Star W M
Department of Clinical Physics, Dr. Daniel den Hoed Cancer Centre, Rotterdam, The Netherlands.
Phys Med Biol. 1995 Jan;40(1):1-8. doi: 10.1088/0031-9155/40/1/001.
The radiant energy fluence rate has been calculated at the wall of a spherical cavity, filled with a non-scattering and non-absorbing material, in a scattering and absorbing infinite medium, illuminated by an isotropic point light source at the centre. Two methods have been used: first, diffusion theory for a spherical geometry; second, integrating sphere theory using reflection factors obtained from diffusion theory for a plane semi-infinite medium illuminated by either a broad collimated perpendicularly incident beam or a broad diffuse incident beam. The two methods give identical results if the condition for the validity of the diffusion approximation is satisfied, that is mu(a) << mu(s) (mu(a) = optical absorption coefficient, mu(s) = scattering coefficient) and if also mu(eff)r1 >> 1, where r1 is the radius of the cavity and mu(eff) is the effective optical attenuation coefficient of the medium. Under the same conditions, the two methods also give identical results when the refractive index of the medium is larger than the refractive index of the material in the cavity. A numerical estimate using optical properties of human bladder indicates that the conditions for validity of the integrating sphere approach are nearly satisfied in whole-bladder photodynamic therapy.
已计算出在充满非散射和非吸收性材料的球形腔壁处的辐射能注量率,该球形腔处于散射和吸收性无限介质中,并由位于中心的各向同性点光源照射。使用了两种方法:第一,球形几何结构的扩散理论;第二,积分球理论,该理论使用从平面半无限介质的扩散理论获得的反射因子,该平面半无限介质由宽准直垂直入射光束或宽漫射入射光束照射。如果满足扩散近似有效性的条件,即μ(a) << μ(s)(μ(a) = 光吸收系数,μ(s) = 散射系数),并且如果μ(eff)r1 >> 1,其中r1是腔的半径,μ(eff)是介质的有效光衰减系数,则这两种方法给出相同的结果。在相同条件下,当介质的折射率大于腔内材料的折射率时,这两种方法也给出相同的结果。使用人膀胱光学特性的数值估计表明,在全膀胱光动力治疗中,积分球方法有效性的条件几乎得到满足。