Finding CM frame velocity in special relativity

In summary, the velocity of the electron-proton CM system is v2 and the available energy to produce new particles is E1+E2.
  • #1
fayled
177
0

Homework Statement


An electron of energy 10 GeV strikes a proton at rest. What is the velocity of the electron-proton CM system? What energy is available to produce new particles?



Homework Equations


Conservation of momentum and energy,
E2=p2c2+m2c4



The Attempt at a Solution


I'm really not sure where to start - solving for the velocity in classical mechanics is simple but the equations here would be really messy so I think there must be a simple way I'm missing. If the two particles were identical it would be easy... Then once I've got that velocity, then would the sum of the energies in the CM frame before the collision be the energy available to produce new particles in the lab frame - i.e the extra energy in the lab frame goes toward conserving momentum? Any clues would be appreciated, thanks.
 
Physics news on Phys.org
  • #3
fayled said:

Homework Statement


An electron of energy 10 GeV strikes a proton at rest. What is the velocity of the electron-proton CM system? What energy is available to produce new particles?

Homework Equations


Conservation of momentum and energy,
E2=p2c2+m2c4

The Attempt at a Solution


I'm really not sure where to start - solving for the velocity in classical mechanics is simple but the equations here would be really messy so I think there must be a simple way I'm missing. If the two particles were identical it would be easy... Then once I've got that velocity, then would the sum of the energies in the CM frame before the collision be the energy available to produce new particles in the lab frame - i.e the extra energy in the lab frame goes toward conserving momentum? Any clues would be appreciated, thanks.
In the lab frame, say the four-momenta of the electron and proton are given by
\begin{align*}
p_e^\mu &= (E, p) \\
p_p^\mu &= (M, 0)
\end{align*} Let ##\beta=v/c## be the speed of the CM frame. Write down the four-momenta in the CM frame. What do you know about the three-momenta in the CM frame?
 
  • #4
Also have a look at the Mandelstam variables. They are very useful invariants!
 
  • #5
vela said:
In the lab frame, say the four-momenta of the electron and proton are given by
\begin{align*}
p_e^\mu &= (E, p) \\
p_p^\mu &= (M, 0)
\end{align*} Let ##\beta=v/c## be the speed of the CM frame. Write down the four-momenta in the CM frame. What do you know about the three-momenta in the CM frame?

Ok so I think using this approach gives the four momenta in the CM frame as

Pe'=(E1,p') and Pp'=(E2,-p').

I used the fact that if I take the sums of each of the 4 momenta in each frame, then the square of this is invariant between frames so I can equate them to give

(E+M)2-(pc)2=(E1+E2)2

If I can find E2 then I can get the speed of the proton which will be the same as the speed of the CM frame. I just need another relation between E1 and E2 though.
 
  • #6
Use the Lorentz transformation to find expressions for the momenta in the CM frame.
 
  • #7
The additional relation are the on-shell conditions in the CM system
[tex]E_1=\sqrt{m_1^2 c^4 + p_{\text{cm}}^2 c^2}, \quad E_2=\sqrt{m_2^2 c^4 + p_{\text{cm}}^2 c^2}.[/tex]
As I already said, using the four-dimensional invariants (the Mandelstam variables), it's a bit simpler, but that was what you did anyway, be it in somewhat implicit form.

To use the rotation-free Lorentz boost directly is also a nice exercise.
 
  • #8
vanhees71 said:
The additional relation are the on-shell conditions in the CM system
[tex]E_1=\sqrt{m_1^2 c^4 + p_{\text{cm}}^2 c^2}, \quad E_2=\sqrt{m_2^2 c^4 + p_{\text{cm}}^2 c^2}.[/tex]
As I already said, using the four-dimensional invariants (the Mandelstam variables), it's a bit simpler, but that was what you did anyway, be it in somewhat implicit form.

To use the rotation-free Lorentz boost directly is also a nice exercise.

So I managed to find the two energies:

E1=2116.575821MeV (electron) and
E2=2315.110569MeV (proton)

I checked and these two energies do correspond to equal momenta as expected in the CM frame.

The velocities from these are

v1=0.9999999709c (electron) and
v2=0.9142439191c (proton)

So as the proton was at rest in the lab frame, I can deduce the speed of the CM frame is simply v2.

However as a further check, I know the speed of the electron in the lab is velab=0.9999999987c. Thus, by using the relativistic velocity addition formula, I would expect that if I add velab to the negative of the CM frame speed (-v2), using the formula, I would obtain the CM speed of the electron...

Vecm=(0.9999999987c-0.9142439191c)/[1+(0.9999999987x-0.9142439191)]=0.999999971c. So clearly either my answer is wrong (which I can't see how it would be given that the momenta come out as equal) or this isn't a valid check (in which case why)... Thanks.

Finally, the energy available to produce new particles in the CM frame is just E1+E2, so how would that relate to the lab frame? I can find the rest mass of the products in the CM frame and these are the same in the lab frame, so surely the energy available for new particle production is just the rest energy in the CM frame?
 
Last edited:
  • #9
fayled said:
So I managed to find the two energies:

E1=2116.575821MeV (electron) and
E2=2315.110569MeV (proton)
Since you apparently used masses with three significant figures, the digits after decimal points are meaningless. You shouldn't be writing them down just because it's what your calculator spit out.

I checked and these two energies do correspond to equal momenta as expected in the CM frame.

The velocities from these are

v1=0.9999999709c (electron) and
v2=0.9142439191c (proton)

So as the proton was at rest in the lab frame, I can deduce the speed of the CM frame is simply v2.

However as a further check, I know the speed of the electron in the lab is velab=0.9999999987c. Thus, by using the relativistic velocity addition formula, I would expect that if I add velab to the negative of the CM frame speed (-v2), using the formula, I would obtain the CM speed of the electron...

Vecm=(0.9999999987c-0.9142439191c)/[1+(0.9999999987x-0.9142439191)]=0.999999971c. So clearly either my answer is wrong (which I can't see how it would be given that the momenta come out as equal) or this isn't a valid check (in which case why)... Thanks.
The speeds from the two methods match. Why do you think they don't agree?
 
  • #10
vela said:
Since you apparently used masses with three significant figures, the digits after decimal points are meaningless. You shouldn't be writing them down just because it's what your calculator spit out.


The speeds from the two methods match. Why do you think they don't agree?

Yeah I realize that is a bit silly, but not as silly as me failing to see that they agree. That is terrible.

But thanks :)
 

1. What is the CM frame velocity in special relativity?

The CM frame velocity, also known as the center-of-mass frame velocity, is the velocity at which the total momentum of a system is zero. In special relativity, it is the velocity at which the center of mass of a system is at rest.

2. How is the CM frame velocity calculated in special relativity?

The CM frame velocity can be calculated by using the Lorentz transformation equations, which relate the velocities and positions of an event in different reference frames. These equations take into account the effects of time dilation and length contraction in special relativity.

3. Why is finding the CM frame velocity important in special relativity?

Finding the CM frame velocity is important in special relativity because it allows us to understand the motion of a system as a whole, rather than looking at the individual components. It also helps us to understand the relationship between energy and momentum in a system.

4. Can the CM frame velocity be greater than the speed of light?

No, according to the principles of special relativity, the speed of light is the maximum velocity at which any object can travel. Therefore, the CM frame velocity cannot exceed the speed of light.

5. How does the CM frame velocity change in different reference frames?

The CM frame velocity remains constant in all inertial reference frames, as long as the system is not experiencing any external forces. This is one of the fundamental principles of special relativity, known as the principle of relativity.

Similar threads

  • Advanced Physics Homework Help
Replies
2
Views
1K
  • Advanced Physics Homework Help
Replies
4
Views
435
  • Advanced Physics Homework Help
Replies
31
Views
2K
Replies
2
Views
1K
Replies
10
Views
2K
  • Advanced Physics Homework Help
Replies
3
Views
1K
  • Advanced Physics Homework Help
Replies
2
Views
1K
  • Advanced Physics Homework Help
Replies
2
Views
2K
  • Special and General Relativity
Replies
11
Views
1K
Back
Top