Gravitational Field
Newton's law can be restated into the format of a gravitational field, which can prove to be a useful means of looking at the situation. Instead of calculating the forces between two objects every time, we instead say that an object with mass creates a gravitational field around it. The gravitational field is defined as the force of gravity at a given point divided by the mass of an object at that point, as depicted to the right. In the simplest form, we define a gravitational field as a region in which gravitational force can be experienced. Forces like gravitational force and electromagnetic force work with "action at a distance". As bodies are not in contact, it is conceptualized that force is communicated to bodies through a force field, which operates on the entities brought in its region of influence.
Electromagnetic interaction, which also abides inverse square law like gravitational force, is completely described in terms of field concept. In particular, we would not conceptualize about physical existence of gravitational field unless we refer "general relativity".
A body experiences gravitational force in the presence of another mass. This fact can be thought to be the result of a process in which presence of a one mass modifies the characteristics of the region around itself. In other words, it creates a gravitational field around itself. When another mass enters the region of influence, it experiences gravitational force, which is given by Newton's law of gravitation Field strength, apart from its interpretation for the action at a distance, is a convenient tool to map a region and thereby find the force on a body brought in the field. We can measure gravitational force on a body without reference to other body responsible for gravitational field. The concept of field strength allows us to study gravitational field in terms of the mass of one body and as such relieves us from considering it always in terms of two body system. The effect of one of two bodies is actually represented by its gravitational field strength.
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