# An Introduction To Diagrammatic Analysis Of Motion

In physics, work is energy that is transferred from or to an object through the application of force along an elastic force field. In its most simple form, it can be represented as the sum of the elastic force and any external force. This includes strain, friction, buoyancy and other kinds of forces. Work may be performed by an individual, an equipment or both.

Any force that acts on an object will provide a certain amount of work, depending on the magnitude of the force and the distance it has to travel. The magnitude of the force is measured in metres per second, and the distance is in metres. Work can be performed on a moving body in one of two ways: it can act directly, with zero displacement, or indirectly, with some constant displacement. For example, when you apply the force of your weight to a table, the table moves with the amount of work you exert. The potential difference is the difference between the amount of work done to the table and the potential difference between the table and your weight. Potential energy is the entire force component that an object exerts against itself.

To measure the potential energy, we need a law that defines it. This law is called the law of conservation of energy. This law states that the total work done to a system is conserved if the system doesn’t change, i.e., it does not go from zero to one and back to zero again. We can find this law useful in various fields, including mechanics, thermodynamics and engineering. For our purposes here, we will only concern ourselves with the definition of work and its relationship to the concept of time. The relationship between work and time can be defined as follows: Work = time x force/mass

Work is the power exerted on an object when its weight is changed. The size of the object does not have any bearing on this number. What makes work interesting is the relationship between force and distance. Work done to an object in one dimension (i.e., the length) is termed as working energy and work done in another dimension (i.e., the distance traveled) is termed as potential energy.

The relationship between working energy and potential energy is well illustrated by Fig. 4. The top panel shows the location of the object in reference to the center of the earth. In the bottom panel, we show the location of the center of the object in reference to an arrow whose direction of motion points in the x axis.

If the arrow shows an upward direction, then the force is going toward the higher left corner. If the arrow shows an downward direction, then the force is going toward the lower right corner. The direction of the force will always be in the x direction if and only if the actual work done is zero (i.e., the object does not move), and will be in the x direction if and only if the work done is positive (i.e., the object moves toward the origin). The integral formula for the force acting on an object can be written as: F = W + T, where F is the force acting on an object, T is the distance from the center of the earth to the center of the object, and W is the weight of the object.