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Table 3.4-4 Infrared molar decadic absorption coefficients organic molecules (Jones and Sandorfy, 1956)

Dir Function:

1n ! 0

Solution The mass absorption coef cient is 17(171)2114 0922 m2/kg The fraction of these b particles that are transmitted is Nt/N0 e 2mt exp[20922 m2/kg (1 1023 m) (27 103 kg/m3)] exp[22489] 0083 The fraction absorbed 10 2 0083 0917 In the distant past, measurements of the attenuation of the b spectrum from a newly discovered isotope were used to identify the energy of the b decay Recently, the attenuation of strong sources has been used to monitor the thickness of materials during manufacturing processes Notice that the monitoring can be continuous, nondestructive, and a physical probe does not need to touch the material being measured The backscattering of energetic electrons from materials is a feature that is extremely rare for heavy charged particles.

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session_id ---------65 66 status --------running suspended command --------------SELECT CREATE DATABASE wait_type -------------NULL PAGEIOLATCH_SH wait_time --------0 6 last_wait_type -------------MISCELLANEOUS PAGEIOLATCH_SH

Backscattering is primarily due to multiple interactions with (heavy) nuclei that signi cantly alter the direction of the incident electron that is enhanced by the fact that two energetic electrons can be created when the incident electron scatters from an atomic electron The coef cient of backscattering is used to quantify the probability that an electron will emerge backwards from a surface that is irradiated with electrons The coef cient is a function of the energy of the incident electron and the atomic number of the absorber Formally, the coef cient is the fraction of time that an electron is emitted from the surface of a material following the entry of an energetic electron The coef cient is approximately 05 for E , 1 MeV electrons in gold, approximately 03, 004, and 01 for copper, aluminum, and carbon, respectively It falls below 0.

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1 for E 10 MeV electrons in gold, below 005 for copper, and to near zero in aluminum and carbon The bremsstrahlung radiation from electron beams has important practical applications even though it is a small contribution to the stopping power Bremsstrahlung forms the basis for operation of X-ray tubes and other controllable high- uence sources of radiation Such devices collide an electron beam with an energy of the order of 10 50 keV with a large electrode, usually made out of a heavy element like tungsten or tantalum The electrons penetrate the electrode and the bulk of their kinetic energy is lost through electron scattering and eventually creates heat However, a small fraction of the incident energy is converted into electromagnetic energy in the X-ray region This is called thick-target bremsstrahlung because the incident electrons are completely stopped inside the material.

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