As described by Picolo (1996), the solid radon source radius b,a large source-diaphragm distance z (relative to b) and collimator a will create a solid measurement angle Ωeff,and in this way, the classic defined solid angle method for absolute alpha counting described by Curtis et al. (1955) can be used. The activity A of the measured solid radon source can be calculated by counting rate C of radon-222 as follows: A=CΩeff/4πwhere, G is defined as geometry factor G=Ωeff/4π And C is the peak counting