A beam of particles scatters classically from a fixed attractive potential well of range

PHYSICS · Multi-part · Fermi University Physics · Mathematical Methods for Physics · Mechanics & Dynamical Systems · Gravitation and central-force motion

Action and Symmetry, Ch Scattering in a central field

Problem

A beam of particles scatters classically from a fixed attractive potential well of range aa. Solving the orbit integral numerically gives the deflection function χ(b)\chi(b) tabulated below, with χ\chi measured so that a negative value means the particle is thrown to the opposite side of the incident direction from a repulsive centre; the physically observed scattering angle is always ∣χ∣|\chi|, between 00 and 180∘180^\circ. b/ab/a: 0, 0.2, 0.4, 0.6, 0.8, 1.0, 1.2, 1.4, 1.6, 2.0 χ\chi (degrees): 180, 150, 100, 40, −10-10, −35-35, −32-32, −22-22, −14-14, −6-6 ((a)) Locate the glory: by linear interpolation between the two bracketing table entries, give the impact parameter (to two significant figures, in units of aa) at which χ(b)\chi(b) passes through zero, and the observed angle there. ((b)) Locate the rainbow: from the table, give the impact parameter and observed angle at the stationary point of χ(b)\chi(b). ((c)) Explain in one or two sentences why dσ/dΩ=(b/sin⁡χ)∣db/dχ∣\mathrm{d}\sigma/\mathrm{d}\Omega=(b/\sin\chi)|\mathrm{d}b/\mathrm{d}\chi| diverges at each of these two impact parameters, and why a real detector of finite solid angle nonetheless records a finite count there.

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