Work Done by a Constant Force:
Work
The general form of the work equation is:
The image below shows a box being pulled by a constant force along a horizontal surface and moved a displacment d. The force is applied parallel to the surface. The amount of word done is given by
The image below shows a box being pulled by a constant force along a horizontal surface and moved a displacment d. The force is applied at an angle q to the surface. Only the component of the force (F cos q) parallel to the displacement does work in the direction of the displacemnt. The amount of work done is given by
Here is an example of a situation where a force is applied and no work is done: A man holds a 50 N weight. No work is done (even though he must exert a force to hold the weight) because there is no displacement parallel to the direction of the weight.
Here is an example of a situation where there is a force applied and there is displacement and no work is done against the object's weight: A man walks around the room holding a 50 N weight. The object's weight acts down. For work to be done against the weight there has to be displacement in the direction of the weight (either up or down). There is none so no work is done against the weight. There is work done against friction as the man walks around the room.
It is important to specify whether you are talking about work done by an object or work done on an object. For example, work done by gravity depends upon the vertical height. You can push an object up an incline and the amount of work done by gravity is the same for all angles of the incline.
Conservative forces Forces such as gravity, for which the work done does not depend upon the path taken are called conservative forces.
Nonconservative forces Forces such as friction, for which the work done does depend upon the path taken are called nonconservative forces.
Since work is scalar, a sign convention must be established for work.
Net work The net work done on an object determines its motion. If the net work is zero, the object moves at constant speed or is at rest. The object accelerates if the net work has a value other than zero.
The moon orbiting the earth is an example of when a force is applied and there is no work done. In the figure below, the gravitational force acts inward (it is the source of the centripetal force) and the velocity of the moon is perpendicular to the gravitational force (or in a direction tangent to the circle or orbit). The moon's displacement is in the direction of the velocity vector, perpendicular to the gravitational force. Thus, there is no component of the gravitational force parallel to the displacement and the work done by the gravitational force is zero. Since the net work done by gravity is zero, the moon moves at constant speed.
In the drawing below, F is applied at angle q to the horizontal. The force doing the work is the horizontal component of the force since it is the component that is parallel to the horizontal displacement. In this type of situation, the form of the work equation would be
Joule
Work can be represented graphically. If you plot force vs displacement, the area under the curve represents the work done.
Work Done by a Varying Force:
Calculus application: Integration is used to find the area under a curve. If you integrate this curve, you have found the work done. This is useful when work is done by a varying force. The work done by a varying force in moving an object between two points is equal to the area under the curve between these two points.
In the graph below, the force is changing. The graph shows how the force varies with displacment. If one wanted to know the work done beteen two points (the shaded area of the graph), one would simply find the area under the curve (or the area of the shaded area).
Power rate of doing work.
Since is the product of force times displacement, power can also be expressed in terms of velocity (which is displacement divided by time).
Watts the SI unit of power
Another unit of power is the horsepower. 1 hp = 746 W
Machine A device that changes the force doing the work. A machine multiplies your force, not work. A machine allows you to apply less force, but you apply it over a greater distance. No machine is 100% efficient; there is always work done against friction.
Types of simple machines:
Efficiency can also be expressed in terms of advantage:
Work-Energy Priciple If net work is done on a particle, its speed is changed. The motion of a particle can be related to the net work done using a property called kinetic energy. If you want to change the kinetic energy of a particle, you must do net work on it.
If positive net work is done on an object, its speed (kinetic energy) increases. If negative net work is done on an object, its speed (kinetic energy) decreases. If the net work done on an object is zero, its speed (kinetic energy) remains constant.
Advanced look at the Work/Energy Theorem If the net work done is positive, the kinetic energy of the object increases by this amount of work. If the net work done is negative, the kinetic energy of the object decreases by this amount of work. The work/energy theorem is a useful tool to predict the final speed of an object. Remember, the net force causes an acceleration and the net work is the product of the net force and the displacement.
AP Multiple Choice Questions on Work
AP Free Response Questions on Work