Force field (physics)
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For other uses, see Force field.
Originally a term coined by Michael Faraday to provide an intuitive paradigm, but theoretical construct (in the Kuhnian sense), for the behavior of electromagnetic fields, the term force field refers to the lines of force one object (the "source object") exerts on another object or a collection of other objects. An object might be a mass particle or an electric or magnetic charge, for example. The lines do not have to be straight, in the Euclidean geometry case, but may be curved. Faraday called these theoretical connections between objects lines of force because the objects are most directly connected to the source object along this line. A conservative force field is a special kind of vector field that can be represented as the gradient of a potential. Note that a force field does not exist in reality, per se, but it is really a Kuhnian construct that allows scientists to visualize the effects of objects on other objects; in other words, it makes the math easy. Examples of force fields
, where Failed to parse (Missing texvc executable; please see math/README to configure.): \hat{z} points in a direction away from the ground, and m refers to the mass, and g refers to the acceleration due to gravity.
, which is just Newton's Law of Gravity, with the radial unit Failed to parse (Missing texvc executable; please see math/README to configure.): \hat{r} vector pointing towards the origin of the sphere (center of the Earth).
, where Failed to parse (Missing texvc executable; please see math/README to configure.): \vec{R} is the position vector that represents the straightest line between the source charge and the other charge.
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