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Momentum
Momentum
Momentum is the
Noether charge of translational invariance. As such, even fields as well as
other things can have momentum, not just particles. However, in
curved spacetime which isn't asymptotically
Minkowski, momentum isn't defined at all.
In
physics, momentum is a physical quantity related to the
velocity and
mass
of an object.
In
classical mechanics, momentum (traditionally written as p)
is defined as the product of
mass
and
velocity. It is thus a
vector quantity.
The
SI
unit of momentum is newton-seconds, which can alternatively be expressed with
the
units kg.m/s.
An
impulse changes the momentum of an object. An impulse is calculated as the
integral of
force with respect to
duration.
-
using the definition of force yields:
-
-
-
I = Δp
See also
angular momentum.
It is commonly believed that the physical laws should be
invariant under
translations. Thus, the definition of momentum was changed when
Einstein formulated
Special relativity so that its magnitude would remain invariant under
relativistic transformations. See
physical conservation law. We now define a vector, called the 4-momentum
thus:
-
[E/c p]
where E is the total energy of the system, and
p is called the "relativistic momentum" defined thus:
-
E = γmc2
-
p = γmv
and
-
.
Setting velocity to zero, one derives the result that objects
have a rest mass which is related by the experession E=mc^2
The "length" of the vector that remains constant is defined
thus:
-
Massless objects such as
photons also carry momentum; the formula is p=E/c,
where E is the
energy the photon carries and c is the
speed of light.
In
quantum mechanics momentum is defined as an
operator on the
wave function. The
Heisenberg uncertainty principle defines limits on how accurately the
momentum and position of a single observable system can be known at once.
A process may be said to gain momentum. The
terminology implies that it requires effort to start such a process, but that it
is relatively easy to keep it going.
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