INGENIA

RAD-32

CSDA range

Straight-ahead slowing down.

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RadiationCSDA

Governing equation

R=E/(−dE/dx)R=E/(-dE/dx)

E∈[0.1,200]E \in \left[0.1, 200\right]

where

E
Energy (MeV)
-dE/dx
Stopping (MeV/cm)
R
Range (cm)

The figure, part by part

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RAD-32 · dose
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①

Governing law — red

R=E/(−dE/dx)R=E/(-dE/dx)

E∈[0.1,200]E \in \left[0.1, 200\right]

E=0.1E = 0.1R=0.02R = 0.02

②

Domain of the variable — blue

Emin⁡=0.1,Emax⁡=200E_{\min} = 0.1,\quad E_{\max} = 200

E∈[0.1,200]E \in \left[0.1, 200\right]

E=0.1E = 0.1E=0.1E = 0.1

③

Response curve — green

R=E/(−dE/dx)R=E/(-dE/dx)

E∈[0.1,200]E \in \left[0.1, 200\right]

E=0.1E = 0.1R=0.02R = 0.02

④

Rate of change — amber

dRdE\frac{\mathrm{d}R}{\mathrm{d}E}

E∈[0.1,200]E \in \left[0.1, 200\right]

E=1.357E = 1.357R′=0.2R^{\prime} = 0.2

Lecture brief

Historical brief

Beer attenuation, Compton (1923), Klein–Nishina, Bragg–Gray cavity and KERMA are the transport of photons and charged particles in matter. The sheets compute fluence, kerma and stopping. This sheet (RAD-32 — CSDA range) is the form associated with CSDA. Working symbols: EE, −dE/dx-dE/dx →\rightarrow RR. Straight-ahead slowing down.

Purpose

Purpose: compute RR from EE, −dE/dx-dE/dx in Radiation physics via R=E/(−dE/dx)R=E/(-dE/dx) Straight-ahead slowing down. Use it when a real radiation physics question must be answered in SI before a code check.

Live realistic example

In symbols

Live case. Given E=10.000 MeVE = 10.000\,\mathrm{MeV}, −dE/dx=5.000 MeV/cm-dE/dx = 5.000\,\mathrm{MeV/cm}, the governing relation R=E/(−dE/dx)R=E/(-dE/dx) yields R=2.000 cmR = 2.000\,\mathrm{cm}. Straight-ahead slowing down. Move a slider: the numbers are this situation, not a canned story.

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Inputs

Outputs

  • Range R2.000 cm
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RAD-32 · dose
00:0 / 00:08

Narration of this film

Straight-ahead slowing down.

Straight-ahead slowing down.

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