Test particle

In

Classical gravity

The easiest case for the application of a test particle arises in Newtonian gravity. The general expression for the gravitational force between any two point masses ${\displaystyle m_{1}}$ and ${\displaystyle m_{2}}$ is:

${\displaystyle F=-G{\frac {m_{1}m_{2}}{|\mathbf {r} _{1}-\mathbf {r} _{2}|^{2}}}}$,

where ${\displaystyle \mathbf {r} _{1}}$ and ${\displaystyle \mathbf {r} _{2}}$ represent the position of each particle in space. In the general solution for this equation, both masses rotate around their center of mass R, in this specific case:^[1]

${\displaystyle \mathbf {R} ={\frac {m_{1}\mathbf {r} _{1}+m_{2}\mathbf {r} _{2}}{m_{1}+m_{2}}}}$.

In the case where one of the masses is much larger than the other (${\displaystyle m_{1}\gg m_{2}}$), one can assume that the smaller mass moves as a test particle in a gravitational field generated by the larger mass, which does not accelerate. We can define the gravitational field as

${\displaystyle \mathbf {g} (r)=-{\frac {Gm_{1}}{r^{2}}}{\hat {r}}}$,

with ${\displaystyle r}$ as the distance between the massive object and the test particle, and ${\displaystyle {\hat {r}}}$ is the unit vector in the direction going from the massive object to the test mass. Newton's second law of motion of the smaller mass reduces to

${\displaystyle \mathbf {a} (r)={\frac {F}{m_{2}}}{\hat {r}}=\mathbf {g} (r)}$,

and thus only contains one variable, for which the solution can be calculated more easily. This approach gives very good approximations for many practical problems, e.g. the orbits of

In simulations with electric fields the most important characteristics of a test particle is its electric charge and its mass. In this situation it is often referred to as a test charge.

Similar to the case of classical gravitation, the electric field created by a point charge q is defined by

${\displaystyle {\textbf {E}}=k{\frac {q}{r^{2}}}{\hat {r}}}$,

where k is the

Multiplying this field by a test charge ${\displaystyle q_{\textrm {test}}}$ gives an electric force (Coulomb's law) exerted by the field on a test charge. Note that both the force and the electric field are vector quantities, so a positive test charge will experience a force in the direction of the electric field.

General relativity

In metric theories of gravitation, particularly general relativity, a test particle is an idealized model of a small object whose mass is so small that it does not appreciably disturb the ambient gravitational field.

According to the