Relativistic Particle Decay: Momentum Conservation

In summary, when dealing with conservation of momentum in a situation where a particle with mass M at rest decays into two particles a and b, it is important to specify the directions of the momenta. Some authors use bold font to denote a vector and an italic font to denote the length of a vector, while others use no special font for vectors. However, as long as the convention is clear, both equations of pa = -pb and pa = pb are correct.
  • #1
whatisreality
290
1
A particle with mass M a rest decays into two particles a and b.

I know that Ea + Eb = Mc2, from conservation of energy. But I'm pretty confused about signs in the conservation of momentum equation, and I've actually seen two versions!

pa + pb = 0, so

pa = - pb.

But I've also seen pa = pb! I know one is magnitudes and the other takes account of directions. Both are right, but which applies for the situation described above? As in, don't they conflict?
 
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  • #2
Momenta include directions as well as magnitudes, so you need to specify directions. In that case, the correct equation is: ##\vec{p}_a+\vec{p}_b=0## assuming you are in the rest frame of the parent particle.
 
  • #3
Some authors use bold font to denote a vector ##\textbf{p}## and an italic font to denote the length of a vector ##p##. Under this convention, $$
\textbf{p}_a = -\textbf{p}_b
$$implies$$
p_a = p_b
$$Similarly for authors who denote a vector with an overarrow: ##\vec{p}##

And then there are some authors who use no special font for vectors who would say:
$$
p_a = -p_b
$$implies$$
|p_a| = |p_b|
$$
 
  • #4
DrGreg said:
Some authors use bold font to denote a vector ##\textbf{p}## and an italic font to denote the length of a vector ##p##. Under this convention, $$
\textbf{p}_a = -\textbf{p}_b
$$implies$$
p_a = p_b
$$Similarly for authors who denote a vector with an overarrow: ##\vec{p}##

And then there are some authors who use no special font for vectors who would say:
$$
p_a = -p_b
$$implies$$
|p_a| = |p_b|
$$
Oh, they were using bold letters on the website. Thanks, that solves it!
 

FAQ: Relativistic Particle Decay: Momentum Conservation

What is relativistic particle decay?

Relativistic particle decay is a process in which a particle spontaneously transforms into one or more different particles. This process is governed by the principles of relativity, which describe the behavior of particles at high speeds.

How does momentum conservation apply to relativistic particle decay?

Momentum conservation states that the total momentum of a closed system remains constant. In the case of relativistic particle decay, the total momentum of the initial particle(s) must equal the total momentum of the resulting particle(s) in order for this law to hold true.

What is the role of energy in relativistic particle decay?

Energy plays a crucial role in relativistic particle decay. According to Einstein's famous equation E=mc², energy and mass are equivalent and can be converted into one another. In particle decay, the change in mass of the initial particle(s) results in the release of energy as the new particles are created.

Can momentum be conserved in all cases of relativistic particle decay?

No, there are some cases in which momentum cannot be conserved in relativistic particle decay. This can occur when the initial particles are not at rest or when the decay products are not emitted in opposite directions. However, the laws of physics still hold true and other properties such as energy and charge must be conserved.

How is the concept of time dilation related to relativistic particle decay?

Time dilation is a phenomenon in which time appears to pass slower for an observer in motion compared to an observer at rest. This concept is related to relativistic particle decay because the speed of the particles involved in the decay can cause a difference in the perception of time between different observers, further complicating the analysis of the decay process.

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