In
physical theories, a 'test particle' is an idealised model of a small object some of whose physical properties (usually
mass and
size) are assumed to be negligible. The concept of a test particle simplifies some problems, and often provides a good approximation for physical phenomena in a specified
domain of applicability.
In
computer simulations, a 'test particle' is a particle whose movement according to potentials and the particles respective
charge is traced (also called
traced particles) but which does not otherwise interact with the system as other types of
simulation particles usually would. The test particle method can be almost synonymous with a
Monte Carlo method, though as a term it does not necessary involve any randomness, for example with respect to its initial location or velocity.
Classical Gravity
The easiest case for the application of a test particle arises in
Newtonian gravity. The general expression for the gravitational force between two masses
and
is:
:
where
and
represent the position of each particle in space. In the general solution for this equation, both masses rotate around their
center of mass, in this specific case:
:
[ Classical Mechanics, 2nd Ed., Herbert Goldstein, , , Addison-Wesley, , ]
In the case where one of the masses is much larger than the other (
), one can assume than the smaller mass moves as a test particle in a
gravitational field generated by the larger mass, which remains immobile. By defining the gravitational field as
with
as the distance between the two objects, the
equation for the motion of the smaller mass reduces to
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
satellites, whose mass is relatively small compared to that of the
earth.
Test particles in 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
Einstein field equation, the gravitational field is locally coupled not only to the distribution of non-gravitational
mass-energy, but also to the distribution of
momentum and
stress (e.g. pressure, viscous stresses in a
perfect fluid).
In the case of test particles in a
vacuum solution or
electrovacuum solution, this turns out to imply that in addition to the tidal acceleration experienced by small clouds of test particles (spinning or not), ''spinning'' test particles may experience additional
accelerations due to
spin-spin forces.
[ The Motion of Point Particles in Curved Spacetime Poisson, Eric ]
Test particles in plasma physics or electrodynamics
In simulations with
electromagnetic fields the most important characteristics of a 'test particle' is its
electric charge and its
mass. In such simulations the particles are moved with the
Lorentz force
,
where q is the particle's
electric charge, 'v' its
velocity and 'E' and 'B' the electric and magnetic fields, respectively.
See also
★
Papapetrou-Dixon equations
★
Magnetogravitic tensor and the
Bel decomposition of the Riemann tensor
References