Classical Electrodynamics · Problem 15.7

Radiating Systems, Multipole Fields and Radiation — John David Jackson

Physics — E&M · bremsstrahlung-nuclear-fission

Problem

Consider the radiation emitted in nuclear fission by the sudden creation of two fragments of charge and mass (Z1e,A1m)(Z_1 e, A_1 m) and (Z2e,A2m)(Z_2 e, A_2 m) recoiling in opposite directions with total c.m.s. kinetic energy EE. Treat the nuclei as point charges and their motion after the very short initial period of acceleration is nonrelativistic, but keep terms up to second order in 1/c1/c, as in Problem 15.1. For simplicity, assume that the fragments move with constant speeds in opposite directions away from the origin for t>0t > 0. The relative speed is cβc\beta. (a) Using the appropriate generalization of Problem 15.1a, show that the intensity of radiation per unit solid angle and per unit photon energy in the c.m. system is d2Id(ℏω) dΩ=αβ2sin⁡2θ4π2∣p+qβcos⁡θ∣2\frac{d^2I}{d(\hbar\omega)\, d\Omega} = \frac{\alpha\beta^2\sin^2\theta}{4\pi^2}|p + q\beta\cos\theta|^2 where θ\theta is the angle between the line of recoil and the direction of observation, and α=e2ℏc;p=Z1A2−Z2A1A1+A2;q=Z1A22+Z2A12(A1+A2)2\alpha = \frac{e^2}{\hbar c}; \qquad p = \frac{Z_1 A_2 - Z_2 A_1}{A_1+A_2}; \qquad q = \frac{Z_1 A_2^2 + Z_2 A_1^2}{(A_1+A_2)^2} Show that the radiated energy per unit photon energy is dId(ℏω)=2αβ23π(p2+β2q25)\frac{dI}{d(\hbar\omega)} = \frac{2\alpha\beta^2}{3\pi}\left(p^2 + \frac{\beta^2 q^2}{5}\right) where the first term is the electric dipole and the second the quadrupole radiation. (b) As an example of the asymmetric fission of 235{}^{235}U by thermal neutrons, take Z1=36Z_1 = 36, A1=95A_1 = 95 (krypton), Z2=56Z_2 = 56, A2=138A_2 = 138 (barium) (three neutrons are emitted during fission), with E=170E = 170 MeV and mc2=931.5mc^2 = 931.5 MeV. What are the values of p2p^2 and q2q^2? Determine the total amount of energy (in MeV) radiated by this ``inner bremsstrahlung'' process, with the substitution β2→β2(1−ℏω/E)\beta^2\to\beta^2(1-\hbar\omega/E), as a crude way to incorporate conservation of energy. What are the relative amounts of energy radiated in the dipole and quadrupole modes? In actual fission, roughly 7 MeV of electromagnetic energy is radiated within 10−810^{-8} s. How does your estimate compare? If it is much smaller or larger, attempt to explain.

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