Classical Electrodynamics · Problem 10.18

Radiating Systems, Multipole Fields and Radiation — John David Jackson

Physics — E&M · diffraction-small-circular-hole-bethe

Problem

Discuss the diffraction due to a small, circular hole of radius aa in a flat, perfectly conducting sheet, assuming that ka≪1ka \ll 1. (a) If the fields near the screen on the incident side are normal E0e−iωt\mathbf{E}_0 e^{-i\omega t} and tangential B0e−iωt\mathbf{B}_0 e^{-i\omega t}, show that the diffracted electric field in the Fraunhofer zone is E=eikr−iωt3πr k2a3[2ckk×B0+kk×(E0×kk)]\mathbf{E} = \frac{e^{ikr-i\omega t}}{3\pi r}\,k^2 a^3\left[2c\frac{\mathbf{k}}{k}\times\mathbf{B}_0 + \frac{\mathbf{k}}{k}\times\left(\mathbf{E}_0\times\frac{\mathbf{k}}{k}\right)\right] where k\mathbf{k} is the wave vector in the direction of observation. (b) Determine the angular distribution of the diffracted radiation and show that the total power transmitted through the hole is P=227πZ0 k4a6(4c2B02+E02)P = \frac{2}{27\pi Z_0}\,k^4 a^6(4c^2 B_0^2 + E_0^2)

Related theory

Browse the problem library