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Wednesday 14 March 2012

1.3 Basic Concepts


The following concepts and definitions are basic to the study of mechanics, and they should be understood at the outset.
·        Space is the geometric region occupied by the bodies whose positions are described by linear and angular measurements relative to a coordinate system. For three-dimensional problems, three independent coordinates are required. For two dimensional problems, only two coordinates are required.
·        Time is the measure of succession of events and is a basic quantity in dynamics. Time is not directly involved in the analysis of statics problem.
·        Mass is a measure of the inertia of a body, which is resistance to a change of velocity. Mass can also be thought of as the quantity of matter in a body. The mass of a body affects the gravitational attraction force between it and other bodies. This force appears in many applications of statics.
·        Force is the action of body on another.A force tends to move a body in the direction of its action. The action of a force is characterized by it magnitude, by the direction of its action, and by the point of its application.
·        Idealizations or Models are used in mechanics in order to simplify application of theory. A few of the more important idealizations will now be defined. Others that are noteworthy will be discussed at points where they are needed. 
·        A particle has a mass, but size that can be neglected. For example, the size of mars is insignifcant compared to the size of its orbit, and therefore the mars can be modeled as a particle when studying its orbital motion. When a body is idealized as a particle, the principles of mechanics reduce to a rather simplified form since the geometry of the body will not be involved in the analysis of the problem.
·        A rigid-body can be considered as a combination of a large number of particles in which all particles remain at a fixed distance from one another both before and after applying a load. As a result, the material properties of any body that is assumed o be rigid will not have to be considered when analyzing the forces acting on the body. In most cases the actual deformations occuring in structures, machines, mechanisms, and the like are relatively small, and the rigid-body assumption is suitable for analysis.
·        A concentrated force represents the effect of a loading which is assumed to act at a point on a body. We can represent a load by a concentrated force, provided the area over which the load is applied very small compared to the overall size of the body. An example would be the contact force between a wheel and the ground.