Multiband radiosity method with ray-traced view factors

Ray-traced view factors account for specular reflection and transmission when a model contains specular or transparent surfaces.

Unlike diffuse view factors, ray-traced view factors include the effects of specular reflections and transmissions but exclude diffuse reflections. As a result, when diffuse reflections are neglected, the ray-traced view factors correspond to gray-body view factors.

Ray tracing is performed independently across multiple spectral bands. Each traced ray carries a separate power value for every band. When a ray interacts with a surface, the power in each band is modified according to the material properties for that band. The ray continues if specular reflection or transmission occurs.

A surface can be transmissive in some bands and specularly reflective in others. In these cases, the original ray is split into two rays, and the power is distributed between them according to the material response.

For the single band radiosity method, the emissivity, diffuse reflectivity, and the area of an element are transformed into effective quantities that depend on the specular reflectivity ρs and transmissivity t. The transformations are:

Applying the same transformations to the multiband radiosity equations defines the following quantities.

ρs,kg—band-averaged specular reflectivity of element k in band g, defined as:

tkg—band-averaged transmissivity of element k in band g, defined as:

Akgeff—band-effective Oppenheim area of element k in band g, defined as:

εkgeff—band-effective emissivity of element k in band g, defined as:

Fk-j,g—view factor between element k and element j in energy band g. Because specularity and transmissivity can vary by band, the view factors can also vary by band.

For ray-traced view factors, the heat balance equation for the band Oppenheim element is:

The heat balance equation for the original radiating element is:

where:

The ray-traced non-gray radiosity equations follow the same form as the original single-band and multiband radiosity equations. The primary differences are that each band uses its own set of view factors and uses effective areas and emissivities instead of the actual areas and emissivities.