ティーキューブ擁壁の内圧の算定 |
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1.設計内圧の基礎式 |
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内圧はサイロの設計に用いられるJanssen(ヤンセン)式により算定する. |
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Janssen式は次のとおりである. |
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鉛直方向の圧力 |
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Pv= |
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水平方向の圧力 |
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ph= |
k・pv |
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壁面摩擦力 |
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pf= |
μ・pv |
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ここで |
μ; |
壁面と内容物との間の摩擦係数 |
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D; |
サイロの内径 |
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γ; |
内容物の単位体積重量 |
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k; |
Rankineの土圧係数 |
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φ; |
内容物の内部摩擦角 |
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x: |
深さ |
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ここで,式中のD/4は,平面形状の面積と周長の比であり,円形以外に拡張すると |
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下式のとおりとなる. |
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鉛直方向の圧力 |
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Pv= |
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ここで |
α; |
換算幅 |
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円形 |
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正方形 |
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正三角形 |
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長方形 |
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短辺をD,長辺をLとし |
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β= |
L/Dとすると |
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帯状の場合 |
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→ |
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2.△ T-1050タイプ |
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辺長 |
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D= |
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0.9 |
m |
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中詰材の単位重量 |
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γ= |
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20 |
kN/m3 |
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中詰材の内部摩擦角 |
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φ= |
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35 |
° |
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中詰材の壁面摩擦角 |
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δ= |
2/3・φ = |
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23 |
° |
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中詰材の壁面との摩擦係数 |
μ= |
tanδ = |
0.431 |
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ランキン土圧係数 |
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k= |
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= |
0.271 |
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高さ |
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x= |
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5.0 |
m |
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換算幅 |
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正方形 |
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= |
0.13 |
m |
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鉛直圧力 |
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22.0 |
kN/m2 |
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水平圧力 |
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ph= |
k・pv= |
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5.96 |
kN/m2 |
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壁面摩擦力 |
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pf= |
μ・kv= |
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9.48 |
kN/m2 |
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3.□ F-1050タイプ |
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辺長 |
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D= |
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0.9 |
m |
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中詰材の単位重量 |
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γ= |
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20 |
kN/m3 |
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中詰材の内部摩擦角 |
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φ= |
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35 |
° |
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中詰材の壁面摩擦角 |
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δ= |
2/3・φ = |
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23 |
° |
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中詰材の壁面との摩擦係数 |
μ= |
tanδ = |
0.431 |
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ランキン土圧係数 |
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k= |
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0.271 |
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高さ |
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x= |
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5.0 |
m |
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換算幅 |
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正方形 |
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α= |
D/4 |
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0.225 |
m |
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鉛直圧力 |
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35.6 |
kN/m2 |
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水平圧力 |
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ph= |
k・pv= |
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9.66 |
kN/m2 |
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壁面摩擦力 |
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pf= |
μ・kv= |
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15.4 |
kN/m2 |
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4.設計内圧 |
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以上より,擁壁の高さは最大でも5m程度と予想されるため,良質材料を使用した場合, |
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設計内圧は10kN/m2を考慮すれば十分である. |
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なお,△ T-1050タイプについては,中詰材料の質を特に指定しない. |
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