TYPES OF FORCEApplication of Newton's LawsCP-04 Page 18Rev. 0Figure 9 Frictional ForcesFluid friction develops between layers of fluid moving at different velocities. This type of frictionalforce is used in considering problems involving the flow of fluids through pipes. Such problems arecovered in the Fundamentals Manual on fluid flow. In this section, problems involving rigid bodieswhich are in contact along dry surfaces are considered.The laws of dry friction are best understood by the following experiment. A block of weight W isplaced on a horizontal plane surface (see Figure 9). The forces acting on the block are its weightW and the normal force N of the surface. Since the weight has no horizontal component, the normalforce of the surface also has no horizontal component; the reaction is therefore normal to the surfaceand is represented by N in part (a) of the figure. Suppose now, that a horizontal force P is appliedto the block (see part (b)). If P is small, the block will not move. Some other horizontal force musttherefore exist which balances P. This other force is the static-friction force F, which is actually theresultant of a great number of forces acting over the entire surface of contact between the block andthe plane. The nature of these forces is not known exactly, but it is generally assumed that theseforces are due to the irregularities of the surfaces in contact and also to molecular action.If the force P is increased, the friction force F also increases, continuing to oppose P, until itsmagnitude reaches a certain maximum value F (see part (c) of Figure 9). If P is further increased,Mthe friction force cannot balance it any more, and the block starts sliding. As soon as the block hasbeen set in motion, the magnitude of F drops from F to a lower value F . This is because there isM Kless interpenetration between the irregularities of the surfaces in contact when these surfaces movewith respect to one another. From then on, the block keeps sliding with increasing velocity (i.e., itaccelerates) while the friction force, denoted by F and called the kinetic-friction force, remainsKapproximately constant.
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