Difference between revisions of "July, 6, 2007 Investigations of Geometry Influence on the Fission Fragments Behaviour"
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- <math>\frac{dE}{dx}</math>=K<math>z^2\frac{Z}{A}</math><math>\frac{1}{\beta^2}</math>[<math>\frac{1}{2}\ln\frac{2m_ec^2\beta^2\gamma^2T_{max}}{I^2}</math> - <math>\beta^2</math> - <math>\frac{\delta}{2}</math>]<br> | - <math>\frac{dE}{dx}</math>=K<math>z^2\frac{Z}{A}</math><math>\frac{1}{\beta^2}</math>[<math>\frac{1}{2}\ln\frac{2m_ec^2\beta^2\gamma^2T_{max}}{I^2}</math> - <math>\beta^2</math> - <math>\frac{\delta}{2}</math>]<br> | ||
| − | <math>\frac{K}{A}</math>0.307075 MeV<math>g^{-1}cm^2</math> | + | <math>\frac{K}{A}</math> = 0.307075 MeV<math>g^{-1} cm^2</math> |
Revision as of 20:55, 6 July 2007
1. Theoretical Calculations
Relativistic charged particles lose energy in matter primarily by ionization. The mean rate of energy loss is given by the Bethe_Bloch equation,
- =K[ - - ]
= 0.307075 MeV