Momentum Guide, Meaning , Facts, Information and Description
In physics, momentum is a physical quantity related to the velocity and mass of an object.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 is not asymptotically Minkowski, momentum isn't defined at all.
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2 Momentum in relativistic mechanics 3 Momentum in quantum mechanics 4 Origin of Momentum 5 Figurative use 6 See also |
In classical mechanics, momentum (traditionally written as p) is defined as the product of mass and velocity. It is thus a vector quantity.
Momentum in classical mechanics
Impulse
The change in momentum, called the impulse, is equal to force times the change in time.
An impulse changes the momentum of an object. An impulse is calculated as the integral of force with respect to duration.
It is commonly believed that the physical laws should be invariant under translationss. 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:
The "length" of the vector that remains constant is defined thus:
Momentum in relativistic mechanics
where E is the total energy of the system, and p is called the "relativistic momentum" defined thus:
where
Setting velocity to zero, one derives the result that objects have a rest mass which is related by the expression
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. In quantum mechanics position and momentum are interchangeble.
For a single particle with no electric charge and no spin, the momentum operator can be written in the position basis as
Momentum in quantum mechanics
where is the gradient operator. This is a commonly encountered form of the momentum operator, though not the most general one.
Momentum arises from the condition that an experiment must give the same results regardless of the position or velocity of the observer. More formally it is the requirement of invariance under translation. Classical momentum is the result of the invariance of translation in three dimensions. Relativistic momentum as proposed by Albert Einstein arises from the invariance of Four-vectors under lorentzian translation. These Four-vectors appear spontaneously in the Green's function from Quantum field theory.Origin of Momentum
