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Forces and Dynamics2.2.1 Calculate the weight of a body using the expression W = mg. In general terms one can describe any force as 'the cause of a deformation or a velocity change'. A force is a vector quantity and the SI units for the measurement of force are Newton’s (N).
Weight W = mg m - The mass of the body measured in kilograms (kg) g - the gravitational field strength of the earth which is measured in Newton’s per kilogram (N kg-1) or sometimes m s-2. On the surface of the earth g= 9.81 N kg -1. 2.2.2 Identify the forces acting on an object and draw free-body diagrams representing the forces acting.
Tension
Figure 2.2.1 - Tension forces Normal Reaction force: If a body touches another body, there is a reaction force(R) between the two bodies. This force is perpendicular to the body exerting the force:
Figure 2.2.2 - Normal reaction forces Drag Force: Drag forces are forces that oppose the motion of a body through a fluid (gas or liquid). They are directed opposite to the velocity of the body and generally depend on the speed of that body. Higher speed equals higher drag force.
Figure 2.2.3 -Air resistance of a plane
Up thrust:
Figure 2.2.4 - Up thrust equal to weight and up thrust less than weight
Frictional Forces:
Figure 2.2.5 - Frictional forces acting on a body Hooke’s Law: Hooke’s law states that up to the elastic limit, the extension, x of a spring is proportional to the tension force, F. The constant of proportionality k is called the spring constant. SI units of spring constant are N m-1. Mathematically, F∞x F = Kx
Figure 2.2.6 - Hooke's law represented graphically 2.2.3 Determine the resultant force in different situations.The resultant force is the overall force acting on an object when all the individual forces acting on that object have been added together.
In order to determine the resultant force acting upon an object, we need to add the individual forces. Consider figure 2.2.7 below: Figure 2.2.7 shows the free body diagram of an object with three forces acting upon it. In order to determine the resultant force we must add these forces together. This is shown in figure 2.2.8 below:
Figure 2.2.8 shows the resultant force attained through simple vector addition, for more on vector addition see section 1.3.2. |
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