Force field (physics)
Appearance
In [[[physics]] a Force Field is a special kind of vector field that models the intensity of a non-contact force at various positions in space-time. The term appears to have been coined by Michael Faraday[1].
=Advantages and Restrictions
An important point to remember when employing force fields is that the vector field in question does not exist. It is a map of the vectors which would exist, were a particle in that location in that moment; this kind of mathematical tool is called a Kuhnian construct. The force field is linked inseparably from the lines of force one object exerts on another object or a collection of other objects. The force field is simple to collection of many of these lines in one location.
Examples of force fields
- A local Newtonian gravitational field near Earth ground typically consists of a uniform array of vectors pointing in one direction---downwards, towards the ground; its force field is represented by the Cartesian vector , where points in a direction away from the ground, and m refers to the mass, and g refers to the acceleration due to gravity.
- A global Gravitational field consists of a spherical array of vectors pointing towards the center of gravity. Its classical force field, in spherical coordinates, is represented by the vector, , which is just Newton's Law of Gravity, with the radial unit vector pointing towards the origin of the sphere (center of the Earth).
- A conservative Electric field has an electric charge (or a smeared plum pudding of electric charges) as its source object. In the case of the point charges, the force field is represented by , where is the position vector that represents the straightest line between the source charge and the other charge.
- A static Magnetic field has a magnetic charge (a magnetic monopole or a charge distribution).
See also
- ^ J. Chem. Soc., Faraday Trans., 1996, 92, 353 - 362, DOI: 10.1039/FT9969200353