Radiation:
Laboratory

All-wave      Incident     Reflected      Transmitted      Laboratory      Infrared

 
Light transmission was also examined in the laboratory using samples taken from ice cores. Sections taken from an ice core are placed inside the white core jacket and the top surface of the core is illuminated with normally incident broadband light. A fiber optic cable is mounted in the housing beneath the jacket, where light transmitted through the core is monitored spectrally. The fiber is coupled to an Ocean Optics spectrophotometer, where the signal is detected. The incident light is monitored by using a second core jacket in “reference mode” with no ice.
The core jacket can be used in two modes. One mode measures single 13 cm long sections of a core. Each section is assumed to have optical properties homogenous in space. The other mode uses a “layer stripping” approach. A core segment as long as 40 cm can be placed in the core jacket and its transmission measured. Obvious changes in the appearance of the ice are used to guide a segmenting process. Sections of core are cut from the top according to this segmentation. The core jacket itself is segmented, allowing for 2-cm increments to be removed from the sample. Each time a layer is removed, the optical transmission is recorded. Finally, the bottom-most 13 cm thick section is used and its transmission recorded. The results from this measurement can be reconstructed to piece together the full vertical profile of scattering in an extended section of ice core.
   
The plot on the right shows a transmission spectra for a 13 cm thick section. Since the ice sample is not horizontally infinite, but rather has finite diameter, a 2D radiative transfer model is used to interpret the observed spectral transmission. The model simulates the effects of the finite core diameter, the optical properties of the interior walls of the core jacket, the refractive boundaries at the top, base, and sides of the ice and the transparent floor that supports the ice sample. Inferences from the model result in determination of a quantitative measure of the scattering within the core.