In solving a problem concerning the equilibrium of a rigid body, it is essential to consider all of the forces acting on the body; it is equally important to exclude any force which is not directly applied to the body. Omitting a force or adding an extraneous one would destroy the conditions of equilibrium. Therefore, the first step in the solution of the problem should be to draw a free-body diagram of the rigid body under consideration. Free-body diagrams have already been used on many occasions in Chap. 2. However, in view of their importance to the solution of equilibrium problems, we summarize here the various steps which must be followed in drawing a free-body diagram. 1. A clear decision should be made regarding the choice of the free body to be used. This body is then detached from the ground and is separated from all other bodies. The contour of the body thus isolated is sketched. 2. All external forces should be indicated on the free-body diagram. These forces represent the actions exerted on the free body by the ground and by the bodies which have been detached; they should be applied at the various points where the free body was supported by the ground or was connected to the other bodies. The weight of the free body should also be included among the external forces, since it represents the attraction exerted by the earth on the various particles forming the free body. As will be seen in Chap. 5, the weight should be applied at the center of gravity of the body. When the free body is made of several parts, the forces the various parts exert on each other should not be included among the external forces. These forces are internal forces as far as the free body is concerned. 3. The magnitudes and directions of the known external forces should be clearly marked on the free-body diagram. When indicating the directions of these forces, it must be remembered that the forces shown on the free-body diagram must be those which are exerted on, and not by, the free body. Known external forces generally include the weight of the free body and forces applied for a given purpose. 4. Unknown external forces usually consist of the reactions, through which the ground and other bodies oppose a possible motion of the free body. The reactions constrain the free body to remain in the same position, and, for that reason, are sometimes called constraining forces. Reactions are exerted at the points where the free body is supported by or connected to other bodies and should be clearly indicated. Reactions are discussed in detail in Secs. 4.3 and 4.8. 5. The free-body diagram should also include dimensions, since these may be needed in the computation of moments of forces. Any other detail, however, should
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