Calculated effective stopping powers and projected ranges for H, He, C, N and O projectiles (0.05-500 keV) in some elements and materials of dosimetric interest

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Published **1989**
by South Bank Polytechnic in London .

Written in English

- Particles (Nuclear physics).,
- Radiation dosimetry.,
- Stopping power (Nuclear physics).

**Edition Notes**

Includes bibliographical references.

Statement | Ihsan A.M. al-Affan. |

Contributions | Polytechnic of the South Bank. Dept. of Physical Sciences and Scientific Computing. |

Classifications | |
---|---|

LC Classifications | QC794.6.S8 A45 1989 |

The Physical Object | |

Pagination | iv, 170 p. : |

Number of Pages | 170 |

ID Numbers | |

Open Library | OL16014485M |

ISBN 10 | 0951445502 |

The Stopping of Energetic Light Ions in Elemental Matter J. F. Ziegler J. Appl. Phys / Rev. Appl. Phys., 85, () ABSTRACT The formalism for calculating the stopping of energetic light ions (H, He and Li) at energies above 1 MeV/u, has advanced to the point that stopping powers may now be calculated Cited by: On the second hole he is m from the green and wants to hit the ball 90 m and let it run onto the green. He angles the shot low to the ground at. to the horizontal to let the ball roll after impact. On the fourth hole he is 90 m from the green and wants to let the ball drop with a minimum amount of rolling after impact. Here, he angles the Author: William Moebs, Samuel J. Ling, Jeff Sanny. A comprehensive collection of interactive, online ballistics calculators! Exterior Ballistics, Recoil Calculator, Wound Channel Calculator, Stopping Power Calculators (mutiple), Round Ball Weight Calculator, Powder Calculators, and more! A one-stop resource for your technical ballistic data needs. The electronic stopping is chosen to act nonlocally for the projectiles, according to the Lindhard-Scharff formula [7] with correction factors for light ions from recent stopping power compilations [25,26]. An equipartition between local (Oen-Robinson [7]) and nonlocal electronic energy loss is employed for the interaction of target atoms.

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