Momentum in special relativity

In summary, the 4-momentum in special relativity is defined as ##P = m V##, with ##V = dX/d\tau## being the 4-velocity, ##m## the invariant mass, ##\tau## the proper time, and ##X## the coordinates along the world line. The 0-component of the 4-momentum is ##m\gamma c##, which can be identified as the total energy of the object. The energy-momentum triangle is a norm relation for the 4-momentum, with one of the sides representing the 3-momentum of the particle. It is important to distinguish between 3-vectors and 4-vectors in order to avoid confusion.
  • #1
Sobhan
35
0
when studying momentum 4 vectors,i encountered the CT momentum which is MC.can some explain where has this come from?
 
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  • #2
In special relativity, the 4-momentum is defined as ##P = m V##, where ##V = dX/d\tau## is the 4-velocity, ##m## the invariant mass, ##\tau## the proper time, and ##X## the coordinates along the world line. It follows directly that the 0-component of the 4-momentum is given by ##m\gamma c##. The classical limit allows the identification of this component with the total energy of the object (as well as of the spatial components with the momentum of the object).
 
  • #3
a question on the energy-momentum triangle:in this triangle one of the sides of it is PC,is this P the momentum in 4 dimensions or 3?
 
  • #4
The energy-momentum triangle is nothing but the norm relation for the 4-momentum. Since the norm of the 4-velocity is 1, the norm of the 4-momentum is always ##m^2 c^2##. With the 4-momentum being ##P = (E/c,\vec p)##, it follows that ##P^2 = E^2/c^2 - \vec p^2 = m^2 c^2##, which may be rewritten as the energy-momentum triangle relation. (So the answer to your question is that the momentum in the triangle is the 3-momentum.)
 
  • #5
Sobhan said:
a question on the energy-momentum triangle:in this triangle one of the sides of it is PC,is this P the momentum in 4 dimensions or 3?
Are you talking about the norm of the four-momentum? If yes, then ## \vec p = (\gamma m_0 c, p_x, p_y, p_z)## and ##|\vec p |^2 = \frac{E^2}{c^2} - p^2 ## where ##p## is the 3-momentum of the particle and ##E## is the particle's total energy (rest+kinetic) in that particular reference frame. (The norm is invariant in all frames.)

EDIT: Orodruin beat me to it. (No surprises there)
 
  • #6
PWiz said:
Are you talking about the norm of the four-momentum? If yes, then ## \vec p = (\gamma m_0 c, p_x, p_y, p_z)##
Generally, I would avoid using a vector arrow for 4-vectors and reserve it for 3-vectors. Things can become very confusing otherwise ...
 
  • #7
Orodruin said:
Generally, I would avoid using a vector arrow for 4-vectors and reserve it for 3-vectors. Things can become very confusing otherwise ...
Okay. It's just that when I think of a vector in a SR, it's almost always a four-vector, so I've sort of got into a habit of putting that arrow :biggrin:
 

1. What is momentum in special relativity?

Momentum in special relativity is a measure of the motion of a particle, taking into account its mass and velocity. It is a fundamental concept in physics and is related to the conservation of energy and momentum.

2. How is momentum calculated in special relativity?

In special relativity, momentum is calculated using the equation p = mv/√(1-v^2/c^2), where p is the momentum, m is the mass of the particle, v is its velocity, and c is the speed of light.

3. What is the difference between momentum in special relativity and classical mechanics?

In classical mechanics, momentum is calculated using the equation p = mv, where v is the velocity. This equation only applies to objects moving at speeds much slower than the speed of light. In special relativity, the equation for momentum takes into account the effects of high speeds and the constant speed of light.

4. Is momentum conserved in special relativity?

Yes, momentum is conserved in special relativity just as it is in classical mechanics. This means that the total momentum of a closed system remains constant, regardless of any internal changes or interactions within the system.

5. How does momentum affect the motion of particles in special relativity?

In special relativity, momentum plays a crucial role in determining the motion of particles. As an object's momentum increases, its mass also increases, making it more difficult for the object to accelerate. This is known as relativistic mass and is a key concept in understanding the behavior of particles at high speeds.

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