Cavity theory is the basis of operation for ionization chambers used in reference dosimetry. Cavity theory relates measured dose in a cavity, such as an ion chamber, to dose at the same point in the medium in absence of the cavity.
Bragg-Gray Cavity Theory
Bragg-Gray (BG) theory relates dose to the medium, Dmed, to dose to the cavity fill gas, Dgas, via the ratio of mass collision stopping powers between the medium and gas, .
All electrons causing ionization in the cavity arise from phantom material
Secondary electron spectrum is unchanged by presence of the cavity
Energy of secondary electrons created inside the cavity are deposited locally
Neglects secondary electrons (delta rays) generated within the cavity as a result of interactions with scattered electrons
Bragg-Gray Limitations
Because of contradictory and non-physical assumptions, Bragg-Gray theory is only an approximate solution for physical systems.
Assumptions 2 and 3 imply a need for a small cavity volume while requirement 4 requires a large volume to collect all electrons. These conditions cannot be met simultaneously.
Requirement 3, that the spectrum be unchanged, would mean that no energy could be collected to rigorously meet this theory. This is generally disregarded as the effect is minimal with a small cavity.
Spencer-Attix Cavity Theory
The Spencer-Attix formulation of cavity theory resolves the issues of the Bragg-Gray so that it applies for small cavities.
Key Point: Bragg-Gray cavity theory provides an approximate theory of operation for ionization but requires contradictory assumptions. Spencer-Attix and Burlin theories improve upon this by assuming that low energy electrons deposit their energy locally.