Difference between revisions of "Determining Momentum Components After Collision in CM Frame"
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(Created page with "The energy and total momentum of the Moller and scattered electron remain the same under a rotation in any frame of reference. After the collision, these quantities remain the s…") |
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| + | [[Phase_space_Limiting_Particles|<math>\vartriangleleft </math>]] | ||
| + | [[VanWasshenova_Thesis#Weighted_Isotropic_Distribution_in_Lab_Frame|<math>\triangle </math>]] | ||
| + | [[Theta_Dependent_Components|<math>\vartriangleright </math>]] | ||
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| + | =4.1.3 Determining Momentum Components After Collision in CM Frame= | ||
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The energy and total momentum of the Moller and scattered electron remain the same under a rotation in any frame of reference. After the collision, these quantities remain the same, but the x, y, z components change. | The energy and total momentum of the Moller and scattered electron remain the same under a rotation in any frame of reference. After the collision, these quantities remain the same, but the x, y, z components change. | ||
In this frame, we can cycle through values of theta from 90 to 180 degrees which physically correspond to a stationary electron being impinged by an electron. | In this frame, we can cycle through values of theta from 90 to 180 degrees which physically correspond to a stationary electron being impinged by an electron. | ||
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| + | ---- | ||
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| + | <center><math>\textbf{\underline{Navigation}}</math> | ||
| + | |||
| + | [[Phase_space_Limiting_Particles|<math>\vartriangleleft </math>]] | ||
| + | [[VanWasshenova_Thesis#Weighted_Isotropic_Distribution_in_Lab_Frame|<math>\triangle </math>]] | ||
| + | [[Theta_Dependent_Components|<math>\vartriangleright </math>]] | ||
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| + | </center> | ||
Latest revision as of 14:59, 30 May 2017
4.1.3 Determining Momentum Components After Collision in CM Frame
The energy and total momentum of the Moller and scattered electron remain the same under a rotation in any frame of reference. After the collision, these quantities remain the same, but the x, y, z components change.
In this frame, we can cycle through values of theta from 90 to 180 degrees which physically correspond to a stationary electron being impinged by an electron.