JP2018172961A - Lattice body - Google Patents

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JP2018172961A
JP2018172961A JP2018059300A JP2018059300A JP2018172961A JP 2018172961 A JP2018172961 A JP 2018172961A JP 2018059300 A JP2018059300 A JP 2018059300A JP 2018059300 A JP2018059300 A JP 2018059300A JP 2018172961 A JP2018172961 A JP 2018172961A
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lattice
wind
twisted
cross
section
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史一 見浦
Fumikazu Miura
史一 見浦
山森 雄介
Yusuke Yamamori
雄介 山森
一元 沢目
Kazumoto Sawame
一元 沢目
弘士 川崎
Hiroshi Kawasaki
弘士 川崎
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Sankyo Tateyama Inc
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Sankyo Tateyama Inc
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Abstract

PROBLEM TO BE SOLVED: To provide a lattice body capable of inhibiting a vibration and noise due to wind.SOLUTION: A plurality of lattice members 1,1,... are provided with interval and a lattice member 1 has an identical cross section from one end 1a to an intermediate position 1b and a range Y from the intermediate position 1b to the other end 1c is twisted and an orientation of the cross section is altering due to a twist gradually.SELECTED DRAWING: Figure 1

Description

本発明は、手摺等に用いられる格子体に関する。   The present invention relates to a lattice used for a handrail or the like.

橋の欄干やベランダの手摺などには、細い棒状の格子材を間隔をおいて取付けた格子体が用いられる。このような格子体は、強風時に振動・騒音が発生する問題がある。振動・騒音が発生するメカニズムを説明すると、図10に示すように、格子材90に風が当たると風下側に左右交互に規則正しい渦91が放出され、渦91が放出される瞬間に格子材90の近傍の圧力が低くなるために格子材90は渦91が放出される側に変位する。渦91が左右交互に周期的に放出されることにより、格子材90も左右に(風の流れと垂直方向に)周期的に変位し、振動となる。断面が一様な格子材90では、どの位置からも同じ状態で渦91が放出されるため、格子材90の長手方向全長に渦91がそろい、加振力が全長にわたって同じ方向に働き、振幅が大きくなる。また、断面が一様な格子材90を両端で支持する場合、支持点間の丁度、中間点の振幅が最大となる一次モード(図11参照)で最も振動し易くなる。   For the railing of the bridge and the railing of the veranda, a lattice body in which thin rod-shaped lattice members are attached at intervals is used. Such a lattice body has a problem that vibration and noise are generated in a strong wind. The mechanism for generating vibration and noise will be described. As shown in FIG. 10, when the grid material 90 is hit by the wind, regular vortices 91 are discharged alternately to the leeward side, and the grid material 90 is instantaneously released. Since the pressure in the vicinity of is reduced, the lattice material 90 is displaced to the side from which the vortex 91 is released. By periodically discharging the vortex 91 alternately left and right, the lattice material 90 is also periodically displaced to the left and right (in the direction perpendicular to the wind flow), resulting in vibration. In the grid member 90 having a uniform cross section, the vortex 91 is released from any position in the same state. Therefore, the vortex 91 is aligned with the entire length in the longitudinal direction of the grid material 90, and the excitation force acts in the same direction over the entire length. Becomes larger. Further, when the lattice member 90 having a uniform cross section is supported at both ends, it is most likely to vibrate in the primary mode (see FIG. 11) in which the amplitude between the support points is just the maximum.

本発明は以上に述べた実情に鑑み、風による振動・騒音の発生を抑えられる格子体の提供を目的とする。   The present invention has been made in view of the above-described circumstances, and an object of the present invention is to provide a lattice body that can suppress generation of vibration and noise due to wind.

上記の課題を達成するために請求項1記載の発明による格子体は、複数の格子材を間隔をおいて備え、格子材は、一端から中間位置までは断面が同一であり、中間位置から他端までの範囲がねじってあり、ねじりにより断面の向きが徐々に変化していることを特徴とする。   In order to achieve the above object, a lattice body according to the first aspect of the present invention comprises a plurality of lattice materials at intervals, and the lattice material has the same cross section from one end to an intermediate position, and the other from the intermediate position. The range to the end is twisted, and the direction of the cross section is gradually changed by twisting.

請求項1記載の発明による格子体は、格子材が一端から中間位置までは断面が同一で、中間位置から他端までの範囲がねじってあり、ねじりにより断面の向きが徐々に変化していることで、風による振動・騒音の発生を抑えられる。これは、格子材がねじってあることで、風を受けたときに格子材の長手方向で渦が放出される位置が徐々に異なり、格子材の長手方向に渦がそろわなくなることで、格子材に働く加振力も一様ではなくなり、位置によって左または右の不均一な力が格子材に同時に働き、左右の力が互いに打ち消しあうことや、ねじることで断面の向きに応じて風と垂直方向の剛性が変化すること、ねじってある部分が片側(他端側)に寄っており、ねじってある部分はねじってない部分よりも剛性が高まるので、格子材の剛性が支持点間の中間点に対して非対称となるため、一次モードの振幅が小さくなることによると考えられる。   In the grid body according to the first aspect, the cross section of the grid material is the same from one end to the intermediate position, the range from the intermediate position to the other end is twisted, and the direction of the cross section gradually changes due to torsion. Therefore, the generation of vibration and noise due to wind can be suppressed. This is because the lattice material is twisted, the position where vortices are released gradually in the longitudinal direction of the lattice material when receiving wind, and the vortices are not aligned in the longitudinal direction of the lattice material. Depending on the position, the left or right non-uniform force acts on the lattice material at the same time, and the left and right forces cancel each other out or twist to twist the wind in a direction perpendicular to the wind. The rigidity of the grid material is intermediate between the support points because the rigidity of the lattice material changes, the twisted part is closer to one side (the other end), and the twisted part is more rigid than the untwisted part. This is considered to be due to a decrease in the amplitude of the primary mode.

本発明の格子体の一実施形態を示す正面図である。It is a front view showing one embodiment of a lattice object of the present invention. (a)は図1のA−A断面図、(b)は図1のB−B断面図、(c)は図1のC−C断面図、(d)は図1のD−D断面図、(e)は図1のE−E断面図である。1A is a cross-sectional view taken along line AA in FIG. 1, FIG. 1B is a cross-sectional view taken along line BB in FIG. 1, FIG. 1C is a cross-sectional view taken along line CC in FIG. FIG. 2E is a cross-sectional view taken along line EE in FIG. 試験装置の概略図である。It is the schematic of a test apparatus. 実施例1の格子体に風を当てたときの風速と振動加速度レベルの関係を示すグラフである。It is a graph which shows the relationship between a wind speed when a wind is applied to the lattice body of Example 1, and a vibration acceleration level. 実施例2の格子体に風を当てたときの風速と振動加速度レベルの関係を示すグラフである。It is a graph which shows the relationship between a wind speed when a wind is applied to the lattice body of Example 2, and a vibration acceleration level. 実施例3の格子体に風を当てたときの風速と振動加速度レベルの関係を示すグラフである。It is a graph which shows the relationship between a wind speed when a wind is applied to the lattice body of Example 3, and a vibration acceleration level. 実施例4の格子体に風を当てたときの風速と振動加速度レベルの関係を示すグラフである。It is a graph which shows the relationship between a wind speed when a wind is applied to the lattice body of Example 4, and a vibration acceleration level. 比較例1の格子体(格子材がねじってないもの)に風を当てたときの風速と振動加速度レベルの関係を示すグラフである。It is a graph which shows the relationship between the wind speed and vibration acceleration level when a wind is applied to the lattice body (what the lattice material is not twisted) of the comparative example 1. 比較例2の格子体(格子材が全長ねじってあるもの)に風を当てたときの風速と振動加速度レベルの関係を示すグラフである。It is a graph which shows the relationship between the wind speed and the vibration acceleration level when a wind is applied to the grid | lattice body (what the grid | lattice material twisted full length) of the comparative example 2. FIG. 従来の格子材に風が当たったときに振動が発生する様子を示す図である。It is a figure which shows a mode that a vibration generate | occur | produces when a wind hits the conventional lattice material. 格子材の振動モードを模式的に示す図である。It is a figure which shows typically the vibration mode of a lattice material.

以下、本発明の実施の形態を図面に基づいて説明する。図1,2は、本発明の格子体2の一実施形態を示している。本格子体2は、ベランダの手摺に用いられるものであって、一対の柱3,3と、柱3,3の上端に架設した笠木4と、柱3,3の下部に架設した下弦材5と、笠木4と下弦材5との間に左右方向に間隔をおいて取付けた複数の格子材1,1,…とからなる。   Hereinafter, embodiments of the present invention will be described with reference to the drawings. 1 and 2 show an embodiment of the lattice body 2 of the present invention. The grid 2 is used for a handrail of a veranda, and includes a pair of pillars 3 and 3, a headboard 4 erected at the upper ends of the pillars 3 and 3, and a lower chord member 5 erected at the lower part of the pillars 3 and 3. And a plurality of lattice members 1, 1,... Mounted between the headboard 4 and the lower chord member 5 at intervals in the left-right direction.

格子材1は、図2に示すように、矩形(正方形)断面の中空のアルミ押出形材で形成されている。格子材1は、図1に示すように、下端1aから中間位置1bまでの範囲Xは、図2(e)に示すように断面が同一であり、中間位置1bから上端1cまでの範囲Yが断面の中心を軸としてねじってあり、ねじることで図2(a)〜(d)に示すように、断面の向きが徐々に変化している。   As shown in FIG. 2, the lattice material 1 is formed of a hollow aluminum extruded shape having a rectangular (square) cross section. As shown in FIG. 1, the lattice material 1 has the same cross section as the range X from the lower end 1a to the intermediate position 1b as shown in FIG. 2E, and the range Y from the intermediate position 1b to the upper end 1c. The center of the cross section is twisted about the axis, and the direction of the cross section is gradually changed by twisting as shown in FIGS.

下記表1に示すように、ねじり角度とねじり割合(格子材の全長のうちのねじってある範囲の割合)を異ならせた格子体2を作成し、図3(a)に示すように、各格子体2に風速を2〜20m/sの範囲で2m/s刻みで変化させた風を、風向き(図中のα)0〜90°の範囲で15°刻みで当てたときに騒音が発生するかどうか試験した。試験体No.1〜15は、ねじり割合を75%とし、ねじり角度を15°から165°の間で変化させた(15°〜75°までと105°〜165°までは15°刻み、75°〜105°までは5°刻みで変化させた。)。試験体No.16〜24は、ねじり角度を90°とし、ねじり割合を55%から95%まで5%刻みで変化させた。
試験の結果、ねじり角度を変化させた試験体No.1〜15の結果より、ねじり角度を85°又は90°とした場合に騒音が発生しなくなることが分かった。また、ねじり割合を変化させた試験体16〜24の結果より、ねじり割合が65%〜95%で騒音が発生しなくなることが分かった。
As shown in Table 1 below, the lattice body 2 with different twist angles and twist ratios (the ratio of the twisted range of the total length of the lattice material) is created, and as shown in FIG. Noise is generated when the wind with the wind speed changed in steps of 2 m / s in the range of 2 to 20 m / s is applied to the grid 2 in the direction of wind (α in the figure) in the range of 0 ° to 90 ° in steps of 15 °. Tested to see if. Specimen No. Nos. 1 to 15 have a twist ratio of 75%, and the twist angle was changed between 15 ° and 165 ° (in increments of 15 ° from 15 ° to 75 ° and from 105 ° to 165 °, 75 ° to 105 ° Until then, it was changed in 5 ° increments.) Specimen No. In Nos. 16 to 24, the twist angle was 90 °, and the twist ratio was changed from 55% to 95% in increments of 5%.
As a result of the test, the test specimen No. whose twist angle was changed was changed. From the results of 1 to 15, it was found that noise was not generated when the twist angle was 85 ° or 90 °. Further, from the results of the test bodies 16 to 24 in which the twist ratio was changed, it was found that noise was not generated when the twist ratio was 65% to 95%.

次に、ねじり角度90°でねじり割合75%のもの(実施例1)、ねじり角度90°でねじり割合65%のもの(実施例2)、ねじり角度90°でねじり割合が95%のもの(実施例3)、ねじり角度85°でねじり割合が75%のもの(実施例4)について、図3(a)に示すように、風向き(図中のα)を0°,30°,60°と変化させ、風速を2〜20m/sの間で変化させたときの、図3(b)に示すように、格子材1の中間位置に取付けた加速度ピックアップ6の振動加速度レベルを測定した。比較のために、格子材1をねじってないもの(比較例1)、格子材1を全長ねじったもの(比較例2)についても測定した(比較例2については、風向き0°のみ)。測定結果を図4〜9に示す。   Next, a twist angle of 90 ° and a twist rate of 75% (Example 1), a twist angle of 90 ° and a twist rate of 65% (Example 2), a twist angle of 90 ° and a twist rate of 95% (Example 2) Example 3) For a sample having a twist angle of 85 ° and a twist ratio of 75% (Example 4), the wind direction (α in the figure) is 0 °, 30 °, 60 ° as shown in FIG. As shown in FIG. 3B, the vibration acceleration level of the acceleration pickup 6 attached to the intermediate position of the lattice material 1 was measured when the wind speed was changed between 2 and 20 m / s. For comparison, the lattice material 1 that was not twisted (Comparative Example 1) and the lattice material 1 that was twisted full length (Comparative Example 2) were also measured (in Comparative Example 2, only the wind direction was 0 °). The measurement results are shown in FIGS.

図8に示すように、格子材1をねじってない比較例1では、風向き0°にて風速10m/sを越えると振動加速度レベルが130db以上となり、風速16m/s以上になると振動加速度レベルが150db以上となったのに対し、格子材1を部分的にねじってある実施例1〜4では、図4〜7に示すように、測定した何れの風向き、風速においても、振動加速度レベルが130db以上になることがなかった。
また、図9に示すように、格子材1を全長ねじってある比較例2では、風向き0°で風速10m/sのときに振動加速度レベルが130db以上となったのに対し、部分的にねじってある実施例1〜4では、測定した何れの風向き、風速においても、振動加速度レベルが130db以上になることがなかった。
部分ねじり(実施例1〜4)と、全長ねじり(比較例2)と、ねじり無し(比較例1)とで、風向き0°のときの振動加速度レベルの大きさを比較すると、ねじり無し>全長ねじり>部分ねじりの順に振動加速度レベルが小さくなった。
なお、比較例についての試験より、振動加速度レベルと官能評価(人が耳で聞いて行う評価)との間には、おおむね下記表2に示すような関係があることがわかっており、振動加速度レベルが130db未満であると、騒音は感じられないか、聴こえても気にならないレベルである。
As shown in FIG. 8, in Comparative Example 1 in which the lattice material 1 is not twisted, the vibration acceleration level becomes 130 db or more when the wind speed exceeds 10 m / s at a wind direction of 0 °, and the vibration acceleration level becomes higher when the wind speed exceeds 16 m / s. In the first to fourth embodiments in which the lattice material 1 is partially twisted, the vibration acceleration level is 130 db in any measured wind direction and speed as shown in FIGS. It was never over.
Further, as shown in FIG. 9, in Comparative Example 2 in which the lattice material 1 is twisted over its entire length, the vibration acceleration level was 130 db or more when the wind direction was 0 ° and the wind speed was 10 m / s, whereas the twist was partially twisted. In Examples 1 to 4, the vibration acceleration level did not become 130 db or higher in any measured wind direction and wind speed.
Comparing the magnitude of vibration acceleration level when the wind direction is 0 ° with partial torsion (Examples 1 to 4), full-length torsion (Comparative Example 2), and no torsion (Comparative Example 1), no torsion> full length The vibration acceleration level decreased in the order of torsion> partial torsion.
In addition, it is known from the test for the comparative example that there is a relationship as shown in Table 2 below between the vibration acceleration level and sensory evaluation (evaluation performed by human hearing). When the level is less than 130 db, noise is not felt or is a level that does not matter even if it is heard.

以上に述べたように本格子体2は、格子材1が一端1aから中間位置1bまでは断面が同一で、中間位置1bから他端1cまでの範囲Yがねじってあり、ねじりにより断面の向きが徐々に変化していることで、風による振動・騒音の発生を抑えられる。これは、格子材1がねじってあることで、風を受けたときに格子材1の長手方向で渦が放出される位置が徐々に異なり、格子材1の長手方向に渦がそろわなくなることで、格子材1に働く加振力も一様ではなくなり、位置によって左または右の不均一な力が格子材に同時に働き、左右の力が互いに打ち消しあうことや、ねじることで断面の向きに応じて風と垂直方向の剛性が変化すること、全長ねじってあるものよりも振動しにくくなるのは、ねじってある部分が片側(他端側)に寄っており、ねじってある部分はねじってない部分よりも剛性が高まるので、格子材の剛性が支持点間の中間点に対して非対称となるために、一次モードの振幅が小さくなるため、風による音や振動を抑えることができると考えられる。   As described above, the grid body 2 has the same cross section from one end 1a to the intermediate position 1b of the grid material 1, and the range Y from the intermediate position 1b to the other end 1c is twisted. Is gradually changing, it is possible to suppress the generation of vibration and noise caused by wind. This is because the lattice material 1 is twisted so that the position where vortices are released in the longitudinal direction of the lattice material 1 gradually changes when the wind is received, and the vortices are not aligned in the longitudinal direction of the lattice material 1. The excitation force acting on the grid material 1 is also not uniform, and depending on the position, the left or right non-uniform force acts on the grid material at the same time, and the left and right forces cancel each other or twist according to the direction of the cross section. The change in rigidity in the direction perpendicular to the wind, and the fact that it is less likely to vibrate than what is twisted over the entire length, the twisted part is closer to one side (the other end), and the twisted part is not twisted Since the rigidity of the lattice material becomes asymmetric with respect to the intermediate point between the support points, the amplitude of the primary mode is reduced, so that it is considered that sound and vibration due to wind can be suppressed.

格子材1が略正方形断面の場合、ねじり角度が略85°〜90°で、ねじってある範囲の割合が65%〜95%であることが好ましい。これにより、上記の振動・騒音を抑える効果が確実に発揮される。略正方形断面には、例えば正方形の角部をR状に面取りしたものなどが含まれる。   When the lattice material 1 has a substantially square cross section, the twist angle is preferably approximately 85 ° to 90 °, and the ratio of the twisted range is preferably 65% to 95%. Thereby, the effect which suppresses said vibration and noise is exhibited reliably. The substantially square cross section includes, for example, a square corner chamfered in an R shape.

本発明は以上に述べた実施形態に限定されない。ねじり角度は、略85°〜90°以外の角度であっても、ねじってないものよりは振動・騒音を軽減できる。ねじってある範囲は、格子材の長手方向の中心に対して非対称であればよく、下端側がねじってあってもよい。格子材は、正方形断面に限らず、長方形断面等であってもよく、また、中空材に限らず、中実材であってもよい。本発明は、手摺に限らず、格子材を間隔をおいて有する格子体に広く適用できる。   The present invention is not limited to the embodiments described above. Even if the torsion angle is an angle other than approximately 85 ° to 90 °, vibration and noise can be reduced as compared with those not twisted. The twisted range may be asymmetric with respect to the longitudinal center of the lattice material, and the lower end side may be twisted. The lattice material is not limited to a square cross section, but may be a rectangular cross section or the like, and is not limited to a hollow material, and may be a solid material. The present invention is not limited to handrails and can be widely applied to lattice bodies having lattice materials at intervals.

1 格子材
2 格子体
1 Lattice material 2 Lattice body

Claims (1)

複数の格子材を間隔をおいて備え、格子材は、一端から中間位置までは断面が同一であり、中間位置から他端までの範囲がねじってあり、ねじりにより断面の向きが徐々に変化していることを特徴とする格子体。   A plurality of lattice materials are provided at intervals, and the lattice material has the same cross section from one end to the intermediate position, and the range from the intermediate position to the other end is twisted, and the direction of the cross section gradually changes due to torsion. A lattice body characterized by being.
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