Momentum
From Wikipedia, the free encyclopedia
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In a game of pool, momentum is conserved;
that is, if one ball stops dead after the collision, the other ball
will continue away with all the momentum. If the moving ball continues
or is deflected then both balls will carry a portion of the momentum
from the collision,
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Common symbol(s): |
p |
SI unit: |
kg m/s or N s |
In
classical mechanics,
linear momentum or
translational momentum (
pl. momenta;
SI unit
kg m/s, or, equivalently,
N s) is the product of the
mass and
velocity
of an object. For example, a heavy truck moving fast has a large
momentum—it takes a large and prolonged force to get the truck up to
this speed, and it takes a large and prolonged force to bring it to a
stop afterwards. If the truck were lighter, or moving slower, then it
would have less momentum.
Like velocity, linear momentum is a
vector quantity, possessing a direction as well as a magnitude:
Linear momentum is also a
conserved quantity, meaning that if a
closed system is not affected by external forces, its total linear momentum cannot change. In classical mechanics,
conservation of linear momentum is implied by
Newton's laws; but it also holds in
special relativity (with a modified formula) and, with appropriate definitions, a (generalized) linear momentum
conservation law holds in
electrodynamics,
quantum mechanics,
quantum field theory, and
general relativity.
Newtonian mechanics
Momentum has a direction as well as magnitude. Quantities that have
both a magnitude and a direction are known as vector quantities. Because
momentum has a direction, it can be used to predict the resulting
direction of objects after they collide, as well as their speeds. Below,
the basic properties of momentum are described in one dimension. The
vector equations are almost identical to the scalar equations (see
multiple dimensions).
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