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in a Nuclear Force Field |
This material is to show the trajectory of a particle subject to a potential of the form
This is the potential for a force carried by particles which decay; as do the π mesons, the carriers of the nuclear force.
A particle moving in a central force field characterized by a potential function V(r) conserves total energy and angular momentum. The conservation of angular momentum q with respect to the center of the force field requires that
be constant. This may be solved for (dθ/dt) and the result substituted into the energy equation to obtain
The ± comes from taking the square root. The equation for the orbit has an upper and lower branch which meet in tangency at the upper and lower limits for r.
The limits on r are established by finding the roots of
For the nuclear force potential V(r) = − H∫_{r}^{∞}(e^{-λs}/s²)ds this reduces to
It is worthwhile to change the variable of integration from s to z=λs. Thus the equations becomes
Now it is desirable to divide through the equation by Hλ to make it nondimensional; i.e.,
Furthermore it is worthwhile to transform the variable in this equation to x=λr. Thus
The angular momentum q is quantized; i.e., q=nh, where n is an integer and
h is Planck's constant divided by 2π. The value of h
is 1.05457×10^{-34} kg m²/s. Thus if q=h then
q²=1.1212×10^{-68} kg^{2} m^{4}/s^{2}. The mass
of the neutron is 1.6749×10^{-27} kg so q²/m is
6.64×10^{-42} kg m^{4}/s^{2}.
The value of λ is 1/(1.522×10^{-15} m^{-1}
and thus q²λ/m is 4.36268×10^{-27} kg m^{3}/s^{2}
An estimate of H is 1.92570×10^{-25} kg*m^{3}/s^{2}. Therefore q²λ/(Hm) is 2.2655×10^{-2}=1/44.14, a dimensionless number.
(To be continued.)
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