That is, the resultant of the forces being applied on it, Res, or the sum of all the forces applying on it, ΣF, equals zero. So statics is just a particular case of dynamics (ΣF = m.a), where acceleration is zero.
To pose this condition of equilibrium in equations we need to remember it’s about a vector relation. So if the forces applying on a body are all headed towards the same direction, a single equation will suffice (ΣF = 0).
If the forces are pointing to various directions within the same plane, then we’ll need 2 equations:
ΣFx = 0
ΣFy = 0
Obviously, never forget to set a clear reference system, x-y. Basically, the same we did with dynamics.
If the forces don’t act all within the same plane, we’ll need 3 equations, one for each of the directions of the tridimensional Reference System.
Because they are punctual bodies, it’s obvious the forces over the body are concurrent. Next chapter we’ll see when this doesn’t happen (large bodies). On with an example.
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