribs, shapes, and skin plates are assembled inside the tank 2, and the joints of each tank member 5 are welded. is being constructed. This type of liquefied gas tanker, which falls under Type B in the IMO Code, is required by the IMO Code to conduct a detailed fatigue strength analysis. This B
The definition of a type tank is that the safety of the tank has been confirmed through accurate analysis and experimentation, and the tank is unlikely to undergo major destruction at any one time.For this reason, emphasis is placed on fatigue analysis and fracture analysis. An independent rectangular tank has a bone structure with many welded tank parts inside, and has a high unsteady constant order, so complete analysis has been difficult, but recently computers have made it relatively easy to analyze. . However, fillet welds and the like are inevitably used frequently in bone structures, and because the weld shape is irregular, it is necessary to conduct fatigue tests on each welded part individually. Conventionally, this fatigue strength analysis of welded joints has been performed based on the nominal stress of the member, and for each type of welded joint, when stress is repeatedly applied, the relationship between the number of times it will fatigue and break and that stress is shown. The fatigue strength of the welded joint with respect to the nominal stress was determined based on the S-N curve obtained through experiments. However, since the fatigue strength differs depending on the shape of the member, the shape of the joint, or the shape of the weld bead, various S-N curves are required, which requires many tests. in fact,
It is impossible to cover all the joints appearing in an independent rectangular tank with the S-N curve determined for each test.

本発明者らは溶接継手部材の疲労強度は溶接部
の継手形状や治金的特性、残留応力などの影響因
子のうち、溶接継手部材の疲労強度にもつとも影
響を与えるのは、溶接継手形状に起因する疲労亀
裂発生部の応力集中係数、特に溶接止端部の応力
集中係数であることを見い出し本発明に至つたも
のである。
The present inventors found that the fatigue strength of welded joint members is influenced by the shape of the welded joint, metallurgical properties, residual stress, and other factors. The inventors have discovered that this is the stress concentration factor of the fatigue crack occurrence area, particularly the stress concentration factor of the weld toe, and have thus arrived at the present invention.

本発明の目的は、上述した独立方形タンクの各
種溶接継手の疲労解析が容易に行なえ、しかも、
各種タンク部材の耐疲労設計が容易に行なえる液
化ガスタンカーの独立方形タンクの製造方法を提
供するものである。
An object of the present invention is to easily perform fatigue analysis of various welded joints of the above-mentioned independent rectangular tank, and to
The present invention provides a method for manufacturing an independent rectangular tank for a liquefied gas tanker, which allows for easy fatigue-resistant design of various tank members.

多数のアルミ合金製のタンク部材から構成し、
かつその部材相互の継ぎ目を溶接した液化ガスタ
ンカーの独立方形タンクの製造方法において、上
記部材相互の溶接継手部の板材に発生する公称応
力に対して、溶接止端部での応力集中係数Ktを
フランク角θと止端半径ρおよびビート高さhの
関数から求め、その応力集中係数Ktより溶接止
端部での局部応力を求めると共にその局部応力を
基にした疲労破壊曲線を作製し、その疲労破壊曲
線から角溶接継手部の許容局部応力を求めると共
に応力集中係数Ktが3.0以下となるように上記フ
ランク角θと止端半径ρおよびビート高さhを制
御して溶接することを特徴とする液化ガスタンカ
ーの独立方形タンクの製造方法にあり、これによ
り、母材を含めた溶接継手部の疲労破壊曲線を応
力集中係数から算出した局部応力に基づいてS−
N曲線を製作し、これをもとに各溶接継手部の耐
疲労強度の設計を行つて溶接継手の溶接形状を制
御することで疲労強度解析が容易な独立方形タン
クを製造できる。
Consists of numerous aluminum alloy tank components,
In addition, in the manufacturing method of an independent rectangular tank for a liquefied gas tanker in which the joints between the members are welded, the stress concentration coefficient Kt at the weld toe is calculated for the nominal stress generated in the plate material at the welded joint between the members. The local stress at the weld toe is determined from the function of the flank angle θ, toe radius ρ, and bead height h, and the local stress at the weld toe is determined from the stress concentration coefficient Kt, and a fatigue fracture curve is created based on the local stress. The method is characterized in that the allowable local stress of the corner welded joint is determined from the fatigue fracture curve, and the flank angle θ, toe radius ρ, and bead height h are controlled and welded so that the stress concentration factor Kt is 3.0 or less. A manufacturing method for an independent rectangular tank for a liquefied gas tanker, in which the fatigue fracture curve of a welded joint including the base metal is determined based on the local stress calculated from the stress concentration factor.
By creating an N curve, designing the fatigue strength of each welded joint based on this, and controlling the weld shape of the welded joint, an independent rectangular tank whose fatigue strength can be easily analyzed can be manufactured.

以下本発明に係る液化ガスタンカーの独立方形
タンクの製造方法の好適一実施例を添付図面に基
づいて説明する。
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS A preferred embodiment of the method for manufacturing an independent rectangular tank for a liquefied gas tanker according to the present invention will be described below with reference to the accompanying drawings.

先ず、第3図に十字溶接継手を例に応力集中係
数Ktを説明する。
First, the stress concentration coefficient Kt will be explained using a cross-welded joint as an example in FIG.

第3図において、6は縦板、7は横板で、その
縦板6と横板7に隅肉溶接8がされていたとす
る。この場合、溶接8の余盛角(以下フランク角
という)をθ、ビード高さをh、溶接8の止端部
9のヒード止端半径をρ、横板7の板厚をtとす
る。
In FIG. 3, it is assumed that 6 is a vertical plate and 7 is a horizontal plate, and a fillet weld 8 is made between the vertical plate 6 and the horizontal plate 7. In this case, the reinforcement angle (hereinafter referred to as flank angle) of the weld 8 is θ, the bead height is h, the heed toe radius of the toe 9 of the weld 8 is ρ, and the thickness of the horizontal plate 7 is t.

今横板7に公称応力σNがかかつたとすると、そ
の応力分布は10で示すように、溶接の施されてい
ない横板7で公称応力σNのままであるが止端部9
に近づくにつれて応力集中が起り、止端部9が略
最大の局部応力σLが作用する。従つてこの止端部
9における応力集中係数をKtとすると、Ktは下
式で表わされる。
Assuming that a nominal stress σ N is now applied to the horizontal plate 7, the stress distribution will be as shown at 10. Although the nominal stress σ N remains at the unwelded horizontal plate 7, the toe 9
Stress concentration occurs as the distance approaches , and approximately the maximum local stress σ L acts on the toe 9. Therefore, if the stress concentration coefficient at this toe 9 is Kt, Kt is expressed by the following formula.

Kt=σL/σN ……(1) またこのKtは、上述したフランク角θ、止端
半径ρ、ビードの高さhの関数で下式で表わされ
る。
K tLN (1) Moreover, this Kt is expressed by the following formula as a function of the above-mentioned flank angle θ, toe radius ρ, and bead height h.

Kt=〔1+f(θ){g(ρ)−1}〕C(a/t)
……(2) ここで、f(θ)はフランク角の影響、g(ρ)
は溶接止端半径の影響、C(a/t)は未溶着部
の存在の影響による関数であり夫々下式で表わさ
れる。
K t = [1+f(θ){g(ρ)-1}]C(a/t)
...(2) Here, f(θ) is the influence of flank angle, g(ρ)
is a function of the influence of the radius of the weld toe, and C(a/t) is a function of the influence of the presence of an unwelded portion, and is expressed by the following formulas.

フランク角; 止端半径; g(ρ)=αt・gt(ρ)+αb・gb(ρ)……(4
) ここでgt(ρ)は引張荷重の場合で次式で与え
られる。
flank angle; Toe radius; g (ρ) = α t・g t (ρ) + α b・g b (ρ)……(4
) Here, gt(ρ) is given by the following formula in case of tensile load.

gt(ρ)=1+βt{(h/ρ)・1/2.8(W/t)−
2}0.65 ……(5) ここでβtは溶接継手形状に応じて次の値をと
る。十字継手2.2、突合せ継手2.0、T継手1.0。
g t (ρ)=1+β t {(h/ρ)・1/2.8(W/t)−
2}0.65...(5) Here, βt takes the following value depending on the shape of the welded joint. Cross joint 2.2, butt joint 2.0, T joint 1.0.

また、曲げ荷重の場合のgb(ρ)は継手形状と
は無関係に次式で与えられる。
In addition, gb (ρ) in the case of bending load is given by the following formula, regardless of the joint shape.

gb(ρ)=1+βb・{tanh1/2(2tp/t+2h
+2ρ/t)} ×〔tanh{t+2h/t−11/4/1−ρ/1}
〕{0.13+0.65(1−ρ/t)4/(ρ/t)1/3}……
(6) ここでβbは溶接継手形状に応じて次の値をと
る。突合せ継手=1.5、T継手=1.9、その他の継
手=1.0。
g b (ρ)=1+β b・{tanh 1/2 (2tp/t+2h
+2ρ/t)} × [tanh{t+2h/t-1 1/4 /1-ρ/1}
] {0.13+0.65 (1-ρ/t) 4 / (ρ/t) 1/3 }...
(6) Here, βb takes the following value depending on the shape of the welded joint. Butt joint = 1.5, T joint = 1.9, other joints = 1.0.

未溶着部; C(a/t)=1+0.64(a/t)2
/(2hp/t)−0.12(a/t)4/(2hp/t)2……(7
) ここで(3)、(5)式中のWは溶接継手形式により次
のように使い分ける。
Unwelded area; C (a/t) = 1 + 0.64 (a/t) 2
/(2hp/t)−0.12(a/t) 4 /(2hp/t) 2 …(7
) Here, W in equations (3) and (5) is used depending on the type of welded joint as follows.

十字継手;W=(t+4h)+0.3(tp+2hp) 突合せ継手;W=t+2h+0.6hp T継手;W=(t+2h)+0.3(tp+2hp) ……(8) 但し、(2)〜(8)式中θはフランク角、ρは止端半
径、tは負荷する部材の板厚、tpは負荷を受けな
い部材の板厚、hはビード高さ(脚長)、hpは溶
接脚長、aは未溶着部の長さ、αtは止端部での引
張応力係数(引張荷重の場合=1、曲げ荷重の場
合=0)、αbは止端部での曲げ応力係数(曲げ荷
重の場合=1、引張荷重の場合=0)である。
Cross joint; W = (t+4h) + 0.3 (tp + 2hp) Butt joint; W = t + 2h + 0.6hp T joint; W = (t + 2h) + 0.3 (tp + 2hp) ... (8) However , (2) to (8), where θ is the flank angle, ρ is the toe radius, t is the plate thickness of the loaded member, tp is the plate thickness of the unloaded member, h is the bead height (leg length), hp is the weld leg length, a is the length of the unwelded part, αt is the tensile stress coefficient at the toe (1 for tensile load, 0 for bending load), αb is the bending stress coefficient at the toe (For bending load = 1, for tensile load = 0).

上記(2)〜(8)式から求められるKtとフランク角
θ、止端半径ρ及びビード高さhをパラメータに
各種継手における応力集中係数Ktをみた結果、
フランク角θ及びビード高さhによる影響は比較
的小さく、主に止端半径ρの大きさにより応力集
中係数Ktが変化することが判つた。この結果を
T字継手の場合と、十字継手の場合を例に第4
図、第5図に示す。
As a result of looking at the stress concentration coefficient Kt in various joints using Kt obtained from equations (2) to (8) above, flank angle θ, toe radius ρ, and bead height h as parameters,
It was found that the influence of the flank angle θ and bead height h is relatively small, and that the stress concentration coefficient Kt changes mainly depending on the size of the toe radius ρ. Using this result as an example for a T-shaped joint and a cruciform joint, the fourth
As shown in Fig. 5.

第4図はT字継手における止端半径/板厚と応
力集中係数との関係を示している。
FIG. 4 shows the relationship between the toe radius/plate thickness and stress concentration factor in a T-joint.

この第4図のグラフより板厚tが一定とすれば
止端半径ρが小さくなるほど応力集中係数Ktが
上昇することが判る。止端半径ρが小さい場合に
おいてフランク角θ(100〜170°)による応力集中
係数の変化が大きくなり、フランク角θが大きく
なれば応力集中係数が増加するか止端半径ρが大
きくなればその変化は少なくなることが判る。
From the graph in FIG. 4, it can be seen that if the plate thickness t is constant, the stress concentration coefficient Kt increases as the toe radius ρ becomes smaller. When the toe radius ρ is small, the stress concentration coefficient changes greatly depending on the flank angle θ (100 to 170°). It can be seen that there are fewer changes.

また、第5図のグラフも同様、板厚tを一定と
すれば止端半径ρが小さければ応力集中係数が増
加することが判る。
Further, similarly to the graph of FIG. 5, it can be seen that if the plate thickness t is constant, the stress concentration factor increases as the toe radius ρ becomes smaller.

以上において、応力集中係数Ktを求めること
により、上式(1)式より上端部9における局部設応
σLが判る。すなわち局部応力σLは下式より求ま
る。
In the above, by determining the stress concentration coefficient Kt, the local response σ L at the upper end portion 9 can be determined from the above equation (1). In other words, the local stress σ L can be found from the formula below.

σL=Kt・σN 従つて今、例えば第3図に示した十字継手部の
横板7に公称応力σNを破壊するまで繰り返し作用
させた場合のS−N曲線を作成する場合、公称応
力σNでなく局部応力σLにてS−N曲線を作図すれ
ば、統一的なS−N線図ができる。このS−N線
図を第6図に示した。図において縦軸は応力範囲
で止端部での局部応力σLを示し、その各応力を繰
り返しかけた場合に突合せ継手、十字継手、T字
継手が破壊した点をプロツトしたもので、グラフ
を示した直線は試験個数中の生存確立を示したも
のである。
σ L =K t・σ N Therefore, for example, when creating an S-N curve when the nominal stress σ N is repeatedly applied to the horizontal plate 7 of the cruciform joint shown in FIG. 3 until it breaks, If the S-N curve is drawn using the local stress σ L instead of the nominal stress σ N , a unified S-N diagram can be obtained. This S-N diagram is shown in FIG. In the figure, the vertical axis shows the local stress σ L at the toe within the stress range, and the graph plots the points at which the butt joint, cruciform joint, and T-joint break when each stress is repeatedly applied. The straight line shown indicates the probability of survival among the number of test specimens.

このS−N曲線は局部応力σLをベースに作図し
てあるため各継手部の疲労強度は容易に求めるこ
とが可能となる。
Since this S-N curve is drawn based on the local stress σ L , the fatigue strength of each joint can be easily determined.

応力集中係数Ktは通常無制御に溶接を行なえ
ば広い範囲に分布する。このため例えばKt値7.0
の場合、止端部にかかる局部応力σLは公称応力σN
に対して7倍となり、大きくなつて耐疲労強度が
落ちる。従つて耐疲労強度を高くするためには板
厚を大きく断面積を大きくして板にかかる全体の
応力を小さく設計する必要がある。すなわち継手
部の溶接において、溶接を無制御に行なえば、そ
の溶接コストは低くなるが反面Kt値が大きくな
り易いため板厚の厚いものを使用しなければなら
ずその材料値が増加する。
The stress concentration factor Kt is normally distributed over a wide range if welding is performed without control. For this reason, for example, Kt value 7.0
, the local stress σ L on the toe is the nominal stress σ N
It becomes 7 times larger than that, and its fatigue strength decreases. Therefore, in order to increase the fatigue strength, it is necessary to design the plate to have a large thickness and a large cross-sectional area to reduce the overall stress applied to the plate. That is, when welding joints, if welding is performed without control, the welding cost will be lower, but on the other hand, the Kt value will tend to increase, so thick plates must be used, and the material value will increase.

本発明は独立方形タンクの各溶接継手の溶接形
状を予め一定に保つて各継手を溶接しその各止端
部での応力集中係数分布を解析したところ応力集
中係数が3.0以下であればタンクを安全に設計で
きることを確認した。
In the present invention, the welding shape of each welded joint of an independent rectangular tank is kept constant in advance, each joint is welded, and the stress concentration coefficient distribution at each toe is analyzed. If the stress concentration coefficient is 3.0 or less, the tank is welded. We confirmed that it can be designed safely.

第7図は、同一条件のもとでT字継手を溶接し
た場合のKt値の分布を示したもので、Kt値の測
定総個数を100%とし、各Kt値ごとにその頻度を
示したものである。この第7図において、溶接条
件を同一とする応力集中計数Ktは略1.5前後で最
大頻度(14%)となり、また分布範囲は、Ktが
1.13〜2.38まで分布する。また、この第7図の分
布曲線を基に第7図に示すようにKtの最大値か
ら最小値までを各々Ktの値ごとに積分してKt値
に対する確率を第8図のグラフに示した。
Figure 7 shows the distribution of Kt values when T-joints are welded under the same conditions.The total number of Kt value measurements is assumed to be 100%, and the frequency is shown for each Kt value. It is something. In this Figure 7, the stress concentration factor Kt under the same welding conditions has a maximum frequency (14%) around 1.5, and the distribution range is as follows:
Distributed from 1.13 to 2.38. Also, based on the distribution curve in Figure 7, the probability for each Kt value was integrated from the maximum value to the minimum value of Kt as shown in Figure 7, and the probability for each Kt value was shown in the graph in Figure 8. .

図において点線のlは無制御に溶接した場合の
グラフを示し、nはその平均Kt値を示し、一点
鎖線の曲線mは第7図の頻度分布を積分したグラ
フを示し、oはその平均Kt値を示したものであ
る。
In the figure, the dotted line l shows the graph when welding is carried out without control, n shows the average Kt value, the dashed-dotted curve m shows the graph integrating the frequency distribution in Figure 7, and o shows the average Kt value. It shows the value.

点線lで示すように無制御で溶接を行うとKt
値は最大から最小まで広い範囲に分布するが、曲
線mで示すように溶接条件を一定にして溶接する
ことで応力集中係数の最大値Ktmaxの出現が3.0
以下で確実に確率ゼロになることが判る。
As shown by the dotted line l, if welding is performed without control, Kt
The values are distributed over a wide range from the maximum to the minimum, but as shown by curve m, by welding under constant welding conditions, the maximum stress concentration factor Ktmax appears to be 3.0.
We can see below that the probability is definitely zero.

従つて、各継手部を溶接設計するにおいて応力
集中係数Ktが3.0以下となるように設計しておけ
ば、公称応力に対して安全な耐疲労強度を実現で
きる。
Therefore, if each joint is designed for welding so that the stress concentration factor Kt is 3.0 or less, a safe fatigue strength can be achieved against the nominal stress.

以上より、母材にかかる最大公称応力σNとKt
値より局部応力σLを求め、第6図のS−N曲線
(疲労破壊曲線)より、その局部応力σLが許容応
力内にあるかどうかが、換言すれば継手部の溶接
形状(フランク各θ、止端半径ρ、ビード高さ
h)が適正かどうかを求め、許容局部応力以内に
入るようKt値を制御する。
From the above, the maximum nominal stress σ N and Kt on the base metal
The local stress σ L is calculated from the value, and the S-N curve (fatigue fracture curve) in Figure 6 is used to determine whether the local stress σ L is within the allowable stress. θ, toe radius ρ, and bead height h) are determined to be appropriate, and the Kt value is controlled so that it falls within the allowable local stress.

次に応力集中係数Ktを3.0以内に制御する溶接
方法を説明する。第9図はT字形継手部を溶接す
る例を示したもので図において、11は下板、1
2は立板で、その下板11と立板12との継目1
3をトーチノズル14でMIG溶接する場合を示
している。この場合、トーチノズル14の先端の
電極15のネライ位置を継目13に向け、かつそ
のトーチ角度θtを一定値(例えば45°)に保つ。
この状態からトーチノズル14を左右にオシレー
トさせる。このオシレート幅は立板12と下板1
1の板厚に応じて十分な溶接強度が得られるよう
な振幅(通常±4mm程度)とする。
Next, a welding method for controlling the stress concentration factor Kt within 3.0 will be explained. Figure 9 shows an example of welding a T-shaped joint. In the figure, 11 is the lower plate, 1
2 is a standing board, and the joint 1 between the lower board 11 and the standing board 12 is
3 is MIG welded using the torch nozzle 14. In this case, the position of the electrode 15 at the tip of the torch nozzle 14 is directed toward the seam 13, and the torch angle θt is maintained at a constant value (for example, 45°).
From this state, the torch nozzle 14 is oscillated left and right. This oscillation width is the vertical plate 12 and the lower plate 1.
The amplitude should be set so that sufficient welding strength can be obtained according to the thickness of the plate (usually about ±4 mm).

通常MIG溶接におけるオシレート数は70〜80
回/分であるが、このオシレート数では応力集中
係数を制御することができない。本発明はオシレ
ート数を150〜250回/分で行なうことにより止端
部の応力集中係数Ktを3.0以下に制御することを
可能にしたものである。この場合オシレート数が
多くなることにより止端部での止端半径ρを大き
くすることが可能となり、例えば止端半径ρを
1.0mm以上とすることが可能となる。
Normally the number of oscillations in MIG welding is 70 to 80.
times per minute, but the stress concentration factor cannot be controlled with this oscillation number. The present invention makes it possible to control the stress concentration coefficient Kt at the toe to 3.0 or less by performing oscillations at a rate of 150 to 250 times/minute. In this case, by increasing the number of oscillations, it is possible to increase the toe radius ρ at the toe, for example, the toe radius ρ can be increased.
It becomes possible to set it to 1.0 mm or more.

また、オシレート数を制御する代りにトーチノ
ズル14からのアルゴンのシールドガス中にヘリ
ウムガスを50%以上混合することもできる応力集
中係数Ktを3.0以下にすることができる。すなわ
ち、ヘリウムガスはアルゴンガスより熱伝導率が
高く、そのため溶加材の溶け込みがよくなり、
Kt値を低くすることが可能となる。
Furthermore, instead of controlling the oscillation number, 50% or more of helium gas can be mixed into the argon shielding gas from the torch nozzle 14, and the stress concentration coefficient Kt can be made 3.0 or less. In other words, helium gas has a higher thermal conductivity than argon gas, so the filler metal melts better.
It becomes possible to lower the Kt value.

この溶接はすべて自動溶接材により行ない、第
1図、第2図に示した独立方形タンク2内のタン
ク部材5の相互の継目をその溶接止端部の応力集
中係数3.0以下で溶接することが可能となる。従
つて各タンク部材5はKt値が3.0以下に押えるこ
とができるため、その板厚応力に見合つた経済的
な板厚とし、かつその疲労強度も充分なものとす
ることができる。
All of this welding is performed using automatic welding materials, and it is possible to weld the mutual joints of tank members 5 in the independent rectangular tank 2 shown in FIGS. 1 and 2 with a stress concentration coefficient of 3.0 or less at the weld toe. It becomes possible. Therefore, since the Kt value of each tank member 5 can be kept to 3.0 or less, the tank member 5 can have an economical thickness commensurate with the thickness stress and also have sufficient fatigue strength.

以上、詳述してきたことから明らかなように本
発明によれば次のごとき効果を発揮する。
As is clear from the above detailed description, the present invention provides the following effects.

(1) 応力集中率Ktは計算によつて求めることが
できS−N曲線は一本でよいので、各継手部の
疲労試験を大幅に簡略化できる。
(1) Since the stress concentration factor Kt can be determined by calculation and only one S-N curve is required, the fatigue test for each joint can be greatly simplified.

(2) 応力集中係数Ktは実際の構造部の溶接形状
を測定することでその値を確認することがでる
ので、実際に仕上つた構造物の疲労強度に対す
る信頼性が高い。
(2) The stress concentration factor Kt can be confirmed by measuring the welded shape of the actual structure, so it is highly reliable for the fatigue strength of the actually completed structure.

(3) 応力集中係数Ktは測定によつて統計的に把
握できるので真の意味で信頼性解析が可能とな
る。
(3) Since the stress concentration factor Kt can be statistically understood through measurement, reliability analysis is possible in the truest sense.

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

第1図は本発明に係る液化ガスタンカーの独立
方形タンクを示す断面図、第2図は独立方形タン
クを示す斜視図、第3図は本発明に係る液化ガス
タンカーの独立方形タンクの製造方法における止
端部の応力集中係数を説明するための十字継手の
断面図、第4図は本発明でのT字継手部における
止端半径と応力集中係数の関係を示すグラフ、第
5図は本発明での十字継手部における止端半径と
応力集中係数の関係を示すグラフ、第6図は本発
明におけるS−N曲線を示すグラフ、第7図は本
発明における応力集中係数の分布を示すグラフ、
第8図は本発明における応力集中係数の分布を積
分した場合のグラフ、第9図は本発明に係る液化
ガスタンカーの独立方形タンクの製造方法におい
て各継手部を溶接する例を示す斜視図である。 図中、2は独立方形タンク、3,5はタンク部
材である。
FIG. 1 is a sectional view showing an independent rectangular tank for a liquefied gas tanker according to the present invention, FIG. 2 is a perspective view showing an independent rectangular tank, and FIG. 3 is a method for manufacturing an independent rectangular tank for a liquefied gas tanker according to the present invention. FIG. 4 is a graph showing the relationship between the toe radius and stress concentration factor in the T-shaped joint of the present invention, and FIG. A graph showing the relationship between the toe radius and the stress concentration factor in the cruciform joint part in the invention, FIG. 6 is a graph showing the S-N curve in the invention, and FIG. 7 is a graph showing the distribution of the stress concentration factor in the invention. ,
FIG. 8 is a graph of integrating the stress concentration coefficient distribution according to the present invention, and FIG. 9 is a perspective view showing an example of welding each joint in the method for manufacturing an independent rectangular tank for a liquefied gas tanker according to the present invention. be. In the figure, 2 is an independent rectangular tank, and 3 and 5 are tank members.

Claims (1)

【特許請求の範囲】[Claims] 1 多数のアルミ合金製のタンク部材から構成
し、かつその部材相互の継ぎ目を溶接した液化ガ
スタンカーの独立方形タンクの製造方法におい
て、上記部材相互の溶接継手部の板材に発生する
公称応力に対して、溶接止端部での応力集中係数
Ktをフランク角θと止端半径ρおよびビード高
さhの関数から求め、その応力集中係数Ktより
溶接止端部での局部応力を求めると共にその局部
応力を基にした疲労破壊曲線を作製し、その疲労
破壊曲線から各溶接継手部の許容局部応力を求め
ると共に応力集中係数Ktが3.0以下となるように
上記フランク角θと止端半径ρおよびビード高さ
hを制御して溶接することを特徴とする液化ガス
タンカーの独立方形タンクの製造方法。
1. In a manufacturing method for an independent rectangular tank for a liquefied gas tanker, which is constructed from a large number of aluminum alloy tank members and whose joints are welded, the nominal stress generated in the plates at the welded joints between the members shall be The stress concentration factor at the weld toe
Kt is determined from the function of the flank angle θ, toe radius ρ, and bead height h, and the local stress at the weld toe is determined from the stress concentration coefficient Kt, and a fatigue fracture curve is created based on the local stress. , find the allowable local stress of each weld joint from the fatigue fracture curve, and weld by controlling the flank angle θ, toe radius ρ, and bead height h so that the stress concentration factor Kt is 3.0 or less. A method for manufacturing an independent rectangular tank for a liquefied gas tanker.
JP19103783A 1983-10-14 1983-10-14 Independent square tank for liquefied gas tanker Granted JPS6082495A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP19103783A JPS6082495A (en) 1983-10-14 1983-10-14 Independent square tank for liquefied gas tanker

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP19103783A JPS6082495A (en) 1983-10-14 1983-10-14 Independent square tank for liquefied gas tanker

Related Child Applications (2)

Application Number Title Priority Date Filing Date
JP17583184A Division JPS6084496A (en) 1984-08-25 1984-08-25 Independent rectangular tank of liquefied gas tanker
JP11463490A Division JPH069752B2 (en) 1990-04-27 1990-04-27 Fatigue strength assurance method for independent rectangular tank welds of liquefied gas tankers

Publications (2)

Publication Number Publication Date
JPS6082495A JPS6082495A (en) 1985-05-10
JPH0333557B2 true JPH0333557B2 (en) 1991-05-17

Family

ID=16267839

Family Applications (1)

Application Number Title Priority Date Filing Date
JP19103783A Granted JPS6082495A (en) 1983-10-14 1983-10-14 Independent square tank for liquefied gas tanker

Country Status (1)

Country Link
JP (1) JPS6082495A (en)

Families Citing this family (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP5646853B2 (en) * 2010-01-20 2014-12-24 ジャパンマリンユナイテッド株式会社 Ship
JP5578921B2 (en) * 2010-04-23 2014-08-27 三菱重工業株式会社 Floating-type liquefied natural gas production and storage and loading facility and liquefied natural gas production and storage and loading method
JP5657147B2 (en) 2012-01-23 2015-01-21 三菱電機株式会社 Elevator rope

Also Published As

Publication number Publication date
JPS6082495A (en) 1985-05-10

Similar Documents

Publication Publication Date Title
Berge On the effect of plate thickness in fatigue of welds
Thomas Analyzing the failure of welded steel components in construction systems
Andrews The effect of misalignment on the fatigue strength of welded cruciform joints
Campagnolo et al. Fatigue strength assessment of as-welded and HFMI treated welded joints according to structural and local approaches
JPH0333557B2 (en)
Crupi et al. Different methods for fatigue assessment of T welded joints used in ship structures
Song et al. Comprehensive fatigue assessment for different types of aluminum fillet welded joints by local approaches
JPH069752B2 (en) Fatigue strength assurance method for independent rectangular tank welds of liquefied gas tankers
US7690553B2 (en) Methods and systems for mitigating residual tensile stresses
Winarto et al. Study the effect of welding position and plate thickness to the mechanical and microstructural properties of the TIG dissimilar metal welded between carbon steel ASTM A36 and stainless steel 304 plates
JPS6083784A (en) Welding method for welded joints
JPS6084496A (en) Independent rectangular tank of liquefied gas tanker
JP7406795B2 (en) Welding methods and welded structures
Thomas Failure analysis of welded constructional steel components
JP6759744B2 (en) Support structure
Skriko et al. Static strength capacity of single-sided fillet welds
Benoit et al. A Study of the Propagation of Fatigue Cracks in the Heat-Affected Zones of Welded Joints in E 36 Steel
Muncner Brittle fracture resistance of repaired welded joints
KR100426267B1 (en) Welding Method For Use In Ships And Welding Part Using The Same
Gooch et al. Review of Welding Practice for Carbon Steel Deaerator Vessels
GAMBRELL et al. Use of photostress and strain gages to analyze behavior of weldments and use of photostress and strain gages to analyze behavior of an aft skirt test specimen(Semiannual Report, 26 Dec. 1992- 26 Jul. 1993)
Berge et al. Wide Plates in Bending: Application of CTOD Design Approach
Kaneko et al. Lectures on Aluminium Fishing Boats Building. IV
JP3007243B2 (en) Prevention method of bend at the bevel on the diagonal side of the bevel of the Uranami bead in multi-groove groove welding
KR20120022513A (en) Weld structure and welded joint having excellent brittle crack propagation resistance