Finding the energy and momenta of massless particles

In summary, a pion spontaneously decays into a muon and an antineutrino, with the antineutrino having a mass no greater than 190 keV and possibly being zero. Using the equations E=pc and E^2=(pc)^2+(mc^2)^2, the energies and momenta of the muon and antineutrino can be calculated if the antineutrino's mass is known. The pion's mass is given, and the muon's mass is known. By setting the energies and momenta of the muon and antineutrino equal to each other and solving the resulting equations, the energies for both particles can be determined.
  • #1
Benzoate
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0

Homework Statement


A pion spontaneously decays into a muon and an antineutrino according to pion^1- => muon^1- +antineutrino.. Current experimental evidence indicates that the mass m of the antineutrino is no greater than about 190 keV and may , in fact, be zero. Assuming that the pion decays at rest in the laboratory , compute the energies and momenta of the muon and muon anti-neutrino a) if the mass of the anti-neutrino is zero and b) if its mass is 190 keV . The mass of the pion is 139.56755 MeV/c^2 and the mass of the muon is 105.65839 MeV/c^2

Homework Equations



E=pc when (m=0)
E^2=(pc)^2 +(mc)^2

E(pion)=E(muon)+E(antineutrino)
p(pion)=p(muon)+E(antineutrino)

The Attempt at a Solution



For part a) since the mass of the anti-neutrino is zero , I apply use the equation E=pc to find the momentum and the Energy for both the muon and anti neutrino particles. To Find E(muon), E(muon)=E(pion)-E(antineutrino) = m(pion)*c^2 - m(antineutrino)*c^2= (139.56755 MeV/c^2 )*c^2 - (105.65839 MeV/c^2)(c^2)= 39.9092 MeV => (E(muon)^2)/c^2= c^2((p(muon))^2) +(m(muon))^2, c^2 cancel out and so I'm left with (p(muon))^2 = (E(muon))^2-(m(muon))^2) => p(muon)=sqrt((E(muon))^2-(m(muon))^2) ). I don't understand how to obtain the momentum and energy of the neutrino .
 
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  • #2
p(pion)=p(muon)+p(antineutrino)

0 = p(muon)+p(antineutrino)

p(antineutrino) = - p(muon)

It is important to remember that in E = pc, p is the magnitude of the momentum... so as not to be confused by the minus signs.

assume p(muon) is towards the right and positive...

E(pion)=E(muon)+E(antineutrino) (1)

now using the equation: E^2 = (pc)^2 + (mc^2)^2, what is E(pion), E(muon) and E(antineutrino). You can get E(muon) and E(antineutrino) in terms of p(muon).

plug in all 3 into equation (1), and then solve for p(muon). Remember that E(antineutrino) is not just m(antineutrino)*c^2, because the antineutrino is not at rest.
 
  • #3
learningphysics said:
p(pion)=p(muon)+p(antineutrino)

0 = p(muon)+p(antineutrino)

p(antineutrino) = - p(muon)

It is important to remember that in E = pc, p is the magnitude of the momentum... so as not to be confused by the minus signs.

assume p(muon) is towards the right and positive...

E(pion)=E(muon)+E(antineutrino) (1)

now using the equation: E^2 = (pc)^2 + (mc^2)^2, what is E(pion), E(muon) and E(antineutrino). You can get E(muon) and E(antineutrino) in terms of p(muon).

plug in all 3 into equation (1), and then solve for p(muon). Remember that E(antineutrino) is not just m(antineutrino)*c^2, because the antineutrino is not at rest.

What equation is equation(1)?
 
  • #4
Benzoate said:
What equation is equation(1)?

It's conservation of energy.
 
  • #5
learningphysics said:
p(pion)=p(muon)+p(antineutrino)

0 = p(muon)+p(antineutrino)

p(antineutrino) = - p(muon)

It is important to remember that in E = pc, p is the magnitude of the momentum... so as not to be confused by the minus signs.

assume p(muon) is towards the right and positive...



E(pion)=E(muon)+E(antineutrino) (1)

now using the equation: E^2 = (pc)^2 + (mc^2)^2, what is E(pion), E(muon) and E(antineutrino). You can get E(muon) and E(antineutrino) in terms of p(muon).

plug in all 3 into equation (1), and then solve for p(muon). Remember that E(antineutrino) is not just m(antineutrino)*c^2, because the antineutrino is not at rest.

So then , E(muon)=(p(muon)*c)
and E^2(anti-neutrino)=(-p(muon)*c)^2 +(m(anti-neutrino)*c^2)^2=E(anti-neutrino)=sqrt((-p(muon)*c)^2 +(m(anti-neutrino)*c^2)^2). Therefore, E(pion)=E(muon)+E(neutrino)=> E(pion)= (p(muon)*c)+(sqrt((-p(muon)*c)^2+(m(anti-neutrino)*c^2)^2). Now I've run into a dilemma: How do I solved for E(pion) if all relevant terms are suppose to be in terms of p(muon)? Why wouldn't the energy of a pion be zero since it decays at rest? since I'm given the mass of the pion in the problem , would the Energy of a pion be : E(pion)=m(pion)*c^2 since the pion particle decays at rest?
 
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  • #6
please somebody, answer my last response
 
  • #7
I can't respond, because I can't make any sense out of it. I suspect other people feel the same way. E(muon)=c*p(muon) is only ok if the muon is massless. And it's not. And then it gets worse. Can you listen to what learningphysics is trying to tell you and clean that mess up?
 
  • #8
Dick said:
I can't respond, because I can't make any sense out of it. I suspect other people feel the same way. E(muon)=c*p(muon) is only ok if the muon is massless. And it's not. And then it gets worse. Can you listen to what learningphysics is trying to tell you and clean that mess up?

Okay, to find E(pion), should I assume that E(pion)=m(pion)*c^2., since the pion particle is at rest, right?

I know , p(antineutrino)=-p(muon).

To find E(anti-neutrino) , I used the equation E^2=(pc)^2 +(mc^2)^2. Therefore, E=sqrt((-p(muon)*c)^2 +(m(muon)*c^2)^2)

I supposed to find E(muon) , I apply the same equation for Energy that I did for the anti neutrino particle. E^2(muon)=(p(muon)*c)^2 +(m(muon)*c^2)^2.

On second thought, since the mass of the anti neutrino is zero in this case, I don't even need E^2(anti-neutino)=(-p(muon))*c)^2 +(m(anti-neutrino)*c^2)^2. Instead , I can say E(antineutrino)=-p(muon)*c

Therefore, E(pion)=E(antineutrino)+E(muon)=> m(pion)*c^2 = -p(muon)*c +sqrt((p(muon)*c)^2 +(m(muon)*c^2)^2)
 
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  • #9
That's better. Now you didn't lose me till the last line. Let's drop the c's, ok? You can always put them back later. You have E(pi)=E(mu)+E(nu). Yes, E(pi)=m(pi). Since you figured out that the momenta are equal, you have E(mu)^2-m(mu)^2=E(nu)^2-m(nu)^2. So:

m(pi)=E(mu)+E(nu)
E(mu)^2-m(mu)^2=E(nu)^2-m(nu)^2

m(pi) and m(mu) are both known. Once you put in a value of m(nu) (either 0 or 190kev) these are two equations in two unknowns E(mu) and E(nu). Just solve them.
 

1. How do you determine the energy of a massless particle?

The energy of a massless particle can be determined using the famous equation E = mc^2, where c is the speed of light. Since massless particles have no mass, their energy is solely determined by their momentum.

2. What is the relationship between energy and momentum for massless particles?

The energy and momentum of massless particles are directly proportional to each other. This means that as the energy of a massless particle increases, so does its momentum.

3. Can massless particles have momentum?

Yes, massless particles can have momentum. Even though they have no mass, they can still possess energy and therefore have momentum. This is due to the fact that momentum is a product of mass and velocity, and massless particles have a velocity of c (the speed of light).

4. How do you calculate the momentum of a massless particle?

The momentum of a massless particle can be calculated using the formula p = E/c, where p is the momentum and E is the energy. Since massless particles have no mass, this formula simplifies to p = E, meaning that the momentum is equal to the energy of the particle.

5. Can the energy or momentum of a massless particle be negative?

No, the energy and momentum of massless particles cannot be negative. This is because both energy and momentum are scalar quantities, meaning they have only magnitude and no direction. Negative values are associated with direction, which does not apply to massless particles.

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