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JP4900236B2 - Shear transmission structure, concrete structure, construction method of shear transmission structure, and design method of shear transmission structure - Google Patents
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JP4900236B2 - Shear transmission structure, concrete structure, construction method of shear transmission structure, and design method of shear transmission structure - Google Patents

Shear transmission structure, concrete structure, construction method of shear transmission structure, and design method of shear transmission structure Download PDF

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JP4900236B2
JP4900236B2 JP2007341044A JP2007341044A JP4900236B2 JP 4900236 B2 JP4900236 B2 JP 4900236B2 JP 2007341044 A JP2007341044 A JP 2007341044A JP 2007341044 A JP2007341044 A JP 2007341044A JP 4900236 B2 JP4900236 B2 JP 4900236B2
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underground wall
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伸和 渡辺
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Obayashi Corp
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Description

本発明は、地中壁と、地中壁と接合して構築されるコンクリート構造物との間に作用するせん断力を伝達するせん断伝達構造、それを備えるコンクリート構造物、そのせん断伝達構造の構築方法、及びそのせん断伝達構造の設計方法に関する。   The present invention relates to a shear transmission structure for transmitting a shear force acting between an underground wall and a concrete structure constructed by joining the underground wall, a concrete structure including the same, and the construction of the shear transmission structure The present invention relates to a method and a design method of the shear transmission structure.

従来より、LNG地下タンクの底面に作用する土圧や水圧等によるタンクの浮き上がりを防止するために、LNG地下タンクの外周に構築される地中壁とタンクの側壁との接合面間に接合鉄筋を設けたり、例えば特許文献1又は2に記載されるようなせん断力を伝達させる構造を構築することにより、タンクの浮き上がり荷重を地中壁に伝達させて、地中壁の自重及び引き抜き抵抗により抵抗させる技術が提案されている。   Conventionally, in order to prevent the tank from rising due to earth pressure or water pressure acting on the bottom surface of the LNG underground tank, the joint reinforcement between the joint surface between the underground wall constructed on the outer periphery of the LNG underground tank and the side wall of the tank Or by constructing a structure that transmits a shearing force as described in Patent Document 1 or 2, for example, the lift load of the tank is transmitted to the underground wall, and due to its own weight and pulling resistance Techniques for resisting have been proposed.

具体的には、特許文献1には、地下連続壁の頂部に内側方向に突出するような突出部と、地下タンクの側壁に当該突出部と係合するような段差部とを設けたせん断伝達構造が開示されている。また、特許文献2には、地下タンクの外周を形成する地下連続壁が深度方向に向けて広がる形状を有するせん断伝達構造が開示されている。
特開2003−41608号公報 特開平7−229321号公報
Specifically, Patent Document 1 discloses a shear transmission in which a protruding portion that protrudes inwardly at the top of a continuous underground wall and a stepped portion that engages with the protruding portion on a side wall of the underground tank. A structure is disclosed. Patent Document 2 discloses a shear transmission structure having a shape in which an underground continuous wall forming the outer periphery of an underground tank expands in the depth direction.
JP 2003-41608 A Japanese Patent Laid-Open No. 7-229321

しかしながら、接合鉄筋を設ける場合には、鉄筋の材料コストが増大するだけでなく、地中壁やコンクリート構造物の施工時にコンクリートの充填が不十分になるおそれがある。また施工に手間がかかる。   However, when jointed reinforcing bars are provided, not only does the material cost of the reinforcing bars increase, but there is a risk that the concrete will be insufficiently filled during construction of underground walls and concrete structures. In addition, it takes time for construction.

また、特許文献1及び2に開示されるせん断伝達構造は構造が複雑であるため、やはり、施工に手間がかかるうえ、施工にあたって高度な技術が要求されるという問題もある。   Moreover, since the structure of the shear transmission structure disclosed in Patent Documents 1 and 2 is complicated, there is also a problem that it takes time for construction, and high technology is required for construction.

本発明は、上記の点に鑑みてなされたものであり、簡易な構成で、地中壁と、地中壁と接合して構築されるコンクリート構造物との間にせん断力を伝達できるようにすることを目的とする。   The present invention has been made in view of the above points, and can transmit a shear force between an underground wall and a concrete structure constructed by joining the underground wall with a simple configuration. The purpose is to do.

上記の目的を達成するため、本発明は、地中壁と、前記地中壁と接合して構築されるコンクリート構造物との間に作用するせん断力を伝達するせん断伝達構造であって、
前記コンクリート構造物と前記地中壁との両接合面が、互いに噛み合うような波状、ノコギリ状、又は略台形状の凹凸形状を有し、
前記コンクリート構造物が前記地中壁に対して鉛直方向に相対移動すると、前記両接合面同士が鉛直方向に相対移動して前記両接合面の一方の凸部の頂部が他方の凸部の頂部に乗り上げることにより、前記両接合面間が離間し、前記接合面が離間することに応じて前記コンクリート構造物及び前記地中壁に作用する荷重と、前記両接合面間の摩擦係数とに基づいて求められた摩擦力が、前記コンクリート構造物に作用する鉛直方向の荷重よりも大きくなることを特徴とする(第1の発明)。
In order to achieve the above object, the present invention is a shear transmission structure that transmits a shear force acting between an underground wall and a concrete structure constructed by joining the underground wall,
The joining surfaces of the concrete structure and the underground wall is wavy to engage each other, sawtooth, or have a concave-convex shape of the substantially trapezoidal shape,
When the concrete structure moves relative to the underground wall in the vertical direction, the joint surfaces move relative to each other in the vertical direction, and the top of one convex portion of the joint surfaces is the top of the other convex portion. On the basis of the load acting on the concrete structure and the underground wall according to the separation of the joint surface and the coefficient of friction between the joint surfaces. frictional force obtained Te, characterized in Rukoto Do greater than the vertical direction of the load acting on the concrete structure (first invention).

本発明のせん断伝達構造によれば、接合鉄筋や特許文献1及び2に記載されるせん断伝達構造のように施工に手間や高度な技術を必要とすることなく簡易に構築でき、コンクリート構造物に作用する浮き上がり荷重等の鉛直方向の荷重を地中壁に伝達することができる。   According to the shear transmission structure of the present invention, it can be easily constructed without requiring labor and advanced techniques for construction, such as the jointed reinforcing bar and the shear transmission structure described in Patent Documents 1 and 2, and can be applied to a concrete structure. It is possible to transmit a vertical load such as a lifting load acting on the underground wall.

また、例えば、コンクリート構造物に鉛直方向の荷重が作用して微小移動した場合に、コンクリート構造物と地中壁との両接合面が離間するので、この離間にともなって、両接合面間に離間を離間前の状態に戻そうとする反力が生じ、この反力に応じて接合面間の摩擦力(=せん断伝達耐力)も増加するので、両接合面間で鉛直方向の荷重を効果に伝達することができる。 In addition , for example, when a vertical load acts on a concrete structure and moves slightly, both joint surfaces of the concrete structure and the underground wall are separated from each other. A reaction force is generated to return the separation to the state before separation, and the frictional force between the joint surfaces (= shear transmission resistance) increases in accordance with this reaction force, so the load in the vertical direction is effective between both joint surfaces. Can be communicated to.

また、コンクリート構造物に作用する鉛直方向の荷重に対してコンクリート構造物と地中壁との接合面が滑ることなく、かかる荷重をコンクリート構造物から地中壁に確実に伝達させる凹凸形状を、施工上効率良く形成することができる。 In addition , an uneven shape that reliably transmits the load from the concrete structure to the underground wall without slipping the joint surface between the concrete structure and the underground wall with respect to the vertical load acting on the concrete structure, It can be formed efficiently in construction.

の発明は、表面に凹凸形状を有する地中壁と接合して構築されるコンクリート構造物であって、
前記地中壁と接合する接合面に、前記地中壁の凹凸形状と噛み合うような波状、ノコギリ状、又は略台形状の凹凸形状を有し、
前記コンクリート構造物が前記地中壁に対して鉛直方向に相対移動すると、前記両接合面同士が鉛直方向に相対移動して前記両接合面の一方の凸部の頂部が他方の凸部の頂部に乗り上げることにより、前記両接合面間が離間し、前記接合面が離間することに応じて前記コンクリート構造物及び前記地中壁に作用する荷重と、前記両接合面間の摩擦係数とに基づいて求められた摩擦力が、前記コンクリート構造物に作用する鉛直方向の荷重よりも大きくなることを特徴とする。
The second invention is a concrete structure constructed by joining with an underground wall having an uneven shape on the surface,
Wherein the joint surface to be bonded to the ground wall, the underground wall of irregular shape and meshes such wavy, serrated, or have a concave-convex shape of the substantially trapezoidal shape,
When the concrete structure moves relative to the underground wall in the vertical direction, the joint surfaces move relative to each other in the vertical direction, and the top of one convex portion of the joint surfaces is the top of the other convex portion. On the basis of the load acting on the concrete structure and the underground wall according to the separation of the joint surface and the coefficient of friction between the joint surfaces. frictional force obtained Te, characterized in Rukoto Do greater than the vertical direction of the load acting on the concrete structure.

の発明は、第の発明において、LNG地下タンクに適用されたことを特徴とする。 3rd invention is applied to the LNG underground tank in 2nd invention, It is characterized by the above-mentioned.

の発明は、地中壁と、前記地中壁と接合して構築されるコンクリート構造物との間に作用するせん断力を伝達するせん断伝達構造の構築方法であって、
その表面に波状、ノコギリ状、又は略台形状の凹凸形状を有し、前記コンクリート構造物が前記地中壁に対して鉛直方向に相対移動すると、前記両接合面同士が鉛直方向に相対移動して前記両接合面の一方の凸部の頂部が他方の凸部の頂部に乗り上げることにより、前記両接合面間が離間し、前記接合面が離間することに応じて前記コンクリート構造物及び前記地中壁に作用する荷重と、前記両接合面間の摩擦係数とに基づいて求められた摩擦力が、前記コンクリート構造物に作用する鉛直方向の荷重よりも大きくなる地中壁を構築し、
前記地中壁の凹凸形状の表面に接触するように、コンクリートを打設し、
前記打設したコンクリートを養生することを特徴とする。
4th invention is the construction method of the shear transmission structure which transmits the shear force which acts between the underground wall and the concrete structure constructed by joining with the underground wall,
Corrugated on its surface, sawtooth, or have a concave-convex shape of the substantially trapezoidal, when the concrete structure is relatively moved in a vertical direction with respect to the diaphragm wall, wherein the joining faces are relatively moved in the vertical direction Then, when the top of one convex portion of both joint surfaces rides on the top of the other convex portion, the two joint surfaces are separated from each other, and the concrete structure and the ground according to the separation of the joint surfaces. a load acting on the middle wall, the friction coefficient and frictional force determined on the basis of the between both joint surfaces, to construct a diaphragm wall ing larger than the load in the vertical direction acting on the concrete structure,
Place concrete so that it touches the uneven surface of the underground wall,
The placed concrete is cured.

の発明は、第1の発明に記載のせん断伝達構造の設計方法であって、前記両接合面の摩擦力を、前記両接合面同士が鉛直方向に相対移動して前記両接合面の一方の凸部の頂部が他方の凸部の頂部に乗り上げることにより、前記接合面が離間することに応じて前記コンクリート構造物及び前記地中壁に作用する荷重と、前記両接合面間の摩擦係数とに基づいて求め、前記両接合面の凹凸形状を、前記摩擦力が、前記コンクリート構造物に作用する鉛直方向の荷重よりも大きくなるように設定することを特徴とする。 A fifth aspect of the invention is a design method for a shear transmission structure according to the first aspect of the invention, in which the frictional forces of the joint surfaces are moved relative to each other in the vertical direction so that the joint surfaces When the top of one convex part rides on the top of the other convex part, the load acting on the concrete structure and the underground wall according to the separation of the joint surface, and the friction between the joint surfaces It is calculated | required based on a coefficient, and the uneven | corrugated shape of the said both joint surfaces is set so that the said friction force may become larger than the load of the perpendicular direction which acts on the said concrete structure.

本発明によれば、簡易な構成で、地中壁と、地中壁と接合して構築されるコンクリート構造物との間にせん断力を伝達することが可能となる。   According to the present invention, it is possible to transmit a shear force between an underground wall and a concrete structure constructed by joining the underground wall with a simple configuration.

以下、本発明の好ましい一実施形態について図面に基づき詳細に説明する。
図1は、本実施形態に係るLNG地下タンク10の縦断面図である。
図1に示すように、LNG地下タンク10は、地盤40中に構築され、仮設の土留めや止水壁の役割をする地中連続壁20(以下、連壁20という)と、連壁20に接合して構築される貯槽本体30とからなる二重の円筒シェル構造を有している。
Hereinafter, a preferred embodiment of the present invention will be described in detail with reference to the drawings.
FIG. 1 is a longitudinal sectional view of an LNG underground tank 10 according to the present embodiment.
As shown in FIG. 1, the LNG underground tank 10 is constructed in the ground 40 and has an underground continuous wall 20 (hereinafter referred to as a continuous wall 20) that functions as a temporary earth retaining wall or a water blocking wall, and a continuous wall 20. It has a double cylindrical shell structure composed of a storage tank main body 30 constructed by being joined to each other.

図2は、図1の連壁20と貯槽本体30の側壁32との接合面の拡大断面図である。
図2に示すように、連壁20と貯槽本体30の側壁32との間に作用するせん断力(=つまり鉛直方向に作用する荷重)を伝達するせん断伝達構造1として、連壁20と貯槽本体30の側壁32との両接合面が、互いに噛み合うような凹凸形状を有している。これにより、例えば、貯槽本体30に浮き上がり荷重等が作用し、側壁32が連壁20に対してせん断方向に移動(つまり鉛直方向に相対移動)する場合、両接合面同士が互いに離間するように移動することになる。そして、両接合面が離間すると、側壁32及び連壁20は円筒構造を有していることから、側壁32には縮径するような圧縮方向の軸荷重が作用し、一方、連壁20には拡径するような引張方向の軸荷重が作用し、また、地盤40には連壁20の拡径にともなって連壁20の接面から押されて圧縮荷重が作用することになり、これら荷重に対する離間を離間前の状態に戻そうとする反力が生じ、この反力に応じて接合面間の摩擦力(=せん断伝達耐力)も増加して、両接合面間にせん断力が確実に伝達されるようになっている。
このようなせん断伝達構造1を有するLNG地下タンク10は、次のようにして構築する。
FIG. 2 is an enlarged cross-sectional view of the joint surface between the continuous wall 20 of FIG. 1 and the side wall 32 of the storage tank body 30.
As shown in FIG. 2, the shear wall 20 and the tank body are constructed as a shear transmission structure 1 that transmits a shearing force (= that is, a load acting in the vertical direction) acting between the wall 20 and the side wall 32 of the tank body 30. Both joint surfaces with the side wall 32 of 30 have the uneven | corrugated shape which meshes | engages mutually. Thereby, for example, when a floating load or the like acts on the storage tank body 30 and the side wall 32 moves in the shearing direction with respect to the continuous wall 20 (that is, relative movement in the vertical direction), the two joint surfaces are separated from each other. Will move. When the two joint surfaces are separated from each other, the side wall 32 and the connecting wall 20 have a cylindrical structure. Therefore, the side wall 32 is subjected to a compressive axial load that reduces the diameter. An axial load in the tension direction that expands the diameter acts, and the ground 40 is pressed from the contact surface of the continuous wall 20 as the diameter of the continuous wall 20 increases, and a compressive load acts on the ground 40. A reaction force that tries to return the load separation to the state before separation occurs, and the friction force between the joint surfaces (= shear transmission resistance) increases according to this reaction force, so that the shear force is ensured between both joint surfaces. To be communicated to.
The LNG underground tank 10 having such a shear transmission structure 1 is constructed as follows.

図3は、せん断伝達構造1を有するLNG地下タンク10の構築手順を示す工程図である。
図3に示すように、LNG地下タンク10の構築手順は、目荒らし35が形成された連壁20を構築する連壁構築工程S1と、貯槽本体30の側壁32が連壁20の目荒らし35の表面に接合するように、貯槽本体30のコンクリート38を打設する貯槽本体コンクリート打設工程S2と、打設したコンクリート38を養生するコンクリート養生工程S3とを備える。
FIG. 3 is a process diagram showing a construction procedure of the LNG underground tank 10 having the shear transmission structure 1.
As shown in FIG. 3, the construction procedure of the LNG underground tank 10 includes a continuous wall construction step S <b> 1 for constructing the continuous wall 20 in which the roughening 35 is formed, and the side wall 32 of the storage tank body 30 is the roughening 35 of the continuous wall 20. A storage tank body concrete placing step S2 for placing the concrete 38 of the storage tank body 30 and a concrete curing step S3 for curing the placed concrete 38 so as to be joined to the surface of the storage tank.

連壁構築工程S1では、先ず地盤40に連壁20を構築する。連壁20の構築は、一般的な公知の施工方法を用いて行うことができる。そして連壁20が充分に養生されて硬化した後に、連壁20の内側(貯槽本体30が構築される側)の表面に、目荒らし35を形成するべくチッピング加工を施す。チッピング加工は、例えば、建機に削岩用のアタッチメントとしてシー・エイ・イー株式会社から販売されるスパイキーハンマー等を用いることにより簡単に施工することができる。ここで、チッピング加工を行うにあたり、目荒らし35の凹凸が所定の高低差となるように形成する。なお、この凹凸の高低差の詳細な設計については後述する。   In the continuous wall construction step S <b> 1, first, the continuous wall 20 is constructed on the ground 40. Construction of the continuous wall 20 can be performed using a general known construction method. Then, after the continuous wall 20 is sufficiently cured and hardened, a chipping process is performed on the surface inside the continuous wall 20 (the side on which the storage tank body 30 is constructed) to form the roughening 35. The chipping process can be easily performed by using, for example, a spiky hammer sold by CAE Co., Ltd. as a rock drilling attachment on a construction machine. Here, when performing the chipping process, the unevenness of the roughening 35 is formed to have a predetermined height difference. The detailed design of the uneven height difference will be described later.

貯槽本体コンクリート打設工程S2では、連壁構築工程S1で構築された連壁20表面の目荒らし35に接するように、貯槽本体30の側壁32となるコンクリート38を打設する。   In the storage tank body concrete placing step S2, the concrete 38 serving as the side wall 32 of the storage tank body 30 is placed so as to be in contact with the roughening 35 on the surface of the continuous wall 20 constructed in the continuous wall construction step S1.

コンクリート養生工程S3では、貯槽本体コンクリート打設工程S2で打設された、貯槽本体30の側壁32を構成するコンクリート38を充分に養生して硬化させる。   In the concrete curing process S3, the concrete 38 constituting the side wall 32 of the storage tank body 30 cast in the storage tank body concrete placing process S2 is sufficiently cured and cured.

これら工程S1〜S3を行うことにより、目荒らし35が形成された連壁20が型枠となって、貯槽本体30の側壁32のコンクリート38が打設及び養生され、連壁20と側壁32との両接合面に互いに噛み合うような波状の凹凸が構築されることになる。   By performing these steps S <b> 1 to S <b> 3, the continuous wall 20 in which the roughening 35 is formed becomes a mold, and the concrete 38 on the side wall 32 of the storage tank body 30 is placed and cured, and the continuous wall 20 and the side wall 32 are Thus, wavy irregularities that engage with each other are constructed.

ただし、実際には、連壁20と側壁32との間に浸入する地下水の水圧等によって、連壁20と側壁32との間にせん断力が作用しなくても、連壁20と側壁32との間に隙間が生じる。これについては、後述の凹凸の高低差の設計と合わせて具体的に説明する。   However, actually, even if a shearing force does not act between the continuous wall 20 and the side wall 32 due to the water pressure of groundwater entering between the continuous wall 20 and the side wall 32, the continuous wall 20 and the side wall 32 A gap is formed between the two. This will be specifically described together with the design of the height difference of the unevenness described later.

次に、貯槽本体30に作用する浮き上がり力について具体的数値を用いて説明する。
図4は、LNG地下タンク10に最大の浮き上がり力が作用するときに、側壁32と連壁20との間に作用する鉛直方向の荷重(以下、作用荷重Wという)を求めるための説明図であり、図5は、LNG地下タンク10の具体的な寸法を示す断面図である。なお、LNG地下タンク10内にはLNGが貯留されてないときを想定している。
Next, the lifting force acting on the storage tank body 30 will be described using specific numerical values.
FIG. 4 is an explanatory diagram for obtaining a vertical load (hereinafter referred to as an applied load W) acting between the side wall 32 and the continuous wall 20 when the maximum lifting force is applied to the LNG underground tank 10. FIG. 5 is a cross-sectional view showing specific dimensions of the LNG underground tank 10. It is assumed that no LNG is stored in the LNG underground tank 10.

作用荷重Wは、図4に示す貯槽本体重量Wtu、揚圧力WU、及び地震時の増加荷重Weを用いて次式(1)により求められる。
W=-Wtu+WU+We ・・(1)
貯槽本体重量Wtuは、例えば、次式(2)のように側壁32の側壁重量Wt1と、底版36の底版重量Wt2と、その他屋根部分等の付帯重量Wt3との和から求められる。
Wtu=Wt1+Wt2+Wt3 ・・(2)
さらに、側壁重量Wt1は、次式(3)のように、側壁32の厚みが一定な一般部33の重量Ws1と、側壁32の下部の厚みが下方に移行するにつれて内側に肉厚になる側壁下端ハンチ部34の重量Ws2との和により求められる。
Wt1=Ws1+Ws2 ・・(3)
例えば、図5に示すような貯槽本体30の寸法の場合には、コンクリートの単位体積重量を24.0kN/m3とすると、一般部33の重量Ws1は、
Ws1=(38.4142-36.0142)×π×(15.800+25.158)×24.0+π×1.20
×{38.4142-(36.0142+36.014×37.214+37.2142)/3}×24.0
=563.84×103kN ・・(4)
となり、側壁下端ハンチ部34の重量Ws2は、
Ws2=π×3.00×{36.0142-(33.0142+33.014×36.014+36.0142)/3}×24.0
=23.76×103kN ・・(5)
となるので、側壁重量Wt1は、
Wt1=563.84×103+23.76×103=587.60×103kN ・・(6)
となる。
Working load W is the reservoir body weight W tu shown in FIG. 4, uplift W U, and is obtained by the following expression (1) using the increased load W e during an earthquake.
W = -W tu + W U + W e (1)
The storage tank body weight W tu is obtained, for example, from the sum of the side wall weight W t1 of the side wall 32, the bottom plate weight W t2 of the bottom plate 36, and the incidental weight W t3 of the roof portion or the like as in the following equation (2). .
W tu = W t1 + W t2 + W t3 (2)
Further, the side wall weight W t1 is increased in thickness as the weight W s1 of the general portion 33 having a constant thickness of the side wall 32 and the thickness of the lower portion of the side wall 32 shift downward as shown in the following equation (3). determined by the sum of the weight W s2 of comprising the side wall lower end haunch portions 34.
W t1 = W s1 + W s2 (3)
For example, in the case of the dimensions of the storage tank body 30 as shown in FIG. 5, if the unit volume weight of the concrete is 24.0 kN / m 3 , the weight W s1 of the general part 33 is
W s1 = (38.414 2 -36.014 2 ) × π × (15.800 + 25.158) × 24.0 + π × 1.20
× {38.414 2- (36.014 2 + 36.014 × 37.214 + 37.214 2 ) / 3} × 24.0
= 563.84 × 10 3 kN (4)
The weight W s2 of the side wall lower end haunch part 34 is
W s2 = π × 3.00 × {36.014 2- (33.014 2 + 33.014 × 36.014 + 36.014 2 ) / 3} × 24.0
= 23.76 × 10 3 kN ・ ・ (5)
Therefore, the side wall weight W t1 is
W t1 = 563.84 × 10 3 + 23.76 × 10 3 = 587.60 × 10 3 kN ・ ・ (6)
It becomes.

また、底版重量Wt2は、
Wt2=38.4142×π×6.4×24.0=712.07×103kN ・・(7)
となる。
The bottom plate weight W t2 is
W t2 = 38.414 2 × π × 6.4 × 24.0 = 712.07 × 10 3 kN (7)
It becomes.

また、付帯重量Wt3は、仮設鋼製屋根、吊デッキ、リングプレート、バレル・ノズル、ステージ、内部足場、メンブレン、保冷パネル等の付帯部材37による重量であり、図5に示すLNG地下タンク10の場合には1698ton程度になるので、重力加速度を乗じて、
Wt3=1698ton×9.80665=16.65×103kN ・・(8)
となる。
したがって、WtuはこれらWt1,Wt2,Wt3の和により、
Wtu=587.60×103+712.07×103+16.65×103=1316.32×103kN ・・(9)
となる。
Further, the incidental weight W t3 is the weight of the incidental member 37 such as a temporary steel roof, a suspended deck, a ring plate, a barrel / nozzle, a stage, an internal scaffold, a membrane, a cold insulation panel, and the LNG underground tank 10 shown in FIG. In the case of, it will be around 1698ton, so multiply by the gravitational acceleration,
W t3 = 1698ton × 9.80665 = 16.65 × 10 3 kN ・ ・ (8)
It becomes.
Therefore, W tu is the sum of W t1 , W t2 , W t3 ,
W tu = 587.60 × 10 3 + 712.07 × 10 3 + 16.65 × 10 3 = 1316.32 × 10 3 kN ・ ・ (9)
It becomes.

揚圧力WUとしては、例えば、地盤40中の地下水の高水位時(地下水位DL+3.300m)に底版36下に作用する浮力を求める。揚圧力WUは次式(10)で求められ、
WUw×g×π×r2×h ・・(10)
具体的に図5の寸法を代入すると
WU =1.00×9.80665×π×38.4142×(3.3+31.558)=1584.72×103kN
となる。ここで、ρwは水の密度、gは重力加速度、rはタンク中心から側壁32の外側面までの距離、hは地下水位から底版36下端までの深さである。
As the lifting pressure W U , for example, the buoyancy acting under the bottom slab 36 at the time of high groundwater level in the ground 40 (groundwater level DL + 3.300 m) is obtained. The lifting pressure W U is obtained by the following equation (10),
W U = ρ w × g × π × r 2 × h (10)
Specifically, if the dimensions of FIG. 5 are substituted,
W U = 1.00 × 9.80665 × π × 38.414 2 × (3.3 + 31.558) = 1584.72 × 10 3 kN
It becomes. Here, [rho w is the density of water, g is the gravitational acceleration, the distance r from the tank center to the outer surface of the side wall 32, h is the depth from the groundwater level to the bottom plate 36 the lower end.

地震時の増加荷重Weは、地震時に鉛直上向方向に作用する慣性力であり、次式(11)のように、LNG地下タンク10の各部分(側壁32、底版36、付帯部材37)により設定される鉛直方向の設計震度(KV1〜3)について、各部分の重量(側壁重量Wt1、底版重量Wt2、付帯重量Wt3)との積を足し合わせることにより求められ、
We=KV1×Wt1+KV2×Wt2+KV3×Wt3 ・・(11)
具体的に図5に示すLNG地下タンク10の場合では、
We=0.119×587.60×103+0.082×712.07×103+0.150×16.65×103=130.81×103 kN
となる。
When increased load W e earthquake, a inertial force acting in a vertical upward direction during an earthquake, the following equation (11), each portion of the LNG underground tanks 10 (side wall 32, bottom plate 36, bearing member 37) The vertical design seismic intensity (K V1-3 ) set by, is obtained by adding the product of the weight of each part (side wall weight W t1 , bottom plate weight W t2 , incidental weight W t3 ),
W e = K V1 × W t1 + K V2 × W t2 + K V3 × W t3 (11)
Specifically, in the case of the LNG underground tank 10 shown in FIG.
W e = 0.119 × 587.60 × 10 3 + 0.082 × 712.07 × 10 3 + 0.150 × 16.65 × 10 3 = 130.81 × 10 3 kN
It becomes.

以上により、作用荷重Wは上向きを正として、式(1)により以下のように算定される。
W=-Wtu+WU+We ・・(1)
=−1316.32×103+1584.72×103+130.81×103=399.21×103 kN
したがって、設計せん断力Wdは、荷重係数を1.1として考慮すると、
Wd=1.1×W=439.13×103kN ・・(12)
となる。
このようにして求められた設計せん断力Wdに対抗する、連壁20と側壁32との両接合面の摩擦力(=せん断伝達耐力)は以下のようにして求められる。
As described above, the applied load W is calculated as follows using the formula (1), with the upward direction being positive.
W = -W tu + W U + W e (1)
= −1316.32 × 10 3 + 1584.72 × 10 3 + 130.81 × 10 3 = 399.21 × 10 3 kN
Therefore, the design shear force W d is taken into account when the load factor is 1.1.
W d = 1.1 × W = 439.13 × 10 3 kN ・ ・ (12)
It becomes.
This as opposed to the design shear force W d obtained by the frictional force the joining surface between the continuous wall 20 and side walls 32 (= shear transfer strength) is obtained as follows.

図2に示すように、貯槽本体30に浮き上がり荷重Sが作用し、側壁32が連壁20に対してせん断方向(つまり鉛直方向に相対移動)に移動するのに伴って、両接合面同士が互いに離間する距離(以下、離れ量という)をδとする。そして、この離れ量δに応じて側壁32、連壁20、及び地盤40に生じる圧縮力をσndとすると、せん断伝達耐力Vcwdは、次式(13)に示すように、圧縮力σndに対する反力-σndに摩擦係数μを乗じたものとして求められる。
Vcwd=μ×(-σnd) ・・(13)
図6は、LNG地下タンク10の側壁32及び連壁20を2重円環として表したLNG地下タンクモデルの横断面図である。
As shown in FIG. 2, as the floating load S acts on the storage tank body 30 and the side wall 32 moves in the shearing direction (that is, relative movement in the vertical direction) with respect to the continuous wall 20, both joint surfaces become Let δ be a distance away from each other (hereinafter referred to as a distance). When the compressive force generated on the side wall 32, the continuous wall 20, and the ground 40 according to the separation amount δ is σ nd , the shear transmission resistance Vcwd is expressed by the following equation (13) with respect to the compressive force σ nd . It is calculated as the reaction force -σ nd multiplied by the friction coefficient μ.
Vcwd = μ × (-σ nd ) (13)
FIG. 6 is a cross-sectional view of the LNG underground tank model in which the side wall 32 and the connecting wall 20 of the LNG underground tank 10 are represented as a double ring.

図6に示すように、Rは2重円環の中心から側壁32と連壁20との境界までの半径、PWは境界から側壁32側に作用する内圧、PSは境界から連壁20側に作用する外圧、Ec,wは側壁32のヤング率、Ec,wは連壁20のヤング率、twは側壁厚、tsは連壁厚を示している。また、連壁20が構築される地盤40をバネとして仮定し、kgバネ係数である。 As shown in FIG. 6, the radius of R from the center of the double ring to the boundary between the side walls 32 and Renkabe 20, P W is the internal pressure acting on the side wall 32 side from the boundary, P S is continuous wall from the boundary 20 The external pressure acting on the side, E c, w is the Young's modulus of the side wall 32, E c, w is the Young's modulus of the continuous wall 20, tw is the side wall thickness, and ts is the continuous wall thickness. In addition, assuming that the ground 40 on which the continuous wall 20 is constructed is a spring, it is a kg spring coefficient.

ここで、側壁32と連壁20との離れ量δは、次式(14)のように、側壁32の貯槽本体30内側への変位量δwと、連壁20の外側への変位量δsとの和として求められる。
δ=δw+δs ・・(14)
ここで円環がδwだけ内側へ変位するとき側壁32に内圧PWが作用する。このとき側壁32の円周方向に作用する軸力Nθ,wは、次式(15)のように表される。
Nθ,w=PW・RW・・(15)
なお、Rwは側壁32の半径である。
Here, the distance δ between the side wall 32 and the continuous wall 20 is determined by the amount of displacement δ w of the side wall 32 to the inside of the storage tank body 30 and the amount of displacement δ to the outside of the continuous wall 20 as shown in the following equation (14). It is calculated as the sum of s .
δ = δ w + δ s (14)
Here, when the ring is displaced inward by δ w , the internal pressure P W acts on the side wall 32. At this time, the axial force Nθ, w acting in the circumferential direction of the side wall 32 is expressed by the following equation (15).
N θ, w = P W ・ R W・ ・ (15)
R w is the radius of the side wall 32.

ここで、Nθ,wは、側壁円周方向歪εθ,wを用いて次式(16)のようにも表され、
Nθ,wθ,w×Ec,w×tw ・・(16)
側壁円周方向歪εθ,wは、次式(17)のように表されるので、

Figure 0004900236
式(15)及び式(16)は、次式(18)のように整理される。
Figure 0004900236
一方、円環がδsだけ外側へ変位するためには、連壁20には、外圧PSから地盤40からの反力kgδsを差引いた力(PS-kgδs)が作用するので、式(15)〜(18)と同様に、連壁円周方向に作用する軸力Nθ,sは、次式(19)のように表される。
Figure 0004900236
ここで、PwとPsとは作用・反作用の関係にあるのでPw=Psであり、またRw≒Rs=Rとすると、式(18)と式(19)は次式(20)のように整理される。
Figure 0004900236
また、式(20)からPw・Rを消去して整理すると、δwは次式(21)のように表される。
Figure 0004900236
ここで、具体的に図5のLNG地下タンク10のケースをあてはめ、DL-12.772m以浅又は以深によってヤング率がE1c,w又はE2c,wに変化すると仮定すると、これらの深度域に対応する側壁32の内側への変位量δw1又はδw2は、次式(22)及び(23)のように計算される。
Figure 0004900236
ただし、上記計算には、E1c,w=28kN/mm2(DL-12.772m以浅)、E2c,w=31kN/mm2(DL-12.772m以深)、tw=2400mm、Ec,s=33kN/mm2、ts=1000mm、Kg =0.0050N/mm2、R=38414mmを用いた。 Here, N θ, w is also expressed by the following equation (16) using the side wall circumferential strain ε θ, w :
N θ, w = ε θ, w × E c, w × t w (16)
Since the side wall circumferential strain ε θ, w is expressed by the following equation (17),
Figure 0004900236
Expressions (15) and (16) are arranged as the following expression (18).
Figure 0004900236
On the other hand, in order for the ring to be displaced outward by δ s, a force (P S -kg δ s ) obtained by subtracting the reaction force kg δ s from the ground 40 from the external pressure P S acts on the connecting wall 20. Similar to the equations (15) to (18), the axial force Nθ, s acting in the circumferential direction of the connecting wall is expressed as the following equation (19).
Figure 0004900236
Here, since P w and P s are in a relationship of action and reaction, P w = P s and when R w ≈R s = R, Equation (18) and Equation (19) are expressed by the following equation ( 20).
Figure 0004900236
Further, when P w · R is deleted from the equation (20) and rearranged, δ w is expressed as the following equation (21).
Figure 0004900236
Here, the case of the LNG underground tank 10 of FIG. 5 is specifically applied, and assuming that Young's modulus changes to E 1c, w or E 2c, w by DL-12.772m shallower or deeper, it corresponds to these depth regions. The amount of displacement δ w1 or δ w2 to the inside of the side wall 32 is calculated as in the following equations (22) and (23).
Figure 0004900236
However, the above calculation, E 1c, w = 28kN / mm 2 (DL-12.772m shallower), E 2c, w = 31kN / mm 2 (DL-12.772m deeper), t w = 2400mm, E c, s = 33 kN / mm 2 , t s = 1000 mm, K g = 0.0050 N / mm 2 , R = 38414 mm were used.

また、式(20)により、深度による境界から側壁32側に作用する内圧Pw1及びPw2は、次式(24)及び(25)のように求められる。

Figure 0004900236
したがって、式(22)及び式(23)を式(24)及び式(25)に代入することにより、内圧Pw1及びPw2、外圧Ps1及びPs2は、次式(26)及び(27)のように整理される。
Pw1=Ps1=0.045×0.375δ=0.017δ (DL-12.772以浅) ・・(26)
Pw2=Ps2=0.050×0.352δ=0.018δ (DL-12.772以深) ・・(27)
一方、図3で説明したように、LNG地下タンク10構築後に、側壁32と連壁20との間にせん断力が作用しない場合でも、連壁20と側壁32との間には隙間が生じる。これは、貯槽本体30内のLNGからの冷熱によって側壁32及び連壁20が収縮したり、貯槽本体30及び連壁20に地下水圧の作用したりすることによる。 Further, the internal pressures P w1 and P w2 acting on the side wall 32 side from the boundary due to the depth are obtained from the equation (20) as the following equations (24) and (25).
Figure 0004900236
Therefore, by substituting the equations (22) and (23) into the equations (24) and (25), the internal pressures P w1 and P w2 and the external pressures P s1 and P s2 are expressed by the following equations (26) and (27 ).
P w1 = P s1 = 0.045 × 0.375δ = 0.017δ (DL-12.772 or less) ・ ・ (26)
P w2 = P s2 = 0.050 × 0.352δ = 0.018δ (DL-12.772 or deeper) (27)
On the other hand, as described with reference to FIG. 3, after the LNG underground tank 10 is constructed, a gap is generated between the continuous wall 20 and the side wall 32 even when a shearing force does not act between the side wall 32 and the continuous wall 20. This is because the side wall 32 and the continuous wall 20 contract due to cold heat from the LNG in the storage tank body 30, or the ground water pressure acts on the storage tank body 30 and the connection wall 20.

図7は、LNGからの冷熱による側壁32及び連壁20の変位を示すグラフである。
図7に示す側壁32の変位は、躯体の構造解析から得られる温度荷重により求めている。また、連壁20の変位は、躯体の温度解析により得られた連壁20の平均温度T=-12.29℃、地盤40の初期温度To=16.6℃、コンクリートの線膨張係数α=1.0×10-5、連壁20の半径R=38414mmとして、次式(28)により変位δを算定している。
δ=R×α×(T−T0)=38414×1.0×10-5×(−12.29−16.6)=−11.1mm ・・(28)
図8は、水圧及び揚圧力による側壁32の変位を示すグラフである。
図8に示す側壁32の変位は、躯体の構造解析から得られる水圧及び揚圧力により求めている。
FIG. 7 is a graph showing the displacement of the side wall 32 and the continuous wall 20 due to cold from LNG.
The displacement of the side wall 32 shown in FIG. 7 is calculated | required with the temperature load obtained from the structural analysis of a housing. In addition, the displacement of the continuous wall 20 includes the average temperature T = -12.29 ° C. of the continuous wall 20 obtained by the temperature analysis of the frame, the initial temperature To = 16.6 ° C. of the ground 40, and the linear expansion coefficient α of the concrete = 1.0 × 10 − 5. The displacement δ is calculated by the following equation (28) assuming that the radius R of the continuous wall 20 is 38414 mm.
δ = R × α × (T−T 0 ) = 38414 × 1.0 × 10 −5 × (−12.29−16.6) = − 11.1 mm (28)
FIG. 8 is a graph showing displacement of the side wall 32 due to water pressure and lift pressure.
The displacement of the side wall 32 shown in FIG. 8 is calculated | required by the water pressure and lifting pressure obtained from the structural analysis of a housing.

図9は、水圧による連壁20の変位を示すグラフである。
図9に示すように連壁20は、側壁32と連壁20との間に浸入する水の圧力により外側に変位する。これは、式(22)及び(23)と、式(26)及び(27)とにより、次式(29)及び(30)のように、深度による境界から連壁20側に作用する外圧Ps1及びPs2による連壁20の変位δs1及びδs2が求められる。
δs1=(1−0.375)δ=0.625δ=0.625/0.017×Ps1(DL−12.772以浅) ・・(29)
δs2=(1−0.352)δ=0.648δ=0.648/0.018×Ps2(DL−12.772以深) ・・(30)
そして、図10は、側壁32及び連壁20について、これら温度、水圧及び揚圧力による合計変位量を示したグラフであり、図11は、図10の側壁32と連壁20との変位差を示すグラフである。
図10及び図11に示すように、側壁32と連壁20との変位の差、すなわち隙間(2〜14mm)は下方に推移するほど大きくなり、その平均は10.8mmである。
FIG. 9 is a graph showing the displacement of the continuous wall 20 due to water pressure.
As shown in FIG. 9, the connecting wall 20 is displaced outward by the pressure of water that enters between the side wall 32 and the connecting wall 20. This is based on the equations (22) and (23) and the equations (26) and (27), as shown in the following equations (29) and (30). The displacements δ s1 and δ s2 of the connecting wall 20 due to s1 and P s2 are obtained.
δ s1 = (1-0.375) δ = 0.625 δ = 0.625 / 0.017 x P s1 (DL-12.772 or less) (29)
δ s2 = (1-0.352) δ = 0.648 δ = 0.648 / 0.018 x P s2 (DL-12.72 or deeper) (30)
FIG. 10 is a graph showing the total displacement amount due to the temperature, the hydraulic pressure, and the lifting pressure for the side wall 32 and the continuous wall 20, and FIG. 11 shows the displacement difference between the side wall 32 and the continuous wall 20 of FIG. It is a graph to show.
As shown in FIGS. 10 and 11, the difference in displacement between the side wall 32 and the continuous wall 20, that is, the gap (2 to 14 mm) increases as it moves downward, and its average is 10.8 mm.

すなわち、以上のような隙間が生じる場合、連壁20の表面にチッピング加工により目高低差15mmの目荒らし35を形成しても、当初側壁32と連壁20との噛み合わせが15mmであったものが、平均4.2mm(=15mm-10.8mm)程度になる。   That is, when the gaps as described above are generated, the meshing between the side wall 32 and the continuous wall 20 is initially 15 mm even if the roughening 35 having a difference in height of 15 mm is formed on the surface of the continuous wall 20 by chipping. The average is about 4.2mm (= 15mm-10.8mm).

そこで、噛み合わせが4.2mmである場合におけるせん断伝達耐力を求める。すなわち、側壁32と連壁20との両接合面同士が、鉛直方向に相対移動して両接合面の一方の凸部の頂部が他方の凸部の頂部に乗り上げることにより、接合面間の離間が4.2mmになったとき(=噛み合わせがゼロとなったとき)の両接面間に生じる摩擦力を求める。   Therefore, the shear transmission resistance when the meshing is 4.2 mm is obtained. That is, the joint surfaces of the side wall 32 and the continuous wall 20 are moved relative to each other in the vertical direction, and the top of one convex portion of both joint surfaces rides on the top of the other convex portion, thereby separating the joint surfaces. Find the frictional force generated between the two contact surfaces when the value becomes 4.2 mm (when the meshing becomes zero).

噛み合わせが4.2mmである場合、側壁32と連壁20とが、両接合面に形成された凹凸を乗り越えるために必要な内圧Pw及び外圧Psは、δ=4.2mmを式(26)及び式(27)に代入することにより、
Pw1=Ps1=0.0714 N/mm2 ・・(31)
Pw2=Ps2=0.0756 N/mm2 ・・(32)
となる。
When the meshing is 4.2 mm, the internal pressure P w and the external pressure P s required for the side wall 32 and the continuous wall 20 to overcome the unevenness formed on both joint surfaces are set as follows: And substituting into equation (27),
P w1 = P s1 = 0.0714 N / mm 2・ ・ (31)
P w2 = P s2 = 0.0756 N / mm 2 (32)
It becomes.

ただし、「コンクリート標準示方書 6.3.7設計せん断伝達力」に準拠して、σndが圧縮の場合、安全側になることを考慮したσnd=-σnd/2を用いることとする。したがって、次式(33)及び(34)の圧縮力を、せん断面に垂直に作用する平均応力度として、せん断伝達耐力Vcwdの式中で取り扱うとする。
―σnd1=Pw1/2=Ps1/2=0.0357N/mm2 ・・(33)
―σnd1=Pw2/2=Ps2/2=0.0378N/mm2 ・・(34)
せん断伝達耐力Vcwdの基本式は次式(35)のように表される。
Vcwd=|(τc+p・τs・sin2θ−α・p・fyd ・sinθ・cosθ)・Ac+Vk|/γb ・・(35)
ただし、本実施形態では、側壁32と連壁20との間のせん断面に鉄筋がないこと、及びせん断キーがないことより、式(35)は、次式(36)のように整理される。
Vcwd=τc・Ac/γb、ただし、τc=μ・f’cdb(−σnd)1−b ・・(36)
ここで、μは固体接触に関する平均摩擦係数、Acはせん断面の面積、γbは部材係数、bは面形状を表す係数である。
However, σ nd = -σ nd / 2 is used in consideration of the fact that σ nd is compressed in accordance with “Concrete Standard Specification 6.3.7 Design Shear Transmission Force”. Therefore, it is assumed that the compressive force of the following equations (33) and (34) is handled in the equation of the shear transfer resistance Vcwd as the average stress acting perpendicularly to the shear plane.
―Σ nd1 = P w1 / 2 = P s1 /2=0.0357N/mm 2・ ・ (33)
―Σ nd1 = P w2 / 2 = P s2 /2=0.0378N/mm 2・ ・ (34)
The basic formula of the shear transmission strength Vcwd is expressed as the following formula (35).
Vcwd = | (τ c + p, τ s , sin 2 θ−α, p, fyd, sin θ, cos θ), Ac + Vk | / γ b (35)
However, in this embodiment, since there is no reinforcing bar on the shear plane between the side wall 32 and the continuous wall 20 and there is no shear key, the expression (35) is arranged as the following expression (36). .
Vcwd = τ c · Ac / γ b , where τ c = μ · f′cd b (−σ nd ) 1−b ·· (36)
Here, μ is an average friction coefficient regarding solid contact, Ac is an area of a shear plane, γ b is a member coefficient, and b is a coefficient representing a surface shape.

具体的に上記式(36)に図5に示すLNG地下タンク10の具体的寸法を以下のように代入すると、
h1:側壁高さ(DL+4.000〜−12.772m):16.772m ・・(37)
h2:側壁高さ(DL−12.772〜−28.358m):15.586m ・・(38)
Ac1=2×R×π×h1=2×38.414×π×16.772=4048m2 ・・(39)
Ac2=2×R×π×h2=2×38.414×π×15.586=3761m2 ・・(40)
γb=1.3 ・・(41)
f’cd=f’ck/γc=30/1.3=23.1N/mm2(DL−12.772m以浅) ・・(42)
f’cd=f’ck/γc=40/1.3=30.8N/mm2(DL−12.772m以深) ・・(43)
σnd:せん断面に垂直に作用する平均応力度 ・・(44)
せん断伝達力Vcwdは、
Vcwd1=τc・Ac1/γb=0.45×(23.1)1/2×(0.0357)1/2×4048×106/1.3≒1,272,000kN ・・(45)
Vcwd2=τc・Ac2/γb=0.45×(30.8)1/2×(0.0378)1/2×3761×106/1.3≒1,405,000kN ・・(46)
により、
Vcwd=Vcwd1+Vcwd2=1272000+1405000=2677000kN ・・(47)
と算定される。
Specifically, substituting the specific dimensions of the LNG underground tank 10 shown in FIG.
h1: Side wall height (DL + 4.000 to −12.772m): 16.772m (37)
h2: Side wall height (DL-12.72 to -28.358m): 15.586m (38)
Ac1 = 2 × R × π × h1 = 2 × 38.414 × π × 16.772 = 4048m 2 (39)
Ac2 = 2 × R × π × h2 = 2 × 38.414 × π × 15.586 = 3761m 2 (40)
γ b = 1.3 (41)
f'cd = f'ck / γ c = 30 / 1.3 = 23.1N / mm 2 (DL-12.772m or less) ・ ・ (42)
f'cd = f'ck / γ c = 40 / 1.3 = 30.8N / mm 2 (DL-12.772m or deeper) (43)
σ nd : Average stress acting perpendicularly to the shear plane (44)
Shear transmission force Vcwd is
Vcwd1 = τ c・ Ac1 / γ b = 0.45 × (23.1) 1/2 × (0.0357) 1/2 × 4048 × 10 6 /1.3≒1,272,000kN ・ ・ (45)
Vcwd2 = τ c・ Ac2 / γ b = 0.45 × (30.8) 1/2 × (0.0378) 1/2 × 3761 × 10 6 /1.3≒1,405,000kN ・ ・ (46)
By
Vcwd = Vcwd1 + Vcwd2 = 1272000 + 1405000 = 2677000kN (47)
Is calculated.

すなわち、このせん断伝達力Vcwd(2677000kN)は、先に式(12)で求めたLNG地下タンク10の貯槽本体30の側壁32と連壁20との間に最もせん断力が大きく作用するときの設計せん断力Wd(439.13×103kN)よりも充分大きい。これにより、当初側壁32と連壁20との噛み合わせが15mmであったものが、平均4.2mm(=15mm-10.6mm)程度になった場合においても、側壁32と連壁20との接合面が互いにその表面に形成された凹凸を乗り越えることなく、せん断力を伝達することができる。 That is, this shear transmission force Vcwd (2677000 kN) is designed when the shear force is the largest between the side wall 32 of the storage body 30 of the LNG underground tank 10 and the continuous wall 20 obtained by the equation (12). It is sufficiently larger than the shearing force W d (439.13 × 10 3 kN). As a result, even though the initial engagement of the side wall 32 and the continuous wall 20 is 15 mm, even when the average is about 4.2 mm (= 15 mm-10.6 mm), the joint surface between the side wall 32 and the continuous wall 20 The shear force can be transmitted without overcoming the irregularities formed on the surfaces of each other.

なお、本実施形態では、上述のように連壁20の表面に形成する目荒らし35の高低差を先に設定して、その高低差から連壁20と側壁32との間に生じる隙間から両接面間の実質的な噛み合わせ量を求め、そして噛み合わせ量に基づいたせん断伝達力Vcwdを求めることにより、その高低差がせん断力を伝達するのに妥当であるか否かを評価したが、これに限らず、想定される設計せん断力Wdに基づいて、それに必要なせん断伝達力Vcwdを計算し、そのせん断伝達力Vcwdに基づいた噛み合わせ量を設定するとともに、連壁20と側壁32との間に生じる隙間を勘案することにより目荒らし35の高低差を求めてもよい。 In the present embodiment, as described above, the level difference of the roughening 35 formed on the surface of the continuous wall 20 is set first, and both the gaps formed between the continuous wall 20 and the side wall 32 are determined based on the height difference. Although the substantial meshing amount between the contact surfaces was obtained, and the shear transmission force Vcwd based on the meshing amount was obtained, it was evaluated whether the height difference was appropriate for transmitting the shearing force. , not limited thereto, together with on the basis of the design shear force W d envisioned, it shear transfer force Vcwd calculates necessary to set the amount engagement based on the shear transmission force Vcwd, continuous wall 20 and the side wall The height difference of the roughening 35 may be obtained by taking into account the gap generated between the two.

具体的には、式(26)及び(27)までの内圧PW1及びPW2、外圧Ps1及びPs2を求めるところまでは、上述のとおりである。 Specifically, the steps up to obtaining the internal pressures P W1 and P W2 and the external pressures P s1 and P s2 up to the expressions (26) and (27) are as described above.

ここで目荒らし35の高低差を求めるにあたっては、「コンクリート標準示方書 6.3.7設計せん断伝達耐力」により、σndが圧縮の場合、安全側となることを考慮してσnd=-σnd/2を用いる事として、式(26)及び(27)を次式(48)及び(49)のように変換する。
−σnd1=−0.0085δ N/mm2 ・・(48)
−σnd2=−0.0090δ N/mm2 ・・(49)
これらの式を、式(36)中の−σndとして取り扱うことにより、式(37)〜(44)で用いた具体的寸法を代入すると、せん断伝達力Vcwdは、
Vcwd1=τc・Ac1/γb
=0.45×(23.1)1/2×(0.0085δ)1/2×4048×106/1.3≒620900×δ1/2kN ・・(50)
Vcwd2=τc・Ac2/γb
=0.45×(30.8)1/2×(0.0090δ)1/2×3761×106/1.3≒685400×δ1/2kN ・・(51)
により、
Vcwd=Vcwd1+Vcwd2
=620900×δ1/2+685400×δ1/2=1306000×δ1/2kN ・・(52)
と算定される。
Here, when calculating the level difference of the roughening 35, σ nd = -σ nd in consideration of the fact that σ nd is a compression side according to “Standard Specification for Concrete 6.3.7 Design Shear Transmission Strength”. Using / 2, equations (26) and (27) are transformed into the following equations (48) and (49).
−σ nd1 = −0.0085δ N / mm 2 (48)
−σ nd2 = −0.0090δ N / mm 2 (49)
By treating these equations as −σ nd in equation (36) and substituting the specific dimensions used in equations (37) to (44), the shear transmission force Vcwd is
Vcwd1 = τ c・ Ac1 / γ b
= 0.45 × (23.1) 1/2 × (0.0085δ) 1/2 × 4048 × 10 6 /1.3≒620900×δ 1/2 kN ・ ・ (50)
Vcwd2 = τ c・ Ac2 / γ b
= 0.45 × (30.8) 1/2 × (0.0090δ) 1/2 × 3761 × 10 6 /1.3≒685400×δ 1/2 kN ・ ・ (51)
By
Vcwd = Vcwd1 + Vcwd2
= 620900 × δ 1/2 + 685400 × δ 1/2 = 1306000 × δ 1/2 kN ・ ・ (52)
Is calculated.

そして、先に求めたLNG地下タンク10の貯槽本体30の側壁32から連壁20に最もせん断力が大きく作用するときの設計せん断力Wd(439.13×103kN)に基づき、せん断伝達のために必要な噛み合わせ量を、次式(53)のようにして求める。
1306000×δ1/2 ≧439130
δ≧0.113mm ・・(53)
なお、側壁32と連壁20の間の離れ量は、上述したように、その接合面の下方に移行するほど大きくなり、2mm〜14mmとなる。したがって、構築時に形成する側壁32と連壁20との接合面の高低差は、最大14mmの離れ量が生じることを想定して次式(54)のように算定される。
δ0=0.113+14.0 ≒15.0 (mm) ・・(54)
以上、本実施形態に係るLNG地下タンク10のせん断伝達構造1によれば、連壁構築工程S1と、貯槽本体コンクリート打設工程S2と、コンクリート養生工程S3により、貯槽本体30に作用する浮き上がり荷重等の鉛直方向の荷重を連壁20に伝達可能な構造を簡単に構築することができる。
Then, based on the design shear force W d (439.13 × 10 3 kN) obtained when the shear force is the largest acting on the continuous wall 20 from the side wall 32 of the storage body 30 of the LNG underground tank 10 previously obtained, The amount of meshing required for the above is obtained as in the following equation (53).
1306000 × δ 1/2 ≧ 439 130
δ ≧ 0.113mm ・ ・ (53)
As described above, the distance between the side wall 32 and the continuous wall 20 increases as it moves below the joint surface, and is 2 mm to 14 mm. Therefore, the height difference of the joint surface between the side wall 32 and the continuous wall 20 formed at the time of construction is calculated as shown in the following equation (54) on the assumption that a maximum distance of 14 mm is generated.
δ 0 = 0.113 + 14.0 ≒ 15.0 (mm) (54)
As mentioned above, according to the shear transmission structure 1 of the LNG underground tank 10 which concerns on this embodiment, the floating load which acts on the storage tank main body 30 by continuous wall construction process S1, storage tank main body concrete placement process S2, and concrete curing process S3. It is possible to easily construct a structure capable of transmitting a vertical load such as the like to the continuous wall 20.

また、連壁20と貯槽本体30の側壁32との両接合面が、互いに噛み合うような凹凸形状を有していることにより、例えば、貯槽本体30に浮き上がり荷重等が作用し、側壁32が連壁20に対してせん断方向に移動(つまり鉛直方向に相対移動)する場合、両接合面同士が互いに離間するように移動することになる。そして、両接合面が離間すると、側壁32、連壁20及び地盤40に荷重が作用することになり、これら荷重に対する離間を離間前の状態に戻そうとする反力が生じ、この反力に応じて接合面間の摩擦力(=せん断伝達耐力)も増加するので、両接合面間でせん断力を確実に伝達することができる。   In addition, since both joint surfaces of the continuous wall 20 and the side wall 32 of the storage tank body 30 have an uneven shape that meshes with each other, for example, a floating load acts on the storage tank body 30 and the side wall 32 is connected. When moving in the shearing direction with respect to the wall 20 (that is, relative movement in the vertical direction), both joint surfaces move so as to be separated from each other. And if both joint surfaces leave | separate, a load will act on the side wall 32, the continuous wall 20, and the ground 40, The reaction force which tries to return separation with respect to these loads to the state before separation arises, and this reaction force Accordingly, the frictional force between the joint surfaces (= shear transmission resistance) also increases, so that the shear force can be reliably transmitted between the joint surfaces.

また、両接合面の凹凸形状は、両接合面同士が鉛直方向に相対移動して両接合面の一方の凸部の頂部が他方の凸部の頂部に乗り上げることにより、接合面が離間することに応じて側壁32、連壁20、及び地盤40に夫々作用する荷重と、両接合面間の摩擦係数μとに基づいて求められた摩擦力(=せん断伝達耐力Vcwd)が、側壁32に作用する鉛直方向の荷重Sよりも大きくなるように形成されていることにより、側壁32に作用する鉛直方向の荷重に対して側壁32と連壁20との接合面が滑ることなく、かかる荷重を貯槽本体30から連壁20に確実に伝達させる凹凸形状を、施工上効率良く形成することができる。   In addition, the concave and convex shapes of both joint surfaces are such that the joint surfaces are separated by the relative movement of both joint surfaces in the vertical direction and the top of one convex portion of both joint surfaces riding on the top of the other convex portion. The frictional force (= shear transmission resistance Vcwd) determined based on the load acting on the side wall 32, the connecting wall 20 and the ground 40 in accordance with the friction coefficient μ between the joint surfaces acts on the side wall 32. By being formed so as to be larger than the vertical load S to be applied, the load is stored in the storage tank without slipping of the joint surface between the side wall 32 and the connecting wall 20 with respect to the vertical load acting on the side wall 32. An uneven shape that is reliably transmitted from the main body 30 to the continuous wall 20 can be efficiently formed in terms of construction.

なお、本実施形態の貯槽本体30と連壁20との両接合面は波型に形成されるとしたが、これに限らず、ノコギリ状、又は略台形状であってもよい。すなわち、両接合面の凹凸形状が、側壁32が連壁20に対してせん断方向に微小移動するときに、接合面間が離間するような形状であればよい。   In addition, although both the joint surfaces of the storage tank main body 30 and the continuous wall 20 of this embodiment were formed in the waveform, it is not restricted to this, A sawtooth shape or a substantially trapezoid shape may be sufficient. That is, the uneven shape of both joint surfaces may be a shape that allows the joint surfaces to be spaced apart when the side wall 32 moves minutely in the shearing direction with respect to the continuous wall 20.

本実施形態に係るLNG地下タンクの縦断面図である。It is a longitudinal cross-sectional view of the LNG underground tank which concerns on this embodiment. 図1の連壁と貯槽本体の側壁との接合面の拡大断面図である。It is an expanded sectional view of the joint surface of the continuous wall of FIG. 1 and the side wall of a storage tank main body. LNG地下タンク10の構築手順を示す工程図である。FIG. 4 is a process diagram showing a construction procedure of the LNG underground tank 10. LNG地下タンク10に最大の浮き上がり力が作用するときに、側壁32と連壁20との間に作用する鉛直方向の荷重を求めるための説明図である。FIG. 5 is an explanatory diagram for obtaining a vertical load acting between the side wall 32 and the continuous wall 20 when the maximum lifting force acts on the LNG underground tank 10. LNG地下タンク10の具体的な寸法を示す断面図である。FIG. 3 is a cross-sectional view showing specific dimensions of the LNG underground tank 10. LNG地下タンク10の側壁及び連壁を2重円環として表したLNG地下タンクモデルの横断面図である。It is a cross-sectional view of the LNG underground tank model in which the side wall and the continuous wall of the LNG underground tank 10 are represented as a double ring. LNGからの冷熱による側壁及び連壁の変位を示すグラフである。It is a graph which shows the displacement of the side wall by the cold from LNG, and a continuous wall. 水圧及び揚圧力による側壁の変位を示すグラフである。It is a graph which shows the displacement of the side wall by water pressure and lifting pressure. 水圧による連壁の変位を示すグラフである。It is a graph which shows the displacement of the continuous wall by water pressure. 側壁及び連壁について、これら温度、水圧及び揚圧力による合計変位量を示したグラフである。It is the graph which showed the total displacement amount by these temperature, water pressure, and lifting pressure about a side wall and a continuous wall. 図10の側壁と連壁との変位差を示すグラフである。It is a graph which shows the displacement difference of the side wall and continuous wall of FIG.

符号の説明Explanation of symbols

10 LNG地下タンク
20 地中連続壁(連壁)
30 貯槽本体
32 側壁
33 一般部
34 側壁下端ハンチ部
35 目荒らし
36 底版
37 付帯部材
38 コンクリート
40 地盤
S1 連壁構築工程
S2 貯槽本体コンクリート打設工程
S3 コンクリート養生工程
10 LNG underground tank 20 Underground continuous wall (continuous wall)
DESCRIPTION OF SYMBOLS 30 Storage tank main body 32 Side wall 33 General part 34 Side wall lower end haunch part 35 Roughening 36 Bottom plate 37 Attached member 38 Concrete 40 Ground S1 Continuous wall construction process S2 Storage tank body concrete placing process S3 Concrete curing process

Claims (5)

地中壁と、前記地中壁と接合して構築されるコンクリート構造物との間に作用するせん断力を伝達するせん断伝達構造であって、
前記コンクリート構造物と前記地中壁との両接合面が、互いに噛み合うような波状、ノコギリ状、又は略台形状の凹凸形状を有し、
前記コンクリート構造物が前記地中壁に対して鉛直方向に相対移動すると、前記両接合面同士が鉛直方向に相対移動して前記両接合面の一方の凸部の頂部が他方の凸部の頂部に乗り上げることにより、前記両接合面間が離間し、前記接合面が離間することに応じて前記コンクリート構造物及び前記地中壁に作用する荷重と、前記両接合面間の摩擦係数とに基づいて求められた摩擦力が、前記コンクリート構造物に作用する鉛直方向の荷重よりも大きくなることを特徴とするせん断伝達構造。
A shear transmission structure for transmitting a shear force acting between the underground wall and a concrete structure constructed by joining the underground wall,
The joining surfaces of the concrete structure and the underground wall is wavy to engage each other, sawtooth, or have a concave-convex shape of the substantially trapezoidal shape,
When the concrete structure moves relative to the underground wall in the vertical direction, the joint surfaces move relative to each other in the vertical direction, and the top of one convex portion of the joint surfaces is the top of the other convex portion. On the basis of the load acting on the concrete structure and the underground wall according to the separation of the joint surface and the coefficient of friction between the joint surfaces. frictional force obtained Te is, shear transfer structures characterized by Rukoto Do greater than the vertical direction of the load acting on the concrete structure.
表面に凹凸形状を有する地中壁と接合して構築されるコンクリート構造物であって、
前記地中壁と接合する接合面に、前記地中壁の凹凸形状と噛み合うような波状、ノコギリ状、又は略台形状の凹凸形状を有し、
前記コンクリート構造物が前記地中壁に対して鉛直方向に相対移動すると、前記両接合面同士が鉛直方向に相対移動して前記両接合面の一方の凸部の頂部が他方の凸部の頂部に乗り上げることにより、前記両接合面間が離間し、前記接合面が離間することに応じて前記コンクリート構造物及び前記地中壁に作用する荷重と、前記両接合面間の摩擦係数とに基づいて求められた摩擦力が、前記コンクリート構造物に作用する鉛直方向の荷重よりも大きくなることを特徴とするコンクリート構造物。
A concrete structure constructed by joining with an underground wall having an uneven shape on the surface,
Wherein the joint surface to be bonded to the ground wall, the underground wall of irregular shape and meshes such wavy, serrated, or have a concave-convex shape of the substantially trapezoidal shape,
When the concrete structure moves relative to the underground wall in the vertical direction, the joint surfaces move relative to each other in the vertical direction, and the top of one convex portion of the joint surfaces is the top of the other convex portion. On the basis of the load acting on the concrete structure and the underground wall according to the separation of the joint surface and the coefficient of friction between the joint surfaces. frictional force obtained Te is, concrete structure, characterized in Rukoto Do greater than the vertical direction of the load acting on the concrete structure.
LNG地下タンクに適用されたことを特徴とする請求項2に記載のコンクリート構造物。   The concrete structure according to claim 2, which is applied to an LNG underground tank. 地中壁と、前記地中壁と接合して構築されるコンクリート構造物との間に作用するせん断力を伝達するせん断伝達構造の構築方法であって、
その表面に波状、ノコギリ状、又は略台形状の凹凸形状を有し、前記コンクリート構造物が前記地中壁に対して鉛直方向に相対移動すると、前記両接合面同士が鉛直方向に相対移動して前記両接合面の一方の凸部の頂部が他方の凸部の頂部に乗り上げることにより、前記両接合面間が離間し、前記接合面が離間することに応じて前記コンクリート構造物及び前記地中壁に作用する荷重と、前記両接合面間の摩擦係数とに基づいて求められた摩擦力が、前記コンクリート構造物に作用する鉛直方向の荷重よりも大きくなる地中壁を構築し、
前記地中壁の凹凸形状の表面に接触するように、コンクリートを打設し、
前記打設したコンクリートを養生することを特徴とする地中壁とコンクリート構造物とのせん断伝達構造の構築方法。
A construction method of a shear transmission structure for transmitting a shearing force acting between an underground wall and a concrete structure constructed by joining the underground wall,
Corrugated on its surface, sawtooth, or have a concave-convex shape of the substantially trapezoidal, when the concrete structure is relatively moved in a vertical direction with respect to the diaphragm wall, wherein the joining faces are relatively moved in the vertical direction Then, when the top of one convex portion of both joint surfaces rides on the top of the other convex portion, the two joint surfaces are separated from each other, and the concrete structure and the ground according to the separation of the joint surfaces. and the load acting on the middle wall, the friction coefficient and frictional force determined on the basis of the between both joint surfaces, to construct a diaphragm wall ing larger than the load in the vertical direction acting on the concrete structure,
Place concrete so that it touches the uneven surface of the underground wall,
A method for constructing a shear transmission structure between an underground wall and a concrete structure, wherein the placed concrete is cured.
請求項1に記載のせん断伝達構造の設計方法であって、
前記両接合面の摩擦力を、前記両接合面同士が鉛直方向に相対移動して前記両接合面の一方の凸部の頂部が他方の凸部の頂部に乗り上げることにより、前記接合面が離間することに応じて前記コンクリート構造物及び前記地中壁に作用する荷重と、前記両接合面間の摩擦係数とに基づいて求め、
前記両接合面の凹凸形状を、前記摩擦力が、前記コンクリート構造物に作用する鉛直方向の荷重よりも大きくなるように設定することを特徴とするせん断伝達構造の設計方法。
A method for designing a shear transmission structure according to claim 1 ,
The joint surfaces are separated by causing the frictional forces of the joint surfaces to move relative to each other in the vertical direction so that the top of one convex portion of the joint surfaces rides on the top of the other convex portion. Obtained based on the load acting on the concrete structure and the underground wall according to the friction coefficient between the joint surfaces,
A method for designing a shear transmission structure, wherein the concave and convex shapes of the joint surfaces are set such that the frictional force is greater than a vertical load acting on the concrete structure.
JP2007341044A 2007-12-28 2007-12-28 Shear transmission structure, concrete structure, construction method of shear transmission structure, and design method of shear transmission structure Expired - Fee Related JP4900236B2 (en)

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KR101548250B1 (en) 2014-07-25 2015-08-28 김진수 Underground push box pipe and underground structure construction method therewith
JP6645098B2 (en) * 2015-09-30 2020-02-12 株式会社大林組 Removal method of existing pile

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CN102953354A (en) * 2012-10-19 2013-03-06 中国核电工程有限公司 Anti-shearing construction method of underground reinforced concrete trench with water pressure at turning part

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