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Stopping Power Due to Ionization and Excitation

It was mentioned earlier that most of the interactions of a charged particle involve the particle and atomic electrons. If the mass of the electron is taken as 1, then the masses of the other common heavy charged particles are the [Pg.124]

Electron mass = 1 Proton mass 1840 Deuteron mass = 2(1840) [Pg.125]

N = number of atoms/m in the material through which the particle moves [Pg.126]

Many different names have been used for the quantity dE/dx names like energy loss, specific energy loss, differential energy loss, or stopping power. In [Pg.126]

As stated earlier, Eqs. 4.2 to 4.4 disregard the effect of forces between atoms and atomic electrons of the attenuating medium. A correction for this density ejfect has been made, but it is small and it will be neglected here. The density effect reduces the stopping power slightly. [Pg.127]


Calculate the stopping power due to ionization and excitation of a 2-MeV electron moving in water. What is the radiation energy loss rate of this particle What is the total energy radiated ... [Pg.173]


See other pages where Stopping Power Due to Ionization and Excitation is mentioned: [Pg.124]   


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