By W. G. Rees
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Additional info for Physical Principles of Remote Sensing, 2nd Edition (Topics in Remote Sensing)
At the low frequency end of the spectrum, the calculations become more difficult because of the effects of screening of the nucleus by the orbital electrons, and the intensity is found to depend on Z and V separately to some extent. Kirkpatrick and Wiedmann show that the component Ix is in general the dominant one, and that it does not vary greatly for different frequencies within the spectrum. The Kramers expression thus has some degree of validity. 2 v0. Iy at the high energy limit is least important when V/Z2 is large, and becomes progressively more important as this parameter is reduced.
13 substantiate this. Turning back to the data on the angular distribution from very thin targets, we can calculate that the data of Kerscher and Kuhlenkampff, and The efficiency of production of continuous X-radiation 45 that of Honerjager, represent a real approach to the condition of ideal thinness. For example, the 25 nm nickel target used by the former workers is only four times the single elastic scattering thickness at 34keV, and Honerjager's magnesium target (10 nm in thickness) is only one half the single elastic scattering thickness at this electron energy.
4b) The sin20 term gives rise to the familiar polar diagram for dipole radiation. When this is integrated over all angles, we obtain for the total radiated power /, 1= f* 1 2e2f7 N2nr2sin6de = ^~ Jo 4ns0 3c* In the theory of X-ray production the radiation is associated with the slowing down of electrons in the target material. Most of the interactions during the slowing down process are essentially with orbital electrons, giving rise to ionization and energy-loss. But interactions also take place with the coulomb fields of nuclei, and it is supposed in the classical theory that those are associated with large decelerations and consequent radiation.
Physical Principles of Remote Sensing, 2nd Edition (Topics in Remote Sensing) by W. G. Rees