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A rigid body subjected to three forces acting at three points is known as a three-force member. These forces must have concurrent lines of action, except for parallel forces, where the lines of action are parallel.

For example, consider a dumpster connected to a pin support at point A and a pin attached to a hydraulic cylinder at point B.

Figure 1

In this case, the hydraulic cylinder is a two-force member in equilibrium. The force due to the weight acts through the center of gravity and the reaction forces due to the support act at point A.

To solve for unknown forces FA and FCB, the first step involves creating a free-body diagram of the entire system, including all the forces acting on the dumpster.

Figure 2

Next, the force and moment equilibrium equations can be used to determine the values of the unknown forces.

Equation 1

Equation 2

Equation 3

The moment equilibrium condition at point A gives the value of the force FCB as 24.08 kN. Meanwhile, the force equilibrium condition along the vertical direction determines the vertical reaction force FAy as 9.74 kN. Similarly, applying the force equilibrium condition along the horizontal direction yields the horizontal reaction force FAx as 25.74 kN.

タグ
Three force MemberRigid BodyConcurrent ForcesParallel ForcesFree body DiagramForce EquilibriumMoment EquilibriumUnknown ForcesDumpsterPin SupportHydraulic CylinderReaction ForcesCenter Of Gravity

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5.6 : Three Force Member

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5.1 : 均衡の条件

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5.2 : サポートの反応

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5.3 : 内力と重心

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5.4 : 平衡方程式の代替セット

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5.5 : 2つのフォースメンバー

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5.7 : 3次元の平衡方程式

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5.8 : 3次元でのサポート反応

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5.9 : 制約と静的な決定性

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