INGENIA

RAD-01

Beer–Lambert

Narrow-beam exponential.

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RadiationBeer

Governing equation

I=I0eμxI=I_0 e^{-\mu x}

where

I_0
Incident ()
\mu
Attenuation (1/cm)
x
Depth (cm)
I
Transmitted ()

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-01 — Beer–Lambert) is the form associated with Beer. Working symbols: I0I_0, μ\mu, xx \rightarrow II. Narrow-beam exponential.

Purpose

Purpose: compute II from I0I_0, μ\mu, xx in Radiation physics via I=I0eμxI=I_0 e^{-\mu x} Narrow-beam exponential. 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 I0=1.000I_0 = 1.000\,\mathrm{—}, μ=0.2001/cm\mu = 0.200\,\mathrm{1/cm}, x=5.000cmx = 5.000\,\mathrm{cm}, the governing relation I=I0eμxI=I_0 e^{-\mu x} yields I=0.3679I = 0.3679\,\mathrm{—}. Narrow-beam exponential. Move a slider: the numbers are this situation, not a canned story.

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Inputs

Outputs

  • Transmitted I0.3679
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RAD-01 · decay
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Narration of this film

Narrow-beam exponential.

Narrow-beam exponential.

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