To as good an approximation as is required in most engineering work, the system of gravity forces acting upon a body may be considered as a parallel force system. Since gravity forces are always present and must in most problems be taken into account, it will be desirable to simplify the treatment of such parallel force systems by means of a general analysis.
We shall first show that the system of parallel gravity forces acting upon a body has a resultant which passes through one particular point in the body, for any orientation of the body. This center of parallel gravity forces is called the center of gravity of the body, and the entire weight of the body can be considered as concentrated at that point, so far as statical considerations are concerned.
Consider a rigid system which is represented by the three particles of Fig. 1.

The system is acted upon by parallel gravity forces
We now resolve each of the parallel forces into the three rectangular components:
Considering the system of forces parallel to the
We have thus defined a point
Applying this principle to a homogeneous body of total weight