| Problem: Show that in a nuclear reaction of the type below
the nuclear disintegration energy (Q value) is given by
where the kinetic energies Ei are << Mic2 and M3 represents the light particle.
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| Problem: (a) Show that in elastic collisions between two particles m1 and m2, with one particle initially at rest, the fractional energy loss of the moving particle is given by
where q is the scattering angle in the center of mass frame.
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| Problem: A fixed force center scatters a particle of mass m and initial velocity u0 according to the force law F(r)=k/r3. Determine the differential scattering cross section.
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| Problem: A particle of mass m moves under a central repulsive force F(r)=km/r3. At its distance of closest approach r0 it has speed v0. (a) Find the orbital equation r(q) for the
particle motion, evaluating constants in terms of r0 and v0.
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| Problem: An excited, very heavy, non-relativistic particle traveling at speed v0, in the z-direction decays by emitting a light particle of mass m (also non-relativistic) at a precise speed vc, at an angle qc, in the rest frame of the emitter. (a) At what corresponding angle qL does an emitted particle of a corresponding speed vL emerge in the laboratory frame? (b) If the angular distribution of such events is isotropic in the rest frame of
the emitter, i.e. if all angles of emission qc
are equally probable in the rest frame of the emitter, what is the angular distribution in
the laboratory frame? (c) Show that when v0>vc there is a maximum angle
of emission qL, which is given by
sinqLmax=vc/v0. (d) Make a qualitative sketch
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