You have seen that each firing sequence can result in a different
charged particle antiparticle pair being formed. The particles are colour coded; it is
your task to identify them by determining their rest masses.
The
relativistic equation connecting momentum, magnetic field and radius is:
|
(units: GeV/c) |
(1) |
Derivation
You should use this equation to determine the momentum of your particle by
making measurements of the radius of curvature of its track.(explanation
of radius calculation).
|
(2) |
where E is the total energy of the particle (kinetic plus rest energy) and
m0 is the rest mass. We can see that for a particle at rest
(p = 0) this
equation reduces to the familiar, E = m0c2.
Because energy is conserved, the total energy before
annihilation equals the total energy after annihilation. In our case,
before annihilation, the electron and positron each have an energy equal
to the beam energy, therefore the total energy of the system is twice this
amount. After annihilation, when a particle-antiparticle pair are formed,
each particle takes half of the available energy: equal to the original
beam energy. Therefore in equation (2), E
= Incident beam energy.
We now know both the energy and momentum of each
particle in the charged particle pair. Equation (2) can be rearranged to
determine their rest masses:
|
(3) |
The computer selects, at random, from four charged particle
pairs, shown below with their rest masses:
proton-antiproton (p,
anti-p)
= 0.938 GeV/c2
kaon+, kaon-
(K+, K-)
= 0.494 GeV/c2
pion+, pion- (π+,
π-) =
0.140 GeV/c2
muon+, muon (μ+, μ-)
= 0.106 GeV/c2 |
Run the experiment several times until you have produced
and identified all four particle antiparticle pairs.
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