In the previous chapter, we focused our discussion on coplanar force systems—that is, forces in two dimensions.
In this chapter, we extend our discussion to forces in three dimensions.
The figure below shows a force F in a three-dimensional system. The components of the force
are proportional to the components of its distance from tail to head. In equation form, it is expressed as:
Problem: Vertical Member with Ball and Socket Support and Three Supporting Cables
A tower is held in place by a ball and socket support at its base and three cables attached at various points along its height. At the mid-height of the tower, a 70-kN lateral force acts along the negative x-axis. Note: The indicated x-axis in the figure is the positive x-axis.
Given:
x=18m
y=22m
The 70-kN horizontal load is applied at the mid-height of the 24-m tower. For the free-body setup used here, translate it into equivalent joint forces shared by the top joint $D$ and the ball-and-socket support at $O$, so the horizontal force used at the top joint is $70/2=35$ kN.
Use cable direction cosines from the top of the tower at $D$ to the ground anchors $C$, $A$, and $B$:
Let $CD$, $AD$, and $BD$ be the cable tensions, and let $OD$ be the vertical reaction at the support. Substituting the actual dimensions into the equilibrium equations:
Due to the direction of the lateral load, cable $BD$ would tend to shorten and go into compression in the trial equilibrium setup. Since a cable can carry tension only and cannot resist compression, set:
$$BD=0$$
Solving with $BD=0$, the equilibrium equations reduce to:
The ball-and-socket support has a vertical component $OD=49.70414$ kN and a horizontal component equal to the translated joint load, $35$ kN. Thus the resultant support reaction is: